AIGO 2K Australia - Italy Workshop 2005 7 th October 2005 7 th October 2005 Pablo Barriga for AIGO group.

AIGO 2KAIGO 2K

Australia - Italy Australia - Italy Workshop 2005Workshop 2005

77thth October 2005 October 2005

Pablo Barrigafor AIGO group

ACIGA Mission High Optical Power Test Facility

Low noise 80m base line advanced interferometer

Advanced gravitational wave interferometer (AIGO)

Primary Institutions:University of Adelaide

Australian National University

University of Western Australia

Affiliate Institutions:Monash University

CSIRO-Optics

Development of high power optics in collaboration with LIGO

Demonstrate noise performance of high power interferometer

First in the SouthernHemisphere

Vacuum SystemSingle increment

3.5m high vacuum tanks

400mm diameter pipes? (R. De Salvo)

Input Laser Injection locked 10W Nd:YAG laser has been developed

by The University of Adelaide.

High power laser clean room near Class 100.

Future laser >100WTalk by Peter Veitch

10

-110

010

1-200

-150

-100

-50

0

50Horizontal Isolator Transfer Function

Frequency [Hz]

Mag

nitu

de [

dB]

Complete Isolator Transfer Function (Y-Axis)Complete Isolator Transfer Function (X-Axis)

High Optical Power Mode Cleaner Astigmatism and thermal lensing calculations.

Isolation system transfer function shows good performance.

Control system design and implementation underway.

X - Axis

Y - Axis

Test Masses

Fused Silica or Sapphire?

Start with small test masses ~10kg

Second stage 40kg (Advanced LIGO)

Sapphire Input Test Mass

Rayleigh Scattering MeasurementsTalk by Zewu Yan

1500.164E+07

.328E+07.492E+07

.656E+07.820E+07

.984E+07.115E+08

.131E+08.150E+08

NODAL SOLUTION

STEP=1SUB =1TIME=1SEQV (AVG)DMX =.752E-05SMN =1472SMX =.350E+08

Suspension SystemStage 1: Niobium Flexures Stage 2 : Fused Silica Flexures

Talk by Ben Lee

Isolation System

0.01 0.1 1 10Frequency Hz

400

300

200

100

0

Bd

Frequency Response

Talk by Jean Charles and Eu-Jeen

Robust isolation system

Built for heavy test masses

Digital Control

Digital Control already under development.

DSP based?

LIGO EPICS?

Is there a way of combining both?

AIGO Dual Recycling Interferometer

M1 M2

M3

To Detector Bench

South Fabry - Perot Cavity

East Fabry - Perot Cavity

Mode Cleaner

100W PSLNd:YAG laser = 1064nm

East - end Station

South - end Station

Main BuildingSignal Recycling Mirror

Beam Splitter

Power Recycling Cavity

N

Mode-Cleaner Geometry

M1 M2

M3

l1200mm

2wo

l 299

00m

m

Incident angle 44.712o

Incident angle 0.579o

Concave end mirror

Flat Mirrors used as input and output couplers

Coating and Substrate Absorptions

High reflectivity coating absorption produces astigmatic thermal lensing. The spot ellipticity produce different distribution between X and Y axis.

M2 used as output coupler the diagonally transmitted beam produces strong astigmatic thermal lensing.

0 20 40 60 80 100 120 140 160 180 200

0

0.02

0.04

0.06

Input Power [W]

Ecc

entr

icity

M3 SpotWaist Size

Input Power [W]

0 20 40 60 80 100 120 140 160 180 2000

0.02

0.04

0.06

Ecc

entr

icity

M3 SpotWaist Size

Eccentricity variation with Power

0 20 40 60 80 100 120 140 160 180 2000

0.02

0.04

0.06

Ecc

entr

icity

M3 SpotWaist Size

Eccentricity variation with Power

M1/M2 = FlatM3 = 22.5 m

M1/M2 = 1000 mM3 = 23.3 m

M1/M2 = 470 mM3 = 23.3 m

AIGO Future Interferometer

M1 M2

M3

To Detector Bench



Mode Cleaner


East - end Station

South - end Station


Beam Splitter


N


M1 M2

M3

To Detector Bench



Mode Cleaner


East - end Station

South - end Station


Beam Splitter


N


M1 M2

To Detector Bench



Mode Cleaner


East - end Station

South - end Station


Beam Splitter


N

M3

M1 M2

M3

To Detector Bench

South Fabry-Perot Cavity

East Fabry-Perot Cavity

Mode Cleaner


ETM

ETM

SRM

BSPRM ITM

ITM

L1

L2

l1

l2

lsr

lpr

LMC


To Detector Bench

South Fabry-Perot Cavity

East Fabry-Perot Cavity

ETM

ETM

SRM

BSPRM ITM

ITM

L1

L2

l1

l2

lsr

lpr


Carrier:Resonant in PRC and Arms

RF Sideband f1:Resonant in PRC

RF Sideband f2:Resonant in PRC and SRC

Actual Interferometer Configuration

Cavities Length

LMC = 10 m

LPRC = 12 m

LArms = 2000 m

LSRC = 12 m

South End Station

East End Station

AIGO Proposed Configuration

Cavities Length

LMC = 10 m

LPRC = 3.6 m

LArms = 2007 m

LSRC = 3.6 m

South End Station

East End Station

Rule of Thumb

• Carrier should be resonant in the arms and the PRC.

• Carrier resonant in the SRC for resonant sideband extraction (RSE), and anti-resonant for signal recycling.

• SB1 should be nearly anti-resonant in the arms, and resonant in the PRC.

• SB2 also nearly anti-resonant in the arms, and resonant in the PRC.

• One of the SB should be resonant in the SRC and the other nearly anti-resonant.

mmLMC 10000

SRCPRC LLmm ,3600

Limiting values for the cavities length are defined by the vacuum envelop:

Integer ratios between the cavities are not recommended, in order to avoid harmonics sidebands to resonate in the recycling cavity.

AIGO Constrains

Actual Configuration

• Length PRC = 11727 mm

Mode Cleaner shorter than Recycling Cavities?

• PRC Free Spectral Range: 12.782 MHz

• PRC as a coupled cavity half integer of PRC FSR

• “Longest” Mode Cleaner 7818 mm FSR = 19.173 MHz

2

21 lllL prPRC

MCm L

cnf

21

For transmission of modulation sidebands by the mode-cleaner, LMC and fm must satisfy:

For sideband coupling into the recycling cavity, LPRC and fm must satisfy:

PRCm L

cnf

22

12

AIGO Interferometer Sidebands

Sideband must not resonate inside the main arms, but also not exactly anti-resonant:

c

Lfn Arm

m

23

Sideband 1 = 19.173 MHz

n1 = 1

n2 = 1

n3 = 255.82

MHzff 20021

To choose the high frequency sideband we look to demodulate at:

Schnupp asymmetry given by:

24 f

cl


For a peak frequency of 300Hz (Adv LIGO) the carrier phase shift will be:

20607.0


l = 434 mm

LSRC = 12569 mm

Proposed Configuration

• Length PRC = 4450 mm

• PRC Free Spectral Range: 33.685 MHz

• PRC as a coupled cavity half integer of PRC FSR

• “Longest” Mode Cleaner 8900 mm FSR = 16.842 MHz

2

21 lllL prPRC

MCm L

cnf

21

For transmission of modulation sidebands by the mode-cleaner, LMC and fm must satisfy:

For sideband coupling into the recycling cavity, LPRC and fm must satisfy:

PRCm L

cnf

22

12


Sideband must not resonate inside the main arms, but also not exactly anti-resonant:

c

Lfn Arm

m

23


n1 = 1

n2 = 0

n3 = 225.55

MHzff 20021

To choose the high frequency sideband we look to demodulate at:

Schnupp asymmetry given by:

24 f

cl


For a peak frequency of 300Hz (Adv LIGO) the carrier phase shift will be:

20605.0


l = 445 mm

LSRC = 5313 mm

Adv LIGO VIRGO AIGO 2K (sh) AIGO 2K (lg)

PRM - BS 4 6 1.8 1.8

BS - ITMInline 4.536 6.4 2.873 10.144

BS - ITMPerp 4.119 5.6 2.427 9.71

L_PRCInline 8.536 12.4 4.673 11.944

L_PRCPerp 8.119 11.6 4.227 11.510

SRM - BS 4.821 5.562 2.663 2.642

AIGO, Adv LIGO and VIRGO

Adv LIGO VIRGO AIGO 2K (sh) AIGO 2K (lg)

L_MC 16.656 143.52 8.9 7.818

L_PRC 8.328 11.96 4.45 11.727

L_Arms 4000 3000 2007 2000

L_SRC 9.148 11.562 5.313 12.569

Asymmetry 0.416 0.399 0.445 0.434

SB 1 (MHz) 9 6.27 16.84 19.17

SB 2 (MHz) 180 188 168.42 172.56

AIGO, Adv LIGO and VIRGO

©LIGO Scientific Collaboration

• Newtonian background

• Seismic ‘cutoff’

• Suspension thermal noise

• Test mass thermal noise

• Unified quantum noise

10 Hz 100 Hz 1 kHz

10-22

10-24

10-21

10-23

Initial LIGO

Advanced LIGON

ewtonian

Seism

ic

Suspension

Test Mass

Qua

ntum

Frequency [Hz]

h(f

) [1

/√H

z]

High Optical Power

©LIGO Scientific Collaboration

• Newtonian background

• Seismic ‘cutoff’

• Suspension thermal noise

• Test mass thermal noise

• Unified quantum noise

10 Hz 100 Hz 1 kHz

10-22

10-24

10-21

10-23

Initial LIGO

Advanced LIGON

ewtonian

Seism

ic

Suspension

Test Mass

Qua

ntum

Frequency [Hz]

h(f

) [1

/√H

z]

High Optical Power

AIGO 2KAIGO 2K

Conclusions

AIGO 2K Dual Recycling Interferometer

Test masses Fused Silica or Sapphire?

Digital control system. EPICS, DSP or both?

Short or long Recycling Cavities?

Conclusions

More information at:

ACIGAhttp://www.anu.edu.au/Physics/ACIGA/

Australian National Universityhttp://www.anu.edu.au/Physics/ACIGA/ANU/

University of Adelaidehttp://www.physics.adelaide.edu.au/optics/res/hi_powerc.html

University of Western Australiahttp://www.gravity.pd.uwa.edu.au/

AIGO 2K Australia - Italy Workshop 2005 7 th October 2005 7 th October 2005 Pablo Barriga for AIGO group.

Documents

salvo slide

aigo group slide

power m1m2

flat m3

heavy test masses slide

zewu yan slide

peter veitch slide

southern hemisphere