Experimental High Energy Physics & Plasma Etching
|
|
- Roy Casey
- 5 years ago
- Views:
Transcription
1 Experimental High Energy Physics & Plasma Etching Samah M. Balouza Purdue University Nikhef Doctoral Interview 07/06/2017
2 Outlines Plasma Physics Research Experimental High Energy PhysicsResearch Samah Balouza - Nikhef Doctoral Interview 2
3 I- Plasma Physics Master Thesis: Modeling of Inductively Coupled Plasma (ICP)Etching RESEARCH OBJECTIVE: To study the plasma parameters that can generate high density plasma in order to enhance the directionality of the beam during the etching process of the microelectronic devices. Samah Balouza - Nikhef Doctoral Interview 3
4 METHODOLOGY Gaseous Electronic Conference RF Reference Cell (GEC): To compare results obtained by different research group. Stainless-steel chamber with parallel-plate electrodes having a diameter of 102 mm. Using COMSOL Multiphysics Simulation tool. Samah Balouza - Nikhef Doctoral Interview 4
5 RESULTS Electron Density (1/m3) Argon Ion Density (1/m3) Effect of Pressure The Figures illustrate the radial distributions of the argon ion density and electron density at the wafer surface respectively at different values of the pressure. The coil power was kept equal to 2000 W. 1.20E E E E E E E E E E E E E r/10^3 (m) 20 mtorr 25 mtorr 30 mtorr r/10^3 (m) 20 mtorr 25 mtorr 30 mtorr 35 mtorr 40 mtorr Electron densities at different pressure values. Argon ion densities at different pressure values. Samah Balouza - Nikhef Doctoral Interview 5
6 Electron Density (1/m3) Argon/Oxygen Mixture 1.20E E E E E E E E E r/10^3 (m) 30% O2 40% O2 50% O2 Electron density distributions at different oxygen concentrations. Samah Balouza - Nikhef Doctoral Interview 6
7 Results Summary I studied the pressure, power and the concentration of the mixture that affected the electron density distribution inside the reactor, the electron energy, and the ions density distribution. In pure argon, increasing the pressure led to increase in the electron density and the argon ion density distributions. By increasing the oxygen gas concentration in the mixture, the electron density decreases and the oxygen ion density increases. Samah Balouza - Nikhef Doctoral Interview 7
8 II- Experimental High Energy Physics: CMS Pixel Detector Working with the detector modules to calibrate the detector and the connected electronics. Detector modules, port cards, optical fibers, front end Controller, and front End driver. Pixel Detector Modules Front End Controller & Front End Driver Samah Balouza - Nikhef Doctoral Interview 8
9 Using XDAQ application to control the required tests to check the performance of the detector. Normal tests to check the efficiency of the detector and Sending/receiving data from the detector and the electronics. Detector Efficiency Scan-PixelAlive Samah Balouza - Nikhef Doctoral Interview 9
10 Pixel Detector Installation at CMS By 1 st of March, the new pixel detectors have been installed at CMS cavern and we are currently testing the whole detector after installation. Pixel Installation at CMS. Ref: Samah Balouza - Nikhef Doctoral Interview 10
11 Top Quark Analysis Spin Correlations Dilepton channel Feynman Diagram for top pair decay Histograms that represent the leptons and jets that have been selected from raw data that contains millions of events. Samah Balouza - Nikhef Doctoral Interview 11
12 Resistive Plate Chamber (RPC) EENP2 Marie Curie International Research Staff Exchange Scheme (IRSES). RPCs consist of two parallel plates, a positively-charged anode and a negativelycharged cathode, both made of a very high resistivity plastic material and separated by a gas volume. My research objective was testing the detector Performance by using the cosmic stand. Samah Balouza - Nikhef Doctoral Interview 12
13 Testing the detector performance by applying different HV values in the cosmic stand. HV Scan for 2 mm Gap HV Scan for 1.8 mm Gap Samah Balouza - Nikhef Doctoral Interview 13
14 CERN Summer School Project The research treated the development of the Micro-Pattern Gas Detectors, more specifically Gas Electron Multiplier (GEM) Detector. It consisted of two parts: Experimental work & Simulation work. In this project, the basic properties of the triple GEM detector were tested and measured, including energy calibration and energy resolution. Samah Balouza - Nikhef Doctoral Interview 14
15 GEM is one approach to the amplification. It is based on accelerating initial electrons with an electric field in order to use them to ionize more gas atoms. Electric field around GEM holes. The image is from Gas Detectors Development Group website 10X10 cm2 Triple GEM Detector Samah Balouza - Nikhef Doctoral Interview 15
16 Simulation of the Woven Mesh By using COMSOL Multiphysics Simulation code, I Calculated the electron transparency by simulating electron trajectories inside the detector. Electron Transparency is the ratio of the electrons that passing through the GEM hole. I studied the effect of changing the electric field on the electron transparency. Three Dimensions Woven Mesh Simulation with COMSOL Samah Balouza - Nikhef Doctoral Interview 16
17 Outreach Activities for CERN The Alphabet of the Universe. A CERN exhibit at the Bibliotheca Alexandrina, Alexandria, Egypt. CMS Virtual visits for Lebanon & Oman. Samah Balouza - Nikhef Doctoral Interview 17
18 My Research Experience! Working in an international organization CERN Experimental skills: state of the art electronics at CERN, graduation project, and modeling. Finding a research problem my master thesis Plasma applications; medical, etching, sputtering, implantation,. Asking experts in the field developed my communication skills. Samah Balouza - Nikhef Doctoral Interview 18
19 Thank You! 19
20 Back-Up Slides 20
21 IEEE-NPSS International Conference of Plasma Physics (ICOPS-2015) Samah Balouza - Nikhef Doctoral Interview 21
22 Electron Density (1/m3) Master Thesis: Model Validation Electron density versus pressure obtained from COMSOL simulation as compared to the experimental values at power 50 W and frequency 6.87 MHz. The experimental result obtained by V. A. Godyak, R. B. Piejak and B. M. Alexandrovich 2.5E+18 2E E+18 1E+18 5E Pressure (mtorr) COMSOL Experimental Electron density versus pressure Samah Balouza - Nikhef Doctoral Interview 22
23 Plasma Chemistry in Inductively Coupled Plasma Modeling Ar: Nobel Gas Increase the Number of Primary Electrons. O 2 : Quencher Gas Stabilize the Plasma. BUT, e + O 2 O 2 - Oxygen Attachment Reaction Samah Balouza - Nikhef Doctoral Interview 23
24 Electron Density (1/m3) The Effect of Coil Power In order to achieve the goal of maintaining the highest plasma density, the 30% oxygen concentration is selected as it gives the highest electron density. 1.60E E E E E E E E E r/10^3 (m) 600W 800W 1000W 1200W Electron density at different power values. Samah Balouza - Nikhef Doctoral Interview 24
25 - Graduation Project: Plasma Nitriding of Stainless Steel The main objective of nitriding the stainless steel is to improve the surface hardness by forming a hard nitrided layer. Material Sample: The AISI 304 Austenitic Stainless Steel. Vacuum Chamber (Stainless Steel 316) Cylindrical (20 cm x 10 cm). Schematic Illustration of the Plasma Nitriding Apparatus Samah Balouza - Nikhef Doctoral Interview 25
26 Results The parameters that changed: Hydrogen concentration and time of exposure. Methods used for testing the hardness: - Checking the nitrogen percentage by testing the alloy constituents before and after the exposure,e.g. XRD & Scanning Electron Microscope. - Mechanical Hardness Test (Vickers )test. Electron microscope scanning photo of Sample # 4T Samah Balouza - Nikhef Doctoral Interview 26
27 Graduation Project Challenges: The figure below shows that the edge of the DC nitrided sample has different colors as compared to the central area. This phenomenon, generally known as edge effect. It is one of the common problems for DC plasma nitriding. It has been explained in terms of the non-uniform sputtering and deposition during nitriding process. Leakage: minimum leakage means high purity. plasma. Material of the chamber should have high chemical and thermal stability. Surface of DC plasma nitrided samples Samah Balouza - Nikhef Doctoral Interview 27
28 Change of temperature with time for sample # 4T (150 minutes- 5% Hydrogen) Change of micro-hardness with time for sample # 4T (150 minutes - 5% Hydrogen) Samah Balouza - Nikhef Doctoral Interview 28
29 Graduation Project Awards Third Place in Best Graduation Project Competition 2010, Faculty of Engineering Alexandria University. Prof. Aly Mortada Award for the Best Graduation Project in 2010, Nuclear & Radiation Engineering Department, Alexandria University. The Project was partially funded by Intel-Egypt. Samah Balouza - Nikhef Doctoral Interview 29
DEPOSITION OF THIN TiO 2 FILMS BY DC MAGNETRON SPUTTERING METHOD
Chapter 4 DEPOSITION OF THIN TiO 2 FILMS BY DC MAGNETRON SPUTTERING METHOD 4.1 INTRODUCTION Sputter deposition process is another old technique being used in modern semiconductor industries. Sputtering
More informationGEM: A new concept for electron amplification in gas detectors
GEM: A new concept for electron amplification in gas detectors F. Sauli, Nucl. Instr. & Methods in Physics Research A 386 (1997) 531-534 Contents 1. Introduction 2. Two-step amplification: MWPC combined
More informationAdvances in the Micro-Hole & Strip Plate gaseous detector
Nuclear Instruments and Methods in Physics Research A 504 (2003) 364 368 Advances in the Micro-Hole & Strip Plate gaseous detector J.M. Maia a,b,c, *, J.F.C.A. Veloso a, J.M.F. dos Santos a, A. Breskin
More informationRate Dependency Study on Gas Electron Multiplier Gain
Rate Dependency Study on Gas Electron Multiplier Gain Final presentation Instructor: Dr. Francisco García Supervisor: Prof. Harri Ehtamo The document can be stored and made available to the public on the
More informationTechnology for Micro- and Nanostructures Micro- and Nanotechnology
Lecture 10: Deposition Technology for Micro- and Nanostructures Micro- and Nanotechnology Peter Unger mailto: peter.unger @ uni-ulm.de Institute of Optoelectronics University of Ulm http://www.uni-ulm.de/opto
More informationTable of Content. Mechanical Removing Techniques. Ultrasonic Machining (USM) Sputtering and Focused Ion Beam Milling (FIB)
Table of Content Mechanical Removing Techniques Ultrasonic Machining (USM) Sputtering and Focused Ion Beam Milling (FIB) Ultrasonic Machining In ultrasonic machining (USM), also called ultrasonic grinding,
More informationGEM at CERN. Leszek Ropelewski CERN PH-DT2 DT2-ST & TOTEM
GEM at CERN Leszek Ropelewski CERN PH-DT2 DT2-ST & TOTEM MicroStrip Gas Chamber Semiconductor industry technology: Photolithography Etching Coating Doping A. Oed Nucl. Instr. and Meth. A263 (1988) 351.
More informationNuclear Instruments and Methods in Physics Research A
Nuclear Instruments and Methods in Physics Research A 712 (2013) 8 112 Contents lists available at SciVerse ScienceDirect Nuclear Instruments and Methods in Physics Research A journal homepage: www.elsevier.com/locate/nima
More informationMicro Pixel Chamber Operation with Gas Electron Multiplier
Contents ts Micro Pixel Chamber Operation with Gas Electron Multiplier Kyoto University dept. of physics Cosmic-ray ygroup K. Hattori 1. μ-pic (Micro Pixel Chamber), micro-tpc (Time Projection Chamber
More informationOPTIMIZATION OF PLASMA UNIFORMITY USING HOLLOW-CATHODE STRUCTURE IN RF DISCHARGES*
51th Gaseous Electronics Conference & 4th International Conference on Reactive Plasmas Maui, Hawai i 19-23 October 1998 OPTIMIZATION OF PLASMA UNIFORMITY USING HOLLOW-CATHODE STRUCTURE IN RF DISCHARGES*
More informationPoS(EPS-HEP2015)232. Performance of a 1 m 2 Micromegas Detector Using Argon and Neon based Drift Gases
Performance of a m Micromegas Detector Using Argon and Neon based Drift Gases a, Otmar Biebel a, Jonathan Bortfeldt a, Ralf Hertenberger a, Ralph Müller a and Andre Zibell b a Ludwig-Maximilians-Universität
More informationUNIT 3. By: Ajay Kumar Gautam Asst. Prof. Dev Bhoomi Institute of Technology & Engineering, Dehradun
UNIT 3 By: Ajay Kumar Gautam Asst. Prof. Dev Bhoomi Institute of Technology & Engineering, Dehradun 1 Syllabus Lithography: photolithography and pattern transfer, Optical and non optical lithography, electron,
More informationElectron transparency, ion transparency and ion feedback of a 3M GEM
Nuclear Instruments and Methods in Physics Research A 525 (2004) 33 37 Electron transparency, ion transparency and ion feedback of a 3M GEM P.S. Barbeau a, J. Collar a, J. Miyamoto b, *, I. Shipsey b a
More informationPlasma parameter evolution in a periodically pulsed ICP
Plasma parameter evolution in a periodically pulsed ICP V. Godyak and B. Alexandrovich OSRAM SYLVANIA, 71 Cherry Hill Drive, Beverly, MA 01915, USA The electron energy probability function (EEPF) has been
More informationChung-Yao Chao Fellowship Interview
Chung-Yao Chao Fellowship Interview Shaobo WANG Shanghai Jiao Tong University, China April 24, 2017 Supervisor: Prof. Xiangdong JI Dr. Ke HAN 1 Outlines Resume: Education Internship Previous Work and Achievements:
More information08 - Miscellaneous and historical detectors
08 - Miscellaneous and historical detectors Jaroslav Adam Czech Technical University in Prague Version 2 Jaroslav Adam (CTU, Prague) DPD_08, Miscellaneous and historical detectors Version 2 1 / 25 Streamer
More informationCombinatorial RF Magnetron Sputtering for Rapid Materials Discovery: Methodology and Applications
Combinatorial RF Magnetron Sputtering for Rapid Materials Discovery: Methodology and Applications Philip D. Rack,, Jason D. Fowlkes,, and Yuepeng Deng Department of Materials Science and Engineering University
More informationA Multi-beamlet Injector for Heavy Ion Fusion: Experiments and Modeling
A Multi-beamlet Injector for Heavy Ion Fusion: Experiments and Modeling G.A. Westenskow, D.P. Grote; LLNL J.W. Kwan, F. Bieniosek; LBNL PAC07 - FRYAB01 Albuquerque, New Mexico June 29, 2007 This work has
More informationBreakdown limit studies in high-rate gaseous detectors
Nuclear Instruments and Methods in Physics Research A 422 (1999) 300 304 Breakdown limit studies in high-rate gaseous detectors Yu. Ivaniouchenkov, P. Fonte, V. Peskov *, B.D. Ramsey LIP, Coimbra University,
More informationPlasma Modeling with COMSOL Multiphysics
Plasma Modeling with COMSOL Multiphysics Copyright 2014 COMSOL. Any of the images, text, and equations here may be copied and modified for your own internal use. All trademarks are the property of their
More informationDefining quality standards for the analysis of solid samples
Defining quality standards for the analysis of solid samples Thermo Scientific Element GD Plus Glow Discharge Mass Spectrometer Redefine your quality standards for the elemental analysis of solid samples
More informationarxiv:physics/ v2 27 Mar 2001
High pressure operation of the triple-gem detector in pure Ne, Ar and Xe A. Bondar, A. Buzulutskov, L. Shekhtman arxiv:physics/0103082 v2 27 Mar 2001 Budker Institute of Nuclear Physics, 630090 Novosibirsk,
More informationElectromagnetics in COMSOL Multiphysics is extended by add-on Modules
AC/DC Module Electromagnetics in COMSOL Multiphysics is extended by add-on Modules 1) Start Here 2) Add Modules based upon your needs 3) Additional Modules extend the physics you can address 4) Interface
More informationR&D on Astroparticles Detectors. (Activity on CSN )
R&D on Astroparticles Detectors (Activity on CSN5 2000-2003) Introduction Results obtained with the R&D activity (2000-2003) with some drift chambers prototypes are reported. With different photocathode
More informationEFFECT OF PRESSURE AND ELECTRODE SEPARATION ON PLASMA UNIFORMITY IN DUAL FREQUENCY CAPACITIVELY COUPLED PLASMA TOOLS *
EFFECT OF PRESSURE AND ELECTRODE SEPARATION ON PLASMA UNIFORMITY IN DUAL FREQUENCY CAPACITIVELY COUPLED PLASMA TOOLS * Yang Yang a) and Mark J. Kushner b) a) Department of Electrical and Computer Engineering
More informationRadioactivity. Lecture 6 Detectors and Instrumentation
Radioactivity Lecture 6 Detectors and Instrumentation The human organs Neither humans nor animals have an organ for detecting radiation from radioactive decay! We can not hear it, smell it, feel it or
More informationChapter 7 Plasma Basic
Chapter 7 Plasma Basic Hong Xiao, Ph. D. hxiao89@hotmail.com www2.austin.cc.tx.us/hongxiao/book.htm Hong Xiao, Ph. D. www2.austin.cc.tx.us/hongxiao/book.htm 1 Objectives List at least three IC processes
More informationElectrical Discharges Characterization of Planar Sputtering System
International Journal of Recent Research and Review, Vol. V, March 213 ISSN 2277 8322 Electrical Discharges Characterization of Planar Sputtering System Bahaa T. Chaid 1, Nathera Abass Ali Al-Tememee 2,
More informationImprovement of MgO Characteristics Using RF-Plasma Treatment in AC Plasma Display Panel
Mol. Cryst. Liq. Cryst., Vol. 531: pp. 73=[373] 81=[381], 2010 Copyright # Taylor & Francis Group, LLC ISSN: 1542-1406 print=1563-5287 online DOI: 10.1080/15421406.2010.499331 Improvement of MgO Characteristics
More informationPerformance of a triple-gem detector for high-rate particle triggering
Performance of a triple-gem detector for high-rate particle triggering G. Bencivenni 1, W. Bonivento 2,4,A.Cardini 2,C. Deplano 2, P. de Simone 1, G. Felici 1, D. Marras 2, F.Murtas 1, D.Pinci 2,3, M.
More informationAn integrated Micromegas UV-photon detector
An integrated Micromegas UV-photon detector Joost Melai a*, Alexey Lyashenko b, Amos Breskin b, Harry van der Graaf c, Jan Timmermans c, Jan Visschers c, Cora Salm a, Jurriaan Schmitz a Abstract a University
More informationDOE WEB SEMINAR,
DOE WEB SEMINAR, 2013.03.29 Electron energy distribution function of the plasma in the presence of both capacitive field and inductive field : from electron heating to plasma processing control 1 mm PR
More informationIntroduction to Plasma
What is a plasma? The fourth state of matter A partially ionized gas How is a plasma created? Energy must be added to a gas in the form of: Heat: Temperatures must be in excess of 4000 O C Radiation Electric
More informationpp physics, RWTH, WS 2003/04, T.Hebbeker
3. PP TH 03/04 Accelerators and Detectors 1 pp physics, RWTH, WS 2003/04, T.Hebbeker 2003-12-16 1.2.4. (Inner) tracking and vertexing As we will see, mainly three types of tracking detectors are used:
More informationPERFORMANCE OF THE ATLAS LIQUID ARGON FORWARD CALORIMETER IN BEAM TESTS
1 PERFORMANCE OF THE ATLAS LIQUID ARGON FORWARD CALORIMETER IN BEAM TESTS P.KRIEGER Department of Physics, University of Toronto, Toronto, Ontario M5S 1A7, Canada E-mail: krieger@physics.utoronto.ca A
More informationMicroscopic Simulation of GEM Signals
Microscopic Simulation of GEM Signals von Moritz Seidel Bachelorarbeit in Physik vorgelegt der Fakultät für Mathematik, Informatik und Naturwissenschaften der RWTH Aachen angefertigt im III. Physikalischen
More informationPlasmonic Hot Hole Generation by Interband Transition in Gold-Polyaniline
Supplementary Information Plasmonic Hot Hole Generation by Interband Transition in Gold-Polyaniline Tapan Barman, Amreen A. Hussain, Bikash Sharma, Arup R. Pal* Plasma Nanotech Lab, Physical Sciences Division,
More informationLECTURE 5 SUMMARY OF KEY IDEAS
LECTURE 5 SUMMARY OF KEY IDEAS Etching is a processing step following lithography: it transfers a circuit image from the photoresist to materials form which devices are made or to hard masking or sacrificial
More informationStudy of DC Cylindrical Magnetron by Langmuir Probe
WDS'2 Proceedings of Contributed Papers, Part II, 76 8, 22. ISBN 978-737825 MATFYZPRESS Study of DC Cylindrical Magnetron by Langmuir Probe A. Kolpaková, P. Kudrna, and M. Tichý Charles University Prague,
More informationPerformance of high pressure Xe/TMA in GEMs for neutron and X-ray detection
Performance of high pressure Xe/TMA in GEMs for neutron and X-ray detection R. Kreuger, C. W. E. van Eijk, Member, IEEE, F. A. F. Fraga, M. M. Fraga, S. T. G. Fetal, R. W. Hollander, Member, IEEE, L. M.
More informationChapter 7. Plasma Basics
Chapter 7 Plasma Basics 2006/4/12 1 Objectives List at least three IC processes using plasma Name three important collisions in plasma Describe mean free path Explain how plasma enhance etch and CVD processes
More informationPHY 599: How it is usually done
PHY 599: How it is usually done This is Particle Physics and Astro-Cosmology Seminar We meet every Wednesday from 3:30 pm to 4:30 pm in Room 506 Nielsen. This seminar series is mainly intended for graduate
More informationHong Young Chang Department of Physics, Korea Advanced Institute of Science and Technology (KAIST), Republic of Korea
Hong Young Chang Department of Physics, Korea Advanced Institute of Science and Technology (KAIST), Republic of Korea Index 1. Introduction 2. Some plasma sources 3. Related issues 4. Summary -2 Why is
More informationStudy of Electronegativity in Inductively Coupled Radio-Frequency Plasma with Langmuir Probe
Study of Electronegativity in Inductively Coupled Radio-Frequency Plasma with Langmuir Probe International Training Program Queen s University Belfast Dept. Energy Sciences Tokyo Institute of Technology
More informationCCD readout of GEM-based neutron detectors
Nuclear Instruments and Methods in Physics Research A 478 (2002) 357 361 CCD readout of GEM-based neutron detectors F.A.F. Fraga a, *, L.M.S. Margato a, S.T.G. Fetal a, M.M.F.R. Fraga a, R. Ferreira Marques
More informationRecent Progress on D 3 - The Directional Dark Matter Detector
Recent Progress on D 3 - The Directional Dark Matter Detector Cosmic ray track (~7mm) detected with µd 3 prototype Motivation Detection Principle Performance of prototypes Plans for future Related activities
More informationPHYS 3446 Lecture #12
PHYS 3446 Lecture #12 Wednesday, Oct. 18, 2006 Dr. 1. Particle Detection Ionization Detectors MWPC Scintillation Counters Time of Flight 1 Announcements Next LPCC Workshop Preparation work Each group to
More informationGas-filled Detectors
Gas-filled Detectors Radiation Gas-filled Detectors In a gas-filled detector, the io9nization provides electrons and positive ions. The acceleration of these charged particles obeys the simple equation
More informationA Report On DESIGN OF NEUTRON SOURCES AND INVESTIGATION OF NEUTRON BASED TECHNIQUES FOR THE DETECTION OF EXPLOSIVE MATERIALS
A Report On DESIGN OF NEUTRON SOURCES AND INVESTIGATION OF NEUTRON BASED TECHNIQUES FOR THE DETECTION OF EXPLOSIVE MATERIALS Name of contact person: Surender Kumar Sharma Name of other contributors: R.
More informationATLAS New Small Wheel Phase I Upgrade: Detector and Electronics Performance Analysis
ATLAS New Small Wheel Phase I Upgrade: Detector and Electronics Performance Analysis Dominique Trischuk, Alain Bellerive and George Iakovidis IPP CERN Summer Student Supervisor August 216 Abstract The
More informationUltra-High Vacuum Technology. Sputter Ion Pumps l/s
Ultra-High Vacuum Technology 30-400 l/s 181.06.01 Excerpt from the Product Chapter C15 Edition November 2007 Contents General General..........................................................................
More informationINTRODUCTION TO THE HYBRID PLASMA EQUIPMENT MODEL
INTRODUCTION TO THE HYBRID PLASMA EQUIPMENT MODEL Prof. Mark J. Kushner Department of Electrical and Computer Engineering 1406 W. Green St. Urbana, IL 61801 217-144-5137 mjk@uiuc.edu http://uigelz.ece.uiuc.edu
More informationThe Gaseous Electronic Conference GEC reference cell as a benchmark for understanding microelectronics processing plasmas*
PHYSICS OF PLASMAS VOLUME 6, NUMBER 5 MAY 1999 The Gaseous Electronic Conference GEC reference cell as a benchmark for understanding microelectronics processing plasmas* M. L. Brake, J. Pender, a) and
More informationTMT4320 Nanomaterials November 10 th, Thin films by physical/chemical methods (From chapter 24 and 25)
1 TMT4320 Nanomaterials November 10 th, 2015 Thin films by physical/chemical methods (From chapter 24 and 25) 2 Thin films by physical/chemical methods Vapor-phase growth (compared to liquid-phase growth)
More informationThe plasma simulation system Brochure.
1 The plasma simulation system 2016 Brochure www.quantemol.com 2 What does Q-VT do? Quantemol-Virtual Tool is an expert software system for the simulation of industrial plasma processing tools. Q-VT builds
More informationHelicon Plasma Thruster Experiment Controlling Cross-Field Diffusion within a Magnetic Nozzle
Helicon Plasma Thruster Experiment Controlling Cross-Field Diffusion within a Magnetic Nozzle IEPC-2013-163 Presented at the 33rd International Electric Propulsion Conference, The George Washington University
More informationPlasma properties determined with induction loop probes in a planar inductively coupled plasma source
Plasma properties determined with induction loop probes in a planar inductively coupled plasma source J. A. Meyer, a) R. Mau, and A. E. Wendt b) Engineering Research Center for Plasma-Aided Manufacturing,
More information3 Gaseous Detectors. Detectors for Particle Physics Manfred Krammer Institute for High Energy Physics, Vienna, Austria
3 Gaseous Detectors Detectors for Particle Physics Manfred Krammer Institute for High Energy Physics, Vienna, Austria 3 Gaseous Detectors Content 3.1 Basic Principles 3.2 Diffusion and Drift 3.3 Amplification
More informationSummer Student Project Report
European Organization for Nuclear Research Summer Student Project Report Vlasios Vasileiou CERN EP/NOE Aristotle University of Thessaloniki Vlasios.Vasileiou@cern.ch August 2002 Supervisors: Igor Garcia
More informationPHOTOELECTRON COLLECTION EFFICIENCY AT HIGH PRESSURE FOR A GAMMA DETECTOR ENVISAGING MEDICAL IMAGING
822 PHOTOELECTRON COLLECTION EFFICIENCY AT HIGH PRESSURE FOR A GAMMA DETECTOR ENVISAGING MEDICAL IMAGING C.D.R. Azevedo 1, C.A.B. Oliveira 1, J.M.F. dos Santos 2, J.F.C.A. Veloso 1 1.University of Aveiro,
More informationATLAS EXPERIMENT : HOW THE DATA FLOWS. (Trigger, Computing, and Data Analysis)
ATLAS EXPERIMENT : HOW THE DATA FLOWS (Trigger, Computing, and Data Analysis) In order to process large volumes of data within nanosecond timescales, the trigger system is designed to select interesting
More informationThe ATLAS Detector - Inside Out Julia I. Hofmann
The ATLAS Detector - Inside Out Julia I. Hofmann KIP Heidelberg University Outline: 1st lecture: The Detector 2nd lecture: The Trigger 3rd lecture: The Analysis (mine) Motivation Physics Goals: Study Standard
More informationEffect of Gas Flow Rate and Gas Composition in Ar/CH 4 Inductively Coupled Plasmas
COMSOL CONFERENCE BOSTON 2011 Effect of Gas Flow Rate and Gas Composition in Ar/CH 4 Inductively Coupled Plasmas Keisoku Engineering System Co., Ltd., JAPAN Dr. Lizhu Tong October 14, 2011 1 Contents 1.
More informationThe BoNuS Detector. A Radial-Drift GEM TPC. Howard Fenker TPC R&D Meeting LBL, March 24, 2005
The BoNuS Detector A Radial-Drift GEM TPC Howard Fenker TPC R&D Meeting LBL, March 24, 2005 Barely Off-shell Nucleon Structure This work was partially supported by DOE Contract No. DE-AC05-84ER40150 under
More informationCHARACTERIZATION AND FIELD EMISSION PROPERTIES OF FIELDS OF NANOTUBES
CHARACTERIZATION AND FIELD EMISSION PROPERTIES OF FIELDS OF NANOTUBES Martin MAGÁT a, Jan PEKÁREK, Radimír VRBA a Department of microelectronics, The Faculty of Electrical Engineeering and Communication,
More informationEtching Issues - Anisotropy. Dry Etching. Dry Etching Overview. Etching Issues - Selectivity
Etching Issues - Anisotropy Dry Etching Dr. Bruce K. Gale Fundamentals of Micromachining BIOEN 6421 EL EN 5221 and 6221 ME EN 5960 and 6960 Isotropic etchants etch at the same rate in every direction mask
More informationLecture 6 Plasmas. Chapters 10 &16 Wolf and Tauber. ECE611 / CHE611 Electronic Materials Processing Fall John Labram 1/68
Lecture 6 Plasmas Chapters 10 &16 Wolf and Tauber 1/68 Announcements Homework: Homework will be returned to you on Thursday (12 th October). Solutions will be also posted online on Thursday (12 th October)
More informationDynamization evolution of Dry Etch Tools in Semiconductor Device Fabrication Gordon Cameron Intel Corp (November 2005)
Dynamization evolution of Dry Etch Tools in Semiconductor Device Fabrication Gordon Cameron Intel Corp (November 2005) Abstract Engineering Systems follow recognized trends of evolution; the main parameters
More informationETCHING Chapter 10. Mask. Photoresist
ETCHING Chapter 10 Mask Light Deposited Substrate Photoresist Etch mask deposition Photoresist application Exposure Development Etching Resist removal Etching of thin films and sometimes the silicon substrate
More information(a) (b) Fig. 1 - The LEP/LHC tunnel map and (b) the CERN accelerator system.
Introduction One of the main events in the field of particle physics at the beginning of the next century will be the construction of the Large Hadron Collider (LHC). This machine will be installed into
More informationTransducers. ME 3251 Thermal Fluid Systems
Transducers ME 3251 Thermal Fluid Systems 1 Transducers Transform values of physical variables into equivalent electrical signals Converts a signal from one form to another form 2 Types of Transducers
More informationAtomic layer deposition of titanium nitride
Atomic layer deposition of titanium nitride Jue Yue,version4, 04/26/2015 Introduction Titanium nitride is a hard and metallic material which has found many applications, e.g.as a wear resistant coating[1],
More informationB. Sitar G. I. Merso n V. A. Chechin Yu. A. Budagov. Ionization Measurement s in High Energy Physics
B. Sitar G. I. Merso n V. A. Chechin Yu. A. Budagov Ionization Measurement s in High Energy Physics Springer Tracts in modern physics ; v. 124) 0. Introduction 1 References 6 1. Ionization Effects in a
More informationAMS MEASUREMENTS OF DEUTERIUM CAPTURED IN TUNGSTEN LAYERS DEPOSITED BY MAGNETRON SPUTTERING
Romanian Reports in Physics, Vol. 65, No. 4, P. 1258 1264, 2013 AMS MEASUREMENTS OF DEUTERIUM CAPTURED IN TUNGSTEN LAYERS DEPOSITED BY MAGNETRON SPUTTERING A.R. PETRE 1,3, T. ACSENTE 2, M. ENACHESCU 1,
More informationD- Charge Exchange Ionizer for the JINR Polarized Ion Source POLARIS
D- Charge Exchange Ionizer for the JINR Polarized Ion Source POLARIS V.P. Ershov, V.V.Fimushkin, G.I.Gai, L.V.Kutuzova, Yu.K.Pilipenko, V.P.Vadeev, A.I.Valevich Λ and A.S. Belov Λ Joint Institute for Nuclear
More informationThermo Scientific ELEMENT GD PLUS Glow Discharge Mass Spectrometer. Defining quality standards for the analysis of solid samples
Thermo Scientific ELEMENT GD PLUS Glow Discharge Mass Spectrometer Defining quality standards for the analysis of solid samples Redefine your quality standards for the elemental analysis of solid samples
More informationThe Plasma Simulation System Brochure.
The Plasma Simulation System 2018 Brochure www.quantemol.com Benefits of Q-VT An experimentally validated simulation system focused on modelling plasma tools User-friendly interface Sets of validated cross-sections
More informationDetectors in Nuclear and High Energy Physics. RHIG summer student meeting June 2014
Detectors in Nuclear and High Energy Physics RHIG summer student meeting June 2014 Physics or Knowledge of Nature Experimental Data Analysis Theory ( application) Experimental Data Initial Conditions /
More informationSupporting Information: Robust production of purified H 2 in a stable, self-regulating, and continuously operating solar fuel generator
Supporting Information: Robust production of purified H 2 in a stable, self-regulating, and continuously operating solar fuel generator Miguel A. Modestino, Karl A. Walczak, Alan Berger, Christopher M.
More informationScintillation Detector
Scintillation Detector Introduction The detection of ionizing radiation by the scintillation light produced in certain materials is one of the oldest techniques on record. In Geiger and Marsden s famous
More informationSTATUS OF ATLAS TILE CALORIMETER AND STUDY OF MUON INTERACTIONS. 1 Brief Description of the ATLAS Tile Calorimeter
STATUS OF ATLAS TILE CALORIMETER AND STUDY OF MUON INTERACTIONS L. E. PRICE Bldg 362, Argonne National Laboratory, Argonne, IL 60439, USA E-mail: lprice@anl.gov (For the ATLAS Tile Calorimeter Collaboration)
More informationSignals in Particle Detectors (1/2?)
Signals in Particle Detectors (1/2?) Werner Riegler, CERN CERN Detector Seminar, 5.9.2008 The principle mechanisms and formulas for signal generation in particle detectors are reviewed. As examples the
More informationEnergetic particles and their detection in situ (particle detectors) Part II. George Gloeckler
Energetic particles and their detection in situ (particle detectors) Part II George Gloeckler University of Michigan, Ann Arbor, MI University of Maryland, College Park, MD Simple particle detectors Gas-filled
More informationTop Physics at CMS. Intae Yu. Sungkyunkwan University (SKKU), Korea Yonsei University, Sep 12 th, 2013
Top Physics at CMS Intae Yu Sungkyunkwan University (SKKU), Korea Seminar @ Yonsei University, Sep 12 th, 2013 Outline Overview of CMS Operation Korea CMS Group Doing Top Physics at LHC Top Production
More informationCharacterization of an Oxygen Plasma by Using a Langmuir Probe in an Inductively Coupled Plasma
Journal of the Korean Physical Society, Vol. 38, No. 3, March 001, pp. 59 63 Characterization of an Oxygen Plasma by Using a Langmuir Probe in an Inductively Coupled Plasma Jong-Sik Kim and Gon-Ho Kim
More informationCarrier lifetime variations during irradiation by 3-8 MeV K in MCZ Si
Carrier lifetime variations during irradiation by 3-8 MeV protons @ 40-300 K in MCZ Si E.Gaubas 1, J.Vaitkus 1, A.Uleckas 1,J.Raisanen 2 Outline 1) Vilnius university, Institute of Materials Science and
More informationDEPOSITION AND COMPOSITION OF POLYMER FILMS IN FLUOROCARBON PLASMAS*
DEPOSITION AND COMPOSITION OF POLYMER FILMS IN FLUOROCARBON PLASMAS* Kapil Rajaraman and Mark J. Kushner 1406 W. Green St. Urbana, IL 61801 rajaramn@uiuc.edu mjk@uiuc.edu http://uigelz.ece.uiuc.edu November
More informationRepetition: Practical Aspects
Repetition: Practical Aspects Reduction of the Cathode Dark Space! E x 0 Geometric limit of the extension of a sputter plant. Lowest distance between target and substrate V Cathode (Target/Source) - +
More informationCharge readout and double phase
Charge readout and double phase Vyacheslav Galymov IPN Lyon 1 st annual meeting AIDA-2020 Liquid argon double-phase TPC Concept of double-phase LAr TPC (Not to scale) Anode 0V 2 mm Collection field 5kV/cm
More informationEFFECT OF REACTOR GEOMETRY ON ION ENERGY DISTRIBUTIONS FOR PULSED PLASMA DOPING (P 2 LAD)*
EFFECT OF REACTOR GEOMETRY ON ION ENERGY DISTRIBUTIONS FOR PULSED PLASMA DOPING (P 2 LAD)* Ankur Agarwal a) and Mark J. Kushner b) a) Department of Chemical and Biomolecular Engineering University of Illinois
More informationOperation Characteristics of Diverging Magnetic Field Electrostatic Thruster
Operation Characteristics of Diverging Magnetic Field Electrostatic Thruster IEPC-07-9 Presented at the 5th International Electric Propulsion Conference Georgia Institute of Technology Atlanta, Georgia
More informationX- ray Photoelectron Spectroscopy and its application in phase- switching device study
X- ray Photoelectron Spectroscopy and its application in phase- switching device study Xinyuan Wang A53073806 I. Background X- ray photoelectron spectroscopy is of great importance in modern chemical and
More informationPartial Energy Level Diagrams
Partial Energy Level Diagrams 460 nm 323 nm 610 nm 330 nm 819 nm 404 nm 694 nm 671 nm 589 / 590 nm 767 / 769 nm Lithium Sodium Potassium Gas Mixtures Maximum Temperatures, C Air-Coal Gas 1825 Air-Propane
More informationAuthors: D.S.Roveri 1, H.H.Bertan 1, M.A.R.Alves 1, J.F.Mologni 2, E.S.Braga 1
Use of Ansoft Maxwell software platform for investigation of electrostatic properties of a hemisphere on a post geometry aimed to model field emission devices Authors: D.S.Roveri 1, H.H.Bertan 1, M.A.R.Alves
More informationR&D and related Simulation Studies for the sphenix Time Projection Chamber
R&D and related Simulation Studies for the sphenix Time Projection Chamber, for the sphenix collaboration Department of Physics and Astronomy, Stony Brook University, SUNY, Stony Brook, New York 1179-8,
More informationCourtesy of ESS and TheRGA web pages part of a series of application and theory notes for public use which are provided free of charge by ESS.
ESS The RGA freenotes Theory page 1 of 14 RGA Theory Notes Courtesy of ESS and TheRGA web pages part of a series of application and theory notes for public use which are provided free of charge by ESS.
More informationArab Journal of Nuclear Sciences and Applications
Ara J. Nucl. Sci. Appl, ol 5,, 8-88 (8) Ara Journal of Nuclear Sciences and Applications ISSN -45 We site: ajnsa.journals.ek.eg (ESNSA) Performance of the Secondary Townsend Emission through the Electric
More informationMicro Pixel Chamber with resistive electrodes for spark reduction
Micro Pixel Chamber with resistive electrodes for spark reduction arxiv:1310.5550v1 [physics.ins-det] 21 Oct 2013 Atsuhiko Ochi a, Yuki Edo a, Yasuhiro Homma a, Hidetoshi Komai a and Takahiro Yamaguchi
More informationGEM-based photon detector for RICH applications
Nuclear Instruments and Methods in Physics Research A 535 (2004) 324 329 www.elsevier.com/locate/nima GEM-based photon detector for RICH applications Thomas Meinschad, Leszek Ropelewski, Fabio Sauli CERN,
More informationExperimental Study of a 1-MW-Class Quasi-Steady-State Self-Field Magnetoplasmadynamic Thruster
Experimental Study of a 1-MW-Class Quasi-Steady-State Self-Field Magnetoplasmadynamic Thruster IEPC-2013-234 1 Kenji Miyazaki and 2 Syun Takenaka Tokai University, Hiratsuka, Kanagawa 259-1292, Japan 3
More information