UUnniivveerrssiittyy ooff RRhhooddee IIssllaanndd DDiiggiittaallCCoommmmoonnss@@UURRII Open Access Master's Theses 1976 IInnffrraarreedd PPhhoottooccoonndduuccttiivviittyy iinn TThhiinn SSiillvveerr SSuullfifiddee FFiillmmss Paul Joseph Aceto University of Rhode Island Follow this and additional works at: https://digitalcommons.uri.edu/theses RReeccoommmmeennddeedd CCiittaattiioonn Aceto, Paul Joseph, "Infrared Photoconductivity in Thin Silver Sulfide Films" (1976). Open Access Master's Theses. Paper 817. https://digitalcommons.uri.edu/theses/817 This Thesis is brought to you for free and open access by DigitalCommons@URI. It has been accepted for inclusion in Open Access Master's Theses by an authorized administrator of DigitalCommons@URI. For more information, please contact [email protected]. INFRARED PHOTOCONDUCTIVITY IN THIN SILVER SULFIDE FILMS BY PAUL JOSEPH ACETO A THESIS SUBMITTED IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE DEGREE OF MASTER OF SCIENCE IN ELECTRICAL ENGINEERING UNIVERSITY OF RHODE ISLAND 1976 MASTER OF SCIENCE THESIS OF PAUL JOSEPH ACETO Approved: Thesis Committee Dean of the Graduate School UNIVERSITY OF RHODE ISLAND 1976 ABSTRACT A study of thermally generated conductivity and photo conductivity in thin layers of silver sulfide is presented. Silver layers were vacuum deposited on sapphire sub- strates and transformed into silver sulfide in a sulfur atmosphere at 120° C. The dark current of single element sensors was investigated as a function of temperature and photocurrent was measured as a function of photon flux and wavelength. The samples were photosensitive to radiation in the spectral range 0.7 µm to 1 .8 µm. A maximum photo response occured at a wavelength of 0.8 µm. The photo- current in general increased with decreasing temperature. The absorption edge for Ag s at 90 K was found to be at 2 .o 1.2 ~m making the calculated energy gap 1 eV. From dark current measurements, recombination centers were found at 0.66 eV below the conduction band. Vidicon type targets made from silver sulfide layers were also investigated and showed an image fade-out effect with a time constant in the order of seconds. Target re solution was found to exceed 10 lp/mm and the targets 2 responded to incident photon flux levels of 30 µW/cm • i TABLE OF CONTENTS ABSTRACT i TABLE OF CONTENTS ii LIST OF FIGURES iii LIST OF SYMBOLS iv ACKNOWLEDGMENT vi INTRODUCTION 1 I. THEORETICAL 3 II. EXPERIMENTAL 13 III. RESULTS 36 IV. DISCUSSION 49 APPENDIX 60 BIBLIOGRAPHY 81 ii LIST OF FIGURES 1. Elemental Sample Geometries 14 2. Transformation Furnace 16 3. Ag s after Transformation 18 2 4. Photomicrograph of an Island Target 20 5. Cryostat Interior 21 6. Circuit Configuration for Elemental Samples 24 7. I-V Phasor Diagrams 27 8. Vidicon Schematic 29 9. Silver Tracks in Thin Ag s Layers 34-35 2 10. Dark Current Versus Voltage 39 11 • Dark Current Versus Temperature 40 12. Photoresponse Versus Photon Flux 41 13. Spectral Response of Ag s 42 2 14. Photocurrent Versus Infrared Flood Time 44 15. Change in Photocurrent Versus Infrared Flood Time 46 1 6. Image using Infrared Irradiation 47 1 7. Comparison of Spectral Responses 54 1 8. Energy Band Diagram of Ag s 56 2 i_ii LIST OF SYMBOLS 8 -1 c - Speed of light in a vacuum, 3 x 10 m-s E - Energy, eV - Energy of bottom of conduction band, eV - Fermi level, eV - Band gap, eV - Energy difference from shallow traps to the conduction band, eV - Energy difference from recombination centers to conduction band, eV E - Energy of top of valence band, eV v e - Electronic charge, 1 .6 x 1 o-19 c F - Photoelectron generation rate, cm-3-s -1 -2 -1 H Photon flux density, cm -s - 34 h Planck's constant, 6.63 x 10- J-s I - Current, A - Photocurrent, A 2 - Current density, A-cm- 2 - Boltzmann's constant, 1 .38 x 10- 3 J-K-l N - Effective density of states in the conduction c band, cm-3 N - Density of recombination centers, cm-3 0 - Density of shallow traps, cm-3 Effective density of states in the valence band, cm-3 n Density of electrons in the conduction band, cm-3 iv - Density of occupied recombination centers, cm-3 - Density of occupied shallow traps, cm-3 - Density of unoccupied recombination centers, cm-3 2 - Capture cross section for electrons, cm T - Temperature, K t - Time, s 1 v - Electronic drift velocity, m-s- Tl - Per cent of photons absorbed A - Wavelength, m T - Electronic lifetime, s p - Resistivity, 0-cm v ACKNOWLEDGMENT I would like to thank Dr. S. Mardix for the guidance he has given me during the course of this research and for the many enlightening discussions which we have had. His keen insight and good humor have helped me through many periods of difficulty. I would also like to thank Dr. H. Roehrig and Dr. S. Nudelman for introducing me to this field. In addition, I wish to thank the United States Army Electroni cs Command, which provided part of the funds to support this project under contract number DAAB0?- 69- C- 0420. Finall y, I which to thank Mrs . Joan Lamoureux for typing a beautiful manuscript. vi 1 INTRODUCTION The purpose of this thesis is to describe the results of an investigation of infrared photoconductivity in thin (in the order of 1 µm) silver sulfide films . Infrared sensitive materials may be useful as both single element IR detectors and scanned, two dimensional IR detectors . Materials with a high resistivity are likely candidates for investigation of photoconductivity. This is true be- cause high resistivity materials have a low dark current, hence low background. This low background allows for a high signal to background ratio. In addition, conductivity changes due to absorption of photons will not appreciably affect a material which already has a high conductivity. Materials with an absorption edge in the infrared are like- ly to be photosensitive in the IR. Silver sulfide (Ag S) was known as a photoconductor as 2 1 early as 1922 . There are two forms of Ag S: a-Ag S and 2 2 s ~-Ag2S. In the alpha form, Ag has a body centered cubic 2 2 arrangement of sulfur atoms and a relatively low electrical resistivity (103 ohm-cm at room temperature)3. ~-Ag2s has 2 a monoclinic structure and a much higher resistivity (105 ohm-cm at room temperature)3. Some research has been per formed on Ag S and it was found to have an absorption edge 2 in the IR4,5 . s· ~ ince has a higher resistivity and ~-Ag2S
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