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Shot noise in GW detectors G González

Shot noise in GW detectors G González. x Power (ASDC) bright dark /2 The dark fringe L+ L L- L i L P=P 0 sin 2 ( t+k l) = (P 0 /2) (1+sin

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Page 1: Shot noise in GW detectors G González. x Power (ASDC) bright dark /2 The dark fringe L+  L L-  L i  L  P=P 0 sin 2 (  t+k  l) = (P 0 /2) (1+sin

Shot noise in GW detectors

G González

Page 2: Shot noise in GW detectors G González. x Power (ASDC) bright dark /2 The dark fringe L+  L L-  L i  L  P=P 0 sin 2 (  t+k  l) = (P 0 /2) (1+sin

x

Power(ASDC)

bright

dark

/2The dark fringe

L+L

L-L

i L

P=P0 sin2 (t+kl) = (P0/2) (1+sin (2t+2kl)): insensitive to l

If we phase-modulate the light:

• If the Michelson arms are equal length in average, power is same (dark) for carrier and sidebands: no signal yet. • If arms are not equal (Schnupp asymmetry), carrier is dark, but sidebands are not. • The “beat” of carrier and sidebands has then a signal (photocurrent):P=|E0+E++E-|2DC+ J0J1sin(kL)sin(kmDL)sin(wmt) + …(2wm t)

•Then, “demodulate” : multiply by sin(wmt) or cos(wmt) to produce I and Q phases

For m=25 MHz (m=12 m), sidebands have wwm=w0(1 1.4 10 -8).

Page 3: Shot noise in GW detectors G González. x Power (ASDC) bright dark /2 The dark fringe L+  L L-  L i  L  P=P 0 sin 2 (  t+k  l) = (P 0 /2) (1+sin

Michelson interferometerShot noise at output : white noise with psd:

φ2 ( f ) = 2hν

ηP

Output signal:

x

Power(ASDC)

bright

dark

/2

Page 4: Shot noise in GW detectors G González. x Power (ASDC) bright dark /2 The dark fringe L+  L L-  L i  L  P=P 0 sin 2 (  t+k  l) = (P 0 /2) (1+sin

Power-recycled Michelson:PNI experiment 1995-1999

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are needed to see this picture.

Page 5: Shot noise in GW detectors G González. x Power (ASDC) bright dark /2 The dark fringe L+  L L-  L i  L  P=P 0 sin 2 (  t+k  l) = (P 0 /2) (1+sin

(green) PNI experiment

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are needed to see this picture.

φ2 ( f ) = 2hν

ηP

φ2 ( f ) = Fns 2hν

ηP= 3

ηP

QuickTime™ and aTIFF (LZW) decompressor

are needed to see this picture.

Lossless, mid fringe:

Lossless, demodulated at dark fringe:

Lossy, demodulated at dark fringe:

PRL, 80, p8131, 1998

Page 6: Shot noise in GW detectors G González. x Power (ASDC) bright dark /2 The dark fringe L+  L L-  L i  L  P=P 0 sin 2 (  t+k  l) = (P 0 /2) (1+sin

Power-recycled Fabry Perot Michelson interferometer

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Page 7: Shot noise in GW detectors G González. x Power (ASDC) bright dark /2 The dark fringe L+  L L-  L i  L  P=P 0 sin 2 (  t+k  l) = (P 0 /2) (1+sin

Fabry Perot cavity

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Page 8: Shot noise in GW detectors G González. x Power (ASDC) bright dark /2 The dark fringe L+  L L-  L i  L  P=P 0 sin 2 (  t+k  l) = (P 0 /2) (1+sin

LIGO cavity parameters

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Page 9: Shot noise in GW detectors G González. x Power (ASDC) bright dark /2 The dark fringe L+  L L-  L i  L  P=P 0 sin 2 (  t+k  l) = (P 0 /2) (1+sin

L1 “noise budget”

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~4x/ ~1e-12 rad/rtHz

Page 10: Shot noise in GW detectors G González. x Power (ASDC) bright dark /2 The dark fringe L+  L L-  L i  L  P=P 0 sin 2 (  t+k  l) = (P 0 /2) (1+sin

Shot noise and radiation pressure

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are needed to see this picture. SSQL () =4h

m 2

Standard quantum limit:

Page 11: Shot noise in GW detectors G González. x Power (ASDC) bright dark /2 The dark fringe L+  L L-  L i  L  P=P 0 sin 2 (  t+k  l) = (P 0 /2) (1+sin

Advanced LIGO: signal recycling

Advance

d LIGO

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Page 12: Shot noise in GW detectors G González. x Power (ASDC) bright dark /2 The dark fringe L+  L L-  L i  L  P=P 0 sin 2 (  t+k  l) = (P 0 /2) (1+sin

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Beyond SQL

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ALESSANDRA BUONANNO AND YANBEI CHEN

PHYSICAL REVIEW D 64 042006

Page 14: Shot noise in GW detectors G González. x Power (ASDC) bright dark /2 The dark fringe L+  L L-  L i  L  P=P 0 sin 2 (  t+k  l) = (P 0 /2) (1+sin

QuickTime™ and aTIFF (LZW) decompressor

are needed to see this picture.

Page 15: Shot noise in GW detectors G González. x Power (ASDC) bright dark /2 The dark fringe L+  L L-  L i  L  P=P 0 sin 2 (  t+k  l) = (P 0 /2) (1+sin

The references I used, in chronological order, were:

VOLUME 80, NUMBER 15 P H Y S I C A L R E V I E W L E T T E R S 13 APRIL 1998 High Power Interferometric Phase Measurement Limited by Quantum Noise and Application to Detection of Gravitational Waves P. Fritschel, G. González,* B. Lantz, P. Saha,† and M. Zucker

Shot noise in gravitational-wave detectors with Fabry–Perot arms Torrey T. Lyons, Martin W. Regehr, and Frederick J. Raab 20 December 2000 Vol. 39, No. 36 APPLIED OPTICS

Quantum noise in second generation, signal-recycled laser interferometric gravitational-wave detectors Alessandra Buonanno and Yanbei Chen PHYSICAL REVIEW D, VOLUME 64, 042006

Second generation instruments for the Laser Interferometer Gravitational Wave Observatory (LIGO) Peter Fritschel SPIE ProceedingsLIGO document P020016-00.pdfhttp://www.ligo.caltech.edu/docs/P/P020016-00.pdf