Localization capabilities of ground based interferometers Lee - - PowerPoint PPT Presentation

localization capabilities of ground based interferometers
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Localization capabilities of ground based interferometers Lee - - PowerPoint PPT Presentation

Localization capabilities of ground based interferometers Lee Samuel Finn Penn State University Goal, assumptions, outline Goal: How well can ground-based detectors localize gravitational wave sources. Assumptions Simultaneous


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SLIDE 1

Localization capabilities of ground based interferometers

Lee Samuel Finn Penn State University

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SLIDE 2

Goal, assumptions, outline

  • Goal: How well can ground-based detectors localize

gravitational wave sources.

  • Assumptions

– Simultaneous observation by at least four geographically distinct interferometric detectors

  • Next 5y: LIGO (2) plus at least three of GEO, TAMA, Virgo
  • > 5 yr horizon: LIGO (2) plus at least three of ACIGA, GEO,

LCGT, Virgo/Ego

  • Outline

– Basic concepts – Methodology – Results

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Basic concepts

  • A single ground-based

interferometer has no directional sensitivity to inspiraling binaries

– NS/NS signal passes through band in ~ 20s

  • Directional information

determined by time-of- arrival information at different detectors

– Two detectors: a circle in sky normal to axis between detectors

– Three detectors: intersection of two circles – Four (or more) detectors: a single point (patch)

  • Arrival time?

– Define in terms of canonical feature of signal: e.g., when is instantaneous frequency 100Hz.

  • Arrival time accuracy?

– No better than 0.1ms (8/SNR)

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SLIDE 4

Methodology

  • Wave incident direction n yields (relative) arrival

times T.

– T = A n

  • N detectors? A is Nx3 matrix whose rows are detector location

vectors

  • Pick point in sky & determine exact arrival times T
  • Introduce timing errors dT

– Assume normally distributed, zero mean, σ ~ 1 ms

  • Invert, in least squares sense, (T+dT) = A n’ to find

best-fit angle of incidence

  • Find angle between n’, n
  • Repeat to determine error distribution
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SLIDE 5

Results

  • GEO, LIGO, Virgo
  • Median localization

error

– I.e., half time error is greater, half time less

  • Error ranges by factor 2

– Maximum error when source direction normal to axis between detectors

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SLIDE 6

Results: GEO, LCGT, LIGO, Virgo

  • Maximum error

significantly reduced

– Minimum error slightly improved

  • Mean error on sky

significantly reduced

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SLIDE 7

Results: Add an Australian Detector

  • ACIGA, GEO, LCGT,

LIGO, Virgo

  • Maximum error

reduced again

  • Mean sky error reduced

further

  • Minimum error never

gets better than ~2 degrees

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SLIDE 8

With, without Australian Detector

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SLIDE 9

Caveats and Conclusions

  • Assumption that all errors are the same

– GEO much less sensitive than LIGO, Virgo to binary inspiral and will have greater timing errors.

  • Gravitational wave astronomy needs at least

four, large, well separated detectors

– Southern Hemisphere detector would be especially helpful