11/8/2000 1 Diagnostic and Etching Studies of Inductively Coupled Plasmas SFR Workshop November 8, 2000 Matthew Radtke, John Coburn, David Graves Berkeley,

Slides:



Advertisements
Similar presentations
1B. PégouriéDITS progress report 27/04/07 Euratom EXPERIMENTAL CAMPAIGN No reliable estimation of the wall inventory WI ~ ??? D atoms (Tsitrone,
Advertisements

High Pressure Plasma with a third electrode James Roberts Physics TSP 2002 Supervised by Dr Kerrie Balla.
Andreas Steinbach, Stefan Wurm, Christian Koelbl Ferdinand Bell, Daniel Koehler, Dirk Knobloch Sematech AEC/APC Symposium X Plasma etch control by.
Lecture 21 QCM and Ellipsometry
TEST GRAINS AS A NOVEL DIAGNOSTIC TOOL B.W. James, A.A. Samarian and W. Tsang School of Physics, University of Sydney NSW 2006, Australia
Fusion Physics - Energy Boon or Nuclear Gloom? David Schilter and Shivani Sharma.
POLYMERISATION PROCESSES IN LOW-PRESSURE FLUOROCARBON PLASMAS
Physics of fusion power Lecture 11: Diagnostics / heating.
ISPC 2003 June , 2003 Consequences of Long Term Transients in Large Area High Density Plasma Processing: A 3-Dimensional Computational Investigation*
The energy influx from an rf plasma to a substrate during plasma processing W.W. Stoffels, E. Stoffels, H. Kersten*, M. Otte*, C. Csambal* and H. Deutsch.
Effects of active mode control on edge profiles and plasma-surface interactions in T2R H. Bergsåker with contributions from S. Menmuir, M. Henriksson et.
Research Opportunities in Radiation-Induced Chemical Dynamics Scientific Opportunities for Studying Laser Excited Dynamics at the LCLS: David Bartels Notre.
ATOMIC EMISSION SPECTROMETRY Chap 10 Sections: Sections: 10A 10A 10A-1 10A-1 10A-3 (skim) 10A-3 (skim) 10A-4 10A-4.
Simulations of Neutralized Drift Compression D. R. Welch, D. V. Rose Mission Research Corporation Albuquerque, NM S. S. Yu Lawrence Berkeley National.
Surface and volume production of negative ions in a low-pressure plasma E. Stoffels, W.W. Stoffels, V.M. Kroutilina*, H.-E. Wagner* and J. Meichsner*,
Center for Materials for Information Technology an NSF Materials Science and Engineering Center Vacuum Evaporation Lecture 8 G.J. Mankey
Remote Plasma Sputtering: Recent Developments in Understanding the Process S. Thornley, P. Hockley, M. Thwaites, J. Dutson Dr James Dutson Senior Development.
Lecture 11.0 Etching. Etching Patterned –Material Selectivity is Important!! Un-patterned.
Plasma Processing Overview
Introduction to Plasma- Surface Interactions G M McCracken Hefei, October 2007.
Plasma-Surface Interactions at a “Spinning Wall”
Submillimeter spectroscopic diagnostics in a semiconductor processing plasma Yaser H. Helal, Christopher F. Neese, Jennifer A. Holt, Frank C. De Lucia.
Spacecraft bus voltage and power DSCS II RCA SATCOM MILSTAR TDRS SKYLAB SPACE TELESCOPE LEASAT ISS HS702 space factory 、 space hotel.
Diode laser-induced fluorescence (LIF)measurements of metastable argon ions in a magnetized inductively coupled plasma ( ICP ) 报告人:李长君 组员:周涛涛 刘皓东 李长君 吴凯.
Mass spectrometry Ions are analyzed on the basis of their m/z Chlorine has 2 isotopes, 35 Cl and 37 Cl, in the approximate ratio of 3 :1. Electrons are.
Edge ECE measurements with the AUG CTS receiver and the effects of ELMs during H-mode Morten Stejner.
HiCAT- a Novel Diagnostic for Mass Loss and Species Composition Analysis Goal: Provide In-situ, real time characterization of ablated/ vaporized materials.
Hiden Analytical Excellence in plasma diagnostics An Introduction to the Hiden EQP Excellence in Plasma Diagnostics An Introduction to the Hiden EQP
Plasma diagnostics using spectroscopic techniques
Spatially Resolved Study of Inter-Cusp Transport and Containment of Primary Electrons Aimee A. Hubble a, John E. Foster b a) University of Michigan, Department.
Introduction to Plasma- Surface Interactions Lecture 3 Atomic and Molecular Processes.
Dust formation : speculated mechanism N i = density of particles with a size i R = nucleation rate (estimated from the chemical kinetics model) G = coagulation/agglomeration.
FLCC March 28, 2005 FLCC - Plasma 1 Fluid Modeling of Capacitive Plasma Tools FLCC Presentation March 28, 2005 Berkeley, CA David B. Graves, Mark Nierode,
11/8/ Microplasma Optical Emission Spectrometer (MOES) on a chip SFR Workshop November 8, 2000 Michiel Krüger, David Hsu, Scott Eitapence, K. Poolla,
Gregory ClarkeTechnological Plasmas Research Group Time resolved diagnostics for pulsed magnetron plasmas.
Passivation of HPGe Detectors at LNL-INFN Speaker: Gianluigi Maggioni Materials & Detectors Laboratory (LNL-INFN) Scientific Manager: Prof. Gianantonio.
Secondary Ion Mass Spectrometry A look at SIMS and Surface Analysis.
Langmuir Probe Plasma parameter measuring system “
11/8/ Damage Profiles of Low-Energy Ion Bombardment: Application to Ion Milling SFR Workshop November 8, 2000 Dave Humbird, David Graves Berkeley,
11/8/ Spatially Resolved Heat Flux Sensor Array on a Silicon Wafer for Plasma Etch Processes SFR Workshop November 8, 2000 Mason Freed, Costas Spanos,
Large Area Plasma Processing System (LAPPS) R. F. Fernsler, W. M. Manheimer, R. A. Meger, D. P. Murphy, D. Leonhardt, R. E. Pechacek, S. G. Walton and.
Submillimeter absorption spectroscopy in semiconductor manufacturing plasmas and comparison to theoretical models Yaser H. Helal, Christopher F. Neese,
Many mass spectra are observed in addition to those of nitrogen (28amu) and benzene (78amu) molecules between 1 and 80amu, when the discharge is not generated.
Materials Analysis of Transient Plasma-Wall Interactions PI: John Slough Post Doc: Samuel Andreason Graduate Student: Jamie Waldock Plasma Dynamics Laboratory.
11/8/ Radical Enhanced Atomic Layer Chemical Vapor Deposition (REALCVD) SFR Workshop November 8, 2000 Frank Greer, John Coburn, David Frazer, David.
Plasma Processing of Niobium SRF Cavities Janardan Upadhyay Department of Physics Center for Accelerator Sciences Old Dominion University Norfolk, Virginia.
化工学院第七届国际交流月系列讲座 邀请人:王文俊 化学工程与生物工程学院 化学工程联合国家重点实验室(浙江大学)
On Wafer Ion Flux Sensors
Experimental Techniques in Characterizing Polymer Adsorption
Study on Monatomic Fraction Improvement with Alumina Layer on Metal Electrode in Hydrogen Plasma Source Bong-Ki Jung, Kyung-Jae Chung, Jeong-Jeung Dang,
Seok-geun Lee, Young-hwa An, Y.S. Hwang
Saurabh J. Ullal, Anna R. Godfrey, Eray S. Aydil
Development of CR Model for OES in Hydrogen Plasma
Frank Greer, David Fraser, John Coburn, David Graves
DOE Plasma Science Center Control of Plasma Kinetics
COMPLEX ELECTRON ENERGY DISTRIBUTIONS IN ASYMMETRIC RF-DC DISCHARGES
Vacuum Beam Studies of Photoresist Etching Kinetics
Testbed for Plasma-Wall and Etch Product Studies
Instabilities in Electronegative Inductive Discharges
1.6 Glow Discharges and Plasma
Characterization of Thin Films
Nanocoating Plasma Systems, Inc.
Autonomous temperature sensor for bake plate calibration
K. Takechi and M. A. Lieberman
Silicon Etch Product Transport by an Inductively Coupled Plasma in Cl2
Instabilities in Electronegative Inductive Discharges
Instabilities in Inductive Discharges
Yaoxi Wu and M. A. Lieberman
On-Wafer Ion Flux Sensors
化工学院第七届国际交流月系列讲座 邀请人:王文俊 化学工程与生物工程学院 化学工程联合国家重点实验室(浙江大学)
Presentation transcript:

11/8/ Diagnostic and Etching Studies of Inductively Coupled Plasmas SFR Workshop November 8, 2000 Matthew Radtke, John Coburn, David Graves Berkeley, CA 2001 GOAL: Detection of depositing etch product in Si-O-Cl system by 9/30/2001.

11/8/ Motivation Increasingly stringent processing demands require better fundamental understanding of gas phase chemistry and plasma-surface interactions. Plasma diagnostic and surface interaction measurements are used to understand plasmas and provide modeling data. CF 4 is a common processing plasma and the radical recombination chemistry is not well understood.

11/8/ Experimental Apparatus – side view

11/8/ Experimental Apparatus – top view Langmuir Probe Ion Analysis Quadrupole Mass Spectrometer Neutral Analysis Quadrupole Mass Spectrometer Quartz Crystal Microbalance Plasma Chamber Optical Emission pressure gauge * industrial processing plasma use optical emission * very few systems have attempted to make all measurements simultaneously chopper beam background Thermocouple

11/8/ Experimental Procedure Measured QuantityMeasurement Diagnostic pressurepressure gauge radical and neutral densitiesquadrupole mass spectrometer (appearance potential mass spectrometry) ion compositionquadrupole mass spectrometer electron densityLangmuir probe electron energy distribution (electron temperature) Langmuir probe plasma potentialLangmuir probe average neutral temperatureoptical emission wall temperaturethermocouple * mass spectrometer measurements are at wall * Langmuir probe can measure profile

11/8/ Quartz Crystal Microbalance Quartz Crystal Microbalance (QCM) –films deposited on microbalance crystal –crystal oscillates at characteristic frequency proportional to its mass –change in mass causes frequency change oscillator crystal film plasma

11/8/ CF 3 Recombination Coefficient F in (CF 4 ) F out (CF 4 ) CF 4 CF 3 plasma Assume CF 4 formation at walls is due entirely to CF 3 recombination CF 4 balance in – out + recombination = reaction CF 4 + e  CF 3, CF 2, CF 3 +, … Walls – fluorocarbon deposited on stainless steel (30 +/- 2 o C) QCM - negligible deposition rate APMS - radical and neutral densities Langmuir Probe - electron energy distribution (f o )

11/8/ K diss calculation P(mTorr)k diss (10 -8 cm 3 /s) = 0.038

11/8/ Result Milestones Studies of plasma-wall interactions (e.g. Si/O/Cl for gate/trench etch) Studies of high-K etching (e.g. etch precursors, by-products, selectivity) Studies of plasma surface interaction (e.g. N 2 plasma / PET; NF 3 plasma / elastomer)