Recent result of ~650-GHz SIS-device fabrication at NRO

Slides:



Advertisements
Similar presentations
Flex Circuit Design for CCD Application ECEN 5004 Jon Mah.
Advertisements

1 Quantum Enabling Technology Materials Research for Superconducting Quantum Computing Materials P.I. - D. P. Pappas Affiliates: Jeff Kline Fabio da Silva.
ELECTROCHEMICAL IMPEDANCE SPECTROSCOPY (EIS): A TOOL FOR THE CHARACTERIZATION OF SPUTTERED NIOBIUM FILMS M. Musiani Istituto per l’Energetica e le Interfasi,
Electro-Ceramics Lab. Preparation and electrical properties of (Ba 1-x,Sr x )(Ti 1-y,Zr y )O 3 thin films for application at high density DRAM thin films.
NIST ARDA/DTO review 2006 Materials David P. Pappas Seongshik Oh Jeffrey Kline.
1 InGaAs/InP DHBTs demonstrating simultaneous f t / f max ~ 460/850 GHz in a refractory emitter process Vibhor Jain, Evan Lobisser, Ashish Baraskar, Brian.
Pattern transfer by etching or lift-off processes
Origin of Coulomb Blockade Oscillations in Single-Electron Transistors
1 Anomaly in fabrication processes for large-scale array detectors of superconducting tunnel junctions M. Ukibe, Y. Chen, Y. Shimizugawa, Y. Kobayashi,
ECE/ChE 4752: Microelectronics Processing Laboratory
Atacama Large Millimeter/submillimeter Array Expanded Very Large Array Robert C. Byrd Green Bank Telescope Very Long Baseline Array NRAO Millimeter/THz.
Thin Film Measurement Facilities Flavio Travasso N.i.p.s laboratory - Università di Perugia and INFN Perugia Flavio Travasso N.i.p.s laboratory - Università.
1 LW 6 Week 6 February 26, 2015 UCONN ECE 4211 F. Jain Review of BJT parameters and Circuit Model HBT BJT Design February 26, 2015 LW5-2 PowerPoint two.
S. J. Parka),b) K.-R. Leea), D.-H. Kob), J. H. Hanc), K. Y. Eun a)
M. FOUAIDY Thin films applied to superconducting RF cavitiesLegnaro Oct.10, 2006 improved accuracy and sensitivity as compared to the usual RF method RS.
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.
Further improvements and developments:  Optimization of ultra-thin NbN (and other nitrides or cuprates) superconducting films on large wafers and of patterned.
~ sis Ken’ichi KIKUCHI 1, Seikoh ARIMURA 1, Junji INATANI 1, Yasunori FUJII 1,2, Toshiaki SUZUKI.
Creative Research Initiatives Seoul National University Center for Near-field Atom-Photon Technology Yongho Seo Wonho Jhe School of Physics and Center.
Growth and Characterization of Co nanoparticles and nanowires 劉全璞國立成功大學材料科學及工程學系半導體奈米材料實驗室.
UNIVERSITY OF NOTRE DAME Origin of Coulomb Blockade Oscillations in Single-Electron Transistors Fabricated with Granulated Cr/Cr 2 O 3 Resistive Microstrips.
INTEGRATED CIRCUITS Dr. Esam Yosry Lec. #4. Ion Implantation  Introduction  Ion Implantation Process  Advantages Compared to Diffusion  Disadvantages.
MIT Lincoln Laboratory NU Status-1 JAB 11/20/2015 Advanced Photodiode Development 7 April, 2000 James A. Burns ll.mit.edu.
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.
High speed (207 GHz f  ), Low Thermal Resistance, High Current Density Metamorphic InP/InGaAs/InP DHBTs grown on a GaAs Substrate Y.M. Kim, M. Dahlstrǒm,
Improvement of Infrared Lights Sensitivity on PZT EMITER Daisuke Takamuro, Hidekuni Takao, Kazuaki Sawada and Makoto Ishida.
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.
Ho-Gun Kim, Seung-Ho Ahn, Jung-Gu Kim, *Se-Jun Park, *Kwang-Ryol Lee, **Rizhi Wang SungKyunKwan University, Korea *Korea Institute of Science and Technology,
Develop (K 0.5 Na 0.5 )NbO 3 Lead-Free Ferroelectric Thin Films by the RF Sputtering Technique Hsiu-Hsien Su.
Electro-Ceramics Lab. Electrical Properties of SrBi 2 Ta 2 O 9 Thin Films Prepared by r.f. magnetron sputtering Electro-ceramics laboratory Department.
Optoelectronics dr Konstanty Marszałek Dense Wavelength Demultiplexing – DWDM Gain Flattening Filter – GFF Coarse Wavelength Demultiplexing – CWDM Microoptics.
3-Stage Low Noise Amplifier Design at 12Ghz
Tunable Passive Devices Keith Tang Supervisor: Sorin Voinigescu.
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.
Etch Process Input and Output Parameters Process Modeling how to use input parameters to achieve desired output parameters Process Model Quality parameter1.
ALD Oxides Ju Hyung Nam, Woo Shik Jung, Ze Yuan, Jason Lin 1.
Effect of sputter-particle flux variations on properties of ZnO:Al thin films S. Flickyngerova 1, M. Netrvalova 2,L. Prusakova 2, I. Novotny 1, P.Sutta.
The Applied Superconductivity Center The National High Magnetic Field Laboratory Florida State University 7 th SRF MW Investigation: Variation of Surface.
TECHNOLOGICAL EDUCATIONAL INSTITUTE OF CENTRAL MACEDONIA DEPARMENT OF INFORMATICS & COMMUNICATIONS Master of Science in Communication.
Roughness and Electrical Resistivity of Thin Films Spencer Twining, Marion Titze, Ozgur Yavuzcetin University of Wisconsin – Whitewater, Department of.
RF Superconducting Materials Workshop at Fermilab, May 23 & 24, 2007 Advanced Nb oxide surface modification by cluster ion beams Zeke Insepov, Jim Norem.
Introduction to JEM/SMILES
Update on MgB2 Front from Temple university
Introduction to GaAs HBT and current technologies
Single Pixel Mixer Tests July 2008 (version 2, posted 11 Aug 2008)
Circuit QED Experiment
Etching Processes for Microsystems Fabrication
TriQuint Semiconductor, Inc.
JLab infusion and LG flux expulsion update
OUTLINE 1. Electrical simulation of VCSELs : standard structures
State of the Art and Future Potential of Nb/Cu Coatings
Introduction Thin films of hydrogenated amorphous silicon (a-Si:H) are used widely in electronic, opto-electronic and photovoltaic devices such as thin.
High Q via N infusion R&D at Jefferson Lab
SUPERCONDUCTING THIN FILMS FOR SRF CAVITIES
HG-Cal Simulation using Silvaco TCAD tool at Delhi University Chakresh Jain, Geetika Jain, Ranjeet Dalal, Ashutosh Bhardwaj, Kirti Ranjan CMS simulation.
P2-D125 Decrement of the Exchange Stiffness Constant of CoFeB thin films with Ar gas pressure. Jaehun Cho, Jinyong Jung, Ka-Eon Kim, Sukmock Lee Chun-Yeol.
High Aspect Ratio Si Etching in STS2
Meeting 指導教授:李明倫 學生:劉書巖.
Strong infrared electroluminescence from black silicon
System Considerations for Submillimeter Receiver
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
Stability of DLC film on stainless steel investigated by tensile-test
Characterization of Mechanical Properties of Diamond-like Carbon Films by Using Residual Compressive Stress Sung-Jin Cho, Jin-Won Chung, Myoung-Woon.
Review of impedance aspects of NEG coatings (a surface scientist perspective)
Continuous tuning of phase transition temperature in VO2 thin films on c-cut sapphire substrates via strain variation Jie Jian and Haiyan Wang, Purdue.
Attempts to deposit Nb3Sn by sputtering
SILICON MICROMACHINING
Alexey Bolgar Superconducting quantum bit coupled to a surface acoustic phonon mode of periodic structure Alexey Bolgar
Fig. 1 Structure and basic properties of EuTiO3 (ETO) films.
Basic Planar Process 1. Silicon wafer (substrate) preparation
Presentation transcript:

Recent result of ~650-GHz SIS-device fabrication at NRO K. Kikuchi 1, W. Shan 2, Y. Fujii 3, and J. Inatani 1 (1NASDA, 2 CRL, 3 Nittuki )

Introduction Purpose: Development of ~650-GHz SIS mixer devices for JEM/SMILES, B-SMILES, and SMA. Difficulties: - Just below the gap frequency of Nb. - Junction size should be as small as ~1mm2. Mixer performance is highly sensitive to fabrication parameters. This work is … - Improvement and optimization of the fabrication processes. - Understanding of controllability of the SIS device parameters.

SIS-device and Fabrication Process IF port 500 mm GND - SIS Junction: Nb/AlOx/Nb - Junction Size: ~1 x 1 mm2 (for JEM/SMILES) - Current Density: ~7 kA/cm2 (for JEM/SMILES) - RF Matching: PCTJ with Integrated Circuit

Cross-section Images by TEM TEM image of junction portion 500 nm Wire-Nb Al2O3 Upper-Nb SiO2 Nb2O5 Lower-Nb Quartz substrate Al-AlOX 20 nm “T96” device: - fabricated in 2001 - moderate RF performance (TRX,DSB ~ 300 K)

Nb-film: Superconductivity - Nb-film samples were fabricated with the parameter changing. - Film having a good superconductivity seems to be obtained by using LN2 shroud or gettering effect of sputtered Nb and Al. TC ~ 9.0 ± 0.1 K r10K ~ 5.0 ± 0.5 mW cm

Nb-film: Surface Roughness Measured by AFM +0.22 GPa, 184 nm Stress -0.49 GPa, 173 nm -0.52 GPa, 359 nm Thickness 1mm

Optimization of Etching Processes - Etching rates and stabilities are investigated in various conditions. Example: introduction of Ar-cleaning process: 50mm Un-developed photo-resist makes rough surface in some conditions. Ar-cleaning is effective to make flat. (SiO2 : Nb ~ 5:1 for 100 W, 50 mTorr.) Surface Profile (nm) Relative Distance (mm)

Improvement of Junction Lift-off Process Introduced paint brush, instead of cotton swab

Controllability: Film Thickness Surface profile is measured at each process to estimate the thickness. JEM/SMILES SIS device 640-GHz PCTJs f35 Test junctions Surface profile measurement (500-GHz PCTJs)

Controllability: Junction Size Rn distribution of KS17 devices ID = 1 76 Mean junction size with 1-s deviation in a wafer L ∝ (Jc・Rn) -0.5 fc ∝ L-1

Peak Structure in PIF-V Curve SIS having peak structure shows poor RF performance. Model Amplitude is affected by magnet. - Position varies with temperature.

Mixer Performance Mixer block for JEM/SMILES TRF~60K, TIF~15K

Summary Improvement of processes (Ar-cleaning, lift-off, …) Understanding of the film properties (TEM, AFM, superconductivity, …) Improvement of processes (Ar-cleaning, lift-off, …) Variation of device parameters: - Superconductivity of Nb film: DTC ~ 0.1 K, Dr10K ~ 0.5 mW cm - Film thickness: DT ~ 2-5 % - Junction size: DL ~ 5-10 % - Repeatability of JC is also poor (~ 10 %) Rough estimation of yield: - Survival rare in DC characteristics: pDC ~ 90 % - No peak structure in PIF-V curve: pno-peak ~ 70 % (?) If the band-width of SIS mixer DB/B = Db ~ 5 %, Db/DL ~ 1 s. Then the maximum “yield” from the view point of RF performance is… pDC x pno-peak x pGaussian(Db/DL) = 0.9 x 0.7 x 0.68 = 0.43