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Modeling of Optical Scattering in Advanced
LIGO
Hunter Rew
Mentors: Joseph Betzwieser, Adam Mullavey
LIGO-G1400923
What is Optical Scattering and Why Do We Care?
Equation 1: The Bidirectional Reflection Distribution Function
Figure 1: http://en.wikipedia.org/wiki/Bidirectional_scattering_distribution_function#mediaviewer/File:BSDF05_800.png
Equation 2: The solid angle
LIGO-G1400923
How Do We Measure It?
Images with a known power incident on the camera
Photodiodes
LIGO-G1400923
Project Motivation
Large particle seen on ETMY
CCD calibration factor needed
Baffle PDs provide scatter information just asking to be modeled
LIGO-G1400923
CCD Calibrations
We need a method for calculating the power seen by a camera from its image
Measurements only existed for long exposures (low power)
Equation 3: The CCD calibration factor
LIGO-G1400923
Experimental Setup
Figure 2: Experimental setup for measuring power incident on a camera
Figure 3: Back view of Figure 2
LIGO-G1400923
Results
8 bit Data:
mean: 1e-9 ± 2e-8 (W)(us)/count
std: 4.7e-11
12 bit data:
mean: 6e-11 ± 1e-11 (W)(us)/count
std: 3.1e-12
Figures 4a (top) and 4b(bottom)
LIGO-G1400923
Analysis of Large Angle ETMY Scatter
The particle shown in the
zoom accounts for over 50%
of the scatter.
Loss from spot: 18 ± 4 ppm
Total loss: 36 ± 7 ppm
Figure 4: Raw tiff of ETMY Figure 5: Zoom in of particle
on ETMY with noise
subtracted
LIGO-G1400923
Baffle PD Data Acquisition
Gather the data from EPICS channels
L1:LSC-POP_A_LF_NORM_MON
Normalized power pick off before the beamsplitter
L1:LSC-POP_A_LF_OUTPUT
Power pick off in Watts
L1:AOS-*TM*_BAFFLEPD_*_VOLTS
PD voltage
L1:AOS-*TM*_BAFFLEPD_*_GAIN
Dimensionless PD gain
Subsequently crash the NDS server (repeatedly)
LIGO-G1400923
Calculations
Equation 4: Power scattered
Equation 5: Uncertainty in power scattered
Equation 7: Uncertainty in the BRDF
Equation 6: Power incident on the test masses
LIGO-G1400923
Figure 6: Scatter from ETMX
LIGO-G1400923
Figure 7: Scatter from ITMX
LIGO-G1400923
Figure 8: Scatter from ETMY
LIGO-G1400923
Figure 9: Scatter from ITMY
LIGO-G1400923
Figure 10: Cavity power for each full lock
LIGO-G1400923
Results
LIGO-G1400923
A Hiro to Save Us
Static Interferometer Simulation (SIS) is the best thing since sliced bread
Models optical scatter in the arm cavities
Figure 11: Top view of modeled
power on ITMY
Figure 12: 3D view of the log10 of the
modeled power on ITMY
LIGO-G1400923
Ongoing Work
3 bumps placed on the phase map
Bump size
waist: 1e-3 m
height: 1e-6 m
Figure 13: Top view of power
distribution with bumps placed on
ETMY phase map in approximate
positions seen on ETMY image.
Figure 14: Comparison of
measured power and modeled
power
LIGO-G1400923
Future Work
Modeling scatter as it is today
Accounting for alignment changes
Calculating power losses
LIGO-G1400923
Acknowledgements
Joseph Betzwieser
David Feldbaum
Hiro Yamamoto
Eugeniy Mikhailov
CalTech
NSF
LIGO-G1400923

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Modeling of Optical Scattering in Advanced LIGO

  • 1. Modeling of Optical Scattering in Advanced LIGO Hunter Rew Mentors: Joseph Betzwieser, Adam Mullavey LIGO-G1400923
  • 2. What is Optical Scattering and Why Do We Care? Equation 1: The Bidirectional Reflection Distribution Function Figure 1: http://en.wikipedia.org/wiki/Bidirectional_scattering_distribution_function#mediaviewer/File:BSDF05_800.png Equation 2: The solid angle LIGO-G1400923
  • 3. How Do We Measure It? Images with a known power incident on the camera Photodiodes LIGO-G1400923
  • 4. Project Motivation Large particle seen on ETMY CCD calibration factor needed Baffle PDs provide scatter information just asking to be modeled LIGO-G1400923
  • 5. CCD Calibrations We need a method for calculating the power seen by a camera from its image Measurements only existed for long exposures (low power) Equation 3: The CCD calibration factor LIGO-G1400923
  • 6. Experimental Setup Figure 2: Experimental setup for measuring power incident on a camera Figure 3: Back view of Figure 2 LIGO-G1400923
  • 7. Results 8 bit Data: mean: 1e-9 ± 2e-8 (W)(us)/count std: 4.7e-11 12 bit data: mean: 6e-11 ± 1e-11 (W)(us)/count std: 3.1e-12 Figures 4a (top) and 4b(bottom) LIGO-G1400923
  • 8. Analysis of Large Angle ETMY Scatter The particle shown in the zoom accounts for over 50% of the scatter. Loss from spot: 18 ± 4 ppm Total loss: 36 ± 7 ppm Figure 4: Raw tiff of ETMY Figure 5: Zoom in of particle on ETMY with noise subtracted LIGO-G1400923
  • 9. Baffle PD Data Acquisition Gather the data from EPICS channels L1:LSC-POP_A_LF_NORM_MON Normalized power pick off before the beamsplitter L1:LSC-POP_A_LF_OUTPUT Power pick off in Watts L1:AOS-*TM*_BAFFLEPD_*_VOLTS PD voltage L1:AOS-*TM*_BAFFLEPD_*_GAIN Dimensionless PD gain Subsequently crash the NDS server (repeatedly) LIGO-G1400923
  • 10. Calculations Equation 4: Power scattered Equation 5: Uncertainty in power scattered Equation 7: Uncertainty in the BRDF Equation 6: Power incident on the test masses LIGO-G1400923
  • 11. Figure 6: Scatter from ETMX LIGO-G1400923
  • 12. Figure 7: Scatter from ITMX LIGO-G1400923
  • 13. Figure 8: Scatter from ETMY LIGO-G1400923
  • 14. Figure 9: Scatter from ITMY LIGO-G1400923
  • 15. Figure 10: Cavity power for each full lock LIGO-G1400923
  • 17. A Hiro to Save Us Static Interferometer Simulation (SIS) is the best thing since sliced bread Models optical scatter in the arm cavities Figure 11: Top view of modeled power on ITMY Figure 12: 3D view of the log10 of the modeled power on ITMY LIGO-G1400923
  • 18. Ongoing Work 3 bumps placed on the phase map Bump size waist: 1e-3 m height: 1e-6 m Figure 13: Top view of power distribution with bumps placed on ETMY phase map in approximate positions seen on ETMY image. Figure 14: Comparison of measured power and modeled power LIGO-G1400923
  • 19. Future Work Modeling scatter as it is today Accounting for alignment changes Calculating power losses LIGO-G1400923
  • 20. Acknowledgements Joseph Betzwieser David Feldbaum Hiro Yamamoto Eugeniy Mikhailov CalTech NSF LIGO-G1400923