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UW LISA Torsion Balance Experiment Scott E Pollack with Stephan Schlamminger, Charlie Hagedorn, & Jens Gundlach Center for Experimental Nuclear Physics.

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Presentation on theme: "UW LISA Torsion Balance Experiment Scott E Pollack with Stephan Schlamminger, Charlie Hagedorn, & Jens Gundlach Center for Experimental Nuclear Physics."— Presentation transcript:

1 UW LISA Torsion Balance Experiment Scott E Pollack with Stephan Schlamminger, Charlie Hagedorn, & Jens Gundlach Center for Experimental Nuclear Physics and Astrophysics University of Washington Workshop on Charging Issues in Experimental Gravity July 27, 2007 LIGO #G070478-00-R

2 July 27, 2007 Pollack 2 UW Apparatus  0.5m 13  m W fiber  Au-coated Si-pendulum – 0.6 mm thick – Low mass  Split Au-coated Cu-plate – Split-plate allows investigation of potential differences laterally across pendulum – Heater elements (light bulbs) imbedded in plates allow thermal control – Movable up to 10 mm from pendulum  Control Electrodes – Used to feedback pendulum to fixed position, i.e., cold damping – Residual pendulum motion at level of ~ 2 nrad/√Hz ≈ 1.5 aNm/√Hz ≈ 0.02 fm/s 2 /√Hz Electrode Tungsten fiber Split Copper Plate Gravitational Compensator  PID V 50.8mm 63.5mm Silicon Pendulum (now quartz fiber)

3 July 27, 2007 Pollack 3 Top down view with pendulum removed Control Electrodes New Tiny Electrodes have 1/10 th N / V 2 response

4 July 27, 2007 Pollack 4 Photo courtesy Mary Levin

5 July 27, 2007 Pollack 5 Torque Noise Performance Calibration Tones

6 July 27, 2007 Pollack 6 Surface Potential Measurements  Electrostatic surface potential defined by potential energy of plate-pendulum capacitor:  Determine SP of each half of split Cu-plate by measuring torque vs. applied voltage V left V left (V) Electrode Voltage 2 ≡ Torque

7 July 27, 2007 Pollack 7 Surface Potential Noise Impacts (V bias ~100mV) Noise level increase due to SP variations Plate-Pendulum Separation = 0.5 mm

8 July 27, 2007 Pollack 8 Surface Potential Noise Impacts

9 July 27, 2007 Pollack 9 Measurement Technique  Switch between two voltages with relatively equal torques on pendulum (minimize transients)  Monitor difference in torque as function of time, convert this into a surface potential V left (V) Electrode Voltage 2 ≡ Torque Torque difference change implies surface potential drift Overall change in torque due to fiber relaxation

10 July 27, 2007 Pollack 10 Initial Drift after Pumping Down Drift after 30 days ~ 0.30 mV/day Drift after 50 days ~ 0.15 mV/day Exponential Fit: τ ~ 2.5 days

11 July 27, 2007 Pollack 11 Surface Potential Spectrum Plate Voltage Surface Potential Level ≈ 30 μV/√Hz 1/ f  Improved by 1. Better plate voltage reference 2. Smaller area electrodes 3. Better contamination prevention  SP level determined by 1. Voltage noise on plate 2. Voltage noise on electrode 3. Surface potential fluctuation

12 July 27, 2007 Pollack 12 Surface Potential Spectrum Thermal Torque Noise Contribution  Improved by 1. Better plate voltage reference 2. Smaller area electrodes 3. Better contamination prevention  SP level determined by 1. Voltage noise on plate 2. Voltage noise on electrode 3. Surface potential fluctuation ≈ 6 μV/√Hz

13 July 27, 2007 Pollack 13  Improved by – Better plate voltage reference – Smaller area electrodes – Better contamination prevention  SP level determined by 1. Voltage noise on plate 2. Voltage noise on electrode 3. Surface potential fluctuation Surface Potential Spectrum Surface Potential Level ≈ 30 μV/√Hz Expected drop of factor 3

14 July 27, 2007 Pollack 14 Top down view with pendulum removed Control Electrodes UV LED placed under can, shinning through window

15 July 27, 2007 Pollack 15 UV has little effect on torque noise

16 July 27, 2007 Pollack 16 SP fluctuations of floating pendulum

17 July 27, 2007 Pollack 17 UV Charging of Floating Pendulum  Charge rate ~ 2—3 mV/s, running LED at ~ 20mA  Couldn’t get electrons onto pendulum for discharge – Discharging through o-ring of support shaft for fiber. – Time constant ~ 230s  1 TΩ from pendulum to ground

18 July 27, 2007 Pollack 18 UV in Duty Feedback at 0.1 Hz Reduction of noise at low frequencies Feedback oscillation peak…

19 July 27, 2007 Pollack 19 UV in Duty Feedback at 0.1 Hz Surface Potential Noise level ~ 10 mV/√Hz

20 July 27, 2007 Pollack 20 UV LED in vacuum (with quartz fiber) Approximate location of Si pendulum Pictures taken July 13 Pumping began the following day

21 July 27, 2007 Pollack 21 Quartz Fiber Surface Potential Noise Surface Potential Noise level ~ 10 mV/√Hz ≡ ~ 2 x 10 6 photoelectrons/√Hz Ambient discharging If discharging through fiber  R ~ 340 TΩ

22 July 27, 2007 Pollack 22 UV Output in Feedback (Going +)  Initial charge rate ~ 1 mV/s – running LED at 0.1mA 5Hz (initially 50%) – Charging rate scales linearly with current and duty  No tuning of PI loop taken place at this point – i.e., could get a much tighter response Target set to 0.5 V Target set to 0 V Feedback V ~ +7V V = 0 V Toggle V = 0 V ~ +3V

23 July 27, 2007 Pollack 23 Issues Charging Negatively…  Sometimes I “find” the pendulum at further negative values, but I have a hard time getting it there myself  Issues like one illustrated probably account for that – Still investigating (this data was taken this past Monday) Feedback V ~ -7V V = 0 V Toggle V = -10V V ~ -5V

24 July 27, 2007 Pollack 24 Summary of Charge work at UW  Surface Potential Measurements with Grounded Pendulum – Both large and small electrodes show level ~30 μV/√Hz @ 1mHz – Reference voltage is at ~10 μV/√Hz – It’s possible that contamination is to blame – i.e., large drifts after pumping system  UV LED used for charge measurements outside vacuum can – No appreciable change in torque noise level with UV light on ~20mA – Spectral amplitude in feedback: ~2x10 6 electrons/Hz 1/2 @ 1mHz – Charge pendulum positively, but not negatively…  In situ UV LED – With close proximity, run LED at low power ~ 1 mA – Can charge negatively now as well. – Will be getting feedback noise level soon!  Quartz Fiber “removes” discharge through o-ring (R>300 TΩ) – No change from tungsten in spectral amplitude: ~10 mV/√Hz @ 1mHz


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