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LIGO-G030395-00-E LIGO Laboratory1 Simulating the LIGO Laser Phase Change Resulting from Gravitational Waves Simulate GW generation and detection Make.

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Presentation on theme: "LIGO-G030395-00-E LIGO Laboratory1 Simulating the LIGO Laser Phase Change Resulting from Gravitational Waves Simulate GW generation and detection Make."— Presentation transcript:

1 LIGO-G030395-00-E LIGO Laboratory1 Simulating the LIGO Laser Phase Change Resulting from Gravitational Waves Simulate GW generation and detection Make use of real physics Implement in e2e Jeff Jauregui SURF Student – Caltech Mentor: Dr. Hiro Yamamoto

2 LIGO-G030395-00-E LIGO Laboratory2 Physics Background Essential physics: how GW’s affect optical path length of FP cavity Extract GW polarization components parallel to arms Convert strain into laser phase shift

3 LIGO-G030395-00-E LIGO Laboratory3 e2e Background e2e: time-domain simulation designed for LIGO A modeled system is described in terms of interacting modules Design new modules: GW sources and detector Example: F-P cavity

4 LIGO-G030395-00-E LIGO Laboratory4 Let’s Approach the Problem What factors must we consider? »GW properties, source location »LIGO location and orientation How do we take them into account? »Transform GW to LIGO coordinate system »Numerically compute phase shift of laser at each time step How can we integrate the results with other modules? »Dynamically pass laser phase information to EM-field propagators

5 LIGO-G030395-00-E LIGO Laboratory5 Outline of Solution Express GW and LIGO in Earth coordinate system »Rotate GW (from TT) to achieve z-incidence Translate strain into laser phase shift »Analytic formula for sinusoidal GW’s (P-980007-00, D. Sigg) »Approximation for general GW’s Write a program to handle computation

6 LIGO-G030395-00-E LIGO Laboratory6 Is the Solution Valid? Accuracy of laser phase shift approximation

7 LIGO-G030395-00-E LIGO Laboratory7 Implement in e2e New modules h+h+ hxhx time r m1m1 m2m2 R ψ h+h+ hxhx t_f m1m1 m2m2 R ψ h+h+ hxhx  x  y      GW signal generationDetection Binary, circular orbitInspiralling binaryInterferometer

8 LIGO-G030395-00-E LIGO Laboratory8 Some Results Binary system »Two 1.5M sun stars »1000 km apart »10 Mpc from Earth »0 o, 0 o incidence Detector »LHO

9 LIGO-G030395-00-E LIGO Laboratory9 More Results Inspiral system »10M sun each »10Mpc from Earth http://www.phys.latech.edu/official/research/ligo.htm

10 LIGO-G030395-00-E LIGO Laboratory10 Future Improvements More signal types: »Supernova »Black hole formation Signal delay between two detectors http://www.mpa-garching.mpg.de/Hydro/RGRAV/ LIGO-G020007

11 LIGO-G030395-00-E LIGO Laboratory11 Applications Study properties of LIGO with incident GW’s »Learn how imperfections distort signal »What types of noise are most detrimental? Data analysis »View photodetector output for signal, embedded in realistic noise »Test existing data analysis techniques

12 LIGO-G030395-00-E LIGO Laboratory12 Conclusion Now e2e has GW detection functionality Can generate variety of signals and study LIGO’s response Will be able to compare responses of multiple LIGO sites

13 LIGO-G030395-00-E LIGO Laboratory13 Acknowledgements Dr. Hiro Yamamoto SURF Program LIGO Project Thanks to:


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