|USFDC Home | USF Electronic Theses and Dissertations||| RSS|
This item is only available as the following downloads:
xml version 1.0 encoding UTF-8 standalone no
record xmlns http:www.loc.govMARC21slim xmlns:xsi http:www.w3.org2001XMLSchema-instance xsi:schemaLocation http:www.loc.govstandardsmarcxmlschemaMARC21slim.xsd
leader nam 2200421Ka 4500
controlfield tag 001 002047316
007 cr mnu|||uuuuu
008 100113s2008 flu s 000 0 eng d
datafield ind1 8 ind2 024
subfield code a E14-SFE0002759
Thin film metal-insulator-metal tunnel junctions for millimeter wave detection
h [electronic resource] /
by Subramanian Krishnan.
[Tampa, Fla] :
b University of South Florida,
Title from PDF of title page.
Document formatted into pages; contains 152 pages.
Dissertation (Ph.D.)--University of South Florida, 2008.
Includes bibliographical references.
Text (Electronic dissertation) in PDF format.
Mode of access: World Wide Web.
System requirements: World Wide Web browser and PDF reader.
Co-advisor: Elias K. Stefanakos, Ph.D.
Co-advisor: Shekhar Bhansali, Ph.D.
ABSTRACT: Millimeter wave imaging systems are the next generation imaging systems being developed for security and surveillance purposes. In this work, thin film metal-insulator-metal (MIM) tunnel junction based detector using Ni-NiO-Cr has been developed for the first time for millimeter wave detection operating at 94 GHz. Extensive process development has been carried out to fabricate the MIM junctions. Arrays of MIM junctions with 1 m contact area and ultra-thin insulator layer of ~3 nanometer have been developed using e-beam lithography and reactive sputtering, respectively. MIM diodes were also fabricated in a bulk-micromachined diaphragm configuration to minimize surface wave loss. DC and millimeter wave measurements were carried out on the fabricated diodes to determine the device characteristics and performance. The current-voltage (I-V) measurements yielded current in the range of few A with significant non-linearity and asymmetry.A maximum sensitivity of 7 V was also obtained from the fabricated diode. These tunnel junctions showed a positive response to millimeter wave signal, with output current in the range of few A. By controlling the input power of the millimeter wave signal, the output current from the device could be varied. Additionally, MIM diodes with 100 m contact area were developed using optical lithography technique. The I-V characteristics of diode demonstrated a uniform behavior, with a sensitivity value of 15 V. Furthermore, the diodes were utilized to observe the effects of post-deposition annealing on the diode I-V behavior. The I-V measurement provided evidence of diode operation up to 350C, with optimal operation at 250C. Finally, the feasibility of using an organic insulator was also investigated. MIM junctions were fabricated with a thin layer of polyaniline using Langmuir-Blodgett deposition process.The electrical characteristics of the polyaniline based MIM junction was determined by evaluating its I-V response. The use of an alternate dielectric proved successful, yielding a significant non-linearity and asymmetry. However, the output current obtained from these junctions was in the order of nano-Amperes. By optimizing the deposition process, the organic MIM junctions can be developed to yield better device characteristics.
Thin film insulator
Millimeter wave detection
x Electrical Engineering
t USF Electronic Theses and Dissertations.
Thin Film Metal Insulator Metal Tunnel Junctions For Millimeter Wave Detection by Subramanian Krishnan A dissertation submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy Department of Electrical Engineering College of Engineering University of South Florida Co Major Professor: Elias K. Stefanakos Ph.D. Co Major Professor: Shekhar Bhansali Ph.D. Yogi D. Goswami, Ph. D. Kenneth A. Buckle, Ph. D. Dennis K. Killinger, Ph. D. Date of Approval: October 29, 2008 Keywords: mim diode, r ectenna, n i n i o c r, t hin film i nsulator, m illimeter w ave d etection Copyright 2008 Subramanian Krishnan
DEDICATION To my parents, brother and my w ife for their unconditional love and support
ACKNOWLEDGEMENT I would like to thank my major professors, Dr. Lee Stefanakos and Dr. Shekhar Bhansali for providing me the opportunity to work on my Masters and continue on for a Doctorate degree. Their ideas and feedback have kept me focused in my research. Dr. Shekhar Bhansali deserves special thanks for all the motivation and support he has provided I have learnt a lot from him both professionally and personally. I would also like to thank Dr. Yogi Goswami for introducing me to the concept of alternate energy conversi on, which has been the backbone for this research. I would like to thank Dr. Ken Buckle and Dr. Dennis Killinger for serv ing as my committee members. T hanks to Dr. Srinivas Katkoori for chairing the dissertation defense. I would a lso like to acknowledge Dr. Weller and Dr. Dunleavy for providing the W band test set up in the Noise lab. Most of the fabrication process an d all materials characterization and testing were carried out at the Nanomaterials and Nanomanufacturing Research Center Thanks to Rob Tufts for maintaining such an excellent facility with his efficient team of engineers (R ich, Jay and Yusuf) and staffs. I am also grateful to Jay Bieber and Dr. Yusuf Emirov for training me in the facility equipments I would like to than k Dr. Bert L gel for showing me the nuances of e beam lithography. I would also like to thank the department and CERC staffs (Becky, Norma, Gayla, Irene, Ginnie and Barbara) for helping with all the academic and administrative tasks.
I would like to acknowled ge and thank Dr Senthil Sambandam for introducing me to thin film deposition s I would also like to thank Kevin Shyam and SP for teaching so much about thin film deposition, lithography and many other lab related equipments. Thanks to Carl and Johnny for keeping the Bio MEMS lab organized and running. I would like to express my regard to Dr. Niranjan Ramgir for constantly encouraging me I cannot forget his sense of humor and audacity. A special t hanks to Praveen for helping me in different walks of my re search at USF I am extremely thankful to Henrry for taking his time out during the weekends to assist me with the RF measurements I would like to thank Jeffy Jiminez for t eaching me the polymer coating technique A big t hank you to Rudran, Joe Register, and Joe Johns for helping me with the diode measurement and characterization. I can never forget our brainstorming sessions about developing "radical" experiments I thoroughly enjoyed mentoring as well as learning several things from them. Thank you Srinath for helping me unwind with our racquetball nights. I wou ld also like to thank all other present and past members of ENB 152. Special mention goes to my friends in Tampa Kaushik, Mahesh, Francis, Tony Vidya and Sandesh. We have bonded so much over the years that I cannot imagine my life in Tampa without them. I am grateful to my friends Shiva, Vasu, Ranjani, Priya, Hari, Vathsan, Srini Suji and Rajesh for their support W ords are not enough to express my appreciation and affection for my beloved wife Lavanya for standing by me patiently and motivating me thr oughout my research and my gratitude to my mother, father and brother I am indebted to my family for their love, support and sacrifice. If not for them, I would not be for what I am today.
i TABLE OF CONTENTS LIST OF TABLES v LIST OF FIGURES v i ABSTRACT xi CHAPTER 1 INTRODUCTION 1 1.1 Thin Film Metal Insulator Metal Junction for Millimeter Wave Detection 1 1.2 Overview of Millimeter Waves 2 1.3 Goals and Objectives 5 1.4 Thesis Organization 6 CHAPTER 2 BACKGROUND 8 2.1 Introduction 8 2.2 Millimeter Wave Detection 10 2.3 Antenna Coupled Detector 16 CHAPTER 3 M ETAL INSULATOR METAL TUNNEL DIODE S 21 3.1 Theory of Operation 22 3.2 Current Voltage Characteristics 26 3.3 Frequency and Area Relationship 30
ii CHAPTER 4 PROCESSING TECHNIQUES 33 4.1 Microfabrication 33 4.1.1 Optical Lithography 33 4.1.2 Electron beam Lithography 36 4.2 Thin Film Deposition 41 4.2.1 Sputtering 41 4.2.2 Reactive Sp uttering 43 4.2.3 Evaporation 44 4.3 Alternate Dielectric Deposition Process 45 CHAPTER 5 DESIGN AND FABRICATION OF MIM DIODES 49 5.1 Design of MIM diode 49 5.1.1 Stacked MIM Design 50 5.1.2 Stepped MIM Design 52 5.2 Material Selection 5 5 5.3 A Typical Fabrication of MIM Diode 58 5.3.1 Substrate Preparation 58 5.3.2 Fabrication of Stacked MIM Structure (100 m 2 Contact Area) 59 5.3.3 Fabrication of Step MIM Structure ( 1 m 2 Contact Area) 61 5.3.4 Fabrication of MIM Diode wi th Polyaniline 67 5.4 Dielectric Deposition technique 68 5.4.1 Nickel Oxide 68 5.4.2 Polyaniline 72
iii 5.5 Comments on Fabrication Procedure 76 CHAPTER 6 RESULTS DC MEASUREMENTS 79 6.1 Experimental I V Characteristics of MIM Diode 79 6.1.1 I V Characteristics of MIM Diode with 100 m 2 Contact Area 79 6.1.2 I V Characteristics of MIM Diode with 1 m 2 Contact Area 84 6.1.3 I V Characteristics of Polymer MIM Diode 88 6.2 Theoretical DC I V Characteristics 90 6.3 Comments on DC Characteristics of MIM Diodes 93 6.4 Temperature dependency of MIM Diodes 95 6.4.1 Electrical Characterization 95 6.4.2 Structural and Morphological Characterization 100 6.5 Thickness dependency of MIM Diodes 109 CHAPTER 7 LOW FREQUENCY AND MI LLIMETER WAVE MEASUREMENTS 113 7.1 Experimental Arrangement 113 7.2 Experimental Results 117 7.2.1 Low Frequency Characteristics of 100 m 2 MIM Diode 117 7.2.2 Low Frequency Characteristics of 1 m 2 MIM Diode 120 7.2.3 Millimeter Wave R esponse of MIM Diode 124 CHAPTER 8 CONLUSION AND FUTURE OUTLOOK 129 8.1 General Comments and Suggestions 130
iv REFERENCES 132 APPENDIX 138 Appendix A: Process Flow for Fabrication o f 100 m 2 MIM Diode 139 Appendix B : Process Flow for Fabrication of 1 m 2 MIM Diode 142 Appendix C: Current Voltage Characteristics of MIM Diode 148 ABOUT THE AUTHOR End Page
v LIST OF TABLES Table 2.1 Thin Film MIM Junctions Developed by Various Research Groups 19 Table 3.1 Work Function of Various Metals Used for Fabricating MIM Diodes 32 Table 5.1 Gas Ratio vs. Roughness and Thickness Estimate of the Dielectric L ayer 71 Table 6.1 Electrical Characteristics of MIM Diode 93 Table 6.2 Comparison of Sensitivity of MIM Diodes Fabricated by CERC with other Re search Groups 112 Table 7.1 Variation in Current with Change in Bias Voltage on 1 m 2 MIM Diode 124
vi LIST OF FIGURES Figure 1 .1 Schematic Illustration of the Concept of mm wave Detection Using an Array of Antenna Coupled MIM Diodes 2 Figure 1.2 Electromagnetic Spectrum Illustrating the Millimeter Wave Regime 3 Figure 1.3 Millimeter Wave Atmospheric Ab sorption for Horizontal Propagation 4 Figure 2.1 Power Radiated by an Object at Room Temperature 9 Figure 2.2 Thermal Radiation Map of a Subject As Seen From an Infrared Imaging System 9 Figure 2.3 Millimeter Wave Image of a Subject by Penetrating Throug h the Clothing 10 Figure 2.4 Schematic Representation of an Active Millimeter Wave Imaging System 14 Figure 2.5 Schematic Illustration of a MIM Diode Fabricated Using Point Contact Configuration 18 Figure 3.1 Schematic Illustration of an Electron Tunnel ing Through a Finite Barrier in a MIM Diode 21 Figure 3.2 Energy Band Diagram of MIM Diode at Zero Bias 22 Figure 3.3 Energy Band Diagram of MIM Diode Showing Barrier Lowering due to Image Force 24
vii Figure 3.4 Effect of Applying Low Voltage s to the Potential B arrier 2 7 Figure 3.5 Effect of Potential Barrier at Intermediate Voltage Ranges 28 Figure 3.6 Effect of Potential Barrier at Very High Voltages 29 Figure 3.7 Theoretical I V Plot of MIM Junctions Operated in the Intermediate Voltage Ranges 30 Figure 4.1 Visual of (a) EVG 620 and (b) Quintel Mask A ligners 34 Figure 4.2 JEOL JSM840 Controlled by Nabity's Nano Pattern Generation System 37 Figure 4.3 Schematic Illustration of JEOL JSM840 38 Figure 4.4 Process Sequence for E beam Lithography 40 Figure 4.5 Sputtering Chamber Used for Depositing MIM L ayers 42 Figure 4.6 Schematic Illustration of a Reactive S putterin g System 44 Figure 4.7 Thermal Evapor ator Used for Fabricating MIM D iodes 45 Figure 4.8 Schematic Illustration of L B Deposition T echnique 46 Figure 4.9 Typical Surface Area Pressure Isotherm Plot of a L B F ilm 47 Figure 5.1 Schematic Representation of (a) Individual MIM Diode Design and (b) Array of Diodes Generated in the Mask L ayout 51 Figure 5.2 Design of Antenna, Diode and Antenna Coupled Diode 52 Figure 5.3 CPW Lines Illustrating the Tra nsition from a Thick to Thin Substrate 54 Figure 5.4 Schematic Illustration of the Cross Section and Top View of MIM Diode 55 Figure 5.5 Process Flow of Stacked MIM D iode 59 Figure 5.6 Process Flow for Step MIM D iode 61
viii Figure 5.7 Etch Set up Developed for Silicon M embra ne E tching 64 Figure 5.8 SEM Micrograph of Silicon Membranes Etched Using TMAH 64 Figure 5.9 Visual Image Showing the Silicon Membranes Etched on a Full Wafer 65 Figure 5.10 SEM Micrograph of a MIM Diode Fabricated with (a) 100 m 2 and (b) 1 m 2 Contact Ar ea 66 Figure 5.11 MIM PANI Process F low 68 Figure 5.12 AFM Micrograph of a Silicon Substrate Deposited with NiO 70 Figure 5.13 SEM Micrograph Showing the Cross Section of a MIM Diode 72 F igure 5.14 Visual of the L B Trough Used for Polyaniline Deposition 73 Figure 5.15 Schematic of a Wilhelmy Plate Balanced in a Langmuir Trough 74 Figure 5.16 Pressure Area I sotherm of PANI 75 Figure 5.17 Profilometer Plot Illustrating the Non Uniformity in Etch Profiles 78 Figure 6.1 Typical I V Characteristics of MIM Diode with 100 m 2 Contact Area 80 Figure 6.2 Distribution of Zero Bias Resistance of 100 m 2 MIM Diode 81 Figure 6.3 Rate of Conductance of MIM D iode with 100 m 2 Contact Area 82 Figure 6.4 Sensitivity of MIM Dio de with 100 m 2 Contact Area 83 Figure 6.5 Distribution of Peak Sensitivity for 100 m 2 MIM Diodes 84 Figure 6.6 Typical I V Characteristics of MIM Diode with 1 m 2 Contact Area 85 Figure 6.7 Distribution of Zero B ias Resistance of 1 m 2 MIM Diode 85 Figure 6.8 Rate of Conductance of MIM Diode with 1 m 2 Contact Area 86
ix Figure 6.9 S ensitivity of 1 m 2 MIM D iode 87 Figure 6.10 Distribution of Peak Sensitivity O btained for 1 m 2 M IM D iodes 87 Figure 6.11 I V C ha racteristics of MIM Diode with Polyaniline I nsulator 88 Figure 6.12 Theoretical I V C urve for s= 3 nm, 1 = 4.5eV and ! = 0.65eV 91 Figure 6.13 Ex perimental and Theoretical I V C haracteristics of MIM Diode 92 Figure 6.14 I V Characteristics of MIM Diode Annealed at D ifferent T emperatures 96 Figure 6.15 Sensitivity of MIM Diode Annealed at Different T emperatures 97 Figure 6.16 Zero Bias Resistance of MIM D iode Anneale d at D ifferent T emperatures 99 Figure 6.17 AFM M icrograph of Samples Annealed at (a) Room Temperature, (b) 250 ¡ C, (c) 350 ¡ C, and (d) 400 ¡ C 102 Figure 6.18 XRD Pattern for NiO Films Deposited Through P lasma Oxidation and A nneale d at Different T emperatures 103 Figure 6.19 TEM Micrograph of MIM diode Annealed at (a) 250¡C and (b) 350¡C 106 Figur e 6.20 TEM Micrograph of MIM Diode A nnealed at 400 ¡ C 106 Figure 6.21 E nergy D ispersive S pectra Sho wing the Diffusion L ength of Annealed M aterials 107 Figure 6.22 I V Characteritics of MIM Diode Deposited with (a) 10 nm, (b) 20 nm and (c) 40 nm NiO 110
x Figure 7. 1 Schematic of the Test Set up Used for M easuring the Low Frequency B ehavior of (a) 100 m 2 and (b) 1m 2 area MIM D iode 114 Figure 7.2 Schematic of the Test Set up U sed for Millimeter Wave Measurement 116 Figure 7.3 Actual Millimete r Wave Test S et up Used to Measure the MIM Diode 116 Figure 7.4 Rectification of 100 m 2 MIM D iode at (a) 100 Hz and (b) 1 KHz 118 Figure 7.5 DC O ut put S ignal of MIM Diode with a Ramp F unction 119 Figure 7.6 AC to DC T esting of the 1 m 2 MIM diode at 200 MHz 121 Figure 7.7 DC R esponse of 1 m 2 Diode with Increase in A mplitude 122 Figure 7.8 Distribution of Output Current for D iodes upon Subjecting to a Millimeter Wave S ignal 125 Figure 7.9 Variation in D C Current with Change in Input Power 126 Figure 7.10 Return Loss of MIM Diode Measured from 75 to 110 GHz 127 Figure C.1 I V Characteristics of Ni NiO Cr MIM Junctions with 100 m 2 Contact Area 148 Figure C.2 I V Characteristics of Ni NiO Cr MIM Junctions with 1 m 2 Contact Area 151 Figure C.3 I V Characteristics of Ni PANI Cr MIM Junctions with 100 m 2 Contact Area 152
xi THIN FILM METAL INSULATOR METAL TUNNEL JUNCTIONS FOR MILLIMETER WAVE DETECTION Subramanian Krishnan ABSTRACT Millimeter wave imaging systems are the next generation imaging system s being developed for security and surveillance purpose s In this work, th in film metal insulator metal (MIM) tunnel junction based detector using Ni NiO Cr has been developed for the first time for millimeter wave detection operating at 94 GHz. Extensive process development has been carried out to fabricate the MIM junction s A rrays of MIM junctions with 1 m 2 contact area and ultra thin insulator laye r of ~3 nm have been developed using e beam l ithography and reactive sputtering, respectively. MIM diodes were also fabricated in a bulk micromachined diaphragm configuration to mi nimize surface wave loss. DC and millimeter wave measurements were carried out on the fabricated diodes to determine the device characteristics and performance. The current voltage (I V) measurements yielde d current in the range of few A with significant non linearity and asymmetry. A maximum sensitivity of 7 V 1 was also obtained from the fabricated diode.
xi i These tunnel junctions showed a positive response to millimeter wave signal, with output current in the range of few A. By controlling the input power of the millimeter wave signal, the output current from the device could be varied. Additionally, MIM diodes with 100 m 2 contact area were developed using optical lithography technique. The I V character istics of diode demonstrated a uniform behavior, with a sensitivity value of 15V 1 Furthermore, the diodes were utilized to observe the effects of post deposition annealing on the diode I V behavior. The I V measurement provided evidence of diode operatio n up to 350¡C, with optimal operation at 250¡C. Finally, the feasibility of using an organic insulator was also investigated. MIM junctions were fabricated with a thin layer of polyaniline using Langmuir Blodgett deposition process. The electrical charact eristics of the polyaniline based MIM junction was determined by evaluating its I V response. The use of an alternate dielectric proved successful, yielding a significant non linearity and asymmetry. However, the output current obtained from these junction s was in the order of nA. By optimizing the deposition process, the organic MIM junctions can be developed to yield better device characteristics.
1 CHAPTER 1 INTRODUCTION 1.1 Thin Film Metal Insulator Metal Junctions for Millimeter Wave Detection Metal Insulator Metal (MIM) junctions are tunnel diodes, which operate on the basis of quantum tunneling phenomenon i.e., when a sufficiently thin barr ier is sandwiched between two electrodes, current can flow between them by means of tunneling. MIM junctions consist of two metal electrodes separated by a very thin barrier and electrons can tunnel through the barrier when a bias is applied. On account of this behavior, MIM diodes were recommended for harmonic mixing and detection when integrated with an antenna   The integrated antenna concept was later extended to other applications such as millimeter (mm) wav e and infrared (IR) detection  due to faster response of these diodes  MIM diodes when coupled with an antenna can absorb the electromagnetic energy from the object emitting the mm wave radiation and convert it to electrical energy. This rectified signal can then be transmitted to an electronic circuit to identify the detected object under o bservation. Several mm wave windows exist in the atmosphere; however the wavelength of interest for the development of mm wave detector is ~3 mm (94 GHz). At this wavelength, the size of the diode is much smaller and is expected to have a faster response. In addition to its faster response, MIM based mm wave detectors provide
2 asymmetric electrical characteristics, device scalability, and wavelength tunability when coupled with an a ntenna. Figure 1.1 illustrates the concept of mm wave detection using an array of antenna coupled MIM diodes. Figure 1.1 : Schematic Illustration of the Concept of mm wave Detection Using an A rra y of Antenna Coupled MIM Diodes. Adapted From  1.2 Overview of Millimeter Waves Millimeter wave refers to the region of the electromagnetic spectrum between mic rowaves and the far infrared. Millimeter waves generally encompass frequencies between 30 and 300 GHz. At these frequencies, the mm wave radiation is well suited for radar and telemetry applications due to its shorter wavelength than microwaves 
3 Figure 1.2 shows the electromagnetic spectrum illustrating the mm wave regime between mi crowaves and IR. Figure 1.2 : Electromagnetic Spectrum Illu strating the Millimeter Wave Regime. From  Millimeter wave radiation is a form of radiated electromagnetic energy obeying the sa me laws as those for visible light, radio waves and X rays  All objects above 0K are expected to emit mm wave radiation and the amount of radiation emitted by a body at a particular w avelength is given by Planck's energy distribution  The boundary between different radiations such as visible, infrared and millimeter waves are not absolute and are segregated primar ily based on the source and detectors that are available and used. Millimeter wave imaging and detection make use of the atmospheric window occurring between 10 mm and 1 mm. In this window the radiation is not reflected or absorbed by the atmosphere and t he atmospheric transmission is the highest. The
4 electromagnetic radiation windows occur, centered at 35, 94, 140, and 220 GHz and the bandwidths available at each of these windows are extremely large, and are approximately equal to 16, 23, 26, and 70 GHz, respectively  These large bandwidths and shorter wavelengths allow for high information rate capability, high resolution for precision tracking, target identificati on in radars, and high sensitivity radiometers than the microwave radars. Figure 1.3 illustrates the main windows occurring in the millimeter wave range  Figure 1.3: Millimeter Wave Atmospheric Absorption for Horizontal P ropagation From  The main characteristic of millimeter wave that makes it suitable for a wide range of application is its ability to penetrate through objects. This noteworthy behavior of the millimeter wave can be used for object detection and imaging using a millimeter wave
5 detector. Additionally, at millimeter wavelengths the atmospheric attenuation due to environmental conditions such as aerosol, dust, smoke, and other contaminants are lesser, making millimeter wave systems ideal for many applications  The short wavelength characteristic of millimeter waves in combination with its interaction with atmospheric constituents and wide operating bandwidths provide many advantages in developing a mm wave detection system. A detailed overview on different techniques used for mm wave detection is presented in the next chapter. 1.3 Goals and Objectives: The primary objective of this research work is to develop thin film MIM tunnel junctions with two different electrodes for mm wave detection. The following goals were ident ified as being pertinent to achieving the objective. (a) To determine a suitable material combination for MIM diodes Materials have to be selected based on its work function. To achieve asymmetrical and non linear electrical characteristics, work functio n difference between two metals should be large. (b) To determine the contact area and processing techniques for fabricating the tunnel junctions In order to develop MIM diodes for utilization as mm wave detectors with faster response, the size of the d etector needs to be small. Also, the fabrication technique should be able to accommodate such a small size. (c) To develop a methodology for depositing thin layers of insulators For the electrons to tunnel, very thin insulator layer needs to be developed with uniformity and minimal roughness.
6 (d) To determine the effect s of dielectric thickness and temperature on the electrical behavior of the diode The electrical characteristics of the diodes depend on various factors. Understanding the diode behavior with respect to those factors will provide more information to develop a robust diode structure. (e) To estimate the performance of the diodes at mm wave frequency The diode characteristics have to be verified for mm wave detection by investigating the AC to DC energy conversion. To accomplish the aforementioned goals, MIM tunnel junctions with Ni NiO Cr were fabricated with 100 m 2 and 1 m 2 cont act area. Optical and e beam lithography techniques were used to fabricate the devices. The electrical characteristics of the diodes were evaluated by subjecting the diodes to dc and mm wave (94GHz) signal. Also, the effect of dielectric thickness on the d iode characteristics was determined by varying deposition parameters. The temperature dependency of the diodes was determined by performing post deposition annealing. Additionally, to determine the feasibility of using an organic insulator layer in MIM jun ctions, polyaniline monolayer was deposited as an alternate insulator and its effect on diodes behavior was studied. 1.4 Thesis Organization A brief overview of mm wave detection systems followed by theoretical background of MIM diodes, processing techniq ues and characterization of diodes for mm wave detection is presented in detail. In chapter 2 a detailed background study on millimeter wave detection, the types
7 of devices used for detecting mm radiation and the current state of the art is presented. In addition, the need for a better detection system and how antenna coupled MIM diodes can be deployed for mm wave detection is addressed. In Chapter 3, the theory of MIM diode and its operation is presented. The various methods used in fabricating MIM diode s are discussed in Chapter 4, including an alternate MIM diode. Chapter 5 elaborately discusses the actual diode design and fabrication used in this research. The dielectric deposition technique is also described in this chapter. It also reports the fabric ation issues faced during the various stages of diode development. Chapter 6 describes the DC characteristics of different MIM diodes, including the polymer MIM diode. The temperature and thickness dependency of these diodes is also discussed. Chapter 7 co vers the measurement section by concentrating on the low frequency and mm wave response of MIM diode. Low frequency measurements yield rectification like behavior for the 100 m 2 diode, whereas the 1 m 2 diode operates well only at mm wave frequency. Chap ter 8 concludes the research work by summarizing the development of MIM diode and provides suggestion for future directions of MI M junction based mm wave detectors.
8 CHAPTER 2 BACKGROUND 2.1 Introduction Thermal imaging can be done at various wavelengths, like m illimeter and infrared (IR) wavelength s. At these wavelengths the primary source of mm and IR radiation is the heat radiation emitted by any object However, the amount of IR power radiated by an object at a given temperature is much higher than power radiated at mm wave as shown by the power radiation pl ot in Figure 2.1. H ence infrared has been the most commonly used wavelength for developing thermal imaging system. Moreover, many objects emits strong infrared radiation in the 10 m wavelength  making IR systems suitable for thermal imaging. Although infrared systems provide higher resolution (smaller wavelength), it suffer s from many disadvantages such as (a) straight line of operation: the radiated or transmitted IR signal must be in line of sight to detect the object, (b) weather sensitivity: adverse c onditions like dust, smoke, fog etc., degrades the IR radiation, thereby reducing the system performanc e, and (c) blockage by common materials: wherein the radiation does not penetrate through many materials, hence provides a outline radiation map of the subject of interest  Figure 2.2 shows the infrared image of a subject color coded to identify the hot and cold spots.
9 Figure 2.1: Power Radiated by an Object at Room T emperature  Figure 2.2: Ther mal Radiation M ap of a Subject As Seen F rom an Infrared Imaging System. From  0.1 1 10 10 0 1000 10 m 0.5 m T = 300 K T = 6000 K Wavelength ( m) Power
10 On the other hand, as mentioned in the previous chapter, mm wave radiations are less affected in adver se conditions  Although millimeter wave systems have lower resolution than IR systems, millimeter waves have better performance in poor weather conditions and can p enetrate through many materials unlike infrared and optical waves. This has rekindled the interest in realizing mm wave detectors for several comme rcial and military applications  Figure 2.3 shows the millimeter wave image of a subject by penetrating through the clothing. Figure 2.3 : Millimeter Wave Image of a Subject by Penetrating Through the Clothing. From  2.2 Millim eter Wave Detection Millimeter wave detector operates as a transducer that converts the electromagnetic radiation to an electrical signal. Millimeter wave imaging/ detection has
11 been investigated and developed using various technologies. In general, mm wav e imaging is classified as (a) passive or (b) active imaging systems. These systems can be operated as a point sensor or a remote sensor based on the device performance. In a point sensor, the object is located in close proximity to the sensor and a transmitter provides the mm wave radiation. Because of the proximity, only l ittle power is required to be transmitted. In a remote or a standoff sensor, the object and the sensor have a relatively larger separation; hence the object collects only a small fraction of the transmitted power. If this small fraction could be detected b ack at the receiver, the device is called active imaging system  Devices operating without illuminating or transmitting an external radiation are called passive imaging system  Some of the devices operating in passive and active mod e are discussed in this section. In addition, the problems faced by these systems are also presented. (a) Passive mm wave imaging: In a passive mm wave imaging system, the image is obtained by natural electromagnetic radiation emitted from the object. All natural objects whose temperatures are above absolute zero emit passive millimeter wave radiation  As mentioned earlier mm waves are much more effective (lower attenuation) than infrared in poor weather conditions  Also, images produced by passive millimeter waves have natural appearances  In the mm wave regime the atmospheric windows occur at 35 GHz, 94 GHz, 140 GHz, and 220 GHz and the choice of frequency depend on the specific application. Generally, i n a passive imaging system, the image is affected when operated
12 indoor s, due to lesser temperature differential between the objects radiation and background radiation. However, several companies such as Mill ivision, Trex Enterprises, Lockheed Martin and TRW, were working on producing passive mm wave radiometric arrays. Millivision initially developed mm wave detectors using a standardized radiometric card with 8 x 8 channel array, but encountered several pro blems while attempting to form a larger array. The detector did not have enough sensitivity to detect objects under a cold sky. The gain and sensitivity could not be balanced. The system took a long time to produce enough independent pixels to form an imag e. Later by using an Indium Phosphide low noise amplifier (LNA) on a Monolithic Microwave Integrated Circuit (MMIC), the noise figures were minimized. Still, the detector suffers from not having enough pixels to form a clear representation of the object. R ecently, Millivision has developed a gateway scanner to be used in airports and other public locations as a point source passive sensor operated by a Focal Plane Array (FPA) of LNA  Trex Enterprises had initially developed a radiometric imager using opto acoustic Bragg Cell. This system was large in size and was developed for battlefield imaging. Although this system could i dentify large metal objects under a cold sky, it could not detect concealed objects when operated indoors. The device performance proved poor when attempted to operate indoors. Later, a smaller lightweight antenna, LNA and an improved digital signal proces sor were employed to improve the device performance. The mm wave radiations were detected directly using a MMIC. In spite of these improvements the sensitivity of the detector was lower when operated indoor 
13 Lockheed Martin developed a dual mode sensor with a sensitive infrared imager and mm wave passive imager. A Cassegrain anten na with an IR camera was used in the system along with a direct detection LNA. The scan rate exhibited by this system was variable, which would increase the noise figure  Millimeter wave imaging systems are also being developed using compound semiconductor materials like High Electron Mobility Transistors (HEMT), which makes the fa brication process very complex  A research team at the Fraunhofer Institute for Applied Solid state Physics is develop ing InAlAs/InGaAs HEMTs for millimeter wave imaging  Also at the Chalmers University the detectors based on Heterojunc tion Barrier Varactors (HBVs) are being developed  These are the current technologies that are being pursued for developing passive milli meter wave imaging systems. (b) Active mm wave imaging: Active imaging systems are those in which an illumination or radiation is transmitted by a source (radar) and the image is detected. Active systems work well indoors or outdoors unlike passive imagin g systems Active imaging systems were initially developed for through the wall detection system (using long wavelength). Later it was developed for operating in shorter wavelengths Since an active imaging system illuminates the target to collect information, a few health concerns are posed. However, the radiation transmitted from an active imaging system is less than most of the routinely used wireless systems. Figure 2.4 shows the s chematic of an active millimeter wave detector.
14 Fig ure 2.4: Schematic Representation of an Active Millimeter W ave Imaging S ystem From  Some of the active imaging systems recently pursued are, (a) Terahertz absorption spectroscopy by Intelligent Optical Systems  The absorbance spectra via both transmission and reflection are obtained and matched with the selected signature wavelength to identify the concealed object. This method utilizes the absorption spectra of a chemical and m atches with the target to identify the target. The detection of this system is limited only to chemical substances. (b) Terahertz Standoff Imager with heterodyne detectors using Quantum Cascade lasers by Spire Corporation  This approach uses a terahertz Fourier Tran sform Interferometer (FTIR) and a heterodyne detection system to increase the sensitivity. A horn antenna is used to transmit the radiation to illuminate the target and detected using
15 the FTIR. This technique was proposed as a remote active imaging system operating at 50 meters target distance. (c) Electromagnetic Conce aled Weapon Detection (CWD) by Pharad, LLC  In this approach, a wideband mm wave signal is transmitted to excite the natural resonance on a concealed weapon and an electromagnetic signature of the specific object is matched with the signature in the database. This appr oach has a potential to create false alarms since many materials have to be identified to match to the target. (d) Non linear acoustic concealed weapon detection ( CWD ) by Luna Innovations, Inc.  This technique utilizes the audio sound to penet rate through clothing and identify the resonance of different material. However, the sound wave spread too quickly and also gets attenuated. Hence an advanced processing technique in needed to classify the sample signature to distinguish different objects. (e) Active mm wave radar for CWD by Personal Protection Technologies, Inc.  This techniques proposed to use off the shelf collision avoidance radar operating at 77 GHz and use it to transmit and receive radiation to a camera, controlled by a computer. At 77 GHz, the attenuation will be more and the resolution will also be compromised. (f) Magnetic signature analysi s by Idaho National Laboratory  This approach uses a magnetic signature procedure to identify targets. Advanced signal pr ocessing is required to discriminate targets. (g) Focal plane array ba sed mm wave imaging system is developed by Lockheed Martin  This utilizes Vanadium oxide based bolometer for detecting the resistance
16 change, which is calibrated to the temperature of the radiation. The bolometer is developed as a pixel when subjected to radiation. However, the devices suffer from slow response time  In general, the mm wave imaging systems developed so far suffer from various problems such as large size, weight, complex device development, poor sensitivity, long integration time and poor imaging capability. Hence there exists a need for developing a high efficiency mm wave detector with simpler fabrication technique in a compact configuration for varied applications. This may be possible by making a shift towards the antenna coupled detectors. In an antenna coupled detector, the antenna is used to couple the electromagnetic energy to a rectifying element with smaller dimensions than the wavelength of the incident radiation. By using a wide band antenna, an entire range of wavelength s can be captured efficiently and converted as a useful energy. In addition, due to the operat ing frequency, the device sizes are much smaller making the mm wave device compact and portable. 2 .2 Antenna Coupled Detector Antenna coupled detectors or Rectenna s have been explored for the past two decades mainly for microwave applications, infrared de tection, terahertz imaging       and even energy harvesting  Antenna coupled detectors with bolometers, metal insulator metal (MIM) diodes   and schottky diodes  have been used for detection in the s ub mm wave and mm wave regions with various antenna configurations. They are discussed hereunder.
17 A bolometer is a device used for measuring the energy of the incident electromagnetic radiation  It consists of a resistive element constructed fro m a material with a very small thermal capacity and a large temperature co efficient so that the absorbed radiation produces a large change in resistance  Typically bolometers are fabricated using metals and metal oxides like Nickel, Bismuth, Niobium, Platinum, Antimony or Vanadium Oxide  The devices are operated at room temperature and have response time of 10 3 seconds with a low sensitivity  Nevertheless, metal film bolometer arrays have been fabricated and employed in IR sensors coupled with antenna array due to ease of fabrication    But the devices are generally fragile, thus limiting their use in certain applications  Recently, research has been conducted to develop bolometers with semiconductors and other composite materials to increase the sensitivity  On the other hand MIM diodes are more stable device that provides a much faster response (10 15 seconds)  and higher sensitivity than bolometers  Higher sensitivity values lead to greater detectivity. Hi storically, antenna coupled M IM diodes have been used for imaging and detection in long wave IR (LWIR) regime. By scaling the device area, the same concept can be utilized for mm wave detection. As mentioned in the previous chapter, MIM diodes consist of two metal electrodes separated by a thin insulator layer. Typically MIM junctions were fabricated using a base metal electrode, the native metal oxide and another top metal electrode. Initially point contact MIM diodes also known as cat whiskers combined with wire antennas were used for sub millimeter wavelength detection and mixing  A sch ematic
18 of point contact diode fabricated using a metal wire in contact with another metal plate is shown in Figure 2.5. Figure 2.5: Schematic Illustration of a MIM Diode Fabricated U sing Point Contact Configuration These types of diodes were difficult to fabricate since the barrier layer that was formed was due to dirt collected on the surface or a native oxide layer forming a barrier layer In spite of the reproducibility issues, the point contact diodes were fabricated and used in the communication field for over twenty years in high frequency rectification from a few GHz to 150 THz   But the drawback was the integration and stability of a point contact MIM configuration in the infrared and optical region. Due to the instability of point contact diode s, thin film MIM diodes were utilized. Thin Film MIM diodes consist of an insulator layer sandwiched between two metal electrodes integrated on a substrate. With the advent of photolithography, stable and reproducible thin film MIM junctions could be fabricated Although stable and reproducibl e thin film MIM
19 junctions can be manufactured, the development of a MIM array with smaller area is a challenge. Various research groups have fabricated and investigated the concept of MIM tunneling with different thin film metals such as Al Al 2 O 3 Al  Cr CrO Au [29 ]  Al Al 2 O 3 Ag  Nb NbOx Au  How ever, published reports state that only few research groups have investigated the development of MIM junctions for mm wave detectors. Most research groups have fabricated MIM junctions for IR detection using same metal electrodes. Table 2.1 shows the thin film MIM junctions fabricated by different groups and its sensitivity values. Table 2.1 : Thin Film MIM J unctions Developed by Various Research Groups Research Group Type of MIM Junction Area Sensitivity Heiblum et. al.  Ni NiO Ni 3.8 m 2 4.3 V 1 Hoofring et. al.  Ni NiO Au 0.64 m 2 4.55 V 1 UCF CREOL  Ni NiO Ni 0.075 m 2 2.75 V 1 ETH, Zurich  Ni NiO Ni 0.056 m 2 1.6 V 1 UND  Ni NiO Pt 0.0025 m 2 13 V 1 UND  Al Al 2 O 3 Pt 0.0025 m 2 1 3 V 1 UND  Al Al 2 O 3 Ni 0.0025 m 2 1 V 1 UND  Al Al 2 O 3 Al 0.0025 m 2 1 .4 V 1
20 As seen from the table most of these junctions yielded low sensitivity value. In order to achieve better device performance, MIM junctions need to be fabricated with two different metal electrodes. The need for using different metal electrodes is discussed in the next chapter. In summary, the antenna coupled MIM detectors offer a new dimension in sensing with many advantages over other imaging techniques. MIM junctions offer more ad vantages than the existing bolometer in the areas of imaging parameters, li ke detectivity, sensitivity etc. Another benefit of the proposed technology is the ease of fabrication and the ability of the device to operate at room temperature These sensors have no mechanical parts and are made of solid state devices which can be fab ricated with the standard processing techniques making them CMOS compatible allowing them to integrate with external circuitry. Thus when developed, these detectors would provide outstanding night vision capabilities and concealed weapon detection systems yet come in compact, lightweight and powerful designs. That, in turn, would cut manufacturing costs considerably and would speed up the use of imaging sensors for an entire new category of applications, including medical equipment, robotics and micro air vehicles.
21 CHAPTER 3 METAL INSULATOR METAL TUNNEL DIODES A MIM tunnel junction is a thin film device, which consists of two metallic plates separated by a very thin insulating layer. It is a quantum device and rectification takes place when electrical charges flow from one side to another by over coming the potential barrier. The tunneling mechanism causes the detection of an applied AC signal resulting in a dc output component. MIM tunnel junctions are typically developed with a small contact area governed by a relationship between operating freq uency and the capacitance of the tunnel junction. Thus in this section, the tunneling current and frequency area relationship of the junctions that explain the operation of MIM tunneling are presented. Figure 3.1 shows the schematic of electron tunneling t hrough a barrier layer. Figure 3.1 : Schematic Illustration of an Electron Tunneling Through a Finite Barrier in a MIM Junction. From 
22 3.1 Theory of Operation The operation of MIM diode can be better understood by observing the energy band diagram for an asymmetric MIM junction at equi librium, shown in Figure 3.2. T he figure shows an in sulator layer with a thickness (s) between two dissimilar electrodes with dif ferent work function. Work function is the minimum voltage required to displace an electron from the Fermi level to the vacuum level. The work functions of metal 1 and metal 2 are denoted by 1 and 2 respectively. The barrier height is the minimum energ y required to move an electron from the metal to the conduction band. The barrier heights of metal 1 and metal 2 are given by 1 and 2 respectively. Figure 3.2 : Energy Band D iagram of MIM Diode at Zero B ias 1 # 1 # 2 2 E F E F $! = 2 1 $# = % 2 % 1 C.B Metal 1 Insulator Metal 2 s
23 When the metal is brought into contact with an insulator layer, thermodynamic equilibrium requires a continuous Fermi level be e stablished across the interface denoted by E F Here the electron in either metal meets a constant potential energy barrier o at the interface of metal and insulator, given by, o = m & (3.1) where, m is the work function of the metal and & is the activation energy of the insulator  The barrier height and work function of the metal are related by, 1 2 = $ = 1 2 = $! (3.2) Hence by determining the barrier height of one metal, the other barrier height can be determined using the above relation. But practically the interface of metal insulato r cannot have a straight cut trapezoidal potential barrier. Instead, the barrier interface will b e a smooth transition due to image forces, which arise due to the coulomb interaction between an electron induced charge in the nearby conductors ( exertion of an attractive force on the electron)  As the electron approaches the dielectric layer, it induces a positive charge on the interface, which acts like an image charge within the layer and reduces the barrier height by rounding off the corners and narrowing the barrier  as shown in Figure 3.3.
24 Figure 3.3 : Energy Band D iagram of MIM Diode Showing Barrier Lowering due to Image F orce However, if the barrier height difference between the two metals is high enough, electrons can tunnel through the insulator without any dc bias. Based on the work function of the two electrodes, the energy band diagram will show more asymmetry and rectific ation When a bias voltage is applied between th e two metal electrodes more current flows through the insulator. The current response by varying the bias voltage has been shown to be a non linear behavior  and the rectifying characteristics of the MIM diode arise from the asymmetry in the current voltage (I V) characteristics. The effect of bias voltage between the two electrodes displaces the Fermi levels of the two electrodes relative to each other. The Fermi level of the negatively biased electrode is moved upward on the energy scale. The electrical characteristic is taken to be # 1 # 2 $# s M1 Insulator M2
25 forward characteristics, when the metal with lower work function is positively biased and a reverse characteristic when it is negatively biased. Applying a bias voltage consequently modulates the height of the potential barrier. When either of the Fer mi level is raised, the height of the barrier is lowered. This is because the barrier potential is referenced to that Fermi level which is higher on the energy scale. When a bias of either polarity is applied, one of the two Fermi levels is elevated, there by increasing the reference energy level. Thus the maximum barrier height for the MIM structure occurs at zero bias. Similarly, the barrier width is also affected by applying a bias voltage. The barrier width is defined as the distance between two metal i nsulator points at zero bias Fermi level. When a bias voltage is applied, the Fermi level is moved above the reference energy level. This facilitates the electrons to tunnel through a minimal thickness, due to barrier lowering. Thus, the electron can tunne l through the insulator with more probability of finding itself on the other side. This behavior is mainly due to the difference in the work functions of the two metals. The limiting factor in the potential performance of a MIM diode is the difference in the work functions of the two metals. The work function of the metal can also affect the potential barrier the same way as the applied bias. In order to achieve a high degree of asymmetry in the I V curve it is therefore desirable to use metals with highl y different work functions.
26 3.2 Current Voltage Characteristics Typically the I V characteristic of a MIM diode is measured under forward biased condition. As mentioned in the previous section, w hen the diode is forward biased, the average height of th e barrier lowers thereby increasing the tunneling probability and hence the current flow. T he tunneling probability is increased when the barrier width of the insulator is also extremely thin. The current obtained from the MIM structure was modeled by Simm ons  using the Sommerfeld and Beth Model and WKB approximation. An approximate expression for the tunneling current in the MIM system can be written as, J = Jo s 2 [ # exp( $ A s # ) $ ( # + eV ) exp( $ A s ( # + eV )] (3.3) where J is the current density at every voltage instance in A/cm 2 Jo and A are constants, $ S is the effective barrier thickness in units and # is the mean barrier height in V. The tunneling current can also be determined according to the bias voltage (V b ) applied to the tunnel junction. At low voltages, when the mean barrier height = ( # 1 + # 2 ) 2 >> V b equation 3.3 can be simplified as, J = # V $ s exp( % A $ s # ) (3.4) where = e 2 m 4 B # 2 2 and A is a constant. Since the mean barrier height >> eV we
27 can consider that # does not depend on V. Thus in the case of small voltage, the tunneling current in proportional to the applied bias. Figure 3.4 shows the effect of potential barrier at low voltages exhibiting minimal change in the band diagram. Figure 3.4: Effect of Applying Low Voltages to the Potential B arrier When the bias volta ge is increased such that # 2 > V b the tunneling is governed by another equation for intermediate voltages given by, J = # $ s exp( % A $ s # )( V + & V 3 ) (3.5) where, = ( Ae ) 2 96 #$ s 2 % ( Ae 2 ) 32 $ s # 3 2 s = s and = ( # 1 + # 2 $ V ) 2 Figure 3.5 shows the effect of potential barrier at intermediate voltage range. # 1 # 2
28 Figure 3.5: Effect of Potential Barrier at Intermediate Voltage R anges When the bias voltage is increased over the barrier height, i.e., V b >> 2 the tunneling current is best explained by Fowler Nordheim equation  given as, J = q 2 E 2 4 h # 0 [exp( $ E o E )] (3.6) where q is the charge of the electron, E is the electric field across t he junction, h is the Planck's constant, o is the barrier height and E o = ( 8 / 3 )( q ) 1 / 2 ( # o ) 3 / 2 Figure 3.6 shows the potential barrier in the MIM system at large voltage. At very high bias voltages the electrons instantaneously tunnels from metal 1 to metal 2 due to lowering of barrier height and width exhibiting a sudden increase in current. Thus, from the electrical # 1 # 2 V b
29 behavior it can be observed that the diode characteristic is highly correlated with its dielectric thickness and hence significantly depends on the fabrication methodologies adopted to develop the device. A typical forward current voltage characteristic of a MIM junction is shown in Figure 3.7. Figure 3.6 : Effect of Potential B arrier at Very High Voltages # 1 # 2 V b
30 Figure 3.7: Theoretical I V Plot of MIM Junctions Operated in the Intermediate Voltage Ranges. Inset Shows the I V Plot at Low Voltage Range. 3.3 Frequency and Area Relationship MIM tunnel junctions can be considered as a parallel plate capacitor with a thin dielectric layer sandwiched between two electrodes. Hence, the operational frequency of the tunnel junctions is determined using the capacitance of the tunnel junction. Accord ing to Sanchez et al.,  the cut off frequency of the device is defined as, f c = 1 2 R a C d (3.7)
31 where, f c is the cut off frequency of the device, R a is the antenna resistance, and C d is the capacitance of the diode Detection is still possible beyond this cut off frequency, but the detectivity of the MIM diode decreases by (f c ) 3 Thus as R a is determined by the fabrication process it can be treated as a constant for a given process. The estimated frequency of operat ion of a MIM diode can be calculated by determining the capacitance of the devi ce. The capacitance of the MIM junction is given by the parallel plate capacitor equation as C = o r A d s (3.8) where, r is dielectric permittivity of the insulator, A d is the active area of the diode and s is the thickness of the insulator. From (3.7) and (3.8) it can be noted that the operation frequency of the tunnel junctions is increased by reducing the capacitance of the device. In order to reduce the capacitance, the contact area A d or the dielectric constant has to be reduced or the insulator thickness s has to be increased. For operating the device at 3mm, a diode with cut off frequency over 94 GHz is needed. By decreasing the contact area or increasing the insulator thickness a smaller capacitance value can be obtained. However, from the current vs. voltage equations it can be seen that the current density of the tunnel junction is exponentially dependant on the insulator thickness. Hence to reduce the capacitance of the tunnel junctions it is preferred
32 to maintain the thickness o f the insulator at a nominal value for electron tunneling (< 4 nm), while reducing the contact area of the diode. Based on the aforementioned equations MIM junctions have been fabricated by various research groups with same as well as different metals. Fro m the energy band diagram of MIM junctions it is understood that by using metals with different work functions, an asymmetric behavior can be achieved. Furthermore, the asymmetry can be increased when the work function between the two metal electrodes is l arge enough Table 3.1 shows the work function of different metals commonly used in developing MIM junctions. Various materials used for fabricating a MIM junction with different electrodes is discussed in Chapter 5. Table 3.1 : Work Function of Various Metals Used for Fabricating MIM D iodes From  Element Work function (eV) Cr 4.5 Ni 5.15 Al 4.3 Au 5.1 Pd 5.1 Pt 5.65 Nb 4.3 Ag 4.26
33 CHAPTER 4 PROCESSING TECHNIQUES 4.1 Microfabrication The fabrication of MIM diodes mainly involves optical lithography as well as SEM based electron beam lithography to pattern diodes with different dimensions. In this section a detailed description of photolithography and e beam lithography process used to define the diode structure is presented. 4.1.1 Optical Lithography Lithography is a proce ss of transferring geometric shapes on a master pattern to the surface of a substrate. Optical lithography is used for producing integrated circuits with high density small scale features on to a substrate. Typically, optical lithography is performed using an ultraviolet lamp with a strong UV signal at the "g line" (436 nm) or "i line" (365 nm). For achieving feature sizes in the nm range deep UV lithography is used. For developing the MIM diode we used a "g line" lithography tool from EV Group (EVG 620) an d Quintel (QC 6000). The mask aligners used for fabricating the MIM diodes are shown in Figure 4.1(a) and 4.1(b). This tool also has the capability to do backside alignment, which was utilized to develop the millimeter wave MIM diode.
34 (a) (b) Figure 4.1: Visual of (a) EVG 620 and (b) Quintel Mask Aligners
35 Generally, the photolithography process involves several steps before the substrate can be used for metallization or thin film deposition. The steps involved in the photolithographic process a re wafer cleaning, photoresist application, soft baking, mask alignment, exposure and development, and hard baking. A brief overview of each process is presented. (a) Wafer Cleaning and Photoresist Application: This is the initial procedure in the lithography process. The wafers are thoroughly cleaned to remove any particulate matters from the surface. Then photoresist is applied to wafer surface by spin coating to form a thin layer. (b) Soft Baking: Soft baking done after c oating the wafer with the photo resist. So ft baking removes the solvents from the resist coating. The photoresist coatings become photosensitive only after soft baking. (c) Mask Alignment and Exposure: The wafer coated with photoresist is loaded in the mask aligner and aligned with a mask, which has the master patterns. Each mask after the first one must be aligned to the previous pattern. After aligning the wafer to the patterns, the photoresist is exposed by a high intensity ultraviolet light. (d) Development: After the wafer is exposed, the pattern is developed in the resist by immersing the wafer in a photoresist developer. The developer dissolves th e un polymerized resist regions and differentiates between the exposed and unexposed regions.
36 (e) Hard Baking: Hard baking is the final step in the photolitho graphic process. This step is necessary in order to harden the photoresist and improve adhesion of the photoresist to the wafer surface  4.1.2 Electron beam Lithography E beam lithography (EBL) is a lithographic process wherein a beam of focused electrons is scanned across an e beam sensitive resists to produce very fine patterns. In an E beam lithography system patterns as small as 10 nm can be produced. The pattern size is dependant on the elec tron accelerating voltage. Typically, EBL systems can operate at high accelerating voltage in the order of 10 50kV offering higher patterning capability than optical lithography due to its shorter wavelength. As mentioned earlier, E beam lithography is used to pattern devices beyond the optical lithography limit. In this work although the devices dimensions were 1 m 2 the e beam litho graphy technique has been utilized to fabricate the devices due to the unavailability of a high resolution optical litho graphy system. The E beam lithography tool used for this research work is a scanning electron microscope (SEM) modified to be used as an e beam litho writer. J.C. Nabity's Nano Pattern Generation System (NPGS) was used with a JEOL JSM840 SEM to perform the e be am lithography shown in Figure 4 .2. A schematic of the SEM E beam litho control led by NPGS is shown in Figure 4 .3.
37 Figure 4 .2: JEOL JSM840 Controlled by Nabity's Nano Pattern Generation System Courtesy NNRC
38 Figure 4.3 : Schematic of JEOL JSM840  The JEOL JSM840 SEM has a t ungsten filament operating by thermionic emission. The electrons emitted from the t ungs ten filament are accelerated towards an anode. The condenser lens does the primary focusing of the e beam. The objective lens aperture serves to stop any stray electrons passing through the system i.e. clean the beam. We use a 75 m objective lens aperture which is th e lowest setting on the system. Astigmatism present in the e beam is corrected by special type of electron lens called the stigmators Astigmatism arises due to the imperfections in the construction and alignment of the e beam column. The obje ctive lens does the final focusing of the beam onto the
39 substrate. The condenser and objective lenses are electron lenses that use magnetic fields to focus e beams. The beam blanker is used to turn the beam on and off. It is a parallel plate with an applie d potential that electrostatically deflects the beam. XY scan coils are used for beam deflection off of the optical axis and hence scanning the beam to desired locations across the substrate. Both the beam blanker and the XY scan coils are controlled by th e NPGS system. The NPGS uses a 16 bit digital to analog (DAC) converter to control the SEM XY scan coils  It also handles turning the beam on and off by taking over the beam blanker controls. E beam lithography Process Polymethyl methacrylate (PMMA) is the e beam sensitive resist used for li thography throughout this work. It is a positive high resolution resist that is widely used in e beam lithography. However, it is a low sensitivity resist. The JEOL JSM 840 requires a dose of about 14 0 C/cm 2 to etch the PMMA. PMMA is spin coated on the surface of a substrate and the thickness of the PMMA film is determined by the spinning speed PMMA is then baked on a hot plate at 180¡ C for 2 minutes. When the PMMA is exposed to the e beam the polymer chains are broken leaving the exposed areas more soluble in the developer. Methyl isobutyl ketone (MIBK) is used as a developer to dissolve the exposed areas in the PMMA film. MIBK being a strong developer is usually mixed with isopropanol (IPA) in a ratio of 1:3 to prevent dissolving unexposed areas of the resist.
40 The patterns are defined on the substrate by an additive process as shown in Figure 4.4, wherein the resist is spun on the substrate. The resist is then exposed and developed resulting in the removal of the resist from the areas it was exposed. A thin film is then dep osited covering the entire surface of the substrate. The substrate is then immersed into a solution that dissolves the resist. The resist dissolves and the thin material above it is lifted off leaving only the deposited material on the exposed areas. Fi gure 4.4: Process Sequence for E beam L itho graphy The optical lithography technique was used for developing a prototype diode and E beam lithography was used for fabricating the high frequency diode. The metal and
41 dielectric deposition techniques followed were the same for developing both diodes. The design and fabrication process are discussed in the next chapter. The next section presents the deposition methods used for fabricating the MIM tunnel junctions. 4 .2 Thin Film Deposition The patterned MIM dio des are metalized using physical vapor deposition methods, namely DC sputtering and thermal evaporation. These are the thin film deposition techniques used to fabricate the devices in this research. Sputtering is a high energy process making the metal depo sition fairly homogeneous, while evaporation yields thin films that are well suited for lift off techniques. Moreover, the choice of using evaporation or sputtering as a deposition technique was due to the availability of materials. 4.2.1 Sputtering The main application of sputtering is for the deposition of thin films. Sputtering is a physical vapor deposition (PVD) technique used for precision coatings of thin films in vacuum. In sputter deposition unlike other vacuum deposition processes, the material usually arrive s in atomic or molecular form. The atom diffuses around the substrate with a motion determined by its binding energy to the substrate. Usually the atoms migrate and then re evaporate and combine with other atoms to form nucleation sites. This in turn grows into an island. Eventually the islands grow large enough to touch; this is the agglomeration or coalescence stage. The coalescence proceeds until the film reaches
42 continuity, this may not occur in some cases until the film is several hundred Angstroms in average thickness  Figure 4.5 : Sputtering Chamber Used for Depositing MIM Layers The sputtering chamber used for this project is shown in Figure 4.5 The substrate is placed in a vacuum chamber with a target of the material to be deposited. Plasma is generated in a passive source gas like Argon in the chamber, and the ion bombardment is directed towards the target, causing material to be sputtered off the target and condense on the chamber walls and the substrate. Sputtering can either be RF or DC. A strong magnetic field (magnetron) can be used to concentrate the plasma near the target to increase the deposition rate. The deposition rate depends on th e pressure, gas flow rate,
43 RF power, substrate temperature and target substrate spacing. The sputtering system used for this project was a home built system with two DC guns and one RF gun. For this project DC power source was utilized to deposit the metals. The thickness of the deposited material is measured using a quartz crystal monitor. The substrate is kept at a distance of 10cm from the target and a DC motor constantly rotates it in order to get a uniform metal deposition. Thus the metal depositi on is done using the sputtering system. 4.2.2 Reactive Sputtering Reactive sputtering is a process wherein a conducting elemental target is DC sputtered, and the sputtered material is combined chemically with a component such as oxygen in the gas phase w ith an inert working gas (Argon). Typically, RF sputtering is used for depositing insulators such as silicon dioxide or metal oxides. However, using the plasma oxidation or reactive sputtering technique can also activate a compound formation. The chemical reaction for sputtering may take place at the cathode, during transport of ejected atoms, at the film surface or a combination of these possibilities  Also, the role of each process depends much on the pressure and the chemical activity of the reacting species. A schematic of the reactive sputtering process is shown in Figure 4.6.
44 Figure 4.6: Schematic Illustration of a Reactive Sputtering System 4.2.3 Evaporation Met al evaporation can be done by utilizing E beam and thermal techniques. In an e beam evaporation electrons are focused on a graphite crucible containing the metal of interest, which melts the materials which are evaporated on to the substrate. In the case o f thermal evaporation, a resistively heated filament or boat consisting of the metal is used. The boat is typically made of a refractory metal such as W, Mo and Ta with or without a ceramic coating. In this project we have used thermal evaporation for depo siting the top electrode (Cr/Au). Similar to e beam evaporation, thermal evaporation also takes place inside an evacuated chamber. Figure 4.7 the actual instrument used for depositing metals.
45 Figure 4.7: Thermal Evaporator Used for Fabricating MIM D iode s In this evaporation technique, the material is heated until melted by means of passing an electrical current through the boat. The evaporated material condenses in the form of a thin film on the substrate surface. Evaporation is a line of sight process, wherein the materials will be deposited only in a straight line; hence the regions that are not accessible from the evaporation source will not be coated. Hence the substrate holder is rotated at a constant speed to get a uniform deposition. 3.3 Alterna te Dielectric Deposition Process The dielectric layer in a solid state MIM diode is typically deposited through sputtering, evaporation, atomic layer deposition, oxidation etc. These techniques require high vacuum conditions and/or high temperature operat ion to achieve a highly oriented homogenous thin dielectric layer. Recently, another technique used in the polymer industry using an immersion technique is exhibiting great prospects in depositing
46 monolayers of organic molecule over any solid surface with extreme accuracy. This process of depositing thin films is known as the Langmuir Blodgett (L B) technique. In a L B process, thin films of organic molecules are built up by a process of successive deposition of individual Langmuir monolayers onto a solid substrate. The monolayer is formed by spreading the organic molecules on the water subphase in a clean L B trough The molecules usually have hydrophilic (head) and hydrophobic (tail) parts, so when the film is formed the molecules stand on their heads. F igure 4.8 shows the schematic of L B deposition process. Figure 4.8: S ch ematic Illustration of L B Deposition T echnique  The solid substrate is raised from the water subphase and the molecules start to adhere to the substrate, which is monitored by recording the change in surface pressure. The surface pressure is usually measured using a Wilhelmy plate  and a preci sion scale When the molecules first are spread on the water they are ve ry loosely packed and
47 form a so called gas phase. This means that the area on the water available for each molecule is rather large a nd the surface pressure is low. At a certain point the surface pressure starts to rise more rapidly indicating a transition to the liquid phase. As the barrier is moved even further the onset of the solid phase can be noted by an even steeper rise in the surface pressure. One or more monolayers can be tran sferred to a substrate by dipping the substrate through the monolayer. The monolayer is kept uniform by controlling the surface pressure with the barriers throughout the process. Typical surface area pressure isotherm showing the different phase is shown i n Figure 4.9. Figure 4.9: Typical Surface Area Pressure I sotherm Plot of a L B film 
48 Thus LB technique is one of the most pro mising techniques for preparing such thin films as it enables (a ) the precise control of the monolayer thickness, (b ) homogeneous deposition of the mon olayer over large areas and (c ) the possibility to make multilayer structures with varying layer composit ion. An additional advantage of the LB technique is that monolayers can be deposited on almost any kind of solid substrate. The above mentioned processing techniques were utilized to fabricate the actual MIM tunnel junctions, described in the next chapter
49 CHAPTER 5 DESIGN AND FABRICATION OF MIM DIODES 5.1 Design of MIM Diodes In this research work, two types of MIM diodes were used. The initial design was a planar, stacked structure, which was designed to prove the concept of the MIM diode. The second design was a stepped layout, which had external bond pads to connect to the probes. Also the diode size was scaled down to accommodate the calibrat ion standards. The diode was designed to be much smaller to operate at high frequencies. Thus, in this section two different designs utilized to fabricate and characterize the MIM diode are presented. As mentioned earlier, the most important factor to be considered in the design of the MIM diode is the size of the contact area between the metal layers and the insulator layers. The reason for keeping a smaller contact area and the need for a thin layer of insulator were discussed earlier A MIM device has i nherent impedance in its device structure. By lowering the size of the active area, the impedance can be reduced  To validate the concep t of the MIM diode a device operating at a very low frequency was designed The low frequency operation require d the area of the MIM diode to be large (100 m 2 ). Upon further verification, with a goal of achieving a reproducible and uniform diode fill fa ctor, a scaled down version with a contact area of
50 1 m 2 centered around a target frequency of 94 GHz was designed and fabricated. The design of 100 m 2 ( d iode A ) was a simple planar structure, wherein the layers were stacked upon each other on a silicon su bstrate. In the case of 1 m 2 (diode B ) a stepped structure with extended contact pads was designed thereby allowing the devices to be probed witho ut damaging th e active area. Both diode structure consisted of a thick layer of Ni ( 100 nm), a thin layer of NiO (~ 1 3 nm), and a layer of Cr (30 nm) topped with a thick layer of Au (100 nm). 5 .1.1 Stacked MIM Design As mentioned earlier, a large area diode design w as made use of to validate the device concept and for experimenting with different diode parameters. This diode design was developed by Krishnan  and the same was utilized for this research work. Figure 5.1 (a) shows the schematic of the initial diode design. The stacked MIM structure design consists of two mask layers. The f irst level of masking defines the base electrode, which has a very large area (1 mm 2 ). Over the base electrode, a smaller square structure was defined, which serves as the top electrode or the active area of the MIM diode. The area of the top electrode was defined to be 100 m 2 This mask was generated from a photo plot sheet, which was transferred to a mask plate using a mask generator. The actual design in the photo sheet was reduced 25X to a glass plate. These plates were then used to generate the final masks by exposing the 4" plate in a step and repeat camera. Figure 5.1 (b) shows the array of diode designs generated in the mask plate.
51 (a) (b) Figure 5.1: S chem atic Representation of (a) Individual MIM Diode Design and (b) Array of Diodes Generated in the Mask L ayout.
52 5.1.2 Stepped MIM Design The second MIM design was developed with the objective to create a diode suitable for high frequency operation able to detect millimeter wave radiation in the 3mm range. The frequency of interest was 94 GHz for diode operation. For high frequency operation, a co planar waveguide configuration was chosen. In this design, the antenna diode detector as well as individual elements were designed to check the device performance. A slot antenna was chosen for this operational frequency with a tunable stub to increase bandwidth. The design of the slot antenna was presented by La Rosa  and the same design was used with a diode integrated in its feed line. A schematic of the antenna, diode, and the integrated device is shown in Figure 5.2. Figure 5.2 : Design of Antenna, D iode and Antenna Coupled Diode
53 The line width required for t he 94 GHz design was optimized by performing simulations in Agilent's Advanced Design Simulator (ADS) system by La Rosa  Sinc e the junction area of the MIM diode should be as small as possible for good detector performance (small junction capacitance, high cutoff frequency), the overlap between the two metal layers of the diode was designed to be around 1 m x 1 m. Due to high frequency operation, several design consideration have to be taken into account. One of the factors that need to be kept in mind is the substrate thickness. At high frequencies, the likelihood of surface waves propagating through the silicon su bstrate increases with increased dielectric constant and thickness. Hence, to minimize the power lost as surface waves, the thickness of the substrate has to be kept lower than the wavelength in dielectric ( d ). At 94 GHz the dielectric wavelength of sili con is approximately 100m, which is smaller than the thickness than of commercially available silicon wafers (400 m and 250 m). According to Gauthier et. al.,  the surface wave loss can be minimized by using thin substrates, t ypically d /10. For this reason, the mm wave devices were developed on a 10 m substrate. Since the whole substrate will be too fragile if a 10 m thick silicon substrate was used, a cavity was etched in the bulk silicon under the actual device. The techn ique used to form a thin silicon membrane is discussed in the next section. In that way, the devices can be connected to the test set up from the thicker part of the substrate. Due to this criterion, the device design had to be modified to accommodate a t hicker as well as thin substrate layout. However, such a modification can cause a mismatch in the input impedance. Hence to maintain a constant input impedance a transition method was
54 devised  Figure 5.3 shows the typical Co Planar Waveguide (CPW) line with the transition from thick to thin substrate. The dotted line will be the edge of the membrane. This transition preserves a n uniform impedance in the transmission line. Figure 5.3: CPW Lines Illustrating the Transition from a Thick to Thin Substrate. From  The diode was designed to fit in the CPW design as shown previously. For the diode design, initially the CPW lines, which also act as contact pads, were laid out as the first layer. Then, the bottom electrode of th e MIM diode is laid overlapping the contact pad. The area of the bottom electrode was designed to be 25 m x 25 m. The next layer is the top electrode, which is designed as a conical structure with a square head connecting to the other end of the contact pad. The top electrode is designed as a conical head to minimize the inductance by a line. The head of the cone defines the active area of the diode, which has an area of 1 m x 1 m. A schematic cross section of the diode design is shown in Figure 5.4
55 F igure 5.4: Schematic Illustration of the Cross Section and Top View of MIM Diode 5.2 Materials Selection P arallel to the diode design, the materials to be used for fabricating the mm wave diode had to be selected. Hence various material combinations were fabricated and evaluated. This section discusses the different materials used for developing the MIM diode and the final choice of material combination used for developing reproducible and robust mm wave detectors is presented Material selection is one of most important criteria for manufacturing of a MIM diode. Materials were selected based on the work function of the metal and dielectric constant of the insulator By fabricating MIM junctions with different work functions, the asymmetry of the device was improved. And when the dielectric constant of the insulator is low, the capacitance can be lowered, which in turn increases the cut off frequency. Thus, the MIM diode needs to be fabri cated with dissimilar materials An asymmetric
56 MIM diode developed w ith dissimilar metal has better sensitivity and low noise performance. Moreover, asymmetric MIM diodes exhibit n onlinear characteristics even in the unbiased state. Hence, various material combinations were tested for stability, reliability and robustness. The main concerns about selecting the materials were formation of a native oxide layer, adhesion to the substrate and homogenous deposition with minimal roughness. MIM diodes were fabricated with base metals of Aluminum and Nickel and top metals of Chromi um, Palladium, and Platinum. The work functions of different metals used for fabricating MIM junctions were given in chapter 3. S o me of the material combinations tried for fabricating the MIM diodes are discussed in this section Initially Aluminum was u sed as the base electrode with aluminum oxide as the insulator and Chromium as the top electrode. Although the work function difference was 0.2 eV, the diode exhibited I V characteristics with slight asymmetry. The thin films were also adhering well to the substrate and the oxide roughness was also very low on the order of 0.5 nm, according to Krishnan  However, the electrical behavior of these diodes was unstable over a period of time. Later using the same base electrode and its native oxide, a MIM diode was fabricated with Pd as the top electrode. Although the work function between Al and Pd is about 0.8 eV, the diodes were unstable and yielded a linear electrical characteristic. Next, Pt was used as the top electrode, which increased the work function difference to 1.35 eV. However, no measurements could be done as the Pt layer peeled off from the oxide surface. Later, Ni replaced the Pt top electrode. The work function difference between Al and Ni is about 0.8 eV and the electrical behavior of these diodes
57 was non linear and very slightly asymmetrical. But these diodes wer e not stable over a period of time. Although the Ni and Pd provided a very high work function difference, the devices did not yield any satisfactory diode characteristics at room temperature. This suggests that the oxide formed over the base electrode is g etting deteriorated causing device failure. Most likely, if the diodes fabricated with an Al base electrode are stored or packaged, stable diode behavior can be expected. But for this application a diode operating at room temperature is required. Hence, t he bottom electrode had to be replaced with a more stable material, which adheres well to the substrate and also forms a stable oxide layer. Nickel was the next choice because of it's higher work function than Aluminum and the ability to get a native oxide Since Ni had a work function of 5.15 eV, a material with work function less than Ni was necessary to create an asymmetric barrier. Cr has a work function of 4.5 eV, providing ~0.65 eV different in work function. The dielectric constant of NiO is 11.9, w hich is comparable to the dielectric constant of Aluminum Oxide (10)  Thus MIM diodes were fabricated with Ni and Cr as the base and top electrode, respectively. MIM diodes fabricated with Ni NiO Cr were found to be very stable and the diode characteristics were reproducible over a very long period of time. Hence for fabricating mm wave detectors, MIM diodes with Ni NiO Cr were selected.
58 5.3 A Typical Fabrication of MIM diode The fabrication process to manufacture the MIM diode is described in this section. In this section the materials that were used to fabricate MIM diodes, and the fabrication techniques used to attain the MIM diodes are discussed. The other noteworthy techniques involved in the diode development are (a) sputter deposition of the Nickel base electrode, (b) reactive sputtering or plasma oxidation of Nickel Oxide to achieve thin barrier layer with the use of lift off technique and (c) incorporation of the top electrode or the active area of the MIM diode by e beam lithography. 5.3.1 Subs trate Preparation The devices were typically fabricated on a 2" <100> silicon substrate. Before using the wafers for further processing, they were first cleaned in acetone and methanol at room temperature, followed by D I water rinse and dried using nitrogen. This is followed by standard wafer cleaning procedure which consist of ammonium hydroxide, hydrogen peroxide and DI water known as standard clean 1 for removing organic contaminants and Hydrochloric acid, hydrogen pe roxide and DI water known as standard clean 2 for removing ionic contaminants, each followed by a DI water rinse. The detailed cleaning process describing the times, temperature and mixing ratio is described in Appendix A. Each solution was heated to 80¡C and the wafers were immersed and cleaned for 20 mins. Next a layer of silicon dioxide was thermally grown on the substrate to provide an isolation layer for the devices. The oxidation process was performed at 1100¡C in a dry wet dry oxygen atmosphere to gr ow an oxide layer approximately 500
59 nm and 1000 nm thick for the low and high frequency device fabrication, respectively. The thickness of the oxide was measured by an ellipsometer (Rudolph AutoEL III). 5.3 .2. Fabrication of Stacked MIM Structure ( 100 m 2 Contact Area ) Figure 5.5: Process Flow of Stacked MIM D iode Figure 5.5 schematically illustrates the fabricating sequence for deve loping the MIM diode with a 100 m 2 contact area. Oxidized Si wafers were subjected to photolithography to define the Ni NiO areas using the first mask. A direct current (DC) magnetron sputtering system, built in house, was utilized to deposit the bottom electrode ( Ni) and the insulator layer (NiO) The patterned substrate is loaded in the sputtering chamber and evacuated to bring it to high vacuum, typically in the 3 torr. Nickel was deposited using the DC magnetron sputtering system built in house. A 3" diameter,
60 0.250" thick, 99.99% pure Ni target was used as the sputter target. The deposition was typically carried out at a power of 100 W and 10 mTorr Argon pressure. A 100 nm of Ni was deposited by maintaining th e gas pressure and DC power The thickness of the deposited film was determined using a quartz crystal monitor. Later oxygen was bled into the chamber and the d eposition was continued. A thin layer (~3 nm) of NiO was deposited in situ by a plasma oxidation process. Following the metal and oxide deposition, the substrate was immersed in acetone to remove the excess layer and define the bottom electrode and dielect ric layer. Some of the resist sticking to edges of the patterns were carefully removed by ultrasonicating the sample for 30 secs. Then Ni and NiO coated samples were subjected to the final photolithography step to pattern the Cr layer. Chromium was depos ited by using a evaporation technique. Similar to sputtering, the sample was loaded in the chamber and evacuated to a pressure of 2 Torr. 30 nm of Cr was deposited by thermal evaporation followed by a Au deposition (100 nm) to protect the top electrode. T he Cr deposition was made at a very low rate (< 0.1 nm/sec) to obtain a smooth surface. Then, the Au was evaporated at a rate of 0.3 nm/sec at a current varying between 180 200A. The substrate was then subjected to lift off and the Cr/Au layer was defined to obtain the 100 m 2 MIM structure.
61 5.3 .3 Fabrication of Step MIM Structure (1 m 2 Contact Area ) Figure 5.6: Process F low for Step MIM D iode Figure 5.6 schematically illustrates the steps involved in fabricating the 1 m 2 MIM diode. Following the oxidation of the silicon substrate a photolithography step was performed to pattern the CPW configuration pads along with the antenna and calibration standards. The contact pads were deposited with a thin layer of chromium (Cr) and gold (Au). The metal d epositions were carried out using thermal evaporation. A Denton DV 502 thermal evaporator was used for this purpose. Cr was deposited for a thickness of ~ 30 nm which acts as an adhesion layer for the top Au (~200 nm) layer. The Cr deposition
62 was made at a very low rate (< 0.1 nm/sec) to obtain a smooth surface. Then, the Au was evaporated at a rate of 0.3 nm/sec at a current varying between 180 200A. The contact pads are deposited with higher thickness to minimize surface wave losses during high frequency measurement. For 94 GHz, the skin depth was determined to be ~ 250nm. However a much thicker conductor is preferred. But due to processing incompatibility, the minimal thickness was used. After the contact pads were made, the lithography for the bottom el ectrode of the MIM diode was done. The Nickel layer was used as the bottom electrode for the MIM structure. Ni was deposited for a thickness of about ~100 nm. In t he case of diode B, all the steps up to Ni and NiO deposition we re similar to those for diode A. Only, the final step of e beam lithography used to define the electrode was different. In particular, for e beam lithography first a 150 nm thick polymethylmethacrylate (MicroChem 950 K with 3% Anisole) was spun on the sample and baked at 180¡C fo r 2hrs. Later, the devices were patterned by a modified JEOL JSM 840 Scanning Electron Microscope (SEM). Nabity`s Nanometer Pattern Generation System was used to control the e beam and pattern the contact area. The patterns were exposed to e beam for a se t area dosage of 110 c/cm 2 and a dwell time of 90 sec to form 1 m 2 windows. The patterns were developed in a 3:1 Isopropanol: methylisobutylketone solution. After that 3 0 nm of Cr and 100 nm of Au were deposited to fabricate the MIM diode with 1 m 2 con tact area Later, photolithography was performed on the backside of the substrate using the EVG backside aligner and windows were opened underneath the devices. Following the lithography step, the top layer was coated with a protective layer of resist Prot ekB2 18
63 from Brewer Science. This resist can withstand etching against typical silicon etchants such as Potassium Hydroxide (KOH) and Tetramethyl Ammonium Hydroxide (TMAH) for prolonged hours (> 10hrs). The resist coated substrates were then placed in a s pecial set up to etch only the windows on the backside. The etch set up used to etch the membrane is shown in Figure 5.7. The etch set up was made using Teflon and viton seals. The silicon substrate was kept face down and sealed from underneath to prevent any etchant leak. Then the set up was immersed in TMAH kept at 80¡C. Since we do not have a etch stop layer, the process had to be stopped quite often to determine the etch rate. The etch rate can be determined by calculating the thickness of the substrat e before immersing in the Si etchant and the thickness etched in the set time. The thickness etched was determined using a surface profilometer. After the etching was completed, the substrate was initially rinsed in Isopropyl alcohol to remove the TMAH s ticking to the membrane and then rinsed thoroughly with Acetone and methanol to remove the protective layer on the front side. Thus the silicon membrane was formed. Figure 5.8 and Figure 5.9 shows the SEM micrograph and the visual image of the membranes et ched in silicon, respectively.
64 Figure 5.7: Etch Set up Developed for Silicon Membrane E tching Figure 5.8: SEM Micrograph of Si licon Membranes Etched Using TMAH
65 Figure 5.9: Visual Image Showing the Silicon Membrane s Etched on a Full Wafer Figures 5.10(a) and (b) show the corresponding micrograph images of the fabricated 100 m 2 and 1 m 2 diodes, respectively. As shown in Figure 5.10 (a), the outer square region defines the Ni NiO region and the smaller square region (Cr/ Au) defines the act ual MIM contact area (100 m 2 ). Similarly, shown in Figure 5.10 (b) is the d iode B with gold contact pads underneath the Ni NiO Cr/Au structure. The conical head defines the active area of the MIM diode. The area of this diode was observed to be 1.45 m 2
66 (a) (b) Figure 5.10: SEM Micrograph of a MIM Diode Fabricated with (a) 100 m 2 and (b)1 m 2 Contact Area
67 5.3.4 Fabrication of MIM with Polyaniline The fabrication process of the thin film Ni Polyaniline Cr/Au MIM diode is schematically illustrated in Figure 5.11. MIM diodes have been fabricated on a 2" bulk silicon substrate with SiO 2 as the insulating layer. These oxidized silicon wafers were used as the substrates. For the fabrication of the polymer based diode 100 m 2 design was used. The first m ask was used to define the Ni and Polyaniline layers and the second mask was used to define the top metal layer (Cr/ Au). The oxidized Si wafers were subjected to photolithography to define the Ni areas. A direct current (DC) magnetron sputtering system, b uilt in house, was utilized to deposit a 120 nm of bottom electrode (Ni). The thickness of the deposited film was determined using a quartz crystal monitor. Later the P Ani was deposited on the Ni surface by LB method Then Ni and P Ani coated samples were subjected to the final processing step to pattern the Cr layer. A 30 nm of Cr was deposited by thermal evaporation followed by Au deposition (100 nm) to obtain the 100 m 2 MIM structure.
68 Figure 5.11 MIM PANI Process Flow 5.4 Dielectric Deposition Tec hnique 5.4 .1 Nickel Oxide As mentioned earlier, in order to achieve tunneling, the dielec tric layer needs to be thin (< 5 nm) and homogeneous. Hence, a controlled process to obtain a thin layer of Nickel Oxide was developed. The dielectric layer was deposited through a controlled plasma oxidation process. The same DC magnetron sputtering system used for Ni deposition was als o used for depositing the dielectric layer. For the NiO deposition process, O 2 was introduced along with Ar to create a reactive sputtering. NiO was deposited at a very low power of 25 Watts for 10 15 mins. During the NiO deposition some of the sputteri ng parameters were varied to study their effect on thickness and roughness of the film. Two sets o f experiments were conducted, (a ) by varying the argon
69 and oxygen gas flow rate and maintaining a constant deposition t ime and (b ) by keeping the gas flow rat e constant and varying the deposition time. Under these conditions, the thickness of the deposited film was measured and the optimal parameters were utilized in the actual fabrication of the MIM diode. T he thickness was monitored using a quartz crystal mon itor and also evaluated by ellipsometry and Atomic Force Microscopy (AFM). The thickness of the dielectric film was found to be in the range of ~ 3 5 nm, assuming the refra ctive index of NiO to be 2.33  The dielectric surface was studied and the roughness was estimated by performing tapping mode AFM. Figure 5.12 shows the AFM morphology of NiO The thin film examined at a scan rate of 1 Hz over an area of 8 m 2 indica ted a surface a roughness of 0.4 0 .6 nm. From the AFM analysis it can be observed that some spikes are present on the film, which might affect the devices if the MIM junctions were fabricated on such regions. The feature sizes of the spike were determined to be varying from 0.5 nm to 3 nm. A possible explanation of these spike formation s may be due to the presence of dirt in the underlying film/ substrate. Moreover, the AFM analysis was performed on a test sample, which was more susceptible to the normal environment. If the spikes were pres ent in an actual diode, the junction would be short circuited, but this scenario was not observed in the fabricated diodes, confirming the presence of a defect free barrier layer.
70 Figure 5.12 AFM M icrograph of a Silicon Substrate Deposited with NiO T able 5.1 shows the thickness of the insulator layer deposited under various conditions. The insulator was deposited for 10 15 mins with varying gas flows of Ar and O 2 with 1:1 and 2:1 gas ratio. From Table 5.1 it is observed that for a 10 mins deposition time with 1:1 gas ratio, the thickness and the roughness of the insulator were very high. Similar results were observed with 2:1 gas ratio for the same time (10 mins). When the deposition time was increased to 15 mins, the thickness of the films was incre ased and the surface roughness was redu ced. As suggested by Chapman  during the sputtering process, the material arriving at the substrate will be in atomic or molecular form. These atoms begin to nucleate forming islands of atoms, at which point the thickness and the roughness of the films will be comparable. But over a period of time, these atoms coalesce to form a thin layer of film with uniform thickness and less surf ace roughness.
71 For the fabrication of the MIM diode, NiO was deposited under 2:1 Ar O 2 gas ratio for 15 mins. Table 5.1: Gas Ratio vs. Roughness and Thickness Estimate of the Dielectric L ayer Gas Ratio Ar: O 2 AFM roughness Ellipsometry thickness 1:1 (1 0 mins) 20.0 24 to 30 1:1 (15 mins) 8.0 28 to 30 2:1 (10 mins) 16.0 15 to 22 2:1 (15 mins) 4.0 to 6.0 20 to 24 The thickness of the NiO layer was also verified from a cross sectional SEM analysis of the MIM diode. It was convenient and accurate to estimate the NiO thickness when Au was used as the top electrode instead of Cr. Figure 5 .13 shows the cross sectional SEM image of the MIM diod e with a thin, homogenous layer (~5.5 nm) of Nickel Oxide.
72 Figure 5.13: SEM Micrograph Showing the Cross Section of a MIM Diode 5.4 .2 Polyani line Polyaniline with 50K mol. w t. was obtained from Sigma Aldrich. Polyaniline was dissolved N methyl 2 pyrrolidinone (NMP) containing 60% CHCl 3 The dissolved mixture containing 0.8 mg/ml of P Ani was taken in a microlitre syringe and kept ready The LB film deposition was done using N IMA Technology's LB trough (model 611D) shown in Figure 5.14
73 Figure 5.14: Visual of the L B Trough Used for Polyaniline D eposition From  This deposition process requires an ultimate clean trough, since any dust particle present in the surface may cause a change in pressure. Hence the trough was thoroughly cleaned with CHCl 3 and dried with N 2 The trough was checked for any unevenness on the surface due to presence of impurities by filling the trough with Millipore DI water. The pH of the DI water was maintained at 7 by the MilliQ system. The surface pressure is measured by the Wilhelmy plate method. In this method a measurement is made by determining the force due to surface tension on a plate suspended so that it is partially immersed in the subphase (see Figure 5 .15 ). This force is then converted into surface tension (mN/m or dynes/cm) with the help of the dimensions of the plate. The Wilhelmy plate is hung from a Langmuir film balance to measure the surface pressure and barriers for the available surface area.
74 Figu re 5.15: Schematic of a Wilhelmy Plate Balanced in a Langmuir T rough Fr om  After establishing a clean surface, the Ni coated substrate was immersed in the LB trough using a computer controlled dipper. A barrier scale used to compress the organic layer was pulled back and polyaniline was introduced in the trough. Later, the dissolved P Ani mix was introduced over the DI water surface, while observing the change in pressure through the Wilhelmy plate and balance After reaching a constant pressure isotherm, the barrier is closed. The pressure area isotherms of the polyaniline monolayer were performed at a barrier compression speed of 10 cm 2 /min at room temperature. Then the dipper was slowly pulled out at a rate of 2 mm/min to deposit a monolayer of polyaniline. The pressure area isotherm obtained while coating the Ni sample with polyaniline is shown in Figure 5.16.
75 Figure 5.16 Pressure Area I sotherm of PANI The pressure area isotherm plot shows the various phases of the polyaniline layer as it gets transferred to the Ni film. When the barrier is compressed, more polyaniline layer is forced into a smaller surface area and when the sample is lifted, the polymer layer sticks to the surface. The base flat line shows the liquid phase of the polymer layer which transforms to a solid phase as observed from the knee of the plot. Thus a monolayer of polyaniline is coated on the Nickel layer forming an ultra thin dielectric for the hybrid MIM diode.
76 5.5 Comments on Fabr i cation Procedure (a) Step Coverage: The contact area of the MIM diodes was designed to be 1 m 2 to operate at 94 GHz. This active area of the device was fabricated using e beam lithography, since a high resolution optical lithography tool was not a vailable. Thus for developing the 1 m 2 diode, optical as well as e beam lithography process had to be utilized. As mentioned in the processing sequence, the contact pads and the bottom electrodes were fabricated using optical lithography, while the top el ectrode was fabricated using e beam lithography. In the e beam lithography process, PMMA was used as the photoresist. PMMA, when dispensed on the wafer yields a very thin layer in the range of 150 nm. This restricts the metal deposition to 70 100 nm. Thi s would cause a potential sidewall coverage issue. By increasing the thickness of the e beam resist the step coverage issue in the diode can be minimized. Adding another layer of e beam resist called the bilayer PMMA (PMMA Co MAA) will increase the thickn ess of the overall resist layer  The additional layer of polymer provides extra thickness of about 500 nm, allowing us to deposit a thicker top electrode and also provides an undercut during the e beam litho process, facilitating the lift off process. (b) Con tact Area Alignment: Another issue with e beam litho graphy wa s the di fficulty in aligning the top electrode to define exactly 1 m 2 by intersecting the bottom electrode. Since no
77 alignment markers were made for the e beam litho process, all the diodes had to be individually patterned. This gives more room for error since every diode has to be manually aligned. A virtual alignment mark, which can be enabled in the JEOL SEM, was used to ballpark the starting point of the design. Hence the contact area of the diode might not be exactly 1 m 2 as expected. This would affect the operational frequency of the diode. (c) Silicon Membrane Etch: The MIM diodes fabricated for MMW measurements were developed on a silicon membrane. The ideal thickness to minimize surfa ce wav e loss was determined to be 10 m. This was accomplished by etching the silicon substrate by performing a wet chemistry process as described earlier. A timed etch procedure was carried out by determining the initial thickness of the substrate and the etch rate of the silicon etchant. Howev er, as the etching process begins, the reactivity of the etchant decreases, causing a slower etch rate. Hence, a close watch had to be kept during the entire etching process to maintain the etch rate by adding newer solution or by determining the extra tim e the etch process would take. Additionally, since the silicon substrate has a native curvature, the etched profile would also display the same trend. Figure 5.17 shows the variation in membrane thickness obtained after performing silicon etching.
78 F igure 5.17: Profilometer Plot Illustrating the Non Uniformity in Etch P rofiles In s ummary, MIM diodes were designed with t wo different contact areas (100 m 2 and 1 m 2 ). Ni NiO Cr was used as the material combination for developing these diodes. The fabrication methodologies were identified and the diodes were fabricated with optical and e beam lithography. Finally, an alternate method to deposit a thin layer of polymer was also identified and the MIM diodes were fabricated with a polymer insulator. In addition, some of the key problem areas were also identified which might affect the device performance.
79 CHAPTER 6 RESULTS DC MEASUREMENTS 6 .1 Experimental I V Characteristics of MIM Diode The dc I V characteristics of the fabricated MIM diodes were measured at room temperature using a HP4145B semiconductor parametric analyzer connected in series with a p robe station (Cascade Micromanipulator) The diodes were probed using titanium coated probe tips with 1 m diameter. The measurement unit w as connected to a PC via a General Purpose Interface Board (GPIB) and the data points were recorded using Metrics In c., Interactive Characterization Software. The dc characteristics of the diodes were measured under a two terminal arrangement s; the measurements being tak en in the forward and reverse bias conditions. The I V behavior of the diodes was obtained by applyin g voltages fro m 0.5 V to +0.5 V. The experiments were limited to these voltages since higher bias voltage s could result in dielectric breakdown of the insulator layer. 6.1.1 I V C haracteristics of MIM Diode with 100 m 2 Contact Area A typical I V curve of Ni NiO Cr MIM diode fabricated with 100 m 2 contact area is shown in Figure 6.1 T he MIM diodes exhibited non linear and asymmetric behavior at 0. 5 V of applied bias. A t very low voltage s (< 0.2 V) the diode exhibits
80 linear response, since the current is proportional to the applied bias. But, beyond this initia l voltage (V > 0.2 V) a non linear response is obtained The MIM junctions exhibited current in the range of 9 A to 11 A when a bias voltage was swept from 0.5 V to +0.5 V. The resistance exh ibited by these diodes was typically in the range of hundred k" Figure 6.2 shows the distribution of zero bias resistance of all the diodes. The I V characteristics of different diodes fabricated in this research are shown in Appendix C. Figure 6.1 : Typ ical I V Characteristics of MIM D iode with 100 m 2 Contact Area
81 Figure 6.2: Distribution of Zero Bias Resistance of 100 m 2 MIM Diode The performance of the diode is characterized by its current sensitivity and detectivity. Maximum sensitivity is obtain ed at a DC bias point where maximum curvature of t he I V characteristics occurs  The sensitivity was obtained from the I V plot by obtaining the first and second derivatives and then taking the ratio of the second to the first, as given by (6.1 ) Where, I ( v ) = d 2 I dv 2 (6.2 ) And,
82 I ( v ) = dI dv (6.3 ) The first derivative of the I V plot shows the measure of rate of change of conductance with applied voltage, and provides a useful way o f comparing the forward and reverse characteristics. The second derivative of the I V plot shows the non linearity of the diode. The ratio of second derivative to the first derivative obtained from the I V plot gives the sensitivity of the diode, which cha racterizes the diode performance. Figure 6.3 shows the first derivative or the rate of conductance obtained from the I V characteristics of the MIM diode. Figure 6.3: Rate of Conductance of MIM Diode with 100 m 2 Contact Area
83 The asymmetry in the I V p lot is more pronounced in the rate of conductance vs. voltage plot, showing the existence of a difference in work function between the metal electrodes. The difference in work function between Ni and Cr is around 0.65 eV. Even though this difference is not large, asymmetrical and non linear behavior was demonstrated. Figure 6.4 shows the sensitivity of the diode. The peak sensitivity was around 15V 1 which is the highest obtained value for a room temperature measurement. The distribution of the peak sensit ivity obtained for the 100 m 2 MIM di odes are displayed in Figure 6.5 The sens itivity of 10 different diodes o n the same substrate was calculated from its corresponding I V characteristics. It can be observed that the sensitivity of all the diodes has bee n consistent throughout the substrate demonstrating a fair level of uniformity. Figure 6.4: Sensitivity o f MIM Diode with 100 m 2 Contact Area
84 Figure 6.5 : Distribution of the Peak S e nsitivity for 100 m 2 MIM D iodes 6.1.2 I V Characteristics of MIM wi th 1 m 2 Contact Area Following the measurement of 100 m 2 diode, the I V characteristics o f 1 m 2 diode was measured using the same test set up. The voltage was swept from 0.5V to 0.5V and the corresponding current was recorded. I V characteristics of a typical MIM diode with 1 m 2 contact area are shown in Figure 6.6. The forward and reverse currents were in the range of 2.5 A to 3 A. From Figure 6.6 it is observed that the diode exhibited a minimal asymmetry. The zero bias resistance of the diodes w as determined to be in the range of few hundred k" Figure 6.7 shows the distribution of zero bias resistance throughout the wafer. The I V characteristics of all the 1 m 2 MIM diodes measured is shown in Appendix C.
85 Figure 6.6 : Typical I V C haracteristi cs of MIM D iode with 1 m 2 Contact Area Figure 6.7: Distribution of Zero Bias Resistance of 1 m 2 MIM Diode
86 Although the I V plot exhibits a minimal asymmetry in the device, the actual asymmetry of the diode can be better observed from the first deri vate plot of the I V behavior. Figure 6.8 shows the rate of conductance plot of a typical MIM diode. This demonstrates the difference in the forward and reverse bias region of the diode. Figure 6.8: Rate of C onductance of MIM D iode with 1 m 2 Contact Ar ea Additionally, the sensitivity of the diode was determined by finding the ratio of the second derivative and first derivative of the I V characteristics. The diodes exhibited a maximum sensitivity value of 7 V 1 as shown in Figure 6.9. The sensitivity o f all the diode fabricated was determined to show the distribution. Figure 6.10 shows the distribution of diode sensitivity through the substrate. The sensitivity values were found to be varying from 7 to 3.5 V 1
87 Figure 6.9: S ensitivity of 1 m 2 MIM dio de Figure 6.10: Distribution of Peak Sensitivity Obtained for 1 m 2 MIM Diodes
88 6.1.3 I V Characteristics of Polymer MIM Diode: After establishing the electrical characteristics of MIM diodes with Ni NiO Cr, MIM diodes fabricated with Ni PANI Cr were i nvestigated. In this section the I V characteristics of MIM diode fabricated with Ni PANI Cr is presented. These diodes were fabricated with a 100 m 2 contact area. The I V characteristics of a polyaniline based MIM diode is shown in Figure 6.11. Figu re 6.11: I V Characteristics of MIM Diode with Polyaniline Insulator The diode exhibited highly non linear and asymmetric I V characteristics at applied bias of 1 V. Although the diodes exhibited very small forward current (in the order of nA), the revers e bias current was very negligible. The forward current at +1 V is ~4.5 nA, and the reverse current at 1 V is in the pA range. Similar to the Ni NiO Cr
89 diodes, the polyaniline based diodes also exhibited very low current in low voltages. When the bias vol tage was increased above 0.2 V the output current increased. However, this increase was not comparable to the Ni NiO Cr diodes. The resistance of these diodes was very high (unlike the solid state diodes discussed earlier); typically in the range of a few hundred M Typically the resistance of the diode increases when the thickness of the dielectric increases, thereby reducing the probability of electron tunneling. The thickness of the polyaniline deposited in this fabrication process is estimated to be 2 to 3 monolayers. However, the thickness of the polyaniline could not be measured. From the I V data of the diode it can be stated that, either the diode has a thick insulator layer sandwiched between the metal electrodes or the barrier height formed by th e Ni Polyaniline interface is high. When compared with the NiO based MIM junction, this diode exhibits better asymmetry suited for detector applications. However, the resistance is higher than the NiO tunnel junctions making it less suitable for any applic ation. Hence the barrier layer needs to be investigated to achieve better diode characteristics. A noteworthy point to mention is that the polyaniline was deposited using the previously mention L B process, after which it was subjected to other harsh chemi cals and a photolithography process for defining the top electrode. Hence, the polymer layer might have degraded resulting in the high resistance I V characteristics. Additionally, the polyaniline was deposited on Ni surface, which tends to form a native o xide upon exposure to air. This could have caused a Nickel Oxide formation thus creating a dual barrier. This native oxide formation could contribute to the increase in dielectric
90 thickness, thereby reducing the tunneling current. Therefore, to achieve bet ter diode characteristics with polyaniline insulator, the diode processing should also be done with minimal chemical exposure and the polyaniline should be carried out in an inert atmosphere to avoid native oxide formation. 6.2 The oretical DC I V Characte ristics The tunneling equation given in chapter 3 was used to compare the actual device data. To do this it was necessary to determine the parameters s, 1 and # The value of # can be determined from the difference in work function of the metals, Ni an d Cr. Thus # is determined to be 0.65 eV. The thickness of the insulator layer was determined to be 3 nm from the ellipsometry measurements. Finally, the barrier height 1 is related to the work function of metal 1 and the activation energy of NiO as descr ibed in Eq. 3.1. The activation energy of NiO is approximately 0.6 eV  Thus the barrier height 1 is determined as, 1 =5.15 0.6 = 4.5 eV. Using these parameters, the theoretical I V c urve was determined. Figure 6.12 shows the I V curve for Ni NiO Cr diode with dielectric thickness as 3 nm 1 as 4.5 eV and # as 0.65eV. It is observed that the the oretical curve is largely asymmetric and non linear with current in the range of pA. Hence exhibiting a huge resistance in the order of hundreds of G
91 Figure 6.12: Theoretical I V C urve for s= 3 nm, 1 = 4.5eV and " = 0.65eV Although the barrier hei ght was determined as 4.5eV from the equation, that may not be the case when considering the actual barrier height between the metal 1 and interface. Hence for a barrier height of 4.5 eV and thickness of 3 nm, the probability of electron tunneling will be low, yielding lower current as demonstrated by the theoretical plot. But the current obtained by the fabricated diodes is higher than the theoretical value for the same dielectric thickness. Hence the barrier height has to be changed to match the experimen tal value. Typical barrier heights reported in the literature for Ni NiO interface were usually 0.2 eV to 1 eV  So the theoretical tunnel equation was calculated using these barrier height values. Figure 6.13 shows the theoretical curve plotted using 1 a s 0 9 5 eV 2 a s 0.3 eV and dielectric thickness as 3 nm. It is observed that this theoretical result matches
92 the actual results than the previously obtained theoretical plot. A possible explanation for the lower effective barrier might be that for thi n oxides (3 nm), the barrier does not necessarily have a long periodic structure, consisting of only few monolayers. This might produce a reduced barrier height, which is not accounted for in the tunneling equation. Additionally, the image charges reduces the barrier height, which is not taken into account. These combinations would have reduced the effect barrier height of the junction. Figure 6.13 : Ex perimental and Theoretical I V C haracteristics of MIM Diode
93 6.3 Comments on DC Characteristics of MIM Diodes MIM diodes with two different contact areas (100 m 2 and 1 m 2 ) were fabricated with Ni NiO Cr and tested for its DC I V characteristics. Although the I V characteristics of the diodes were similar, the output current, sensitivity and the zero b ias resistance (ZBR) exhibited by the diodes vary. Table 6.1 shows the variation in the electrical characteristics of the measured diodes. Table 6.1 Electrical Characteristics of MIM D iode Diode Area 100 m 2 1 m 2 Current 10 A 5 A ZBR 500 K 800 K ~ 900 K Sensitivity 15 V 1 7 V 1 It is observed that as the diode area decreases from 100 m 2 to 1 m 2 the current and sensitivity drops while the zero bias resistance increases. However, the size of the contact area affects the diode behavior, there are other factors that contribute to this variation. Upon close observation of each diode, it can be noted that, the current varies from diode to diode on the same substrate. This is due to the variation in dielectric thickness across the device. The variatio n in dielectric thickness or roughness can change the device parameters. The dielectric thickness in the fabricated MIM diode was determined to be 3 nm using an ellipsometry technique, but was observed to be ~ 5 nm in the cross sectional SEM image shown in the previous chapter. As reported in 
94 disorder effects in MIM junctions are highly unpredictable. Hence even a small thickness variation i n the dielectric layer could cause a large fluctuation in its electrical behavior of the diode. The formation of the dielectric layer seems to be very sensitive, which alters the uniformity of the film even when the samples were pr ocessed under the same c onditions. Although an optimized deposition condition was established, the dielectric thickness varies from device to device as observed from the output current. Sze  indicated that even if the dielectric is not uniform, the thinnest portion in the oxide la yer seems to be responsible for the tunneling current. This ensures that, as long as the dielectric layer is thin and without any micro or nano pores, conduction would take place and the current observed will be an inverse function of dielectric thickness. Furthermore, the roughness of the dielectric layer was determined in the previous chapter to be ~ 0.6 nm in a 3 nm film. The surface non uniformity influences the current voltage characteristics by increasing the active area of the diode. Eventhough the contact area of the diode is estimated to be 1 m 2 due to film roughness and lithographic misalignment the actual area responsible for conduction can be more than expected. This can further reduce the device performance. S everal other factors can also con tribute to the dielectric variation beginning with the sample placement on the substrate holder to the slight environmental variation in oxide deposition conditions which might alter the roughness of the top and bottom interfaces of the oxide layer 
95 6.4 Temperature Dependency of MIM Diodes Tunnel diodes are capable of carrying large currents. The flow of this current results in joule heating of the diode stack. Hence the thermal stability and response of the diode is a critical parameter that needs to be understood to ensure that the diode is not overloaded. In this section the temperature dependency of a MIM diode at high temperature will be discussed. The MIM diodes developed earlier reported the electrical parameters and other figures of merit exh ibited at room temperature  However, the performance of the Ni NiO Cr with an ultra thin insulator layer at elevated temperatures has never been report ed A comprehensive understanding of thermal stability and response of the MIM diodes is critical prior to its use in commercial products. In this experiment the diodes were heated to different temperatures up to 400C and then tested again to evaluate th eir electrical characteristics, particularly the I V characteristics, zero bias resistance and sensitivity of MIM junctions. The resistance and the sensitivity were extracted from the curre nt voltage (I V) curve. For this experiment a MIM diode with 100 m 2 contact area was selected, due to the relative ease of measurement and an insulator are large enough to verify the morphology at different temperatures. 6.4.1 Electrical Characterization For the post deposition annealing process, a ceramic hot plate was utilized. The samples were annealed at 250 ¡ C, 350 ¡ C and 400 ¡ C for 15 minutes under ambient conditions and then the I V measurements were determined for the diffe rent temperature
96 variants at room temperature. Post deposition annealing is known to improve t he electrical properties of thin film diodes [63, 64] and the resistivity of NiO thin films have been reported to change w hen the structure changes from amorphous to polycrystalline at higher substrate temperatures  Figure 6.14 shows the I V plot of the MIM diodes measured after annealing at four different temperatures. Figure 6.14: I V Characteristics of MIM Diode Annealed at Different T emperatures As can be seen from F igure 6.14 all the diodes exhibited non linear and highly asymmetric characteristics with higher current output than the unannealed diodes. From
97 F igu re 6.14 it can be observed that the un annealed diode exhibits a forward bias current of ~ 2 mA. When the diodes were subjected to heat treatment; at 250 ¡ C, the forward bias current increased to ~20 mA. Upon increasing the annealing temperature to 350 ¡ C, the current reduced to 10 mA. Finally, when the diodes were subjected to a temperature of 400 ¡ C, a steep drop in current to the range of few nA was observed. Additionally, from the I V characteristics, the sensitivity of the dio des was also extracted. Figu re 6.15 shows the sensitivity of the MIM diodes annealed at various temperatures. Figure 6.15: Sensitivity of MIM Diode Annealed at Different T emperatures For the un annealed dio des, the sensitivity was foun d to be 14V 1 which was typical for the 100 m 2 MIM diode The diodes annealed at 250 ¡ C had an increased electrical response with a very high sensitivity of 42V 1 Upon increasing the annealing
98 temperature to 350 ¡ C, the diode current dropped, but still was higher than the room temperature diode and the sensitivity was determined to be 23V 1 This demonstrates that the diode is still operational, even though the current and sensitivity dropped. When the diode was further annealed at 400 ¡ C, the current dropped instantaneously ; exhibiting a very low sen sitivity of 4V 1 To better understand this behavior, the resistance at zero bias was determined from the I V characteristics, since it is exponentially dependant on the width of the tunneling layer. Figure 6.16 shows the variation in sensitivity and zero bias resistance with change in the annealing temperature on the MIM diode. T he un annealed diode exhibits a zero bias resistance of ~800 which decreases to ~300 whe n the diode was annealed at 250 ¡ C. When the diode was further annealed the zero bias res istance increased to ~ 1400 However, when the annealing temperatures exceeded 400 ¡ C, the zero bias resistance increased sharply to the G range causing the diode to be un operational.
99 Figure 6.16: Zero Bias Resistance of MIM Diode Annealed at Differe nt T emperatures A simil ar phenomenon was observed in [63, 64] wherein the current increases upon increasing the annealin g temperature causing lowering of barrier height between the oxide and metal interface. This decrease in barrier height causes more electrons to tunnel through the insulator layer. However, when the annealing t emperature was increased to 350 ¡ C, we observe a drop in current and sensitivity. This can be attributed to the increase in barrier height and width due to the interdiffusion of metal and oxides which reduces the probability of electron tunneling Also the structural transformation of th e insulator la yer and possible O 2 deficiency in the insulator layer can be contributed to the
100 degradation in the electrical characteristics of the MIM diode. The un annealed diodes exhibit a low electrical response, which is enhanced by annealing it to 250 ¡ C and degrade s upon subjecting them to further annealing. At 250 ¡ C, the electrical as well as structural changes affect the MIM stack, especially the insulator layer. Hence the structural analys is of the MIM junction needs to be analyzed. 6.4.2 Structural and Morphol ogical Characterization (a)
1 01 (b) (c)
102 (d) Figure 6.17: AFM Micrograph of Samples Annealed at (a) Room Temperature, (b) 250¡C, (c) 350¡C, and (d) 400¡C AFM data shown in Figure 6.17 represents the effect of annealing temperature on the surface mo rphology of NiO films deposited by plasma oxidation. T he un annealed sample exhibits a uniform amorphous film as seen in Figure 6.17(a), over the 10 m 2 area. The surface roughness of the un annealed film was determined to be 0.6 nm on a ~ 5 nm thick NiO film. A s t he temperature was increased, NiO grains of varying sizes st arted to appear. Figure 6.17(b) shows the AFM morphology of the sample annealed at 250 ¡ C. It is observed that the film is very uniform with 0.37 nm surface roughness. Upon annealing at 250 ¡ C the roughness of the diode decreases, causing enhanced electrical response. However, the roughness of the NiO film increases as the annealing temperature
103 further increases. Figures 6.17(c) and (d) show the NiO film annealed at 350 and 400 ¡ C respectively, exhibiting larger grain size and inhomogeneous surface. The roughn ess of the 350 and 400 ¡ C samples was determined to be 5.4 and 7 .2 nm respectively. The roughness of the NiO film initially drops at 250 ¡ C, but tends to increase with higher temperature, suggesting the formation of a crystalline phase and also due to dimini shing grain boundaries. But with higher temperatures lattice mismatch occurs increasing the grain growth and making the structure more crystalline. Figure 6.18: XRD Pattern for NiO Films Deposited Through Plasma Oxidation and A nnealed at Different T emper atures
104 Figure 6.18 shows the XRD pattern for NiO films deposited with plasma oxidation and annealed at temperatures varyi ng from room temperature to 400 ¡ C. From the XRD spectra of the NiO films it was found that the oxide films had both amorphous and pol ycrystalline structures. The diffraction pattern for the un annealed sample shows a NiO peak with low intensity. These films exhibited less current due to the amorphous nature of the film. On the other hand, the diffraction patterns of the annealed samples show the presence of diffraction peaks with a NiO (200) orientation. As the annealing temperature increases, the crystallinity increases (shown by increased peak intensity), causing an increase in current tunneling through the insulator layer. At 350 ¡ C, w e observe a drop in tunneling current, which drops steeply when the annealing temperature was increased to 400 ¡ C. Also it is noted that the intensity of the peak increases with a strong (200) peak indicating increased crystalline structure. Hence this data agrees with the AFM as well as the electrical response of the MIM diode at different tempera ture. The XRD and AFM analysis clearly shows the structural transformation for NiO films annealed at different temperatures. This analysis suggests that although amorphous structure s yield good electric al characteristics, annealing to 250 ¡ C improves the electrical response By annealing to 250 ¡ C, the insulator layer undergoes a phase transformation from being amorphous to polycrystalline, forming a homogenous film with less surface roughness than the un annealed film. This causes the diode to conduct more current through the NiO layer. The samples annealed at 350 and 400 ¡ C exhibited a more crystalline surface with much larger grain sizes, thus impeding the tunneling of electrons through the insulator layer.
105 As mentioned earlier, the insulator layer was deposited by plasma oxidation at low substrate temperatures, typically depositing a uniform amorphous film. Formation of polycrystalline NiO seems to stabilize the el ectrical property and enhance the thermal stability of the material. However a crystallized film demonstrates degradation in electrical characteristics. In order to understand the physical nature of the insulator layer changing from amorphous to crystallin e by post deposition annealing, a cross sectional TEM study was performed. Figure 6.19 shows the microstructural TEM images of a MIM diode annealed at different temp eratures. (a)
106 (b) Figure 6.19: TEM M icro graph of MIM diode Annealed at (a) 250¡C and (b) 3 50 ¡ C Figure 6.20: TEM M icrog raph of MIM Diode Annealed at 40 0 ¡ C
107 Figure 6.21: E nergy D ispersive S pectra Showing the Diffusion L ength of Annealed M aterials. Data shown in Figures 6.19 (a) and (b) were obtained fro m samples subjected to 250 and 350 ¡ C anneal ing, respectively. The cross sectional micrograph of the as deposited MIM diode shown in a previous chapter exhibits a distinct transition between each layer. Similarly the sample annealed at 250 ¡ C shown in Figure 6.19(a) also exhibits a defini te boundary between each layer. Moreover, the insulator region exhibits a polycrystalline structure with finer grain as confirmed by the AFM morphological analysis. However, the sample annealed at 350 ¡ C shows a clear crystalline structure as can be observe d in Figure 6.19(b), which correlates with the XRD data. The inset micrograph shows the MIM stack with different layers. This phase transformation of the insulator layer provides evidence for the decrease in current and sensitivity.
108 When compared with the TEM image of the MIM junction annealed at 350 ¡ C, the film annealed at 400 ¡ C shown in Figure 6.20 has a deteriorated film structure. Specifically, the individual layers were merged at the higher annealing temperature. A diffused boundary between the Ni and Au layer can be observed from Figure 6.20. In order to identify the composition of the film annealed at 400 ¡ C, the energy dispersive spectrum (EDS) was obtained on the TEM. The spectrum with different layers in the MIM stack is shown in Figure 6.21. It i s well known that the high temperature annealing can cause diffusion of the elements in different layers. As shown in Figure 6.21, the EDS spectrum shows a large intensity of Ni and Au than any other element, revealing the diffusion length of different el ements in the MIM structure. As evaluated earlier, the Au layer has diffused all the way to the Ni layer through the insulator suggesting the diffusion of Au as the cause for the device breakdown at annealing temperatures over 350 ¡ C. Thus, these experimen ts provide the data for efficient operation of MIM diodes up to 350 ¡ C. Although the diode operates well at room temperature, annealing it to an optimal temperature (250 ¡ C in this case) enhances the performance of the diode. The annealed diode exhibits high er current, sensitivity and low zero bias resistance. Based on these results, it is suggested that the annealing temperature must be restricted to temperature below 350 ¡ C to minimize the degradation in electrical properties caused by the crystalline nature as well as the interdiffusion of the MIM layers. Nevertheless, the electrical and structural analysis suggests 250 ¡ C i s the optimal temperature at which the MIM can perform with better characteristics
109 6.5 Thi ckness Dependency of MIM Diodes As mentioned e arlier, the conduction in a tunnel junction is limited by the dielectric thickness. In order to facilitate electron tunneling, the insulator layer has to be fabricated with a very thin film on the order of few nanometers. In this section, the thickness d ependency of a MIM diode on its electrical performance will be discussed. For energy conversion and detection purpose MIM diodes are typically fabricated with an ultra thin insulator layer. In this experiment, MIM diodes were fabricated with three differen t thicknesses of insulator; specifically 40, 20 and 10 nm thick dielectric was deposited. The electrical characteristic of each diode was then measured using the previously mentioned test set up. Figure 6.22 (a), (b), (c) shows the I V characteristics of M IM diodes with different dielectric thicknesses. (a)
110 (b) (c) Fi gure 6.22: I V Characteristics of MIM Diode Deposited with (a) 10 nm, (b) 20 nm and (c) 40 nm NiO
111 As can be seen from F igure 6.22 all the diodes exhibited non linear and hi ghly asymm etric characteristics, but with much lower current The diode deposited with 10 nm of NiO exhibited a maximum forward bias current of ~ 100 n A. When the thickness was increased to 20 nm, the diode exhibited a drop in tunneling current. The maximum forward bias current at 1V was in the order of ~ 20 nA. The diodes with the hig hest thickness of 40 nm yielded a maximum tunneling current of 1 nA. Hence, when the thickness of the dielectric doubles, the current decreases by a factor of five. It is observed that the variation in current at forward bias for a 10 nm thick dielectric is noticeably large compared to 20 nm and 40 nm MIM junctions. This suggests that at lower thickness, the uniformity is being compromised across the diode. This experiment verifies the dependency of tunneling current on dielectric thickness. Thus, in order to obtain higher current output, the dielectric thickness should be very thin and uniform In summary, all the MIM diodes fabricated with NiO as well as polyaniline insulator exhibited significant asymmetry and nonlinearity. The sensitivity obtained from these diodes was also significantly higher than any reported value. Also, when the diodes were subjected to heat treatment, the electrical characteristics were observed to be stable up to 350¡C, while the optimal anneal temperature for better diode perform ance was determined to be 250¡C. The sensitivity of the diodes also increased upon annealing. In addition, when the dielectric thickness was increased a significant drop in the current was observed proving the dependency of electrical characteristics on the insulator thickness. A comparison table is presented showing the sensitivity obtained by different research
112 groups. Table 6.2 presents a comparative table showing the sensitivity valu es obtained by different research groups using different design and material combinations. Table 6.2: Comparison of Sensitivity of MIM D iodes Fabricated by CERC with other Research Groups Research Group Type of MIM diode Junction Area Sensitivity Heiblu m et. al.  Ni NiO Ni 3.8 m 2 4.3 V 1 Hoofring et. al.  Ni NiO Au 0.64 m 2 4.55 V 1 UCF CREOL  Ni NiO Ni 0.075 m 2 2.75 V 1 ETH, Zurich  Ni NiO Ni 0.056 m 2 1.6 V 1 UND  Ni NiO Pt 0.0025 m 2 13 V 1 UND  Al Al 2 O 3 Pt 0.0025 m 2 1 3 V 1 UND  Al Al 2 O 3 Ni 0.0025 m 2 1 V 1 UND  Al Al 2 O 3 Al 0.0025 m 2 1 .4 V 1 CERC Ni NiO Cr 100 m 2 14 V 1 CERC Ni NiO Cr 1 m 2 7 V 1 CERC Ni NiO Cr Annealed at 250 ¡ C 100 m 2 4 2 V 1
113 CHAPTER 7 LOW FREQUENCY AND MILLIMETER WAVE MEASUREMENTS In this chapter the low frequency and mm wave wav e response of the MIM diode is discussed. Low frequency measurements were performed on the 100 m 2 area diode and the 1 m 2 area diode while mm wave measurements were carried out on the 1 m 2 MIM diode. Millimeter wave measurements were performed by feeding a 94 GHz signal to the individual diode elements through a waveguide. The rectified output was observed and recorded through a high precision digital multimeter. 7.1 Experimental Arrangement: The low frequency mea surement of 100 m 2 diode and 1 m 2 diode was performed using a different set of measurement units. For the 100 m 2 diode, since the operation frequency was much lower, a function generator from Agilent Technologies (Model 33220A) was used as the input sou rce. The output from the diode was recorded using a digital oscilloscope from Tektronix (Model TDS 3014). The diodes were connected via a coaxial cable through a probe station from Micromanipulator Company, Inc., (Model 6200). The function generator can pr oduce frequencies up to 20 MHz with a maximum 10 V peak peak, while the oscilloscope was capable of exhibiting up to 5 MHz signal on 4 channels. A schematic arrangement for measuring the 100 m 2 MIM diode is
114 shown in Figure 7.1 (a). The input signal from the function generator was also hooked up to one of the channels in order to compare the input and output signal. (a) (b) Figure 7.1 : Schematic of the Test Set up U sed for Measuring the Low Frequency B ehavior of (a) 100 m 2 and (b) 1 m 2 Area MIM D iod e
115 The low frequency response of the 1m 2 diode was measured in a different set up since the input signal source had to be more than 20 MHz. For this purpose, a network analyzer was used as the signal source along with a high frequency oscilloscope. The ne twork analyzer used for this purpose was Agilent's 8713D capable of generating signals up to 13 GHz. Similar to the low frequency measurement, the input from the network analyzer was connected to one of the channels on the oscilloscope and to the input of the diode through a high frequency gold coated probe. A Karl Suss semi automatic (Model SA 5) probe station was used for this purpose. The output of the diode was connected to the digital oscilloscope via the probe station. The experimental arrangement fo r this measurement is very similar to the previous measurement set up, shown in Figure 7.1 (b). The mm wave measurements were carried out with the experimental arrangement shown in Figure 7.2. A Wiltron 360B vector network analyzer (VNA) was used as the s ignal source for mm wave measurement through a waveguide conversion module. The input signal was fed to the diode through the gold transmission line and the output of the diode was connected to a high precision digital multimeter from Keithley Instruments Inc., (DMM 2000). The VNA also has the capability to change the input power that can be added to the source signal. The probe station used for this measurement was the same as the one used for low frequency measurements. However, for the high frequency mea surement, to minimize signal losses, special types of probes were used. The probes were connected to the waveguide of the VNA module and had a probe pitch of 150 m, which was the spacing for the CPW lines fabricated along with the MIM diodes.
116 Figure 7.2: Schematic of the Test Set up U sed for Millimeter Wave Measurement Figure 7.3 : Actual Millimeter Wave Test Set up Used to Measure the MIM Diode
117 7.2 Experimental Results 7.2.1 Low Frequency Characteristics of 100 m 2 MIM Diode In order to verify the concept of rectification in the MIM diode, the low frequency behavior of MIM diode fabricated with 100 m 2 contact area was measured. A function generator provided an AC signal and the DC out was measured using an oscilloscope. The function generator w as connected to one terminal of the diode and the output was connected to the oscilloscope. The cut off frequency was determined to be around 1 MHz from the previous chapter; hence the input frequency was kept on the lower end and gradually increased. The input and the output signals observed on the oscilloscope are shown in Figure 7.4. Initially, the input frequency was kept at 100 Hz with 0 V offset voltage and a 2 V peak peak voltage. The forward voltage was observed to be 29 mV and reverse voltage was 3 4 mV. This reversal in polarity is due to the interchange of input and output lines.
118 (a) (b) Figure 7.4: Rectification of 100 m 2 MIM D iode at (a)100 Hz and (b)1 KHz
119 Figure 7.5: DC O ut put S ignal of MIM Diode with a Ramp F unction Later the input frequency was increased to 1 KHz and the corresponding output was observed. Figure 7.4 shows the AC and DC signal observed form the diode at 100Hz and 1KHz. The diodes exhibited the same response when the frequency was increased. The forwar d voltage was observed to be 26 mV and the reverse voltage was 38 mV. Figure 7.5 shows the DC behavior of the diode when a ramp signal was given as the input. From the figure it can be observed that the DC out looks exactly like the I V plot. Since the dio de exhibits conduction in forward and reserves bias conditions, we can observe the DC out signal in both polarities. It is also observed that the DC output signal turns on after the input signal reaches a certain voltage and then turns off. The similar beh avior is noticed in the reverse bias. The diode also demonstrates an asymmetric behavior showing different voltage out in the forward and reverse bias exhibiting MIM diode characteristics.
120 However, when the frequency was increased to 1 MHz, the DC signal started to lose the typical trend that was seen at lower frequencies and became more like a triangular wave. Although the cut off frequency was determined to be ~ 1 MHz, the diode seems to lose its rectification property at much lower frequency. This chan ge can be attributed to several diode issues, such as, aging, roughness in dielectric, and capacitance variations due to variation in dielectric thickness. 7.2.2 Low Frequency measurement of 1 m 2 MIM Diode Following the 100 m 2 diode measurement, MIM dio de with 1 m 2 contact area was set up for rectification measurement. Although the diodes were designed to operate at 94 GHz, the testing was carried out in the upper MHz regime. Since the function generator could produce only up to 20 MHz signal, a network analyzer capable of generating 13 GHz was used. As mentioned earlier this measurement was carried out in a different probe station setup. The signal from the network analyzer was connected to the input of the diode through a 150 m pitch probe and the osc illoscope. The output from the diode was also connected to the oscilloscope. Since the oscilloscope could measure only up to 500 MHz, the input signal from the VNA was limited to 200 MHz. Figure 7.6 shows the AC to DC testing of the 1 m 2 MIM diode at 200 MHz.
121 Figure 7.6 : AC to DC Measurement of the 1 m 2 MIM D iode at 200 MHz The input frequency was set at 200 MHz with 500mV peak peak signal. The diode did not demonstrate any rectification like behavior like the 100 m 2 diode; instead the diodes exhib ited an offset sine wave output with much smaller amplitude. Also it can be noticed that the output signal from the diode displayed larger amplitude in the forward cycle (20 mV) than the reverse (15 mV). This suggests that the diode exhibits asymmetric cha racteristics. The same characteristics was demonstrated when the frequency was changed from 50 200 MHz. When the amplitude was increased, the diode exhibited a slight form of charging and discharging effect like a RC circuit. Figure 7.7 shows the diode res ponse with change in amplitude.
122 Figure 7.6 : DC R esponse o f 1 m 2 Diode with Increase in Amplitude A slight slant in the signal can be observed from Figure 7.7. Initially, the diode behavior exhibited an output signal with 20 mV. When the amplitude of the input signal was increased, the dc output voltage exhibited an increase in diode response. Although the diode did not exhibit rectification characteristics, it displayed a charging behavior suggesting a capacitor like structure. In a way a MIM diode i s like a parallel plate capacitor structure. Moreover, the diode was fabricated for mm wave testing, hence the lead lines and the transmission were designed to operate at high frequency, operating the diode at a lower frequency would not yield desirable r esult as observed.
123 Later, an external power supply (Keithley 2400) was connected to the diode input through the VNA to apply an external bias along with the RF signal. A high precision multimeter (Keithley 2000) was also connected in parallel to the oscill oscope to measure the output current. The RF power was set at 10 GHz to be sourced from the VNA. The bias voltage was varied from 50 mV to 300 mV in steps of 50 mV and the corresponding current was measured. Also the RF power was switched changed from zero RF power to 0 dBm (1 mW). Thus current was measured by biasing the diode with RF power ON and OFF. When the input signal was turned ON the diodes responded positively, resulting ~9.5 A at 50 mV bias voltage and no RF power. When the RF power was turned on, the output current increased to ~ 10 A. This behavior was also noticed when the bias voltage was gradually ramped up. From this experiment it is observed that apart from the external bias, applying an RF power also provides an extra bias, thus increa sing the output current. Different diodes exhibited change in current upon applying external bias or power, which was typically in the range of tens of A. This suggests that although the diodes did not exhibit typical rectification characteristics, applyi ng a signal with and without external bias could generate an output current. Table 7.1 shows the change in current with change in bias voltage and RF power.
124 Table 7.1 Variation in Current with Change in Bias V oltage on 1 m 2 MIM D iode Bias Voltage (mV) Current at No RF power (A) Current at 1mW power (A) 50 9.55 9.92 100 19.2 20.1 150 29.3 30.6 200 39.7 41.5 250 49.4 51.5 300 59.2 62.2 7.2.3 Millimeter Wave Response of MIM Diode The MIM diodes fabricated on silicon substrates were used for 94 GHz measurements. Wiltron 360B Network analyzer was used for the diode testing along with Wiltron SM5184 transmission and reflection module. After the on wafer calibration was performed, the probes were moved to the edge of the diode contact pads and gently placed to make a good contact. A 94 GHz signal with a 0 dBm power (1 mW) was given as a n input to the MIM diode using the VNA as a continuous signal generator. The diode was connected to a multimeter to record the output current. When the input signal was provided, the diodes responded positively and output current was measured in the multimeter. The current recorded was predominantly in the
125 order of low A. The amplitude and Vp p was not n oted since, the VNA was not hooked up to an oscilloscope, which is the only way of know the input voltage. Due to the unavailability of a high frequency oscilloscope, the amplitude of the input signal could not be observed. Figure 7.8 shows the distributio n of current recorded for different diodes upon feeding a 94 GHz signal. From the distribution it can be seen that all of the diodes exhibited various current output. This suggests that the 1 m 2 diode fabricated with the aforementioned procedures have a n on uniform dielectric. Figure 7.8: Distribution of Output C urren t for D iodes upon Subjecting to Millimeter Wave Signal From the low frequency measurement of the 1 m 2 diode discussed in the previous section, it was determined that by applying a bias voltage and RF power, a higher output current can be achieved. Hence even in the mm wave measurement,
126 external bias was applied to the diode and the current was measured. The RF power was varied from 15 dBm to 5 dBm and the corresponding current was measu red. Figure 7.9 shows the variation in current with input RF power in different diodes. Figure 7.9: Variation in DC Current with Change in Input P ower As can be seen from F igure 7.8, all the diodes exhibited the same trend of increase in current with increase in RF power. From the AC measurements it can be noted that the current was in the same range as the DC I V measurement discussed in the previous chapter. Although the diodes displayed acceptable level of out put current, when considering the efficiency, the diode performance is on the lower side. At 0 dBm or 1mW input power, and no external bias the diodes yielded a maximum of 2 A with mega
127 ohms resistance. The efficiency (! ) of a device can be defined as the ratio of output power to the input power. Hence the efficiency was determined to be 0.4%. Finally, to measure the reflection coefficient or the return loss of the MIM diodes, the S11 pattern of the diodes were measured. The on chip calibration standards w ere initially calibrated, and then using the two port configuration the return loss was measured. Figure 7.10 shows the return loss of different MIM diode measured from 75 GHz to 110 GHz. Figure 7.10: Return Loss of MIM Diode M easure d from 75 to 110 GHz From Figure 7.10, it is observed that all the diodes exhibited very high return loss. Typically, a perfectly matched device will have very low return loss approaching This suggests that the diodes are rejecting most of the signal that is transmitted through the lead lines. This can be resolved by providing a matching network between the
128 transmission line and the diode or by developing the diode with much less resistance. But, in order to achieve maximum efficiency, a matching netwo rk would be preferred. Thus the experiment provides evidence of AC to DC conversion in spite of the issues. In summary, the diodes when subjected to 94 GHz signal yielded about A current output as exhibited from the I V characteristics. However, when the diode was operated at a lower frequency, did not display any rectification like behavior. This might be because the diodes were designed for high frequency operation and hence the frequency mismatch causes the diode not to demonstrate rectification charac teristics. In addition to mismatch, the diodes can be considered as a classic parallel plate capacitor with a thin dielectric layer. At high frequencies, a typical capacitor will behave as a short. Similarly, the diodes also displayed capacitor like behavi or by exhibiting the characteristics of a short circuit as seen from the oscilloscope data.
129 CHAPTER 8 CONCLUSION AND FUTURE OUTLOOK Thin Film MIM tunnel junctions with Ni NiO Cr with 1 m 2 contact area were fabricated on bulk micromachined silicon substrate and its ability to convert mm wave signal to DC output was investigated. These devices were developed using a one step e beam lithography process to define the active area of the tunnel junction. The electrical behavior of the device was evaluated by testing its dc I V an d mm wave characteristics. The diodes exhibited significant asymmetry and non linearity with a maximum sensitivity of 7 V 1 MIM tunnel junctions were subjected to mm wave measurement by directly feeding the signal to the diode through a VNA and the outpu t current was measured using a high precision digital multimeter. The devices responded well to mm wave signals yielding dc current output. When the diode was fed with a 94 GHz signal with 0 dBm (1 mW), a rectified output in the range of A was observed. T he output current was controlled by varying the bias and the input power of the mm wave signal. Thus, thin film MIM tunnel junctions with dissimilar electrodes were developed on silicon membrane for the first time for mm wave detection. In addition, MIM junctions were also fabricated with larger device area (100 m 2 ) using conventional photolithography on silicon substrates. The electrical response of
13 0 these diodes was investigated by measuring it dc I V response at room temperature. Further, the effects of post deposition annealing on the device stability were analyzed. The diodes demonstrated enhanced electrical characteristics up to 250¡C, with a maximum sensitivity of 45V 1 These diodes exhibited the highest sensitivity ever reported by any research g roup. As an alternate method of fabricating MIM junctions, the feasibility of using an organic layer as the dielectric was investigated. For this, a monolayer of polyaniline was used as the dielectric layer. The organic insulator layer was deposited using Langmuir Blodgett technique and its electrical characteristics were evaluated by I V measurement. The polyaniline based MIM junctions yielded a better asymmetry and non linearity than the NiO based tunnel junctions. However, the current exhibited by the p olyaniline tunnel junctions were lower than NiO tunnel junctions. 8.1 G eneral Comments and Suggestions The NiO based tunnel junctions exhibited non linear and asymmetrical electrical characteristics. However, the current exhibited varied with every device. This can be attributed to the non uniformity in the dielectric thickness. Although the thickness of the diele ctric was experimentally determined to be 3 nm, even a slight variation in the thickness can contribute to deviation in current output. The surface roughness of the film can also contribute to this discrepancy. From the fabrication process it is identifie d that the NiO layer is deposited at 30 mTorr. This is fairly high for a thin film deposition process and would increase the roughness of the film, causing a large non uniformity. This non uniformity will contribute to the variation
131 in diode output. Hence, to achieve uniform current output the dielectric deposition process has to be done at lower pressures. Also, the diodes were fabricated as a step by step process, wherein a photolithography process was involved after each layer. This causes the thin film s to be exposed to several chemicals, potentially causing the device to perform less effectively. Hence a multi step deposition process has to be adopted to preserve the MIM stack especially the insulator layer. The diode development has to be done by cons idering composite materials, alternate dielectric with smaller barrier height and width. Only by using smaller barrier height materials, can we achieve conduction at very small voltages. In that view, using organic layers as dielectric seems promising, but it has to be optimized to achieve an ultra thin layer of the organic material. The mm wave measurements were carried out by directly connecting the 94 GHz source to the tunnel junction and the rectified current was measured using a multimeter. However, th e tunnel junctions need to be coupled with an antenna to determine the radiation and coupling parameters. Thus as a next step towards enhancing the mm wave detector, the MIM junctions have to be integrated with an antenna and evaluated.
132 REFERENCES  D.A. Jennings, F.R. Petersen, and K. M. Evenson, "Extension of Absolute Frequency Measurements to 148 THz: Frequencies of 2.0 and 3.5 m Xe Laser," Applied Physics Letters, vol. 26, pp. 510 511, 1975.  C. W. Slayman and T. K. Gustafson, "Metal Barrier Metal Junctions for Room Temperature Millimeter Wave Mixing and Detection," in Microwave Symposium Digest, MTT S International 1981, pp. 338 340.  J. W. Dees, "Detection and harmonic generation in the sub millimeter wavelength region," Microwave Journal, vol. 9, pp. 48 55, 1966.  A.B. Hoofring, V.J. Kapoor, and W. Krawczonek, "Submicron Nickel Oxide Gold Tunnel Diode Detectors for Rectennas," Journal of Applied Physics, vol. 66, pp. 430 437, 1989.  S. E. Borek, "An Overview of Through the Wall Surveillance for Homeland Security," in Proceedings of the 34th Applied Imagery and Pattern Recognition Workshop 2005, pp. 42 47.  L.R. Wicker and D. C. Webb, "The Potential Military Application of Mil limeter Waves," in Millimeter and Submillimeter Wave Propagation and Circuits 1978, pp. 1.1 1.6.  C.R.Nave, "Hyperphysics: Electromagnetic Spectrum," 2006.  J. D. Vincent, Fundamentals of Infrared Detector Operation and Testing New York, NY John Wiley& Sons, 1989.  P. Bhartia and I. J. Bahl, Millimeter Wave Engineering and Applications New York, NY: John Wiley & Sons, 1984.  NASA, "Infrared Waves," in The Electromagnetic Spectrum 2007.  Maureen Kaine Krolak and M. E. Novak, "An In troduction to Infrared Technology: Application in the Home, Classroom, Workplace, and Beyond..", 1995.
133  FLIR, "FLIR Thermal Imaging Infrared Camera," 2005.  TSA, "Millimeter Wave: Whole Body Imaging," 2008.  E.R.Brown, "Fundamentals of Terres trial Millimeter Wave and THz Remore Sensing," in Terahertz Sensing Technology vol. 2, Dwight L. Woolard, William R. Loerop, and M. S. Shur, Eds.: World Scientific, 2003.  I. M. Blankson, "Passive Millimeter Wave Imaging with Super Resolution: Application to Aviation Safety in Extremely Poor Visibility," 2001.  G. R. Huguenin, "Millimeter Wave Concealed Weapon Detection and Through the Wall Imaging Systems," in ", Proceedings of SPIE 1997, pp. 152 159.  D.D. Ferris Jr. and N. C. Currie, "Overview of current technology in mmw radiometric sensors for law enforcement applications," in Proceedings of SPIE 2000, pp. 61 71.  M. Schlechtweg, A. Tessmann, A. Leuther, C. Schwrer, H. Massler, M. Mikulla, M. Walther, and R. Lsch, "Advanced millimeter wave ICs using metamorphic HEMT technology," Physica Status Solidi C, vol. 3 pp. 465 468, 2006.  R. Stevenson, "Chip innovators eye airport surveillance equipment," in Compound Semiconductor vol. 13, 2007.  S. E. Borek, "An Overview of New Surveillance Technologies," in 7th Annual Technologies For Critical Incident Preparedness Conference San Diego, 2005.  P. J. Costianes, "An Overview of Concealed Weapons Detection for Homeland Security," in Proce edings of the 34th Applied Imagery and Pattern Recognition Workshop 2005, pp. 2 6.  K.J. Linden, W. R. Neal, J. Waldman, A.J. Gatesman, and A. Danylov, "Terahertz Laser Based Standoff Imaging System," in Proceedings of the 34th Applied Imagery and Pa ttern Recognition Workshop 2005, pp. 7 14.  D. Novak, R. Waterhouse, and A. Farnham, "Millimeter Wave Weapons Detection System," in Proceedings of the 34th Applied Imagery and Pattern Recognition Workshop 2005, pp. 15 20.  A. Achanta, M.Mckenna J. Heyman, K. Rudd, M. Hinders, and P. Costianes, "Non linear Acoustic Concealed Weapons Detection," in Proceedings of the 34th Applied Imagery and Pattern Recognition Workshop 2005, pp. 21 27.
134  C. Fumeaux, W. Herrmann, F.K. Kneubhl, and H. Rothui zen, "Nanometer Thin Film Ni NiO Ni Diodes for Detection and Mixing of 30 THz Radiation," Infrared Physics and Technology, vol. 39, pp. 123 183, 1998.  M.R. Abdel Rahman, F.J. Gonzalez, and G. D. Boreman, "Antenna Coupled Metal Oxide Metal Diodes for Dual Band Detection at 92.5 GHz and 28 THz," Electronics Letter, vol. 40, 2004.  J. Piotrovski and A. Rogalski, "Uncooled Long Wavelength Infrared Photon Detectors," Infrared Physics and Technology, vol. 46, 2004.  C.C. Fumeaux, D.F Spenser, and G. D. Boreman, "Microstrip Antenna Coupled Infrared Detector," Electronics Letter, vol. 35, pp. 2166 2167, 1999.  B. Berland, "Photovoltaic Technologies Beyond the Horizon: Optical Rectenna Solar Cell," 2003.  G. P. Gauthier, J. P. Raskin, and G. M. Rebeiz, "A 140 170 GHz low noise uniplanar subharmonic Schottky receiver," Microwave Theory and Techniques, IEEE Transactions on, vol. 48, pp. 1416 1419, 2000.  Wikepedia, "Wilhelmy plate Wikipedia, The Free E ncyclopedia," 2008.  I. Codreanu and G. D. Boreman, "Influence of Dielectric Substrate on the Responsivity of Microstrip Dipole Antenna Coupled Infrared Microbolometers," Appl. Opt., vol. 41, pp. 1835 1840, 2002.  E. N. Grossman, J. E. Sauvageau, and D. G. McDonald, "Lithographic spiral antennas at short wavelengths," Applied Physics Letters, vol. 59, pp. 3225 3227, 1991.  F. J. Gonzalez, M. Abdel Rahman, and G. D. Boreman, "Antenna coupled VOx thin film microbolometer array," Microwave and O ptical Technology Letters, vol. 38, pp. 235 237, 2003.  O. Acef, L. Hilico, M. Bahoura, F. Nez, and P. D. Natale, "Comparison between MIM and Schottky diodes as harmonic mixers for visible and microwave sources," Optics Communications, vol. 109, pp. 4 28 434, 1994.  G. M. Elchinger, A. Sanchez, J. C. F. Davis, and A. Javan, "Mechanism of detection of radiation in a high speed metal metal oxide metal junction in the visible region and at longer wavelengths," Journal of Applied Physics, vol. 47, pp. 591 594, 1976.
135  E. Wiesendanger and F. Kneubhl, "Thin film MOM diodes for infrared detection," Applied Physics A: Materials Science & Processing, vol. 13, pp. 343 349, 1977.  D. Diesing, A. W. Hassel, and M. M. Lohrengel, "Aluminium oxide tunnel junctions: influence of preparation technique, sample geometry and oxide thickness," Thin Solid Films, vol. 342, pp. 282 290, 1999.  M. Heiblum, W. Shihyuan, J. Whinnery, and T. Gustafson, "Characteristics of integrated MOM junctions at dc and at optical frequencies," Quantum Electronics, IEEE Journal of, vol. 14, pp. 159 169, 1978.  I. Wilke, Y. Oppliger, W. Herrmann, and F. K. Kn eubhl, "Nanometer Thin Film Ni NiO Ni Diodes for 30 THz Radiation," Applied Physics A: Solids and Surfaces, vol. 58, pp. 329 341, 1994.  P. Esfandiari, G. Bernstein, P. Fay, W. Porod, B. Rakos, A. Zarandy, B. Berland, L. Boloni, G. Boreman, B. Lail, B. Monacelli, and A. Week, "Tunable antenna coupled metal oxide metal (MOM) uncooled IR detector," in Proceedings of SPIE 2005, pp. 470 482.  J. G. Zhu and C. Park, "Magnetic tunnel junctions," Materials Today, vol. 9, pp. 36 45, 2006.  J. G. Simmons, "Electric Tunnel Effect between Dissimilar Electrodes Separated by a Thin Insulating Film," Journal of Applied Physics, vol. 34, pp. 2581 2590, 1963.  A. Gehring, "Simulation of Tunneling in Semiconductor Devices." vol. PhD Dissertation 2003.  S. M. Sze, Physics of Semiconductor Devices 2 nd Edition ed. New York, NY: Wiley Inter Science Publication, 1981.  A. Sanchez, J. C. F. Davis, K. C. Liu, and A. Javan, "The MOM tunneling diode: Theoretical estimate of its performance at microwave and infrared frequencies," Journal of Applied Physics, vol. 49, pp. 5270 5277, 1978.  D. R. Lide, "CRC Handbook of Chemisty and Physics," 74 ed: CRC Press, 1993 1994.  G. Tech., "Photolithography."  "JEOL JSM 840 Training Manual."
136  J. C. Nabity, "Nanopattern Generation System software."  B.N.Chapman, Glow Discharge Processes: Sputtering and Plasma Etching New York, NY: Wiley Inter Science Publication, 1980.  K. I. USA, "Langmuir and Langmuir Blodgett Films: What and How?."  S. Maleki and P. Kosky, "Frontiers of Nanotechnology," 2005.  S. Krishnan, "Design, Fabrication and Characterization of Thin Film MIM diodes for Rectenna Array," in Electrical Engineering vol. Masters Tampa: University of South Florida, 2004.  H. LaRosa, "Investigation of the Rectenna Concept for Millimeter Wave Detection," in Electrical Engineering vol. Masters: University of South Florida, 2007.  R. J. Powell and W. E. Spicer, "Optical Properties of NiO and CoO," Physical Review B, vol. 2, p. 2182, 1970.  Nima, "611D Conventional LB Trough."  K. V. Rao and A. Smakula, "Dielectric Properties of Cobalt Oxide, Nickel Oxide, and Their Mixed Crystals," Journal of Applied Physics, vol. 36, pp. 2031 2038, 1965.  P.C. Hobbs, R. B. Laibowitz, and F. R. Libsch, "Ni NiO Ni tunnel junctions for terahertz and infrared detection.," Applied Optics, vol. 44, pp. 6813 6822, 2005.  V. Da Costa, M. Romeo, and F. Bardou, "Statistical properties of currents flowing t hrough tunnel junctions," Journal of Magnetism and Magnetic Materials, vol. 258 259, pp. 90 95, 2003.  V. Da Costa, C. Tiusan, T. Dimopoulos, and K. Ounadjela, "Tunneling Phenomena as a Probe to Investigate Atomic Scale Fluctuations in Metal/Oxide/Met al Magnetic Tunnel Junctions," Physical Review Letters, vol. 85, p. 876, 2000.  S. Krishnan, H. La Rosa, E. Stefanakos, S. Bhansali, and K. Buckle, "Design and development of batch fabricatable metal insulator metal diode and microstrip slot antenna a s rectenna elements," Sensors and Actuators A: Physical, vol. 142, pp. 40 47, 2008.
137  S. W. Jeong, H. J. Lee, K. S. Kim, M. T. You, Y. Roh, T. Noguchi, W. Xianyu, and J. Jung, "Effects of annealing temperature on the characteristics of ALD deposited HfO2 in MIM capacitors," Thin Solid Films, vol. 515, pp. 526 530, 2006.  M. J. Lee and K. S. Chung, "Effects of Post annealing on Current Voltage Characteristics of Metal Insulator (Ta2O5) Metal Type Thin Film Diodes," Journal of Korean Physical Society, vol. 39, pp. 686 691, 2001.  H. L. Chen, Y. M. Lu, and W. S. Hwang, "Characterization of sputtered NiO thin films," Surface and Coatings Technology, vol. 198, pp. 138 142, 2005.  M. R. Abdel Rahman, B. Monacell i, A. R. Weeks, G. Zummo, and G. D. Boreman, "Design, fabrication, and characterization of antenna coupled metal oxide metal diodes for dual band detection," Optical Engineering, vol. 44, pp. 066401 7, 2005.
! "# $ Appendix A : Pro cess Flow for Fabrication of 1 00 m 2 MIM diode Step 1 : Substrate Cleaning RCA Clean 1: To remove organic contaminants Immerse the substrate in 1:1:5 solution of NH 4 OH + H 2 O 2 + H 2 O at 75 ¡ C for 15 min ute s Oxide removal: Short Immersion of 1:10 HF+H 2 0 to remove the native silicon dioxide formed on the surface of the substrate RCA clean 2: To remove Ionic contaminants Immerse the subs trates in 1:1:5 solution of HCl+ H 2 0 2 +H 2 0 at 75 ¡ C for 15 min ute s. Rinse it with water and N 2 dry. Step2: Thermal Oxidation Load sample in oxidation tube furnace. Heat it up to 1100 ¡ C. Determine the oxidation time for achieving 1 m thick oxide and grow oxide. Step 3 : Photo lithography Layer 1 Bottom Electrode Spin coat Futurrex 3000 PY negative resist; spin speed 3000 RPM; time 40 sec ond s Soft bake Hot plate; T=155 o C for 60 sec onds Expose Quintel Mask aligner ; 17 sec onds exposure to UV
! "%& Appendix A (Continued) Hard bake Hot plate; T=110 o C for 60 sec Develop RD 6 developer; Immersion developing at room temp erature for 25 sec onds Rinse in DI water and N 2 dry Pattern check : Optical Microscope Step 4 : Metal Deposition Sputtering Ni Base pressure 3 Torr Power 100 W; Working pressure 15 mTorr, Reactive Sputtering NiO Power 25 W; working pressure 30 mTorr; Deposition time 15 minutes Step 5: Lift Off and Ultrasonic clean Immerse the substrate in Acetone till all the unwanted metals peels off from the s ubstrate. Lift off aided with ultrasonic bath Check thickness using the Profilometer Step 6 : Photolithography Layer 2 Top Electrode
! "%" Spin coat Futurrex 3000 PY negative resist; spin speed 3000 RPM; time 40 sec ond s Appendix A (Continued) Soft bake Hot plate; T=155 o C for 60 sec onds Expose Quintel Mask aligner ; 17 sec exposure to UV Hard bake Hot plate; T=110 o C for 60 sec onds Develop RD 6 d eveloper; Immersion developing at room temp for 25 sec onds Rinse in DI water and N 2 dry Pattern check : Optical Microscope Step 7 : Metal Deposition Thermal Evaporation Cr and Au Pressure 4 Torr, Current 80 and 200 A for Cr and Au, respectively; Deposition rate 1/sec for Cr and 3/sec for Au. Step 8 : Lift Off and Ultrasonic clean Immerse the substrate in Acetone till all the unw anted metals peels off from the substrate. Lift off aided with ultrasonic bath Check thickness using the Profilometer
! "#$ Appendix B: Pro cess Flow for Fabrication of 1 m 2 MIM diode Step 1 : Substrate Cleaning RCA Clean 1: To remove organic contaminants Immerse the substrate in 1:1:5 solution of NH 4 OH + H 2 O 2 + H 2 O at 75 ¡ C for 15 min ute s Oxide removal: Short Immersion of 1:10 HF+ H 2 0 to remove the native silicon dioxide formed on the surface of the substrate RCA clean 2: To remove Ionic contaminants Immerse the subs trates in 1:1:5 solution of HCl+ H 2 0 2 +H20 at 75 ¡ C for 15 min ute s. Rinse it with water and N 2 dry. Step2: Thermal Oxida tion Load sample in oxidation tube furnace. Heat it up to 1100 ¡ C. Determine the oxidation time for achieving 1 m thick oxide and grow oxide. Step 3 : Photolithography Layer 1 contact pads, calibration standards and Antenna design: Spin coat Futurrex 3000 PY negative resist; spin speed 3000 RPM; time 40 second s Soft bake Hot plate; T=155 o C for 60 sec onds E xpose EVG 620; 17 seconds exposure to UV
! "#% Appendix B (Continued) Hard bake Hot plate; T=110 o C for 60 sec onds Develop RD 6 developer; Immersion developing @room temp for 25 sec onds Rinse in DI water and N 2 dry Pattern check : Optical Microscope Step 4: Metal Deposition Thermal Evaporation Cr and Au Pressure 4 Torr, Current 80 and 200 A for Cr and Au, respectively; Deposition rate 1/sec for Cr and 3/sec for Au. Step 5: Lift Off and Ultrasonic clean Immerse the substrate in Acetone till all the unwanted metals peels off from the substrate. Lift off aided with ultrasonic bath Check thickness using the Profilometer Step 6: Photolithography Layer 2 Bottom electrode Spin coat Futurrex 3000 PY negative resist; spin speed 3000 RPM; time 40 seconds Soft bake Hot plate; T=155 o C for 60 seconds
! "## Appendix B (Continued) Expose EVG 620; 17 seconds exposure to UV Hard bake Hot plate; T=110 o C for 60 seconds Develop RD 6 developer; Immersion developing @room temp for 25 seconds Rinse in DI water and N 2 dry Pattern check : Optical Microscope Step 7: Metal De position Sputtering Ni Base pressure 3 Torr Power 100 W; Working pressure 15 mTorr, Reactive Sputtering NiO Power 25 W; working pressure 30 mTorr; Deposition time 15 min ute s. Step 8: Lift Off Immerse the substrate in Acetone till all the unwanted metals peels off from the substrate. Lift off aided with ultrasonic bath Check thickness using the Profilometer Step 9: E beam lithography Layer 3 Top electrode
! "#& Appendix B (Continued) Spin coat Microchem ¨ PMMA A3 positive resist; spin speed 3500 RPM; time 25 second s Soft bake Hot plate; T=180 o C for 120 seconds Working Distance 15 mm; Accelerating Voltage 30kV; Probe current 60 pA Expose Using JEOL JSM 840 SEM exposure to e beam, controlled by NPGS Develop 3:1 IPA: MIBK developer; Immersion developing @room temp for 70 seconds Rinse in IPA and DI water and N 2 dry Pattern check : Optical Microscope Step 10: Metal Deposition Thermal Evaporation Cr and Au Pressure 4 Torr, Current 80 and 200 A for Cr and Au, respectively; Depos ition rate 1/sec for Cr and 3/sec for Au. Step 11: Lift Off and Ultrasonic clean Immerse the substrate in Acetone till all the unwanted metals peels off from the substrate. Lift off aided with ultrasonic bath Check thickness using the Profilometer
! "#' Step 12: Photolithography Layer 4 Silicon membrane Spin coat back side of the wafer Shipley S1813 positive resist; spin speed 2500 RPM; time 25 second s Soft bake Hot plate; T=90 o C for 60 second Expose EVG 620; back side alignment and 9 second exposu re to UV Develop MF319 developer; Immersion developing @room temp for 45 seconds Hard bake Hot plate; T=110 o C for 60 seconds Rinse in DI water and N 2 dry Pattern check : Optical Microscope Step 13: Front side protection from HF Spin coat Futurrex 300 0 PY negative resist; spin speed 3000 RPM; time 40 second s Hard bake Hot plate; T=110 o C for 60 seconds Rinse in DI water and N 2 dry Step 14: Etch Oxide layers from the silicon window Immerse the substrate in 10:1 HF: H 2 0 for 15 minutes to etch the ox ides. Check for complete oxide removal Step 15: Resist Removal
! "#( Immerse the substrate in acetone to remove the photoresists from both sides Step 16: Si Etch protection layer Front side Spin Coat Brewer Science ProTek Primer; Spin speed 1500 RPM; Time 60 second s Bake Hotplate, Temp 120 o C for 60 second s Spin coat Brewer Science ProTek B2 18 ; Spin speed 2000 RPM; spin time 90 second s First hard bake Hotplate Temp 120 o C for 2 min ute s Second hard bake Hotplate Temp 155 o C for 2 min ute s Th ird hard bake 205 o C for 1 min ute
! "#$ Appendix C : Current Voltage Characteristics of MIM Junctions Figure C.1: I V Characteristics of Ni NiO Cr MIM Junctions with 100 m 2 Contact Area ! ! !
! "#% Appendix C (Continued) ! !
! "&' Appendix C (Continued) ! !
! "&" Appendix C (Continued) ! Figure C.2: I V Chara cteristics of Ni NiO Cr MIM Junctions with 1 m 2 Contact Area !
! "&( Appendix C (Continued) ! ! Figure C.3: I V Characteristics of Ni PANI Cr MIM Junctions with 100 m 2 Contact Area
ABOUT THE AUTHOR The author received his Bachelors degree in Electronics and Communications Engineering from the Univers ity of Madras, India in 2000. Following this, h e received his Masters degree in Electrical Engineering with specialization in Micro electronics from the University of South Florida, Tampa in 2004. He worked with Dr. Elias Stefanakos and Dr. Shekhar Bhansali at the Clean Energy Research Center to study the feasibility of developing thin film diodes for alternate energy conversion for hi s Masters thesis. He continued with the same group for a PhD degree in Electrical Engineering. In his doctoral work, he was involved in the development of thin film tunnel junctions for thermal dete ction at millimeter wave range His research focus is in development o f next generation energy conversion device based on thin films. His research interests are in the areas of micro/nanofabrication, materials science and thin film sensors.