Transcript Document

S. V. DHURANDHAR
IUCAA
PUNE
30th January 2009
25th IAGRG meeting Kolkata
General Relativity and other disciplines
• GR finds its home in astronomy & astrophysics
- The binary blackhole problem
- No exact two body solution: PN + Numerical Relativity
- Cosmology: observational data, COBE, WMAP, PLANCK
• Mathematics: Commutative algebra, differential
geometry in statistics
• Statistics: Hypothesis testing, statistical tests, maximum
likelihood, etc. - Signal processing
• Gravitation has gone experimental: Gravitational waves
30th January 2009
25th IAGRG meeting Kolkata
Effect on a ring of test particles
Metric:
 2 1  
   2 2  hik  0
c t 

General Wave: hik
30th January 2009
 h (t  z c ) eik  h (t  z c ) eik
25th IAGRG meeting Kolkata
But h is awfully small !
Quadrupole formula :
ns
4G K .E.
h ~ 4
c
R
1
 E


R
 21



~ 
10
2 

0
.
1
M
c
100
Mpc



kin ns
Change in arm-length:
dL ~ h L
30th January 2009
25th IAGRG meeting Kolkata
LIGO Louisiana 4 km armlength (US)
30th January 2009
25th IAGRG meeting Kolkata
We did it !
*http://www.ligocaltech.edu/~lazz/distribution/LSC_Data
30th January 2009
25th IAGRG meeting Kolkata
LISA: Space based detector for detecting low
frequency GW
30th January 2009
25th IAGRG meeting Kolkata
Laser frequency noise
30th January 2009
25th IAGRG meeting Kolkata
30th January 2009
25th IAGRG meeting Kolkata
30th January 2009
25th IAGRG meeting Kolkata
Tinto, Eastabrook, Armstrong; SVD, Nayak, Vinet, Pai
30th January 2009
25th IAGRG meeting Kolkata
30th January 2009
25th IAGRG meeting Kolkata
30th January 2009
25th IAGRG meeting Kolkata
30th January 2009
25th IAGRG meeting Kolkata
30th January 2009
25th IAGRG meeting Kolkata
Open Problems
30th January 2009
25th IAGRG meeting Kolkata
Inspiraling compact binaries
GW
• Broadband source best for interferometric detectors
• Waveform is well modeled by PN approximations –
waveform obtained to 3.5 PN
• Numerical Relativity: great advances – merger
• Signal is way below the noise – data analysis: filtering
30th January 2009
25th IAGRG meeting Kolkata
Breakthrough in Numerical Relativity
Numerical Relativity
solves
• merger waveform
• 3.5% of total
restmass energy as
compared to 1.5 % in
inspiral waveform!
Work in progress on stitching together waveforms
India has the right talent/aptitude for NR
30th January 2009
25th IAGRG meeting Kolkata
Example of a filter
A sinusoidal signal is embedded in noise
Data:
x(t )  s(t )  n(t )
Signal:
s(t )  A0 cos 2  f 0 t
f0  256 Hz
30th January 2009
25th IAGRG meeting Kolkata
Filtering the data
Best filter is the Fourier Transform:

x( f ) 

x(t ) e 2 ift dt

Statistic:
C ( f )  | x( f )|
Provides parameters of
the signal: eg. frequency
Generalisation: Matched Filter
30th January 2009
25th IAGRG meeting Kolkata
Matched filtering the inspiraling binary signal
c( )   x (t ) q (t   ) dt
~
~
q( f ) 
30th January 2009
h (f)
Sh ( f )
25th IAGRG meeting Kolkata
Statistics and geometry
• Statistic: c()
• Where does one set the threshold? – False alarm
probability – choose threshold such that this is small
• Detection probability: choose this high
• Signal depends on many parameters: masses,
kinematical parameters: initial phase, time of arrival …
• Parameter space
• Parameter space can be viewed as a manifold with the
parameters as coordinates
• Metric: mismatch between signal and template
30th January 2009
25th IAGRG meeting Kolkata
Parameter space metric
Coordinates: li
gik Dli Dlk  e
Choose coordinates so that metric is simplest: Cartesian coordinates
For inspiral choose chirp times instead of masses: 0 , 3
Metric const: Uniform placement of templates
Number of templates = volume of parameter space / template size
30th January 2009
25th IAGRG meeting Kolkata
International Network of GW Interferometers
1. Detection confidence 2. Source direction 3. Polarisation info
GEO: 0.6km
LIGO-LHO: 2km, 4km
VIRGO: 3km
TAMA: 0.3km
LIGO-LLO: 4km
AIGO: (?)km
30th January 2009
25th IAGRG meeting Kolkata
Need for a (or two) detector(s) in Asia/Australia
• AIGO: Australian project
• INDIGO: Indian detector?
• Advantages: sky coverage, resolution of sources
30th January 2009
25th IAGRG meeting Kolkata
Optimum location of a detector
Courtesy A. Sengupta & S. Mitra
30th January 2009
25th IAGRG meeting Kolkata
Optimum location
30th January 2009
25th IAGRG meeting Kolkata
Network Sensitivity
AIGO/INDIGO network doubles sensitivity
30th January 2009
25th IAGRG meeting Kolkata
Angular Resolution
An order of magnitude improvement
30th January 2009
25th IAGRG meeting Kolkata
Summary
 Connection of GR to several fields:
Astrophysics, Mathematics, Statistics, Engineering …
Numerical Relativity
Gravitation going experimental
30th January 2009
25th IAGRG meeting Kolkata