Update on aLIGO Charging Issues

Slides:



Advertisements
Similar presentations
Mitigation of AC Induced Voltage On Buried Metallic Pipelines
Advertisements

Hiro Yamamoto LLO April 3, 2014 LIGO-G Core Optics related loss hierarchy of aLIGO Hiro Yamamoto LIGO/Caltech Introduction Loss related to geometry.
Advanced LIGO1 Laser Induced Damage due to Particulate Contamination Billingsley, Gushwa, Phelps, Torrie, Zhang LVC meeting March 2014.
CONDUCTORS + CAPACITORS
Electric Potential and Field
Chapter 23: Electrostatic Energy and Capacitance
One Arm Cavity M0 L1 L2 TM M0 L1 L2 TRIPLE QUAD 16m R = 20m, T=1% R = ∞, T=1%  Optimally coupled cavity (no mode matched light reflected back)  Finesse.
Wednesday, Sept. 28, 2005PHYS , Fall 2005 Dr. Jaehoon Yu 1 PHYS 1444 – Section 003 Lecture #9 Wednesday, Sept. 28, 2005 Dr. Jaehoon Yu Quiz Results.
Nonstationary electrical charge distribution on the fused silica bifilar pendulum and its effect on the mechanical Q-factor V.P. Mitrofanov, L.G. Prokhorov,
LIGO-G9900XX-00-M LIGO R&D1 Gold Coatings in Advanced LIGO Phil Willems.
LIGO-G W Commissioning Data on Vibration Isolation & Suspensions Fred Raab 24 October 02.
L 24 Electricity & Magnetism [2]
Test Mass Discharging System (TMDS) Design Review 20 Nov 2014 Rich Abbott, Dennis Coyne, Eddie Sanchez, Calum Torrie 1 LIGO-G v1.
Electricity and Magnetism Electrostatics Capacitance and Capacitive Circuits.
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 –
SUSPENSION DESIGN FOR ADVANCED LIGO: Update on GEO Activities Norna A Robertson University of Glasgow for the GEO 600 suspension team LSC Meeting, Louisiana,
Conceptual Design for Advanced LIGO Suspensions Norna A Robertson University of Glasgow and Stanford University for the GEO suspension team +contribution.
G M 1 Advanced LIGO Update David Shoemaker LSC/Virgo MIT July 2007.
Y Z Bai, H Yin, L Liu, D Y Tan, Z B Zhou Center for Gravitational Experiments, School of Physics, Huazhong Univ. of Science &
G Amaldi Meeting 2015, Gwangju, South Korea1 Status of LIGO June 22, 2015 Daniel Sigg LIGO Hanford Observatory (on behalf of the LIGO Scientific.
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.
Cavity Work at LASTI LSC-VIRGO Meeting, Hannover - 24 th October 2007 Lisa Barsotti and Matthew Evans for the LASTI group G D.
G Advanced LIGO Coating Research Overview of Optics Handling and Cleaning Procedures Helena Armandula LSC – March 2006.
PeTeR: a hardware simulator for LISA PF TM-GRS system 23/05/ th LISA Symposium May 2012, BnF Paris L. Marconi and R. Stanga Università degli.
LIGO-G R Gold Barrel Coatings- Our Savior Phil Willems LIGO/Caltech LSC/Virgo Meeting, Caltech 3/20/2008.
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.
Investigation of effects associated with electrical charging of fused silica test mass V. Mitrofanov, L. Prokhorov, K. Tokmakov Moscow State University.
Introduction to Capacitors
Capacitor Device that can store electric charge Two conducting objects are placed near one another but not touching Power source charges up the plates,
Practical considerations for quad suspension upgrades Giles Hammond, Norna Robertson, Travis Sadecki, Brett Shapiro, Betsy Weaver G v3.
ELEC 3105 Basic EM and Power Engineering
Electrostatic actuators - ESD
Chapter 26A - Capacitance
Capacitance, Polarization and Dielectrics
H1 Squeezing Experiment: the path to an Advanced Squeezer
SWBAT calculate the electrostatic force acting on an object.
Electrostatics.
Unit 3: Electricity and Magnetism Lesson 1
Polyimide sheet (5 mils)) AZ-93 Thermal Paint (5 mils))
Equipotential Lines Are Topographical Maps
Fields: Forces and Energy
Applications of Electro-statics
Electrostatics Objects become charged due to the movement of electrons
Static Eliminator Maintenance.
Reaching the Advanced LIGO Detector Design Sensitivity
First Lessons from the Advanced LIGO Integration Testing
Generation of a Strong Pressure Wave
WORKSHOP PRACTICE WEEK-3 OBJECTIVE OF LAB-2 To be familiar with the capacitor and the inductor.
Capacitors.
Electric Potential and Electrical Field
Practice #6—Electric Charge, Fields, and Capacitors
Chapter 17 Electric Potential
Teacher Imarlys Cajigas 5th grade Science
Concepts sheet Electrostatics Exam
L 25 Electricity & Magnetism [2]
KICKER STATUS G-2 meeting March 5, 2014
Charging without contact
Intro to Electricity.
But why did they sink in the first place?
Electrons & Energy Levels
Electrostatics Electrostatics- study of charges that can be collected in one place (static electricity) Electric charge, the forces between them, and.
Electrostatics Electric charges at rest (static electricity)
Lessons Learned from Commissioning of Advanced Detectors
Objectives: After completing this module, you should be able to:
FIGURE 12-1 A Leyden jar can be used to store an electrical charge.
Chapter 16 Electric Field of Distributed Charges
Capacitance and Capacitors
Presentation transcript:

Update on aLIGO Charging Issues Need a catchy title for the talk, but drawing a blank… Update on Charging Issues, First Contact/Contamination Control, and Other Headaches? TITLE Talk Notes Update on aLIGO Charging Issues Kate Gushwa LIGO Laboratory California Institute of Technology On behalf of LIGO Engineering Team LVC Meeting September 2015 LIGO-G1501076-v1 LIGO-G1501076-v1

Electrostatic Charging TITLE Talk Notes WHAT TO SAY This is where ideas go… Rai gave talk in March… so this is just a quick overview/recap of the problem QUAD damping & control Top 3 stages: coil- magnet actuators Bottom stage: electrostatic actuator Quads use electrostatic drive (ESD) system instead of coil-magnet actuators on lowest stage to reduce noise coupling due to magnets Each pair of electrodes forms a capacitor, whose fringe field attracts the test mirror surface (dielectric). Distance between electrodes and ETM is 5mm. 5 channels to drive electrodes; 1 common BIAS, 4 driving channels (1 per quadrant). Electrostatic Charging Electrostatic drive (ESD) 4 electrode pairs coated onto reaction mass xcfb Main (Test) Chain Reaction Chain Finish / fix: Slide content Animations What to say Did part Denis want get deleted? NOTES QUAD damping & control: Stage 1-3: coil-magnet actuators Stage 4: electrostatic actuator Electrostatic drive (ESD) Pattern of 4 interleaving electrode pairs coated onto the inner surfaces of the reaction chain masses (CP for ITMs, ERM for ETMs). Each pair or electrodes forms a capacitor 1 electrode from each pair/quadrant is connected to a common bias potential, and control signals are applied to the remaining electrode. Applying a potential difference creates a fringing field that attracts the dielectric test mass. Capacitance of the pattern depends on the distance between the test mass and reaction mass. So changing the voltage on the electrodes changes the attractive force between the masses. Effects of charging: Interferers with optical position control Attracts dust Reducing reflectance Increasing scattering & absorption Accumulation & motion of charge is a potentially limiting noise source References & Related Documents Diagram of reaction & main chain: LIGO-G1200077 Quadruple Suspension Design for Advanced LIGO Notes format good LIGO-G1501076-v1 LIGO Laboratory LIGO-G1501076-v1

Electrostatic Charging TITLE Talk Notes Electrostatic Charging Refer to LIGO-G1500264 Update on Test Mass Charging Rai’s slide 4: Best strategy (for the moment) is to eliminate charge MIT LASTI tests Showed charge on Test Mass was small & stable <10-10 C/cm2 or < ~10V of equivalent bias voltage Not expected to be a major noise issue Observations at LLO & LHO Charge much higher than expected Typical:100V bias equivalent, sometimes 200-300 V Surface densities: ~10-12 C/cm2 per TM Different story from each optic High enough to significantly affect the electrostatic actuation Why? Many potential sources… NOTES References: G1500722 LIGO-G1501076-v1 LIGO Laboratory LIGO-G1501076-v1 Notes; [ref]: G1500722 - Reitze’s NSF talk G1500264 – Rai’s March LVC talk alog 19547 - Graph from alog referenced in email (leo/kissel) #’s: Both polarities, ~10-9 C per TM Surface densities ~10-12 C/cm2 per TM

How Much Charge? Refer to Rai’s March 2015 LVC talk LIGO-G1500264 TITLE Talk Notes How Much Charge? Refer to Rai’s March 2015 LVC talk LIGO-G1500264 NEEDS MASSIVE WORK NEEDS MASSIVE WORK LIGO-G1501076-v1 LIGO Laboratory LIGO-G1501076-v1

What are we doing about it? TITLE Talk Notes LIGO-G1501076-v1 LIGO Laboratory LIGO-G1501076-v1

Mitigate Known Sources First contact photo Ion Pumps First Contact

Remove Existing Charge TITLE Talk Notes In vacuum In-air LIGO-G1501076-v1 LIGO-G1501076-v1

Mitigation Investigate Charging Due to First Contact TITLE Talk Notes Mitigation Investigate Charging Due to First Contact Charging experiments at LHO March 2015 Setup: NOTES Part of the charging experiments performed at LHO in March 2015 (by T. Sadecki, B. Weaver, C. Torrie, K. Gushwa). See references below. Experimental setup: ETM06 (pilot optic) on V-block inside a grounded metal box. ~2 year old First Contact sheet on the AR side. Electrometer 1” from the center of the HR side. All other items, including the table, are also grounded. Procedure: Measured charge just before, during, and after removing the old First Contact. Stuck the dry FC sheet back on the AR side, and repeated. Variables: Top Gun Test #1 – 1 test with and 1 test without Top Gun (per procedure) Test #3 – TG during peel, after peel, after peeling and pausing, etc. References: LIGO-T1500170 Charge Experiments at LHO – March 2015 (Day 3, First Contact Tests #1 & 3) LIGO-G1500539 “You can look but you can’t touch” LIGO-E1300017 First Contact Spray Application & Removal Procedure LIGO-G1501076-v1 LIGO Laboratory LIGO-G1501076-v1

Mitigation Investigate Charging Due to First Contact TITLE Talk Notes Mitigation Investigate Charging Due to First Contact Procedure: Measured charge just before, during, and after peeling First Contact Stuck sheet back on AR side & repeated Variable: Top Gun NOTES Part of the charging experiments performed at LHO in March 2015 (by T. Sadecki, B. Weaver, C. Torrie, K. Gushwa). See references below. Experimental setup: ETM06 (pilot optic) on V-block inside a grounded metal box. ~2 year old First Contact sheet on the AR side. Electrometer 1” from the center of the HR side. All other items, including the table, are also grounded. Procedure: Measured charge just before, during, and after removing the old First Contact. Stuck the dry FC sheet back on the AR side, and repeated. Variables: Top Gun Test #1 – 1 test with and 1 test without Top Gun (per procedure) Test #3 – TG during peel, after peel, after peeling and pausing, etc. References: LIGO-T1500170 Charge Experiments at LHO – March 2015 (Day 3, First Contact Tests #1 & 3) LIGO-G1500539 “You can look but you can’t touch” LIGO-E1300017 First Contact Spray Application & Removal Procedure LIGO-G1501076-v1 LIGO Laboratory LIGO-G1501076-v1

Residual charge is not always negative TITLE Talk Notes Top Gun start Top Gun stop Peel start First Contact removed NOTES Residual charge is not always negative LIGO-G1501076-v1 LIGO Laboratory LIGO-G1501076-v1

Not as effective if not used per procedure LIGO-G1501076-v1 LIGO Laboratory

Mitigation Ion pumps First Contact Ion pumps TITLE Talk Notes Mitigation Ion pumps First Contact Investigated charging during removal procedure Residual charge is not always negative Removal procedure is effective when followed Performed other experiments associated with static residue First Contact is not the devil Many potential sources of charge The Top Gun is our friend Significantly improved FC removal procedure Charge levels of several volts or less achieved at chamber closing Low charge levels under vacuum subsequently verified Ion pumps Being moved 250 m down beam tube Investigating better UV baffling Adding non-evaporable getter (NEG) to chambers NOTES Reference: G1500722 Charging, Paramet instabilities, and Squeeze film damping (2015 NSF review) E1300017-v5 First Contact Spray Application & Removal Procedure LIGO-G1501076-v1 LIGO Laboratory LIGO-G1501076-v1

Removing Charge: In-Vacuum Test Mass Discharge System (TMDS) Ions injected at low pressure without opening the chamber MIT LASTI tests Can neutralize surface charge densities as large as 10-10 C/cm2 on mirrors in BSC chambers [ref] Status update from March LVC Meeting (LIGO-G1500264) Tested with fair success in-situ on L1 & H1 LHO: NEEDS MASSIVE WORK LIGO-G1501076-v1 LIGO Laboratory

TMDS TITLE Caveat: not able to neutralize charge in gap To do/future: Talk Notes TMDS Caveat: not able to neutralize charge in gap All performed on far side of chamber pointing centrally To do/future: Use TMDS via an injection point closer to the QUAD (and pointed at gap) via custom flange NOTES Drawings from T1500056 V3 = far side chamber port V5 = proposed chamber port LIGO-G1501076-v1 LIGO Laboratory LIGO-G1501076-v1

TMDS TITLE Caveat: not able to neutralize charge in gap To do/future: Talk Notes TMDS Caveat: not able to neutralize charge in gap All performed on far side of chamber pointing centrally To do/future: Use TMDS via an injection point closer to the QUAD (and pointed at gap) via custom flange NOTES Drawings from T1500056 V3 = far side chamber port V5 = proposed chamber port LIGO-G1501076-v1 LIGO Laboratory LIGO-G1501076-v1

TITLE Talk Notes LIGO-G1501076-v1 LIGO Laboratory LIGO-G1501076-v1

TITLE Talk Notes LIGO-G1501076-v1 LIGO Laboratory LIGO-G1501076-v1

TITLE Talk Notes LIGO-G1501076-v1 LIGO Laboratory LIGO-G1501076-v1

TITLE Talk Notes LIGO-G1501076-v1 LIGO Laboratory LIGO-G1501076-v1