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Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005 Seismic Noise Coherence Measurements in Deep Salt Mines F. Acernese a , F. Barone b , R. Burns c , G. Cella d , R. De Rosa a , F. De Salvo e , R. De Salvo f , S. Menegon f , L. Milano a , G. Pellerito f , J. Strands c a Università di Napoli “Federico II” b Università di Salerno c California State University- Pomona d INFN – Sezione di Pisa e Realmonte Italkali f LIGO – Caltech LIGO-G050053-00-Z

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Page 1: Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005 Seismic Noise Coherence Measurements in Deep Salt Mines F. Acernese a,

Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005

Seismic Noise Coherence Measurements in Deep Salt Mines

F. Acernesea, F. Baroneb, R. Burnsc, G. Cellad, R. De Rosaa, F. De Salvoe, R. De Salvof, S. Menegonf, L. Milanoa, G. Pelleritof, J.

Strandsc

aUniversità di Napoli “Federico II”bUniversità di Salerno

cCalifornia State University- PomonadINFN – Sezione di Pisa

eRealmonte ItalkalifLIGO – Caltech

LIGO-G050053-00-Z

Page 2: Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005 Seismic Noise Coherence Measurements in Deep Salt Mines F. Acernese a,

Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005

OverviewOverview

• Introduction

• Realmonte salt mine

• Measurement Set Up

• Results

• Next Step

• Conclusions

Page 3: Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005 Seismic Noise Coherence Measurements in Deep Salt Mines F. Acernese a,

Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005

IntroductionIntroduction

One of the main problems involved in developing high sensitivity terrestrial interferometer for gravitational waves is the contribution of the newtonian noise in the low frequency region.

A partial solution to this problem can be obtained by building new detector underground in order to reduce the effect due to the surface waves.

In addition it is possible to arrange a set of seismic sensors in order to monitor and subtract the contribution of the newtonian noise from the interferometer output.

Page 4: Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005 Seismic Noise Coherence Measurements in Deep Salt Mines F. Acernese a,

Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005

IntroductionIntroduction

To verify these hypothesis we perform a seismic noise data acquisition in a deep salt mine

The preliminary results of this survey are reported and the future foreseen steps.

Page 5: Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005 Seismic Noise Coherence Measurements in Deep Salt Mines F. Acernese a,

Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005

Realmonte Salt MineRealmonte Salt MineThe Realmonte salt deposit is located on the Southern coast of Sicily, about 4 km from

Agrigento and 1 km from Porto Empedocle.

Page 6: Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005 Seismic Noise Coherence Measurements in Deep Salt Mines F. Acernese a,

Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005

Realmonte Salt MineRealmonte Salt Mine

The layers of rock salt and kainite run underground in a line dropping from mountain to sea, with the rock salt layer acting as a roof to the kainite to a depth of 40 meters and a presence of NaCl of 97-98% pure.

Page 7: Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005 Seismic Noise Coherence Measurements in Deep Salt Mines F. Acernese a,

Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005

Measurement Set UpMeasurement Set Up

The measurement of the seismic noise inside the mine was performed using triaxial accelerometers model FBA ES-T (Episensors) from Kinemetrics:

Sensitivity: 40V/g

Bandwidth: 0.1 – 200 Hz

10-1

100

101

102

-20

-10

0

10

Frequency (Hz)

Ma

gn

itud

e (

dB

)

10-1

100

101

102

-200

-100

0

100

200

Frequency (Hz)

Ph

ase

(d

eg

ree

s) Frequency (Hz)

Am

plit

ude

(dB

)

Page 8: Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005 Seismic Noise Coherence Measurements in Deep Salt Mines F. Acernese a,

Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005

Measurement Set UpMeasurement Set Up

The data coming from the episensor were acquired by using a VME based digital acquisition system composed by:

- 1 CPU board running LynxOs;

- 1 ADC board with 8 input channels and 16 bit resolution;

- 2 SCSI Disks, 9 Gb size, for storing data.

In order to match the episensor output and the ADC input dynamic ranges, and to avoid aliasing problems, a conditioning electronics with an amplifying (G=100) element and a filtering element (8th order Chebyshev filter with cut off at 200 Hz).

Page 9: Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005 Seismic Noise Coherence Measurements in Deep Salt Mines F. Acernese a,

Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005

Measurement Set UpMeasurement Set Up

Each acquisition system was used to manage two episensors.

10-1

100

101

102

103

-100

-50

0

Frequency (Hz)

Ma

gn

itud

e (

dB

)

10-1

100

101

102

103

-200

-100

0

100

200

Frequency (Hz)

Ph

ase

(d

eg

ree

s)

ADC Board

CPU Board

Conditioning

Electronic

Epi 1

Epi 2

Oscillator F=800Hz

Storage Disk

VME bus

A local oscillator was used to provide the trigger for data acquisition. (No external synchronization)

SCSI bus

Page 10: Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005 Seismic Noise Coherence Measurements in Deep Salt Mines F. Acernese a,

Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005

Measurement Set UpMeasurement Set Up

The measure was carried out by placing two acquisition systems in two caves at different depth in the mine.

Level 1: -141 m

Sensors: 1A, 1B

Level 2: -128 m

Sensors: 2A, 2B

Acquisition systemsSensors

26 m

50 m

Top view

13 m

1A

2A 2B

2A

Page 11: Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005 Seismic Noise Coherence Measurements in Deep Salt Mines F. Acernese a,

Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005

Measurement Set UpMeasurement Set Up

A single oscillator was used to trigger both the acquisition systems, in order to synchronize at least the data with themselves.

The acquisition was carried out starting from July 7 to August 1, 2004 (26 days), with a sampling frequency of 800 Hz.

A total of 12 seismic channels plus 2 monitor channels were acquired during this period.

Page 12: Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005 Seismic Noise Coherence Measurements in Deep Salt Mines F. Acernese a,

Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005

ResultsResults

Power spectral density of acceleration inside the mine (NS)

10-1

100

101

102

10-8

10-7

10-6

10-5

10-4

10-3

NS Direction

Frequency (Hz)

Acc

elle

ratio

n (m

/s2 /H

z-1/2

* )

Frequency (Hz)

Acc

eler

atio

n P

SD

(m

/s^2

/sqa

rt(H

x)

Page 13: Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005 Seismic Noise Coherence Measurements in Deep Salt Mines F. Acernese a,

Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005

ResultsResults

Power spectral density of acceleration inside the mine EW

10-1

100

101

102

10-8

10-7

10-6

10-5

10-4

10-3

WE Direction

Frequency (Hz)

Acc

elle

ratio

n (m

/s2 /H

z-1/2

* )A

ccel

erat

ion

PS

D (

m/s

^2/s

qart

(Hx)

Frequency (Hz)

Page 14: Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005 Seismic Noise Coherence Measurements in Deep Salt Mines F. Acernese a,

Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005

ResultsResults

Power spectral density of acceleration inside the mine (z)

10-1

100

101

102

10-8

10-7

10-6

10-5

10-4

10-3

Vertical Direction

Frequency (Hz)

Acc

eler

atio

n (m

/s2 /H

z-1/2

)A

ccel

erat

ion

PS

D (

m/s

^2/s

qart

(Hx)

Frequency (Hz)

Page 15: Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005 Seismic Noise Coherence Measurements in Deep Salt Mines F. Acernese a,

Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005

ResultsResults

Searching for seismic noise sources… (PCA)

Page 16: Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005 Seismic Noise Coherence Measurements in Deep Salt Mines F. Acernese a,

Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005

ResultsResults

Test of noise subtraction (multicoherence method)

Page 17: Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005 Seismic Noise Coherence Measurements in Deep Salt Mines F. Acernese a,

Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005

Next StepNext Step

Arrangement of another acquisition system in a (possibly) spherical cave to optimize the noise subtraction procedure and to enhance the reduction of newtonian noise.

Sensors

Page 18: Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005 Seismic Noise Coherence Measurements in Deep Salt Mines F. Acernese a,

Gravitational Wave Advanced Detector Workshop – Aspen (CO) - Jan. 16 - 22, 2005

ConclusionsConclusions

Building new interferometers underground can effectively enhance their sensitivity in the low frequency region.

The newtonian noise subtraction procedure can even increase this enhancement (if performed correctly).

Preliminary results on both this effects, base on experimental data, give us encouraging results.