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Search for gravitational waves

Jo van den Brand

(2)

Introduction

Einstein gravity :

Gravity as a geometry

Space and time are physical objects

8

G    T 

Gravitational waves

• Dynamical part of gravitation, all space is filled

• Very large energy, almost no interaction

• Ideal information carrier, almost no scattering or attenuation

• The entire universe has been transparent for GWs, all

the way back to the Big Bang

(3)

Gravitational waves `squeeze’ space: small effects

Proper distance between x

and x

+dx

Plane GW propagating in z-direction Define

Wave equation

(4)

Gravitational waves

L

hL

 2

GW

time L- L L+ L

 Predicted by general relativity

 GW = space-time metric wave

Distance variation

Strain amplitude h:

 GW produced by mass acceleration

d = source distance

Q = quadrupole moment dt d

Q d c

h 2 G 1

2 2

 4

 Small coupling factor → astrophysical sources

1 1 2

10

44

s kg

m

s J L

G

 10

16

/

L=20 m, d = 2 m, 27 rad/s

J E

Hz

m

2 absorbed 54

25

10

10

 

Earth-sun: 313 W

(5)

Evidence for gravitational waves

 PSR 1913+16

R. Hulse, J. Taylor (1974)

Binary pulsar (T = 7.75 hr)

1 pulsar (17 rev/s) → get the orbital parameters

Orbital period decreases

– Energy loss due to GW emission (~3 x 10

24

W) – Good agreement with GR

– Inspiral lifetime about 300 Myears (3.5 m/yr)

– Expected strain, h~10

-26

m

(6)

GW source: coalescing binary

 End of the life of compact binary systems

Neutron stars, systems have been observed

 Rare events

~ 0.1 event/year (@20Mpc) ±1 order of magnitude

 Typical amplitude (NS-NS): h ~ 10

-22

@ 20 Mpc

 “Known” waveform

Search with matched filtering

General relativity tests

Standard candles: get the distance from the waveform

– Coincidence with short gamma ray burst?

(7)

Two body problem in general relativity

 Collision of two black holes

 Numerical solution of Einstein equations required

 Problem solution started 40 years ago (1963 Hahn &

Lindquist, IBM 7090)

 Wave forms critical for

gravitational wave detectors

 A PetaFLOPS-class grand

challenge

(8)

Numerical relativity

First merger of three black holes simulated on a supercomputer ScienceDaily (Apr. 12, 2008)

Manuela Campanelli, Carlos Lousto and Yosef Zlochower—Rochester Institute of Technology Center for Computational Relativity and Gravitation

Triple quasar (10.8 Gly) S. G. Djorgovski et al., Caltech, EPFL (Jan. 2007)

ly m

m m

L m

L  1   ( 10

6

) /( 10

22

)  10

16

 1

 

km m

m m

L m

L  10

18

  ( 10

18

) /( 10

22

)  10

4

 10

(9)

Interferometric detectors: an international dream

GEO600 (British-German) Hanover, Germany

LIGO (USA)

Hanford, WA and Livingston, LA

TAMA300 (Japan) Mitaka

VIRGO (French-Italian) Cascina, Italy

AIGO (Australia),

Wallingup Plain, 85km north of Perth

(10)

Virgo: science case

First (?) direct observation of gravity waves

Better understanding of gravity

GW produced in high density area

Strong field

Tests GR

Open a new window on the universe

GW very weakly absorbed

Standard candle: Hubble constant

GW + Gamma Ray Bursts?

Supernova understanding?

Neutron stars/black hole physics?

Early universe picture??

Pushing interferometer techniques to their limits

(11)

Interferometer as GW detector

 Principle: Measure distances between free test masses

Michelson interferometer

Test masses = Interferometer mirrors

Sensitivity: h = L/L

– We need large interferometer – For Virgo L = 3 km

2 L hL 2

LhL

Suspended

mirror Suspended

mirror

Beam splitter LASER

Light Detection

Virgo: CNRS+INFN

(

ESPCI-Paris, INFN-Firenze/Urbino, INFN-Napoli, INFN-Perugia, INFN-Pisa, INFN-Roma,LAL-Orsay,

LAPP-Annecy, LMA-Lyon, OCA-Nice)

+ NIKHEF joined 2007

First science run: May – September 2007

(12)

Interferometer Concept

As a wave passes, the arm lengths

change in different

ways….

…causing the interference pattern

to change at the

photodiode Suspended

Masses

(13)

Laser 20 W

Input Mode Cleaner (144 m)

Power Recycling

3 km long Fabry-Perot Cavities

Output Mode Cleaner (4 cm)

Input mode cleaner

 Mode cleaner cavity: filters

laser noise, select TEM00

mode

(14)

Installation in IMC end tower

Each switch has been tested in open and closed position.

The mirror and RM are moved 55 mm for- and backwards.

(15)

Eric Hennes

Nikhef: redesign and replace dihedron

Optronica Marinebedrijf Den Helder

Zorg dat je erbij komt…

(16)

Nikhef: Linear alignment of VIRGO

N W

EOM

 Phase modulation of input beam

 Demodulation of photodiode signals at different output beams

=> longitudinal error signals

 Quadrant diodes in output beams

=> Alignment information

(differential wavefront sensing)

 Anderson-Giordano technique

2 quadrant diodes after arm cavities

+ Han Voet

(17)

Linear alignment setup

(18)

 Rotating asymmetric neutron star

 GW Amplitude function of the unknown asymmetry

ε = star asymmetry = ??

Upper limit set by the pulsar spin down

 A few pulsars around a few 100 Hz

Only 800 pulsars plotted out of 10

9

in the galaxy

 Weak signal but could be integrated for months

But a complex problem due to the Doppler effect

CPU issues

GW source: pulsars

 

 

 

 

 

 

 

 

 

6

2

2 45

27

10 200

10 10 10

3 

Hz f cm

g I r

h kpc

zz

f (Hz) N

LIGO: <10% of energy in GW

Crab pulsar

(19)

Periodic Sources – all sky search – Roma / NIKHEF

• Doppler shifts

• Frequency modulation: due to Earth’s motion

• Amplitude modulation: due to the detector’s antenna pattern.

• Assume original frequency is 100 Hz and the maximum variation fraction is of the order of 0.0001

• Note the daily variations

• After FFT: energy not in a single bin, so the SNR is highly reduced

• Bin in galactic coordinates

• Re-sampling

• Short FFTs

• Hough maps

ALL SKY SEARCH

enormous computing challenge

(Sipho van der Putten, Henk Jan Bulten, Sander Klous)

(20)

GWs from binaries

 Frequency changes a lot due to Doppler: df/f~10

-3

Hulse-Taylor:

_

Towards Detector

V

Grid-based analysis

Extension of LIGO – Virgo CW analysis

Calibration systems for LISA

(21)

Virgo sensitivity compared to LIGO and GEO600

May 2

Inspiral range 6.5 Mpc

The horizon (best orientation) for a binary system

of two 10 solar mass black holes is 63 Mpc

(22)

Discovery potential first event

 Hypothesis:

Finesse = 150 (now : 50)

Same losses & power recycling as today

 Horizon (Virgo+)

BNS: 150 Mpc (optimal orientation)

BBH: 750 Mpc (optimal orientation)

 BNS Rates: (most likely and 95% interval)

Initial Virgo (30Mpc) 1/100yr (1/500 -1/25 yr)

Enhanced LIGO (60Mpc) 1/10yr (1/50- 1/2.5yr)

Virgo+ limit (150Mpc) 1.2/yr (1/4yr-5/yr)

Advanced detectors (350Mpc) 40/yr (8-160/yr)

Kalogera et al; astro-ph/0312101; Model 6

 BBH and other sources rates are more difficult to predict

(23)

LIGO and VIRGO: scientific evolution

 At present hundreds of galaxies in range for 1.4 M

o

NS-NS binaries

 Enhanced program

In 2009 about 10 times more galaxies in range

 Advanced detectors

About 1000 times more galaxies in range

In 2014 expect 1 signal per day or week

Start of gravitational astrophysics

Numerical relativity will

provide templates for

interpreting signals

(24)

Advanced Virgo: vacuum – cryo links

6885 985

Gas load from mirror 10-4 mbar l/s

mbar

Element number Start pressure

Intermediate Final pressure Pressure

(25)

LN2 GN2

Beam vacuum Isolation vacuum

LN2 Fixed 300 K

3.2 mm/m

3.2 mm/m

Reinforce rib

Forces

Vacuum + super isolation Tie rod

Advanced Virgo: vacuum – cryo links

(26)

Advanced Virgo: superattenuator

FEA:

Frans Mul

Corijn

(27)

Other activities in GW program

 Einstein Telescope – conceptual design study

Approved in May 2008

Funded for 3 years

Nikhef responsible for Working Group 1 on site selection

Design Study Proposal approved by EU within FP7

Large part of the European GW community involved EGO, INFN, MPI, CNRS, NIKHEF, Univ. Birmingham, Cardiff, Glasgow

(28)

28

GRB050509B

3RD GENERATION INTERFEROMETER

2ND

GENERATION 1ST GENERATION

Credit G.Cagnoli

NS - NS INSPIRAL RANGE

(29)

Virgo

LOI to ESA – LISA analysis Nikhef, VU, RUN and SRON

Netherlands: Bulten/Nelemans

(30)

Beyond Einstein is the umbrella program for a series of

NASA/ESA missions linked by powerful new technologies and common science goals to answer the questions:

Gravitational Waves Can Escape from Earliest Moments of the Big

Bang

Inflation

(Big Bang plus 10-34 Seconds)

Big Bang plus 300,000 Years

gravitational waves

Big Bang plus 14 Billion Years

light

Now

What powered the Big Bang?

Is Einstein’s theory still right in these conditions of

extreme gravity? Or is new physics awaiting us?

Chandra - Each point of x-ray light is a Black Hole!

What happens at the edge of a Black Hole?

Dark energy and matter interact through gravity

We do not know what 95%

of the universe is made of!

What is the mysterious Dark Energy pulling the Universe apart?

September 6, 2007: Committee on NASA's Einstein Program: An Architecture for Implementation, National Research Council

Finding 4. LISA is an extraordinarily original and technically bold mission concept. LISA will open up an entirely new way of observing the universe, with immense potential to enlarge our understanding of physics and astronomy in unforeseen ways.

LISA, in the committee’s view, should be the flagship mission of a long-term program addressing Beyond Einstein goals.

Finding 8. The present NASA Beyond Einstein funding wedge alone is inadequate to develop any candidate Beyond Einstein mission on its nominal schedule. However, both JDEM and LISA could be carried out with the currently forecasted NASA

contribution if DOE's contribution that benefits JDEM is taken into account and if LISA's development schedule is extended and funding from ESA is assumed.

(31)

Summary

 Gravitational wave physics

Component of our Astroparticle Physics initiative

Exciting new physics program

– Important questions are addressed

– Program with a long-term scientific perspective

 VIRGO

Sensitivity is improving fast

First science run underway

Data sharing and analysis between LIGO and Virgo

 NIKHEF commitment

Modest at this moment

Expand to FOM research program in 2009 / 2010

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