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.

Slides:



Advertisements
Similar presentations
Università degli Studi di Perugia Università degli Studi di Perugia IMM Bologna 1 Measurements and Simulations of Charge Collection Efficiency of p+/n.
Advertisements

For the exclusive use of adopters of the book Introduction to Microelectronic Fabrication, Second Edition by Richard C. Jaeger. ISBN © 2002.
Silicon Carbide Department of Electronics Prof. Dr. Toomas Rang Ehitajate tee Tallinn ESTONIA.
1 Design, Fabrication, and Characterization of GaN High Power Rectifiers Kwang H. Baik Materials Science and Engineering, Univ. of Florida, Gainesville,
SOGANG UNIVERSITY SOGANG UNIVERSITY. SEMICONDUCTOR DEVICE LAB. Introduction SD Lab. SOGANG Univ. Gil Yong Song.
Metal-semiconductor (MS) junctions
5.1 Introduction 5.2 Equilibrium condition Contact potential
EE143 – Ali Javey Section 8: Metallization Jaeger Chapter 7.
Spring 2007EE130 Lecture 13, Slide 1 Lecture #13 ANNOUNCEMENTS Quiz #2 next Friday (2/23) will cover the following: – carrier action (drift, diffusion,
Lecture #12 OUTLINE Metal-semiconductor contacts (cont.)
Characterisation and Reliability Testing of THz Schottky Diodes Chris Price University of Birmingham, UK
Unit-II Physics of Semiconductor Devices. Formation of PN Junction and working of PN junction. Energy Diagram of PN Diode, I-V Characteristics of PN Junction,
Basic Electronics Dr. Imtiaz Hussain Assistant Professor Mehran University of Engineering & Technology Jamshoro
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.
Lecture 8 OUTLINE Metal-Semiconductor Contacts (cont’d)
Chapter 3 Solid-State Diodes and Diode Circuits
Spectroscopy of Hybrid Inorganic/Organic Interfaces Transport Properties Dietrich RT Zahn.
Integrated Circuit Devices Professor Ali Javey Summer 2009 MS Junctions Reading: Chapter14.
National Science Foundation Identification of an intrinsic difficulty in fabricating efficient power devices Sokrates T. Pantelides, Vanderbilt University,
Gavin W Morley Department of Physics University of Warwick Diamond Science & Technology Centre for Doctoral Training, MSc course Module 2 – Properties.
Plasma Application LAB Wide range dielectric spectroscopy of ZnO-based varistors as a function of sintering time 발표자 : 권득철.
Introduction Trapped Plasma Avalanche Triggered Transit mode Prager
ENE 311 Lecture 9.
SILICON DETECTORS PART I Characteristics on semiconductors.
MIT Lincoln Laboratory NU Status-1 JAB 11/20/2015 Advanced Photodiode Development 7 April, 2000 James A. Burns ll.mit.edu.
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.
Fowler-Nordheim Tunneling in TiO2 for room temperature operation of the Vertical Metal Insulator Semiconductor Tunneling Transistor (VMISTT) Lit Ho Chong,Kanad.
Introduction to semiconductor technology. Outline –6 Junctions Metal-semiconductor junctions –6 Field effect transistors JFET and MOS transistors Ideal.
President UniversityErwin SitompulSDP 11/1 Lecture 11 Semiconductor Device Physics Dr.-Ing. Erwin Sitompul President University
College Name : Shree Swami Atmanand Saraswati Institute Of Technology(SSASIT)(076) Year : 2 nd year(3 rd sem) EC-2015 Subject Name : Electronic Devices.
CHAPTER 6: MOSFET & RELATED DEVICES CHAPTER 6: MOSFET & RELATED DEVICES Part 1.
Extraction of Doping Profile in Substrate of MNOS capacitor Using Fast Voltage Ramp Deep Depletion C-V method.
Physics of Semiconductor Devices
Barrier Current Flow in Nitride Heterostructures
Recall-Lecture 3 Atomic structure of Group IV materials particularly on Silicon Intrinsic carrier concentration, ni.
Lecture 10 Power Device (1)
PN-junction diodes: Applications
I. Rashevskaya on behalf of the Slim5 Collaboration, Trieste Group
Lecture 8 OUTLINE Metal-Semiconductor Contacts (cont’d)
3) The University of Electro-Communications, Tokyo, , Japan
Chapter 14. MS Contacts and Practical Contact Considerations
Diodes Introduction Textbook CD
Revision CHAPTER 6.
CHAPTER 4: P-N JUNCTION Part 2
Government Engineering College, Bhavnagar.
Strong infrared electroluminescence from black silicon
Recall-Lecture 3 Atomic structure of Group IV materials particularly on Silicon Intrinsic carrier concentration, ni.
EXPERIMENTAL PROCEDURE EXPERIMENTAL PROCEDURE
Lecture #12 OUTLINE Metal-semiconductor contacts (cont.)
Metal-Semiconductor Junction
Lecture 8 OUTLINE Metal-Semiconductor Contacts (cont’d)
Lecture 8 OUTLINE Metal-Semiconductor Contacts (cont’d)
High-temperature Properties of Schottky Diodes Made of Silicon Carbide
Carbon Nanotube Diode Design
EE130/230A Discussion 5 Peng Zheng.
Chapter 4.1 Metal-semiconductor (MS) junctions
POWER SEMICONDUCTOR DEVICES OVERVIEW
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,
Lecture 7 OUTLINE Work Function Metal-Semiconductor Contacts
Ministry of teaching& high education Al- Mustansiriya University College of engineering Computer &
05/05/28 Optical Characterization of Stem Well with Low Density Modulation-Doping Toshiyuki Ihara Abstract. I measured PL and PLE spectra of low density.
Conduction of Electricity in Solids
Lecture 10 Power Device (1)
PN-JUNCTION.
Solid State Electronics ECE-1109
Presentation On Schottky Diode. Course Code:3208 Course Title : Microwave radar and satellite communication lab Presented By Salma Akter BKH F.
Chapter 3 Solid-State Diodes and Diode Circuits
Fig. 1 Schottky junctions based on a layered PdCoO2 and β-Ga2O3 for high-temperature operation. Schottky junctions based on a layered PdCoO2 and β-Ga2O3.
Presentation transcript:

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 Irradiated Up to 1.75 MGy Dosen: Prof Dr. Usman Sudjadi, Dipl. Ing. U. Sudjadi1), T. Ohshima1), N. Iwamoto1, 2), S. Hishiki1), and K. Kawano2) 1) The University of Electro-Communications, Tokyo, 182-8585, Japan Japan Atomic Energy Agency (JAEA), Gunma 370-1292, Japan 2) Abstract Annealing effect on the electrical properties change of P-type 6H-SiC Schottky diodes with SiO2 ramp profile after irradiated up to 1.75 MGy at RT were investigated. A perpendicular edge termination based on oxide ramp profile around the Schottky contact is used on Al Schottky rectifier fabricated on a 10 μm p-type 6H- SiC epi-layer on p-type 6H-SiC substrate (3.50 off, Si face), Na: 5.9 x 1015/cm2 . The samples were irradiated with gamma-ray up to 1.75 MGy after that the samples annealed at 100 0C - 500 0C for 30 minute, respectively. The electrical characteristics of the diodes are evaluated before and after irradiated, before and after irradiated plus annealed. The results have shown that the forward current increases with increasing annealing temperature. Introduction Metal-silicon carbide (SiC) interfaces play very important roles in many high- performance devices in optoelectronics, high-temperature, high-frequency, and power applications [1]. Annealing effects on the SiC Schottky diodes were studied by several researchers. G. Brezeanu et al. [2] have annealed Nickel-6H-SiC Schottky barrier diodes with simple termination of the planar at 800-10000C. The results shown that reverse characteristics, near–ideal parallel plane breakdown at a voltage of 800 V and very low leakage current after vacuum of Schottky contact at 900 0C for 2 min. A- remarkable weak reverse current-voltage dependence for VR > 100 V has been obtained. The forward characteristics of the Ni/6H-SiC SBD agreed very well thermo-ionic emission theory. The 8000C vacuum annealing led to devices with ideality factors near one and specific on resistance higher than theoretical value due to ohmic backside contact. By increasing the annealing temperature to 10000C, the Ron is reduced but dramatic degradation of the breakdown voltage was observed. The samples of Ni/6H-SiC Schottky diodes of G. Brezeanu et al were not irradiated with gamma-ray. O. Noblanc et al. have investigated about physical and electrical characterization of WN Schottky contacts on 4H-SiC. They have deposited WN by reactive sputtering on 4H-SiC to make Schottky rectifiers. The physical properties of http://www.mercubuana.ac.id 1

250 C, 300 C, and 500 C, for 30 minute, respectively. Fig. 2 shows the forward current versus forward bias with difference of p-type 6H-SiC Schottky diodes with 250 μm circular diameters.This sample annealed 150 C, 250 C, 300 C, and 500 C, for 30 minute, respectively. The leakage current versus annealing temperature of p-type 6H-SiC Schottky diodes with 150 μm circular diameter is shown in Fig. 3: with increasing annealing temperature the forward current increases. The sample in Fig. 3 annealed at 100 C, 300 C, 400 C, and 500 C, for 30 minute, respectively. The forward current versus forward bias with difference annealing of p-type 6H-SiC Schottky diodes with 300 μm circular diameter is shown in Fig. 4. The sample in Fig 4 annealed at 100 C, 200 C, 300 C, 400 C, and 500 C, for 30 minute, respectively. Fig. 5 shows the leakage current versus annealing temperature with difference of p-type 6H-SiC Schottky diodes with 250 μm circular diameters.This sample annealed at 150 C, 250 C, 300 C, and 500 C, for 30 minute, respectively. The leakage current versus annealing temperature of p-type 6H-SiC Schottky diodes with 150 μm circular diameter is shown in Fig. 6. The sample in Fig. 6 annealed at 100 C, 300 C, 400 C, and 500 C, for 30 minute, respectively. Figs. 1-3 show that with increasing annealing temperature the forward current increases. Figures 4, 5, and 6 are shows also that with increasing annealing temperature, the leakage current increases. G. Brezeanu et al. [2] have reported that the typical JF – VF characteristics of a Schottky barrier diode with oxide ramp profile are shown that, 800 0C annealed sample revealed that the current conduction mechanism follows the thermionic emission theory for at least six orders of magnitude into current density levels. However, at high levels, the series resistance comes into effect and this contributes to an additional voltage drop across the diode. The forward voltage drop is VF = (nkT/q)ln(JF/A*T2) + ΦBn + Ron JF Where k is the Boltzman’s constant, T is the temperature and A* is the Richardson’s constant. These results have also reported that the current conduction mechanism also follows the thermionic emission theory. http://www.mercubuana.ac.id 3

-7 100C Forward voltage [V] 10 10 10 Forward current [A] 10 10 10 10 Fig. 2 Forward current versus forward voltage with difference annealing temperature (Φ = 250 μm) 10 3 1 10 -1 -3 -5 10 -7 -9 -11 -13 100C 300C 400C 500C BT59-150micro Forward current [A] 10 10 10 10 -15 2 4 6 8 10 Forward voltage [V] Fig. 3 Forward current versus forward voltage with difference annealing temperature (Φ = 150 μm) 10 1 10 -1 -3 -5 -7 -9 BTA4-300 micro Leakage current [A] 10 -11 -13 -15 10 100 200 300 400 500 Annealing temperature [C] http://www.mercubuana.ac.id 5