stefan hild for the geo600 team 14th ilias wg1 meeting, october 2007, hannover mystery noise in...

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Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

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Page 1: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild for the GEO600 team

14th ILIAS WG1 meeting, October 2007, Hannover

Mystery noise in GEO600

Page 2: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 2

Intro: What is „mystery noise“?

There is a big gap between the uncorrelated sum (pink) of all known noise contributions and the actually measured sensitivity (red).

Page 3: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 3

Intro: What is „mystery noise“? (2)

Also the fundamental noise contributions, especially thermal noises are far below the current sensitivity.

Page 4: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 4

Mystery noise => High Priority

Limits the GEO sensitivity bet- ween 100 and 800 Hz.Around 200 Hz without mystery noise the sensitivity would be 3 times better. The peak sensitivity (550 Hz) could be improved by about a factor sqrt(2).As long as mystery noise is present, i.e. GEO is not shot noise limited over the major part of the detection band, improvements like increased laser power, DC-readout, squeezing are partly worthless.

We need to find the mystery noise! (There is NO other option)

Page 5: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 5

How to tackle the mystery noise ?

Mystery noise

Page 6: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 6

How to tackle the mystery noise ?

Mystery noise

Characteristics ofthe mystery noise

Displacement noiseYes / No ?

Any clues from the observation? Displacement-like or not? Stationary? Related to glitches? ....

Page 7: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 7

How to tackle the mystery noise ?

Mystery noise

Fundamentalnoises

Projectednoises

Characteristics ofthe mystery noise

Displacement noiseYes / No ?

Is the gap real? All projections correct? Are all noises projected? Calculations of fundamental noises correct?

Page 8: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 8

How to tackle the mystery noise ?

Mystery noise

Fundamentalnoises

Projectednoises

UpconversionScattered light

Characteristics ofthe mystery noise

Exotic noises

Displacement noiseYes / No ?

Can we rule out the usual candidates: non-linearly coupling noises? How about exotic noises ? ....

Page 9: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 9

Page 10: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 10

History of the mystery noise

Broadband noise (without significant structure /features)

Mystery noise is found to be fairly stable over 15 months (within about 25%).

Seems to be independent from environmental conditions.

Spectrum (roughly): 1/f^2 below 200 Hz, 1/f above 200 Hz

Characteristics ofthe mystery noise

Page 11: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 11

Mystery noise is independent of the glirchrate

Characteristics ofthe mystery noise

Eventhough we observe strong fluctuations in the glitchrate, the mystery noise stays always constant.

Page 12: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 12

Page 13: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 13

Does the mystery noise behave like displacement noise ??

If we could find out life would be much easier...

If the mystery noise doesn‘t look like displacement noise:

Can rule out all thermal noises

Can rule out any noise of the test masses

....

If the mystery noise looks like displacement noise:

We can rule out many technical noises like oscillator phase noise, oscillator amplitude noise, frequency noise

.....

Displacement noiseYes / No ?

Page 14: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 14

Checking the mystery noise for different Signal Recycling tunings (1)

Mystery noise has different shape and level in 1kHz and 550Hz tuning.

=> Indication: does not look like displacement noise

Displacement noiseYes / No ?

Page 15: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 15

103

10-22

10-21

10-20

Str

ain

[1

/sq

rt(H

z)]

Frequency [Hz]

myst_350 Hz, August 2007

myst-2006-05-06, 550 Hz

myst-2007-06-13, 550 Hz

myst-2007-03-12, 550 Hz

Checking the mystery noise for different Signal Recycling tunings (2)

Mystery noise has same shape and level in 350Hz and 550Hz tuning.

=> Indication: does look like displacement noise

Displacement noiseYes / No ?

Page 16: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 16

Displacement noise like: YES / NO ?

Mystery noise has same shape and level in 350Hz and 550Hz tuning.

=> Indication: does look like displacement noise.

Mystery noise has different shape and level in 1kHz and 550Hz tuning.

=> Indication: does not look like displacement noise.

Observation 1:

Observation 2:

Summary:

We cannot decide whether the mystery noise is displacment noise or not. (Perhaps it consists of two different components.)

=> We have to investigate both: displacement AND non-displacement noises.

Displacement noiseYes / No ?

Page 17: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 17

Page 18: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 18

What do we have to check in terms of noise projections?

Are the noise projections we do correct?

Did we miss to project any relevant noise source?

Are the transferfunctions used for the projections correct?

Projectednoises

Page 19: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 19

Which noise projections are relevant for the mystery noise frequency range ?

Oscillator phase noiseOscillator amp noiseLaser power noiseFrequency noiseDetection dark noise

Two main suspects: OPN: shape would fit

and is not too far from limiting.

PR-noise: Was never really understood (In-loop, high gain)

Projectednoises

Page 20: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 20

OPN investigations 1: 2f local oscillator

103.06

103.08

103.1

103.12

103.14

103.16

10-4

X: 1185Y: 0.0005243

Spectrum plot using Hanning window

Frequency [Hz]

Am

plit

ude [

V/ H

z]

X: 1185Y: 4.322e-005

03: G1:LSC_MID_EP-P_HP

04: G1:LSC_MID_EP-Q_HPP quadrature using the 2 signal

Nominal setup: Signal passes optical system, while LO is electrically.Using 2f signal from darkport (devided by 2) as LO => Signal and LO travel the same path.

Suppression of OPN

101

102

103

10-5

10-4

10-3

10-2

10-1

Spectrum plot using Hanning window

Frequency [Hz]

Am

plit

ude [

V/ H

z]

01: G1:LSC_MID_EP-P_HP

02: G1:LSC_MID_EP-Q_HPP quadrature using 2f signal

Using 2f LO givessame sensitivity

Indication: mystery noise is not related to OPN

Projectednoises

Page 21: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 21

OPN investigations 2: wire instead of MI

Idea: Replacing the IFO by a wire should give lower limit of OPN.

Replacing:• EOM, • IFO and • photodiode by a ‘good‘ wire

Projectednoises

Page 22: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 22

OPN investigations 2: wire instead of MI

‚Wire projection‘ gives a noise (yellow trace) close to shot noise.=> Mystery noise gap gets smaller.

Projectednoises

Page 23: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 23

Frequency noise projection: A smoking gun ?

The change of the mystery noise from 550Hz to 1kHz tuning looks suspiciously similar to the change of the frequency noise transfer function.

Projectednoises

Page 24: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 24

Frequency noise projection (2)Main problem of this loop: In-loop measurement with high gain.

One important experiment is to set up an out-of-loop photodiode.

Projectednoises

Can rule out any sensing noise of the PR-loop. Left over: Any frequency noise on the light (4 above detection noise) could be the mystery noise.

Page 25: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 25

Noise projections summary

improved existing projections added a few missing projections checked for any non-linearities in the transferfunctions (compared swept sine and random noise measurements) the gap got smaller, but is still there....

We believe that OPN is not causing the mystery noise.

We believe that the mystery is not related to magnetic fields.

We believe that frequency noise is still a good candidate. Can rule out the electronics (?) Can rule out the detection Frequency noise on the light could explain the mystery

noise.

Projectednoises

Page 26: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 26

Page 27: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 27

Checking correctness of shot noise (1)

102

103

10-22

10-21

10-20

G1:DER_DATA_Hfs = 16384 : 240s, nfft=16384, nolap=0.50, enbw=1.5, navs=479

Frequency [Hz]

Am

pli

tud

e [V

/ Hz]

attenuated HPD path

reference day

reference night

Attenuation experiment:

Attenuated the detected light at main photodetector. The sensitivity measured matches the shot noise calculations.

Nominal light power

Expected sensitivity decrease found (all

frequencies)

Fundamentalnoises

Page 28: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 28

Checking correctness of shot noise (2)

Shot noise simulations using FINESSE:

Fundamentalnoises

Page 29: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 29

Revisiting the thermal noise calculations

The Glasgow group (Reid, Rowan, Hough) revisited all thermal noise calculations:

Draft version of a nice and detailed document is available now (includes all equations, references and used parameters).

Fundamentalnoises

Page 30: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 30

Revisiting the thermal noise calculations

The Glasgow group (Reid, Rowan, Hough) revisited all thermal noise calculations:

Draft version of a nice and detailed document is available now (includes all equations, references and used parameters).

Coating TN now distingished in thermorefractive, thermoelastic and brownian. Brownian is the dominant contribution. Didn‘t change.

Substrate Brownian noise. Changed slope and level. Now lower, but less steep.

BS thermorefractive noise. Now 3.5 times higher. => Dominating TN for frequencies up to 1.5kHz.

Fundamentalnoises

Page 31: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 31

New thermal noise calculations

Revisited thermal noises cannot explain the mystery noise.

Fundamentalnoises

Page 32: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 32

Increased thermal noise due to excess damping ?

IDEA: Testmass is close to touching its catcher There might be conditions where additional damping is

caused Could such damping reduce the Q of the modes and

therfore increase the thermal noise ???

(Famous Livingston Earthquake stops???)

We tried to take photographs of the testmasses. Due to the restricted view angles for 4 of the 5 main optics we cannot say how far they are from their catchers.

Fundamentalnoises

Page 33: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 33

Page 34: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 34

Is there any indication for upconversion?

Scatter plots:

low freq signal vs sensitivity

Used low-freq channels: Seismic, MI differential lenght, MI differential auto-alignment

Usually no indication of significant upconversion

So far only a single data set showed indication for upconversion (0.1 –0.3 Hz) from MID long and MID AA.

Upconversion

Page 35: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 35

Page 36: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 36

Scattering Overview

External Scattering (outside the vacuum)

All interferometer ports

Detection bench

In-vacuum-Scattering

Scattered light from catchers

Scattering inside the central cluster

Small angle scattering in the folded arms

‚Grating‘-scattering from coating defects

Scattered light

Page 37: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 37

External ScatteringAll interferometer ports

We did 2 complete rounds of filter / blocking experiments for all ports outside the vacuum. => No limiting scattering observed

Detection bench

Ruled out scattering from HPD-path and quadrant path by using an opto-mechanical phase shifter.

102

103

10-21

10-20

10-19

Spectrum plot using Hanning window

Frequency [Hz]

Am

pli

tud

e [V

/ Hz]

2007-06-29 12:34:10 - scrambler off

2007-06-29 12:37:00 - scrambler off

2007-06-29 12:38:15 - scrambler active

2007-06-29 12:35:50 - scrambler active

2007-06-29 03:27:00 - night ref, no scattering

Scattered light reduction

of the o.m. phase shifter

Scattered light

Page 38: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 38

Scattered light from the catchers (1)

Scattered light

Light on the catchers from small angle scattering.

Catchers are not seismically isolated

Light scattered back into IFO mode can harm sensitivity

Page 39: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 39

Scattered light from the catchers (2)

Scattered light

Displacement noise from scattering

Displacement of catcher

Preliminary.Uncertanties=

f_cat and X_cat

Page 40: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 40

Scattered light from the catchers (3)

Seismic excitation of catchers => no change in h(t) => ruled out scattering from catchers

However, probably not far from limiting => preparing baffles

102

103

10-21

10-20

10-19

10-18

10-17

03: G1:DER_DATA_H fs = 16384 : 60s nfft=81920, nolap=2.50, enbw=0.3, navs=23

Frequency [Hz]

Ampl

itude

[V/

Hz]

new viewport, with flowbox from 2007-06-14 14:18:00 -

new viewport, without flowbox from 2007-06-14 14:20:00 -

Seismic excitation

No seismic excitation

Scattered light

Page 41: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 41

Scattering inside the central cluster(involving tank walls)

Idea: We observe a lot of scattered light inside the central cluster.Some of the stray light from the tank wall might mind find the way to the detection portRuled out by external shaking of the tank walls:

102

103

10-5

10-4

10-3

10-2

Frequency [Hz]

Am

plit

ud

e [V

/H

z]

102

103

10-22

10-21

10-20

Frequency [Hz]

Am

plit

ud

e [V

/H

z]

shaking the tank walls no influence to mystery noise

Scattered light

Page 42: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 42

Small angle scattering in the folded arms

Scattered light

IDEA:

Some light hitting the far mirrors is directly scattered back.

Can be ruled out as mystery noise:

Far mirrors only move a few microns (rms)

Mirrors are isolated by triple pendulum

Page 43: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 43

‚Grating‘-scattering from coating defects

IDEA:Coating defects can be described as grating. Scattering path: Coating defect => tank wall => Coating defectBeam jitter would cause phase noise analogous to a grating.

Inverted photographs of a far mirror (IFO is flashing)

Not completely understood so far. However, could be ruled out by shaking experiments.

Scattered light

Page 44: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 44

Scattering Overview

External Scattering (outside the vacuum)

All interferometer ports

Detection bench

In-vacuum-Scattering

Scattered light from catchers

Scattering inside the central cluster

Small angle scattering in the folded arms

‚Grating‘-scattering from coating defects

Scattered light

We think we ru

led out NEARLY ALL scatte

red processes we can think of.

Page 45: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 45

Page 46: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 46

Controlled increase of pressure inside the vacuum system (1)

Is the mystery noise caused by residual gas pressure?

Experiment:Closed all valves to turbo pumps.

Pressure at all sensors increa-sed by about a factor 30.

Exotic noises

Page 47: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 47

Controlled increase of pressure inside the vacuum system (2)

102

103

10-21

10-20

10-19

Spectrum plot using Hanning window

Frequency [Hz]

Am

plitu

de [

V/

Hz]

2007-07-31 13:30:00 - 2007-07-31 12:30:00

2007-07-31 11:30:00

2007-07-31 10:30:00

2007-07-31 14:30:00 2007-07-31 15:30:00

No effect seen in sensitivity.

Can ruled out residual pressure as cause of the mystery noise.

Exotic noises

Page 48: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 48

Effects from test mass charging?

Exotic noises

Charges on test masses

• Measured posi-tive charging of testmasses

• Discharged by using a UV-lamp (electrons are freed from

ESD electrodes)

BEFORE AFTER

100V 15V

Problem: charges on test masses effect out calibration.However, we believe the charges did not harm the sensitivity.

Page 49: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 49

What else is left over ??

Barkhausen noiseUnlikely: Only MSR and MPR have magnets directly at the mirror

Maybe the mystery noise is a new type of noise (GEO specific):

ESDs ? Signal-Recycling ? Monolithic suspensions ? Folded arms ? High power in BS substrate ? High PR gain ?

Exotic noises

Page 50: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 50

102

103

10-22

10-21

10-20

Frequency (Hz)

AS

D [

h/s

qrt

(Hz)]

Noise projection to h 2007-10-15 02:10:00

MID AA FB Rot

MID AA FB Tilt

SR longitudinal noiseOscillator phase noise

Oscillator amplitude noise

Laser amplitude noise

PR errorMagnetic field

RF noise

Dark noiseModel Shot 550Hz

Sum of the noise

H- deg 70 (good time)

Does the mystery noise depend on the optical power ??

Using only 66% of nominal optical power reduces the ‚gap‘. Above 300 Hz the mystery noise is smaller with low power, while below 300 Hz it stays constant. Another indication that we are looking for more than one mystery noises.

Exotic noises

Page 51: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 51

Additional Slides

Page 52: Stefan Hild for the GEO600 team 14th ILIAS WG1 meeting, October 2007, Hannover Mystery noise in GEO600

Stefan Hild ILIAS WG1 10/2007 Slide 52

The Vacuum system of GEO600