LIGO-G070079-00-Z D. Ugolini, LSC March 2007 1 Progress Report on Charging Measurements at Trinity University Dennis Ugolini, Robert McKinney, Mark Girard.

Slides:



Advertisements
Similar presentations
Fluorescent Lamps.
Advertisements

Status of test beam data analysis … with emphasis on resistive coating studies Progress and questions 1Meeting at CEA Saclay, 25 Jan 2010Jörg Wotschack,
1 LSC/VIRGO Meeting, Caltech, March 18, 2008 Overview of Charging Research Valery Mitrofanov Moscow State University On behalf of charging subgroup LIGO-G Z.
Bellow valve (trap&pump) Inside glove box. (Note: Ar glove box is not necessary, if you work with single crystalline organic materials like rubrene that.
LIGO Charging Workgroup Telcon 12/12/ GRS LSC_Charging_ ppt K. Sun UV LED Charge Management Progress Report LIGO Charging Workgroup Telcon.
Atomic Absorption Spectroscopy Prof Dr Hisham E Abdellatef 2011.
LIGO Science Collaboration Meeting Hanford, March 19-23, GRS LIGO_LSC_Sun_UVLED_ ppt, K. Sun LIGO Test Mass Charging Mitigation Using Modulated.
Unit 24 Gas Laws Definition and units of pressure (6.6) Simple gas laws: Boyles, Charles (6.6) Ideal Gas Law (6.7)
Photolithography Photolithography is the transfer of patterns, circuits, device structures, etc. to a substrate or wafer using light and a mask.
Second Sound in Superfluid Helium. Superfluids “Superfluid” describes a phase of matter. In this phase, a liquid has no viscosity and may exhibit several.
Nonstationary electrical charge distribution on the fused silica bifilar pendulum and its effect on the mechanical Q-factor V.P. Mitrofanov, L.G. Prokhorov,
CAMERA MATERIALS TEST CHAMBER Jack Singal 9/17/08 LSST Camera Workshop Turbo pump Optics table scroll pump and LN trap (for roughing A1, A3, and LL)
Prototype TPC Tests C. Lu 12/9/98 V = 0. Gas gain test for the low pressure chamber The chamber is constructed with the following parameters: D anode.
Magneto-optical study of InP/InGaAs/InP quantum well B. Karmakar, A.P. Shah, M.R. Gokhale and B.M. Arora Tata Institute of Fundamental Research Mumbai,
Progress in water vapour spectroscopy at RAL Dr Robert McPheat CAVIAR Progress Meeting Cosners’ House, 14/12/2009.
Progress in water vapour spectroscopy at RAL Dr Robert McPheat CAVIAR Progress Meeting University of Leicester, 24/09/2009.
ITO(24nm)/parylene( = 1.14  m)/rubrene OFETs, made device #1 device #3device #4 device #2 Please, look at the top surface of each device under.
Top Side Conductor vacuum deposition Aluminum sputter deposit in Argon plasma CVC 601-sputter deposition tool.
BA , 1 Principles of Acoustic Measurements Exercises: Basic Concepts of Sound Measuring Sound Measuring Sound in Practice Basic Frequency Analysis.
PEEM III Endstation Design Review
Active Seismic Isolation Systems for Enhanced and Advanced LIGO Jeffrey S. Kissel 1 for the LSC 1 Louisiana State University The mechanical system for.
LIGO-G Z D. Ugolini, Charging Workshop July UV Illumination Studies at Trinity University Dennis Ugolini, Mark Girard 2007 Workshop on.
Solar Cell conductive grid and back contact
Charge Mitigation Studies Stuart Reid, I. Martin, A. Cumming, W. Cunningham, J. Hough, P. Murray, S. Rowan. Glasgow M. Fejer, A. Markosyan, R. Route Stanford.
Threshold ionization mass spectroscopy of radicals in RF silane discharge Peter Horvath 5/19/2004 Progress of experiments.
LIGO-G Z D. Ugolini, LSC March Developing a Kelvin Probe for Measuring Surface Charge on LIGO Optics Dennis Ugolini, Robert McKinney Trinity.
Overview of Research in the Optics Working Group Gregory Harry, on behalf of the OWG Massachusetts Institute of Technology July 25, 2007 LSC Meeting –
LIGO-G Z August, 2006 LSC R&D for AdLIGO ASC Detectors LSC Meeting August 2006 Richard Abbott.
Trinity Charging Experiment Gregg Harry, MIT On behalf of Dennis Ugolini, Trinity LIGO-G R.
STREGA WP1/M1 mirror substrates GEO LIGO ISA Scientific motivation: Mechanical dissipation from dielectric mirror coatings is predicted to be a significant.
Spectrophotometer Prof.Dr. Moustafa M. Mohamed Vice Dean Faculty of Allied Medical Science Pharos University in Alexandria, EGYPT.
Creative Research Initiatives Seoul National University Center for Near-field Atom-Photon Technology - Near Field Scanning Optical Microscopy - Electrostatic.
IPM status and plans 1.Yellow vertical detector has extremely low coupling to beam and to signal-gating grid. It also has improved resolution due to reduced.
Test mass charge relaxation V.P.Mitrofanov, P.E.Khramchenkov, L.G.Prokhorov Moscow State University LIGO/VIRGO LSC Meeting, Baton Rouge, March 2007 G Z.
SQUID Performance in a HV Environment
Stanford High Power Laser Lab Status of high power laser development for LIGO at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert.
HEC strange signals 1 09 Feb 2012 E.Ladygin Status of HEC spikes study in Protvino E.Ladygin, M.Kazarinov, A.Kozelov.
Test mass charge relaxation V.P.Mitrofanov, P.E.Khramchenkov, L.G.Prokhorov Moscow State University.
Effect of Charging on Thermal Noise Gregory Harry Massachusetts Institute of Technology - Core Optics and Suspensions Working Groups - March 19, 2004 –
D. Ugolini, Joint APS-AAPT Meeting at UT-Arlington, October 2006 Developing a Capacitive Probe for Measuring Charging Effects on In-Vacuum Optics Dennis.
The basics of in-situ Electrochemcial FTIR spectroscopy
Investigation of effects associated with electrical charging of fused silica test mass V. Mitrofanov, L. Prokhorov, K. Tokmakov Moscow State University.
1 Al Moretti, APC, Fermilab MAP- Winter Meeting February 28 - March 4, 2011 TJNAF Newport News, VA.
Solar Cells need a top side conductor to collect the current generated They also need a conductive film on the backside.
Vacuum Studies of LHCb Vertex Locator Sensors Gwenaëlle Lefeuvre, Ray Mountain, Marina Artuso Department of Physics, Syracuse University Abstract : The.
MONALISA Update David Urner ATF2 Meeting Dec
HBD Transmission Monitor Update III: Noise Analysis B. Azmoun & S. Stoll BNL HBD Working Group Meeting 10/10/06.
Cooling Test Results on fuzzy carbon substrate Setup in Lotima Room Used water/glycol mix (70/30 by wt) Neslab chiller to set temp Small pump to get the.
Properties of the bakelite used for standard RPC chambers as a function of the operating temperature F. Bruni – G. Hull – S.M. Mari 4 digital thermometers.
TRIUMF laboratory studies Christopher Hearty University of British Columbia/IPP 27-Sep-2010.
Lessons from CLIO Masatake Ohashi (ICRR, The University of TOKYO) and CLIO collaborators GWADW2012 Hawaii 2012/5/16.
Date of download: 6/22/2016 Copyright © 2016 SPIE. All rights reserved. Experimental setup of the optical parametric oscillator (OPO)-based photoacoustic.
Mg Films Grown by Pulsed Laser Deposition as Photocathodes: QE and surface adsorbates L. Cultrera INFN – National Laboratories of Frascati.
Roughness and Electrical Resistivity of Thin Films Spencer Twining, Marion Titze, Ozgur Yavuzcetin University of Wisconsin – Whitewater, Department of.
BNL-SLAC-Annecy TeleConference
Photolithography Photolithography is the transfer of patterns, circuits, device structures, etc. to a substrate or wafer using light and a mask.
Plans for this week MWPC: wire stretching today
Ultrasound.
Circuit QED Experiment
Potential and Current Control
K. H. Lee, H. Y. Lee, Young-Gi Kim, J. Yang, S. M. Yang, K.J. Chung, Y.S. Na and Y. S. Hwang Residual Gas analysis during Glow discharge cleaning, Baking.
Generation of a Strong Pressure Wave
CAS 2017 Vacuum simulations
Nano Cost Nano Patterned Template for
大強度
CAS 2017 Vacuum simulations
HVCMOS Detectors – Overview
Synthetic Sapphire Absorbance at 1064 nm
ME instrument and in-orbit performance
Status/plans for the development of small scale lab. experiments
Presentation transcript:

LIGO-G Z D. Ugolini, LSC March Progress Report on Charging Measurements at Trinity University Dennis Ugolini, Robert McKinney, Mark Girard Trinity University March LSC Meeting March 21, 2007 Goal: To develop a vacuum-compatible capacitive probe to measure the charge magnitude and relaxation time constant on LIGO optics

LIGO-G Z D. Ugolini, LSC March The Capacitive Probe  Use chopper to alternately expose/occlude sample  Aluminum probe body with Kapton-shielded wire  Sensitivity calibrated with surface DC voltmeter to be (3.5 +/- 0.5) × 10 5 e - /cm 2 (to be published in Rev. Sci. Instr.)

LIGO-G Z D. Ugolini, LSC March Optical Measurement Setup  Chopper shielded by aluminum box  Optic held by viton O-rings epoxied to aluminum clamps

LIGO-G Z D. Ugolini, LSC March Measurement Setup (cont.) Viton O-rings

LIGO-G Z D. Ugolini, LSC March Vacuum System Pfeiffer-Balzers Turbomechanical drag pump (~10 -5 torr) Pressure gauge goes here (returned for servicing) Feedthrough (on either side) Glass viewport

LIGO-G Z D. Ugolini, LSC March Obstacles in Moving to Vacuum  Pickup by probe signal lead from chopper driver wires »Used two feedthroughs, one for chopper, one for probe »Chopper wires tied to optical table, kept far from probe lead  Intermittent probe noise peak »Caused by contact between probe lead and nearly anything (chopper shielding box, optical table, walls of the vacuum chamber) »Vibrational or electrical? »Kapton wire is rigid, hold position well  Applied charge decays too rapidly to pump down system »Strong function of humidity, dehumidifier purchased »Spark? »Options for applying charge inside chamber (brush?)

LIGO-G Z D. Ugolini, LSC March Readout Problem  Finally trapped large charge on optic on February 20 th  Probe readout oscillated, didn’t damp out over many hours  Drift in chopper frequency shifted peak on spectrum analyzer  Switched to lock-in amp, used chopper driver as reference

LIGO-G Z D. Ugolini, LSC March Day Results Corresponds to time constant of ~170 days Appears to level off around day 13 Large phase change on “dropouts” – problem with reference?

LIGO-G Z D. Ugolini, LSC March UV Discharging Exposed to Hg discharge tube (no UV) for several hours – no effect Exposed to Pen-Ray UV Lamp (253.7nm, 4.4mW/cm 2 at 19mm), exhibits discharging shown Glass viewport has ~15% transmission at this wavelength

LIGO-G Z D. Ugolini, LSC March Summary  Probe has been successfully moved to vacuum  Decay of charge deposited on optical sample has been observed with a time constant of ~170 days »What are the differences between this setup and Moscow State? Optical substrate? Surface contact? Pressure?  Demonstrated UV discharging with glass viewport  Next steps Longer timeTriplicate setup Charge vs. positionDifferent substrates, coatings, etc. Besocke Kelvin probeQuartz viewport? Discharging vs. λ ?