Localization capabilities of ground based interferometers Lee - - PowerPoint PPT Presentation
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
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
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)
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
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
Results: GEO, LCGT, LIGO, Virgo
- Maximum error
significantly reduced
– Minimum error slightly improved
- Mean error on sky
significantly reduced
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
With, without Australian Detector
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