Experimental High Energy Physics & Plasma Etching

Similar documents
DEPOSITION OF THIN TiO 2 FILMS BY DC MAGNETRON SPUTTERING METHOD

GEM: A new concept for electron amplification in gas detectors

Advances in the Micro-Hole & Strip Plate gaseous detector

Rate Dependency Study on Gas Electron Multiplier Gain

Technology for Micro- and Nanostructures Micro- and Nanotechnology

Table of Content. Mechanical Removing Techniques. Ultrasonic Machining (USM) Sputtering and Focused Ion Beam Milling (FIB)

GEM at CERN. Leszek Ropelewski CERN PH-DT2 DT2-ST & TOTEM

Nuclear Instruments and Methods in Physics Research A

Micro Pixel Chamber Operation with Gas Electron Multiplier

OPTIMIZATION OF PLASMA UNIFORMITY USING HOLLOW-CATHODE STRUCTURE IN RF DISCHARGES*

PoS(EPS-HEP2015)232. Performance of a 1 m 2 Micromegas Detector Using Argon and Neon based Drift Gases

UNIT 3. By: Ajay Kumar Gautam Asst. Prof. Dev Bhoomi Institute of Technology & Engineering, Dehradun

Electron transparency, ion transparency and ion feedback of a 3M GEM

Plasma parameter evolution in a periodically pulsed ICP

Chung-Yao Chao Fellowship Interview

08 - Miscellaneous and historical detectors

Combinatorial RF Magnetron Sputtering for Rapid Materials Discovery: Methodology and Applications

A Multi-beamlet Injector for Heavy Ion Fusion: Experiments and Modeling

Breakdown limit studies in high-rate gaseous detectors

Plasma Modeling with COMSOL Multiphysics

Defining quality standards for the analysis of solid samples

arxiv:physics/ v2 27 Mar 2001

Electromagnetics in COMSOL Multiphysics is extended by add-on Modules

R&D on Astroparticles Detectors. (Activity on CSN )

EFFECT OF PRESSURE AND ELECTRODE SEPARATION ON PLASMA UNIFORMITY IN DUAL FREQUENCY CAPACITIVELY COUPLED PLASMA TOOLS *

Radioactivity. Lecture 6 Detectors and Instrumentation

Chapter 7 Plasma Basic

Electrical Discharges Characterization of Planar Sputtering System

Improvement of MgO Characteristics Using RF-Plasma Treatment in AC Plasma Display Panel

Performance of a triple-gem detector for high-rate particle triggering

An integrated Micromegas UV-photon detector

DOE WEB SEMINAR,

Introduction to Plasma

pp physics, RWTH, WS 2003/04, T.Hebbeker

PERFORMANCE OF THE ATLAS LIQUID ARGON FORWARD CALORIMETER IN BEAM TESTS

Microscopic Simulation of GEM Signals

Plasmonic Hot Hole Generation by Interband Transition in Gold-Polyaniline

LECTURE 5 SUMMARY OF KEY IDEAS

Study of DC Cylindrical Magnetron by Langmuir Probe

Performance of high pressure Xe/TMA in GEMs for neutron and X-ray detection

Chapter 7. Plasma Basics

PHY 599: How it is usually done

Hong Young Chang Department of Physics, Korea Advanced Institute of Science and Technology (KAIST), Republic of Korea

Study of Electronegativity in Inductively Coupled Radio-Frequency Plasma with Langmuir Probe

CCD readout of GEM-based neutron detectors

Recent Progress on D 3 - The Directional Dark Matter Detector

PHYS 3446 Lecture #12

Gas-filled Detectors

A Report On DESIGN OF NEUTRON SOURCES AND INVESTIGATION OF NEUTRON BASED TECHNIQUES FOR THE DETECTION OF EXPLOSIVE MATERIALS

ATLAS New Small Wheel Phase I Upgrade: Detector and Electronics Performance Analysis

Ultra-High Vacuum Technology. Sputter Ion Pumps l/s

INTRODUCTION TO THE HYBRID PLASMA EQUIPMENT MODEL

The Gaseous Electronic Conference GEC reference cell as a benchmark for understanding microelectronics processing plasmas*

TMT4320 Nanomaterials November 10 th, Thin films by physical/chemical methods (From chapter 24 and 25)

The plasma simulation system Brochure.

Helicon Plasma Thruster Experiment Controlling Cross-Field Diffusion within a Magnetic Nozzle

Plasma properties determined with induction loop probes in a planar inductively coupled plasma source

3 Gaseous Detectors. Detectors for Particle Physics Manfred Krammer Institute for High Energy Physics, Vienna, Austria

Summer Student Project Report

PHOTOELECTRON COLLECTION EFFICIENCY AT HIGH PRESSURE FOR A GAMMA DETECTOR ENVISAGING MEDICAL IMAGING

ATLAS EXPERIMENT : HOW THE DATA FLOWS. (Trigger, Computing, and Data Analysis)

The ATLAS Detector - Inside Out Julia I. Hofmann

Effect of Gas Flow Rate and Gas Composition in Ar/CH 4 Inductively Coupled Plasmas

The BoNuS Detector. A Radial-Drift GEM TPC. Howard Fenker TPC R&D Meeting LBL, March 24, 2005

CHARACTERIZATION AND FIELD EMISSION PROPERTIES OF FIELDS OF NANOTUBES

Etching Issues - Anisotropy. Dry Etching. Dry Etching Overview. Etching Issues - Selectivity

Lecture 6 Plasmas. Chapters 10 &16 Wolf and Tauber. ECE611 / CHE611 Electronic Materials Processing Fall John Labram 1/68

Dynamization evolution of Dry Etch Tools in Semiconductor Device Fabrication Gordon Cameron Intel Corp (November 2005)

ETCHING Chapter 10. Mask. Photoresist

(a) (b) Fig. 1 - The LEP/LHC tunnel map and (b) the CERN accelerator system.

Transducers. ME 3251 Thermal Fluid Systems

Atomic layer deposition of titanium nitride

B. Sitar G. I. Merso n V. A. Chechin Yu. A. Budagov. Ionization Measurement s in High Energy Physics

AMS MEASUREMENTS OF DEUTERIUM CAPTURED IN TUNGSTEN LAYERS DEPOSITED BY MAGNETRON SPUTTERING

D- Charge Exchange Ionizer for the JINR Polarized Ion Source POLARIS

Thermo Scientific ELEMENT GD PLUS Glow Discharge Mass Spectrometer. Defining quality standards for the analysis of solid samples

The Plasma Simulation System Brochure.

Detectors in Nuclear and High Energy Physics. RHIG summer student meeting June 2014

Supporting Information: Robust production of purified H 2 in a stable, self-regulating, and continuously operating solar fuel generator

Scintillation Detector

STATUS OF ATLAS TILE CALORIMETER AND STUDY OF MUON INTERACTIONS. 1 Brief Description of the ATLAS Tile Calorimeter

Signals in Particle Detectors (1/2?)

Energetic particles and their detection in situ (particle detectors) Part II. George Gloeckler

Top Physics at CMS. Intae Yu. Sungkyunkwan University (SKKU), Korea Yonsei University, Sep 12 th, 2013

Characterization of an Oxygen Plasma by Using a Langmuir Probe in an Inductively Coupled Plasma

Carrier lifetime variations during irradiation by 3-8 MeV K in MCZ Si

DEPOSITION AND COMPOSITION OF POLYMER FILMS IN FLUOROCARBON PLASMAS*

Repetition: Practical Aspects

Charge readout and double phase

EFFECT OF REACTOR GEOMETRY ON ION ENERGY DISTRIBUTIONS FOR PULSED PLASMA DOPING (P 2 LAD)*

Operation Characteristics of Diverging Magnetic Field Electrostatic Thruster

X- ray Photoelectron Spectroscopy and its application in phase- switching device study

Partial Energy Level Diagrams

Authors: D.S.Roveri 1, H.H.Bertan 1, M.A.R.Alves 1, J.F.Mologni 2, E.S.Braga 1

R&D and related Simulation Studies for the sphenix Time Projection Chamber

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.

Arab Journal of Nuclear Sciences and Applications

Micro Pixel Chamber with resistive electrodes for spark reduction

GEM-based photon detector for RICH applications

Experimental Study of a 1-MW-Class Quasi-Steady-State Self-Field Magnetoplasmadynamic Thruster

Transcription:

Experimental High Energy Physics & Plasma Etching Samah M. Balouza Purdue University Nikhef Doctoral Interview 07/06/2017

Outlines Plasma Physics Research Experimental High Energy PhysicsResearch Samah Balouza - Nikhef Doctoral Interview 2

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

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

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+16 3.00E+16 2.50E+16 1.00E+16 2.00E+16 8.00E+15 1.50E+16 6.00E+15 1.00E+16 4.00E+15 5.00E+15 2.00E+15 1 11 21 31 41 51 61 71 81 0.00E+00 1 11 21 31 41 51 61 71 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

Electron Density (1/m3) Argon/Oxygen Mixture 1.20E+15 1.10E+15 1.00E+15 9.00E+14 8.00E+14 7.00E+14 6.00E+14 5.00E+14 4.00E+14 1 11 21 31 41 51 61 71 81 r/10^3 (m) 30% O2 40% O2 50% O2 Electron density distributions at different oxygen concentrations. Samah Balouza - Nikhef Doctoral Interview 6

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

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

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

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: www.cern.ch/ Samah Balouza - Nikhef Doctoral Interview 10

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

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

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

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

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

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

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

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

Thank You! 19

Back-Up Slides 20

IEEE-NPSS International Conference of Plasma Physics (ICOPS-2015) Samah Balouza - Nikhef Doctoral Interview 21

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+18 1.5E+18 1E+18 5E+17 0 0 20 40 60 80 100 120 Pressure (mtorr) COMSOL Experimental Electron density versus pressure Samah Balouza - Nikhef Doctoral Interview 22

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

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+15 1.40E+15 1.20E+15 1.00E+15 8.00E+14 6.00E+14 4.00E+14 2.00E+14 0.00E+00 1 11 21 31 41 51 61 71 81 r/10^3 (m) 600W 800W 1000W 1200W Electron density at different power values. Samah Balouza - Nikhef Doctoral Interview 24

- 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

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

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

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

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