e instein gravitational wave t elescope
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Topology Identification - Plans for WP3. E instein gravitational wave T elescope. Andreas Freise 09.10.2007 ILIAS-GW, Tübingen . What is the Detector Topology?. Geometry : Number of sites, detector orientation, overall size - PowerPoint PPT PresentationTRANSCRIPT
Andreas Freise 09.10.2007 ILIAS-GW, Tübingen
Einstein gravitational wave Telescope
Topology Identification - Plans for WP3Topology Identification - Plans for WP3
A. Freise ILIAS-GW 10/2007 Slide 2
What is the Detector Topology?
Geometry: Number of sites, detector orientation, overall size
Topology: type of each interferometer (Michelson, Sagnac, …), number and position of main interferometer optics
Configuration: interferometer operating point, mode of operation (detuned, narrow- band, …), sensing and control scheme
A. Freise ILIAS-GW 10/2007 Slide 3
NEW laser, suspensions, optical scheme, mirrors Same Infrastructure, Similar Topology
NEW laser, suspensions, optical scheme, mirrors,vibration isolators. Cryogenics. New Infrastructure, New Topology
1st generation
2nd generation
3rd generation New Topology = New Interferometry
A. Freise ILIAS-GW 10/2007 Slide 4
Topology Identification
Motivation: Why a new topology? Because we can! Third generation (3G) detectors will require a new infrastructure
The Michelson interferometer is the optimal topology for maximising the optical signal of a gravitational wave with ideal polarisation
It is, however, not necessarily the best choice for maximising the signal-to-noise ratio detecting both polarisations of a gravitational wave
A. Freise ILIAS-GW 10/2007 Slide 5
3 detectors in a triangle configuration
Early Ideas
Rüdiger, ‘85
Topology example
A. Freise ILIAS-GW 10/2007 Slide 6
A. Freise ILIAS-GW 10/2007 Slide 7
A. Freise ILIAS-GW 10/2007 Slide 8
Advanced Configurations
A. Freise ILIAS-GW 10/2007 Slide 9
Advanced Configurations
A. Freise ILIAS-GW 10/2007 Slide 10
WP 3 Tasks and Milestones1. Evaluation of available and developing technologies for the suppression of
quantum noise 2. Evaluation of technologies for suppressing thermal noise or generally
displacement noise3. Modelling of Interferometer Topologies. Parameterise the quantum noise
limited sensitivity of each technology 4. Modelling of Interferometer Geometries. Quantify the signal extraction and
possible noise reduction capabilities of multiple detectors in dependence of their relative geometry (co-located, co-linear, etc)
5. Study the effects of very high laser power and compute requirements with respect to circulating light power values
6. Analyse the cross-compatibilities of the technologies above 7. Trade-off analysis and system design8. Modelling of Interferometer Configuration
A. Freise ILIAS-GW 10/2007 Slide 11
WP 3 Tasks and Milestones
Evaluation of detector geometry
Evaluation of (quantum-) noise reduction schemes
Evaluation of high-power instabilities
Trade-off analysis and draft design
Final design and component specifications
A. Freise ILIAS-GW 10/2007 Slide 12
The E.T. Work Package 3Topology Identification
Commitment stated in the proposal: 149 person months
Equally large contributions from Birmingham, Glasgow, Max-Planck, CNRS
Smaller contributions from INFN, EGO This is a seed corn for a wider activity
Funding through the proposal: 3 Post-doctoral scientists for 2 years in Birmingham,
Hannover and Glasgow Coordination through Birmingham
A. Freise ILIAS-GW 10/2007 Slide 13
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A. Freise ILIAS-GW 10/2007 Slide 14
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h(f) [1/sqrt(Hz)]
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(a) 3rd Generation (b) LCGT (c) advanced LIGO (d) advanced Virgo (e) LIGO (f) Virgo (g) GEO600
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Credit: M. Punturo, G. Losurdo
A. Freise ILIAS-GW 10/2007 Slide 15
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(a) 3rd Generation (b) LCGT (c) advanced LIGO (d) advanced Virgo (e) LIGO (f) Virgo (g) GEO600
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A. Freise ILIAS-GW 10/2007 Slide 16
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