MOCVD growth of GaN on SiC at VCU Projects completed: Study of the temperature dependence of the GaN buffer layer on SiC. GaN HT epilayer overgrowth on.

Slides:



Advertisements
Similar presentations
Speaker: Xiangshi Yin Instructor: Elbio Dagotto Time: April 15, 2010 (Solid State II project) Quantum Size Effect in the Stability and Properties of Thin.
Advertisements

starting substrates were undoped 5  m thick GaN films grown by hydride vapor phase epitaxy (HVPE) on c-plane sapphire. 60 nm thick SiOx film was then.
Synthesis of metal hydrides employing vapor deposition technologies Irmantas Barnackas, prof.L. Pranevičius Lithuanian Energy Institute
Condensation and Boiling  Until now, we have been considering convection heat transfer in homogeneous single-phase ( HSP ) systems  Boiling and condensation,
Compact Power Supplies Based on Heterojunction Switching in Wide Band Gap Semiconductors NC STATE UNIVERSITY UCSB Effects of surface oxide on wafer bonding.
Techniques of Synthesizing Wafer-scale Graphene Zhaofu ZHANG
1 NEG films: recent R&D progress Paolo Chiggiato (for the EST-SM-DA section) Vacuum Issues of the LHCb Vertex Detector 28 November NEG films: choice.
Tin Based Absorbers for Infrared Detection, Part 2 Presented By: Justin Markunas Direct energy gap group IV semiconductor alloys and quantum dot arrays.
I.1 ii.2 iii.3 iv.4 1+1=. i.1 ii.2 iii.3 iv.4 1+1=
1 Properties of GaN Films Grown by Atomic Layer Deposition Using Low-temperature III-nitride Interlayers J. R. Gong Department of Materials Science and.
I.1 ii.2 iii.3 iv.4 1+1=. i.1 ii.2 iii.3 iv.4 1+1=

1 Reunion SOS nanotube12 13 octobre 2011 H. Okuno, J. Dijon, E. De Vito, E. Quesnel CEA Grenoble Liten-DTNM SOS nanotubes octobre 2011.
Unsteady Heat Transfer in Semi-infinite Solids Solidification process of the coating layer during a thermal spray operation is an unsteady heat transfer.
Experiment Questions Enzyme Temperature.
Wide Bandgap Semiconductor Detectors for Harsh Radiation Environments
Kansas State University III-Nitride Deep Ultraviolet Photonic Materials and Structures Jingyu Lin & Hongxing Jiang DMR Growth of III-nitride Photonic.
Zn x Cd 1-x S thin films were characterized to obtain high quality films deposited by RF magnetron sputtering system. This is the first time report of.
Growth and Analysis of MOCVD Grown Crystalline GaAs Andrew Howard, Dr. S. Phillip Ahrenkiel SDSM&T Nanoscience Department NSF REU Grant # Objectives.
Improvement in light-output efficiency of Near-Ultraviolet InGaN–GaN LEDs Fabricated on Stripe Patterned Sapphire Substrate 指導教授 : 管鴻 教授 報告學生 : 林耀祥 日 期:
In this study, it has been found that annealing at ambient air at 500 ˚C of DC sputtered Mo bilayer produce MoO x nanobelts. Evolution of MoO x nanobelts.
1 Effects of rapid thermal annealing on the morphology and electrical properties of ZnO/In films Tae Young Ma, Dae Keun Shim Department of Electrical Engineering.
Characteristic MOKE Loops for S320 Strong signals up to 320 K (upper limit of the measurements) Nearly square loops at high temperatures Low saturation.
Purpose  To analyze, through theoretical and experimental methods, the relative luminescence of a series of images produced by multiple reflections in.
Low dislocations density GaN/sapphire for optoelectronic devices Low dislocations density GaN/sapphire for optoelectronic devices B. Beaumont, J-P. Faurie,
Eurocode 1: Actions on structures – Part 1–2: General actions – Actions on structures exposed to fire Part of the One Stop Shop program Annex A (informative)
Nanowires and Nanorings at the Atomic Level Midori Kawamura, Neelima Paul, Vasily Cherepanov, and Bert Voigtländer Institut für Schichten und Grenzflächen.
Electrical and optical properties of organic materials are closely related to its molecular orientation. SE is employed in the understanding of molecular.
1 Nano-aluminum-induced crystallization of amorphous silicon 指導教授:管 鴻 學 生:郭豐榮 學 號: M98L0213.
Weekly Group Meeting Report Renjie Chen Supervisor: Prof. Shadi A. Dayeh.
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.
Growth evolution, adatom condensation, and island sizes in InGaAs/GaAs (001) R. Leon *, J. Wellman *, X. Z. Liao **, and J. Zou ** * Jet Propulsion Laboratory,
日 期: 指導老師:林克默 學 生:陳冠廷. Outline 1.Introduction 2.Experimental 3. Results and discussion 4. Conclusions.
Control of Carbon Nanotube Nucleation Rate with a Hydrogen Beam Plasma Paolo Santos 1, Dorothée Alsentzer 3, Thomas B. Clegg 2,3, Sergio Lemaitre 2,3,
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.
M.S. Hossain, N.A. Khan, M. Akhtaruzzaman, A. R. M. Alamoud and N. Amin Solar Energy Research Institute (SERI) Universiti Kebangsaan Malaysia (UKM) Selangor,
Weekly Group Meeting Report Renjie Chen Supervisor: Prof. Shadi A. Dayeh.
FULTEC / RPI GaN MESFET Process Flow
1 BYU Deposition Facility Previous Turbine Accelerated Deposition Facility (TADF) Design Parameters to match: temp, velocity, angle, materials, particle.
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.
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.
Slide # 1 PL spectra of Quantum Wells The e1-h1 transition is most probable and observed with highest intensity At higher temperature higher levels can.
Thermal annealing effect of tetrahedral amorphous carbon films deposited by filtered vacuum arc Youngkwang Lee *†,Tae-Young Kim*†, Kyu Hwan Oh†, Kwang-Ryeol.
Gallium Nitride Research & Development Rakesh Sohal
Page 1 Sapphire Training Report in Mineral ~
課 程:高等物理冶金 課堂教師:戴子堯 副教授 報 告 者:蔡中銘
Date of download: 5/30/2016 Copyright © 2016 SPIE. All rights reserved. The stages of the SU-8 process along with their interdependence and effect on final.
Epitaxial films of tetragonal Mn 3 Ga: magnetism and microstructure F. Casoli 1,*, J. Karel 2, P. Lupo 3, L. Nasi 1, S. Fabbrici 1,4, L. Righi 1,5, F.
Time-dependent hydrogen annealing of Mg-doped GaN Ustun R. Sunay J. Dashdorj M. E. Zvanut This work is funded the National Science Foundation, Grant No.
Date of download: 7/6/2016 Copyright © 2016 SPIE. All rights reserved. X-ray diffraction (XRD) 2θ-ω scans around (00·2) reflection for InxGa1−xN layers.
Effect of dopant density on contact potential difference across n-type GaAs homojunctions using Kelvin Probe force Microscopy C. Kameni Boumenou1, Z.N.
MBE Growth of Graded Structures for Polarized Electron Emitters
1 Tyndall National Institute, Lee Maltings, Dyke Parade, Cork, Ireland
Centro de Investigación y de Estudios Avanzados del Institúto Politécnico Nacional (Cinvestav IPN) Palladium Nanoparticles Formation in Si Substrates from.
へき開再成長法により作製された(110)GaAs 量子井戸における表面原子ステップの観察
31/08/ GaAs and 5629 GaAs growth 5622 GaAs,
Yuanmin Shao, and Zuimin Jiang
ОПШТИНА КУРШУМЛИЈА.
Tweet summary of article I
Molecular Beam Epitaxy (MBE) C Tom Foxon
Characterization of III-Nitrides on Hydrogen-Etched 6H-SiC
Regular Bio Characteristics of Life
Major Scales at the nut C F G C Box A G C D G VII D G A D F Bb C F X A
Index Notation Sunday, 24 February 2019.
I  Linear and Logical Pulse II  Instruments Standard Ch 17 GK I  Linear and Logical Pulse II  Instruments Standard III  Application.
2. SEM images of different SiNW structures 3.Results and discussion
Yuanmin Shao, and Zuimin Jiang
8 Core Steps of success: I.Step:1 : DREAM SETTING: II. Step: 2 : LIST MAKING : IV. Step: 4 : SHOW THE PLAN: III. Step: 3 : INVITATION: V. Step: 5 : FOLLOW.
Presentation transcript:

MOCVD growth of GaN on SiC at VCU Projects completed: Study of the temperature dependence of the GaN buffer layer on SiC. GaN HT epilayer overgrowth on nano-network of HT GaN buffer layer and comparison with growth on LT continuous GaN buffer layer. Effect of deposition of SiN on the GaN epilayer both on HT and LT buffer layer (scope of future work)

Temperature dependence of the GaN buffer layer on SiC GaN buffer layer deposited on 6H-SiC, miscut samples at four different temperatures: –565 0 C (~temp. used for buffer layer deposition on sapphire, reference (a) –900 0 C –950 0 C –970 0 C (~temp. range recently reported in reference (a) below) (a)Thin solid films, 289 (1996), 256 (b)J. Cryst. Growth, 248 (2003), 533

Temperature dependence of the GaN buffer layer on SiC C, 7 min950 0 C, 4.5 min C, 4.5 min Buffer layer at C showed featureless continuous surface in SEM.

Temperature dependence of the GaN buffer layer on SiC XRD data of the buffer layer on SiC. SampleTemp.(time) 0 C (mins) XRD FWHM (arcminutes) Sym.Asym. SiC_ C (4.5)Broadbroad SiC_ C (7) SiC_ C (4.5)513.2 SiC_ C (4.5) Conclusion: HT buffer layer at C is the optimum for epilayer growth.

HT epilayer growth on LT (565 0 C) and HT (950 0 C) buffer layer XRD data: SampleBuffer layer Temp. Buffer layer XRD (arcminutes) Epi layer XRD (arcminutes) SymAsymSymAsym SiC_ CBroad SiC_ C nm of HT ( ) epilayer GaN was deposited on 100 nm of both LT (565 0 C) and HT(565 0 C) buffer Layer to study the effect of the buffer layer on the quality on the overgrown film. Conclusion: Based upon the xrd data, there is a significant improvement on the epi-layer quality grown on HT buffer layer. This may be due to two reasons: 1.The starting buffer layer quality is better for HT buffer layer. 2.Lateral overgrowth taking place in the film grown on the nano-network of the HT buffer layer, as opposed to the growth on a continous LT GaN buffer layer, as shown in the SEM images on the next two slides.

HT epilayer growth on LT (565 0 C) and HT (950 0 C) buffer layer (continued from the previous slide) SEM: - HT epilayer on the continuous LT buffer layer showed a continuous featureless epilayer. - HT epilayer on the “nano-network” buffer layer at C showed a continuous epilayer but with pinholes. These pinholes result from the partial coalescence of the GaN epilayer after nucleating at nano network the buffer layer. 100 nm buffer layer at C 400 nm epi layer at C on C buffer layer.

HT epilayer growth on LT (565 0 C) and HT (950 0 C) buffer layer (continued from the previous slide) To study the evolution these pinholes, two HT epilayers of different thickness (200 nm and 400 nm) were grown on the HT nano-network buffer layer. The following SEM image shows that the density of these pinholes decreased significantly with the thickness of the epilayer. In addition, these pinholes are hexagonal in shape (more visible in the 400 nm thick layer) whose walls are in the a-direction, the direction of the lateral overgrowth. 100 nm buffer layer at C200 nm epi-layer at C400 nm epi-layer at C

Effect of deposition of SiN on the GaN epilayer both on HT and LT buffer layer Two series of experiments done: 1. SiN deposition on HT buffer layer and then 2  m epilayer growth. 2. SiN deposition on LT buffer layer and then 400 nm epilayer growth. Experiment 1. Growth detail: C C IIIIII IV VVI VII VIII I.13.5 min. temp ramp-up. II.3 min. temp stabilization III.4.5 min. buffer layer deposition (100nm) IV.1.5 min. temp. ramp up. V.SiN treatment. VI.5 min. annealing. VII.90 min. GaN epi layer deposition (2  m) VIII.40 min. cool down. time

Effect of deposition of SiN on the GaN epilayer both on HT and LT buffer layer (continued from the previous slide) Experiment 1. SiN deposition on HT buffer and then 2  m epilayer growth at C. Comments: 1. Substrate: 6H SiC, on-axis, h-etched. 2. The surface of the epilayer shows pinholes due to the partial coalescence. XRD results SEM of the epilayer

Effect of deposition of SiN on the GaN epilayer both on HT and LT buffer layer (continued from the previous slide) Experiment 2. SiN deposition on LT buffer and then 400 nm epilayer growth at C C C IIIIII IV VVI VII VIII I.13.5 min. temp ramp-up. II.3 min. temp stabilization III.4.5 min. buffer layer deposition (100nm) IV.1.5 min. temp. ramp up. V.SiN treatment. VI.18 min. GaN epi layer deposition (400nm) VII.30 min. cool down. time Growth detail:

Effect of deposition of SiN on the GaN epilayer both on HT and LT buffer layer (continued from the previous slide) Experiment 2. SiN deposition on LT buffer and then 400 nm epilayer growth at C. XRD results asym sym SEM: SEM shows flat featureless GaN surface. Comments: 1. Substrate: 6H SiC, miscut, h-etched. 2. XRD value does not change as much as in the case of the growth on the HT buffer layer. 3. The XRD value of the films grown on the HT buffer layer (with or without the SiN deposition is far better than the film on LT buffer layer with SiN deposition. Sym: ~2 arcmins for film on HT buffer layer: ~ 10 arcmins LT buffer layer Asym: ~ 8 arcmins for film on HT buffer layer (3 min SiN deposition): ~ 13 arcmins for film on LT buffer layer (5 min. SiN deposition)

SampleTime (minutes) Temp. ( 0 C) XRD(arcmin)Comments symasym SiC_ HT buffer layer SiC_ HT buffer layer SiC_ HT buffer layer SiC_ HT buffer layer SiC_ HT buffer layer+200 nm epi layer SiC_ HT buffer layer nm epi layer SiC_ broad LT buffer layer SiC_ LT buffer layer nm epi layer SiC_ LT buffer layer + 1  m HT GaN (reference sample for SiN experiment) SiC_394.5+(5) (1020) st SiN (5 min) deposition on LT buffer layer and then HT GaN growth, 1 mu. (90min) SiC_404.5+(10) (1020) nd SiN (10 min) deposition on LT buffer layer and then HT GaN growth, 1 mu. (90min) SiC_414.5+(15) (1035) rd SiN (15 min) deposition on LT buffer layer and then HT GaN growth, 1 mu. (90min) SiC_424.5+(10) (1035) th SiN (10 min) deposition on LT buffer layer and then 5 min. annealing and then HT GaN growth, 1 mu. (90min) Summary of the growths done at VCU in weeks 3