30
30 th January 2009 25 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

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Page 1: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30th January 2009 25th IAGRG meeting Kolkata

S. V. DHURANDHAR

IUCAA

PUNE

Page 2: 30 th January 200925 th IAGRG meeting Kolkata 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

Page 3: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30th January 2009 25th IAGRG meeting Kolkata

Effect on a ring of test particles

01

222

ikhtc

Metric:

ikikik ecztheczthh )()(General Wave:

Page 4: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30th January 2009 25th IAGRG meeting Kolkata

But h is awfully small !

L ~ h L

Quadrupole formula :

21

1

2410

1001.0~

..4~

Mpc

R

cM

E

R

EK

c

Gh

nskinns

Change in arm-length:

Page 5: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30th January 2009 25th IAGRG meeting Kolkata

LIGO Louisiana 4 km armlength (US)

Page 6: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30th January 2009 25th IAGRG meeting Kolkata

We did it !

*http://www.ligocaltech.edu/~lazz/distribution/LSC_Data

Page 7: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30th January 2009 25th IAGRG meeting Kolkata

LISA: Space based detector for detecting low frequency GW

Page 8: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30th January 2009 25th IAGRG meeting Kolkata

Laser frequency noise

Page 9: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30th January 2009 25th IAGRG meeting Kolkata

Page 10: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30th January 2009 25th IAGRG meeting Kolkata

Page 11: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30th January 2009 25th IAGRG meeting Kolkata

into, Eastabrook, Armstrong; SVD, Nayak, Vinet, Pai

Page 12: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30th January 2009 25th IAGRG meeting Kolkata

Page 13: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30th January 2009 25th IAGRG meeting Kolkata

Page 14: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30th January 2009 25th IAGRG meeting Kolkata

Page 15: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30th January 2009 25th IAGRG meeting Kolkata

Page 16: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30th January 2009 25th IAGRG meeting Kolkata

Open Problems

Page 17: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

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

Page 18: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

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 waveformsIndia has the right talent/aptitude for NR

Page 19: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30th January 2009 25th IAGRG meeting Kolkata

Example of a filter

A sinusoidal signal is embedded in noise

0 0

( ) ( ) ( )

( ) cos 2

x t s t n t

s t A f t

Data:

Signal:

0 256f Hz

Page 20: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30th January 2009 25th IAGRG meeting Kolkata

Filtering the data

2( ) ( )

( ) | ( )|

iftx f x t e dt

C f x f

Best filter is the Fourier Transform:

Statistic:

Generalisation: Matched Filter

Provides parameters of the signal: eg. frequency

Page 21: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30th January 2009 25th IAGRG meeting Kolkata

Matched filtering the inspiraling binary signal

)(

)()(

)()()(

~~

fS

fhfq

dttqtxc

h

Page 22: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30th January 2009 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

Page 23: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30th January 2009 25th IAGRG meeting Kolkata

Parameter space metric

Coordinates: i

gik

ik

Choose coordinates so that metric is simplest: Cartesian coordinates

For inspiral choose chirp times instead of masses: 03

Metric const: Uniform placement of templates

Number of templates = volume of parameter space / template size

Page 24: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30th January 2009 25th IAGRG meeting Kolkata

International Network of GW InterferometersInternational Network of GW Interferometers

LIGO-LLO: 4km

LIGO-LHO: 2km, 4kmGEO: 0.6km VIRGO: 3km

TAMA: 0.3km

AIGO: (?)km

1. Detection confidence 2. Source direction 3. Polarisation info1. Detection confidence 2. Source direction 3. Polarisation info

Page 25: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30th January 2009 25th IAGRG meeting Kolkata

eed for a (or two) detector(s) in Asia/Australia

• AIGO: Australian project

• INDIGO: Indian detector?

• Advantages: sky coverage, resolution of sources

Page 26: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30th January 2009 25th IAGRG meeting Kolkata

Optimum location of a detector

Courtesy A. Sengupta & S. Mitra

Page 27: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30th January 2009 25th IAGRG meeting Kolkata

ptimum location

Page 28: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30th January 2009 25th IAGRG meeting Kolkata

Network Sensitivity

IGO/INDIGO network doubles sensitivity

Page 29: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30th January 2009 25th IAGRG meeting Kolkata

Angular Resolution

An order of magnitude improvement

Page 30: 30 th January 200925 th IAGRG meeting Kolkata S. V. DHURANDHAR IUCAA PUNE

30th January 2009 25th IAGRG meeting Kolkata

Summary

Connection of GR to several fields:

Astrophysics, Mathematics, Statistics, Engineering …

Numerical Relativity

Gravitation going experimental