E-MRS 2006 Spring Meeting (E-MRS), May 29 to June 2, 2006, Nice, France. Al Schottky contact on p-GaSe Wen-Chang Huang, Shui-Hsiang Su 1, Yu-Kuei Hsu 2,

Slides:



Advertisements
Similar presentations
Optical sources Lecture 5.
Advertisements

LECTURE- 5 CONTENTS  PHOTOCONDUCTING MATERIALS  CONSTRUCTION OF PHOTOCONDUCTING MATERIALS  APPLICATIONS OF PHOTOCONDUCTING MATERIALS.
Università degli Studi di Perugia Università degli Studi di Perugia IMM Bologna 1 Measurements and Simulations of Charge Collection Efficiency of p+/n.
Structural Properties of Electron Beam Deposited CIGS Thin Films Author 1, Author 2, Author 3, Author 4 a Department of Electronics, Erode Arts College,
William Cunningham Properties of SiC radiation detectors W. Cunningham a, J. Melone a, V.Kazukauskas b,c P. Roy a, F. Doherty a, M. Glaser d, J.Vaitkus.
SOGANG UNIVERSITY SOGANG UNIVERSITY. SEMICONDUCTOR DEVICE LAB. Introduction SD Lab. SOGANG Univ. Gil Yong Song.
Metal-semiconductor (MS) junctions
Cell and module construction. Photovoltaic effect and basic solar cell parameters To obtain a potential difference that may be used as a source of electrical.
Characterisation and Reliability testing of THz Schottky diodes. By Chris Price Supervisor: Dr Byron Alderman December 2006 Preliminary.
Spring 2007EE130 Lecture 10, Slide 1 Lecture #10 OUTLINE Poisson’s Equation Work function Metal-Semiconductor Contacts – equilibrium energy-band diagram.
Deviations from simple theory and metal-semiconductor junctions
Characterisation and Reliability Testing of THz Schottky Diodes Chris Price University of Birmingham, UK
Chapter V July 15, 2015 Junctions of Photovoltaics.
Simulation of InGaN violet and ultraviolet multiple-quantum-well laser diodes Sheng-Horng Yen, Bo-Jean Chen, and Yen-Kuang Kuo* *Department of Physics,
Radiation Detection and Measurement II IRAD 2731.
Techniques for achieving >20% conversion efficiency Si-based solar cells Presenter: TSUI, Kwong Hoi.
ELCT564 Spring /17/20151ELCT564 Diodes, Transistors and Mixers.
Wide Bandgap Semiconductor Detectors for Harsh Radiation Environments
APPLIED PHYSICS LETTERS 96, , 2010
PREPARATION OF ZnO NANOWIRES BY ELECTROCHEMICAL DEPOSITION
Page 1 Band Edge Electroluminescence from N + -Implanted Bulk ZnO Hung-Ta Wang 1, Fan Ren 1, Byoung S. Kang 1, Jau-Jiun Chen 1, Travis Anderson 1, Soohwan.
The Sixth International Workshop on Junction Technology (IWJT), May 15-16, 2006, Shanghai, China. Formation and characterization of aluminum-oxide by stack-
E-MRS 2007 Spring Meeting (E-MRS), May 29 to June 2, 2007, Strabourg, France. The contact characteristic of p-GaSe crystal Wen-Chang Huang*, Chia-Tsung.
GaN Metal–Semiconductor–Metal Ultraviolet Sensors With Various Contact Electrodes Y. K. Su, Senior Member, IEEE, S. J. Chang, C. H. Chen, J. F. Chen, Member,
Barcelona, 31 May- 2 June Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel.
Introduction Trapped Plasma Avalanche Triggered Transit mode Prager
Photoacoustic Spectroscopy of Surface Defects States of Semiconductor Samples 1) M.Maliński, 2) J.Zakrzewski, 2) F.Firszt 1) Department of Electronics.
ENE 311 Lecture 9.
SILICON DETECTORS PART I Characteristics on semiconductors.
APPLICATIONS OF THERMOACOUSTIC TECHNIQUES FOR THERMAL, OPTICAL AND MECHANICAL CHARACTERIZATION OF MATERIALS, STRUCTURES AND DEVICES Mirosław Maliński.
日 期: 指導老師:林克默、黃文勇 學 生:陳 立 偉 1. Outline 1.Introduction 2.Experimental 3.Result and Discussion 4.Conclusion 2.
指導教授:王聖璋 博士 (Pro.S-C Wang) 學生 : 黃伯嘉 (Bo-Jia Huang) 2015/11/22 Temperature effects on the growth of SnS nanosheet structure using thermal decomposition.
Introduction P. Chelvanathan 1, Y. Yusoff 2, M. I. Hossain 1, M. Akhtaruzzaman 1, M. M. Alam 3, Z. A. AlOthman 3, K. Sopian 1, N. Amin 1,2,3 1 Solar Energy.
Lecture 7 OUTLINE Poisson’s equation Work function Metal-Semiconductor Contacts – Equilibrium energy band diagrams – Depletion-layer width Reading: Pierret.
Meta-stable Sites in Amorphous Carbon Generated by Rapid Quenching of Liquid Diamond Seung-Hyeob Lee, Seung-Cheol Lee, Kwang-Ryeol Lee, Kyu-Hwan Lee, and.
ZnCo 2 O 4 : A transparent, p-type, ferromagnetic semiconductor relevant to spintronics and wide bandgap electronics Norton Group Meeting 4/1/08 Joe Cianfrone.
Advisor: Prof. Yen-Kuang Kuo
Use the same contacts for GaN based UV Photodetectors Y.C. Chiang.
STANFORD High-Power High-Speed Photodiode for LIGO II David Jackrel Ph.D. Candidate- Dept. of Materials Science & Eng. Advisor- Dr. James S. Harris March.
日 期: 指導老師:林克默 博士 學 生:陳冠廷. Outline 1.Introduction 2.Experimental 3. Results and discussion 4. Conclusions.
Conductive epitaxial ZnO layers by ALD Conductive epitaxial ZnO layers by ALD Zs. Baji, Z. Lábadi, Zs. E. Horváth, I. Bársony Research Centre for Natural.
In-situ Scanning Tunneling Microscopy Study of Bismuth Electrodeposition on Au(100) and Au(111) S.H. Zheng a, C.A. Jeffrey a,b, D.A. Harrington b E. Bohannan.
UNIT- IV SOLID STATE PHYSICS. 1)Electrical conductivity in between conductors & insulators is a) high conductors b) low conductors c) Semiconductors d)
From: S.Y. Hu Y.C. Lee, J.W. Lee, J.C. Huang, J.L. Shen, W.
Electro-Ceramics Lab. Electrical Properties of SrBi 2 Ta 2 O 9 Thin Films Prepared by r.f. magnetron sputtering Electro-ceramics laboratory Department.
1 Enhanced efficiency of GaN-based light-emitting diodes with periodic textured Ga-doped ZnO transparent contact layer 指導教授 : 管 鴻 (Hon Kuan) 老師 學生 : 李宗育.
The Sixth International Workshop on Junction Technology (IWJT), May 15-16, 2006, Shanghai, China. Stack-layered metals AuSiNi ohmic contact to n-InP Wen-Chang.
1. EXPERIMENTAL  We used n-type GaN epilayers on sapphire with carrier concentration of ~3 x cm -3.  Native oxide was removed in the NH 4 OH: H.
ELECTRICAL, CHEMICAL, AND STRUCTURAL CHARACTERIZATION OF THE INTERFACE FORMED BETWEEN Au/Pd CONTACT STRUCTURES AND CLEANED p-TYPE GaN (0001) SURFACES.
Influence of deposition conditions on the thermal stability of ZnO:Al films grown by rf magnetron sputtering Adviser : Shang-Chou Chang Co-Adviser : Tien-Chai.
Fowler-Nordheim Tunneling in TiO2 for room temperature operation of the Vertical Metal Insulator Semiconductor Tunneling Transistor (VMISTT) Lit Ho Chong,Kanad.
Highly transparent solution processed In-Ga-Zn oxide thin films 指導教授 : 林克默博士 學生 : 董祐成 日期 :99/08/16 Y. Wang S. W. Liu X. W. Sun J. L. Zhao G. K. L. Goh.
President UniversityErwin SitompulSDP 11/1 Lecture 11 Semiconductor Device Physics Dr.-Ing. Erwin Sitompul President University
National Cheng Kung University Institute of microelectronics OEIC Lab. Jun P. 1 ZnO-based thin film double heterostructured- ultraviolet light-emitting.
Introduction to Thin Film CIGS Solar Cells
Deep Level Transient Spectroscopy study of 3D silicon Mahfuza Ahmed.
Light and Optics  The Electromagnetic Spectrum  Interference, Diffraction, and Polarization Wave Properties of Light.
Production of NTCR Thermistor Devices based on NiMn2O4+d
MODUL 11 Investigation of Annealing Effect on the Forward bias and Leakage current Changes of P-Type 6H-SiC Schottky Diodes with SiO2 Ramp Profile after.
THE EFFECT OF SPIN COATING RATE ON MICROSTRUCTURES OF CUPROUS OXIDE THIN FILM PREPARED BY SOL-GEL TECHNIQUE DEWI SURIYANI BT CHE HALIN School of Material.
A Study on Aluminum Oxide (Al2O3) Insulator Deposited by Mist-Chemical Vapor Deposition based on atmospheric pressure Dong-Hyun Kim1,Hyun-Jun Jung1 and.
Strong infrared electroluminescence from black silicon
Centro de Investigación y de Estudios Avanzados del Institúto Politécnico Nacional (Cinvestav IPN) Palladium Nanoparticles Formation in Si Substrates from.
Lecture 7 OUTLINE Poisson’s equation Work function
Lecture 8 OUTLINE Metal-Semiconductor Contacts (cont’d)
Chapter 4.1 Metal-semiconductor (MS) junctions
Surface morphology of p-GaAs
Effect of Cryogenic Temperature Deposition of Various Metal Contacts to Bulk, Single-Crystal n-type ZnO J. Wright1, L. Stafford1, B.P. Gila1, D.P. Norton1,
Characterization of Thin Films
Lecture 7 OUTLINE Work Function Metal-Semiconductor Contacts
Presentation transcript:

E-MRS 2006 Spring Meeting (E-MRS), May 29 to June 2, 2006, Nice, France. Al Schottky contact on p-GaSe Wen-Chang Huang, Shui-Hsiang Su 1, Yu-Kuei Hsu 2, Chih-Chia Wang 3, Chen-Shiung Chang 2 半導體元件研究室 Abstract-- A new Schottky diode, Al/p-GaSe was presented at this study. It shows an effective barrier height of 0.96 eV with an ideality factor of 1.24 last over five decades and a reverse leakage current density of 4.12  A/cm 2 at - 2V after rapid thermal annealing at 400  C for 30 sec. The generation- recombination effect of the Schottky diode was decreased as the annealing temperature was increased. The formation of Al 1.33 Se 2 was observed by X-ray diffraction analysis after the thermal annealing at 400  C for 30 sec. A rougher surface morphology of the contact was observed both by AFM and SEM, as the annealed temperature was increased. Introduction -- gallium selenide (GaSe) are known to present outstanding nonlinear optical properties. Their refractive index anisotropy makes them suitable for second harmonic generation,[1] parametric oscillation,[2] and frequency mixing[3] in the middle infrared spectral zone where they are transparent. It also has a relatively large band gap energy of 2.0 eV, so it is potential applications to realized visible light emitter diode.[4] The Gallium selenide crystal was also used as material for nuclear particle detectors.[5] In order to attain devices such as light emitter diode or nuclear particle detector with acceptable characteristics, high quality metal contacts to GaSe are necessary. Experiments -- The p-type Er:GaSe crystals used in this study were obtained by the Bridgmann method. The carrier concentration of the GaSe:Er crystal is 1.53  cm -3 and resistivity is  -cm. Thermal evaporator was used to deposit aluminum on the front surface of GaSe substrate. The thickness of the aluminum is 100nm. After metal deposition, the samples were treated by rapid thermal annealing (RTA) at 200  C, 300  C and 400  C, respectively for 30 sec. The ohmic contact on the back side of GaSe substrate was then formed by soldering high-purity indium. Results and discussions— The effective Schottky barrier height --is 0.99eV, 0.98eV and 0.96eV for the as deposited, 300  C-annealed, and 400  C-annealed contacts, respectively. The ideality factor-- of the as-deposited contact is 2.1, of the 300  C-annealed contact is 1.84 and of the 400  C-annealed contact is The reverse leakage current density --is equal to 5.73  A/cm 2, 9.28  A/cm 2 and 6.4  A/cm 2 for the as deposited, 300  C-annealed and 400  C-annealed, respectively, at -3V. The XRD-- analysis of the Al/p-GaSe diode before and after thermal annealing, respectively. The AFM pictures-- RMS value is equal to 1.56, 2.74 and 2.87 for the as deposited diode, 300  C-annealed diode and 400  C-annealed diode, respectively. The SEM pictures-- of the as deposited diode, the 300  C- annealed diode, and the 400  C-annealed diode, respectively. Conclusion-- A new Schottky diode, Al/p-GaSe was realized in the research. It shows a effective barrier of 0.94eV with an ideality factor of 1.24 at the 400  C annealed diode. The contact interface of the diode was passivated after thermal annealing. The passivation gave rise to a lower reverse leakage current and a better ideality factor. A new phase of Al 1.33 Se 2 was formed and the surface became rough after the thermal annealing. Acknowledgments-- The authors would like to thank the National Science Council of the Republic of China, for financially supporting the research under Contract No. NSC E References-- [1] E. Bringuier, A. Bourdon, N. Piccioli, and A. Chevy, Phys. Rev. B, 49 (1994) [2] K. L. Vodopyanov, L. A. Kulewskii, V. G. Voevodin, A. Y. Gribenyukov, K. R. Allakhverdiev, and T. A. Terimov, Opt. Commun., 83 (1991) 322. [3] A. Bianchi, A. Ferrario, and M. Mucsi, Opt. Commun. 25 (1978) 256. [4] M. Budiman, Tamotsu Okamoto, Akira Yanada and Makoto Konagai, Jpn. J. Appl. Phys., 37 (1998) [5] Sakai, H. Nakatani, C. Tatsuyama and F. Takeda, IEEE Tran. on Nucl. Sci., 35 (1988) 85.