Picture Sora Kawamura Several Fun Research Projects at

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Picture: Sora Kawamura Several Fun Research Projects at NAOJ for the Future GW Detectors

Picture: Sora Kawamura Several Fun Research Projects at NAOJ for the Future GW Detectors LIGO Seminar @ Caltech Aug. 8, 2006 Seiji Kawamura National Astronomical Observatory of Japan

National Astronomical Observatory of Japan (NAOJ) NAOJ is located in Tokyo. TAMA 300 is

National Astronomical Observatory of Japan (NAOJ) NAOJ is located in Tokyo. TAMA 300 is located on the NAOJ campus.

Other research projects at NAOJ l l l Displacement-noise free Interferometer RSE DECIGO MHz

Other research projects at NAOJ l l l Displacement-noise free Interferometer RSE DECIGO MHz GW detection QND

Displacement-noise free Interferometer

Displacement-noise free Interferometer

Motivation l l Displacement noise: seismic Noise, thermal noise, radiation pressure noise Cancel displacement

Motivation l l Displacement noise: seismic Noise, thermal noise, radiation pressure noise Cancel displacement noise shot noise limited sensitivity Increase laser power sensitivity improved indefinitely Diplacement noise Displacement noise Cancel displacement noise Shot noise PD Laser Sensitivity l Increase laser power Frequency

Principle 1: GW and mirror motion interact with light differently On reflection GW On

Principle 1: GW and mirror motion interact with light differently On reflection GW On propagation Light Mirror motion Difference outstanding for GW wavelength distance between masses

Principle 2: Mirror motion can be cancelled by combining interferometer outputs Mirror motion Laser

Principle 2: Mirror motion can be cancelled by combining interferometer outputs Mirror motion Laser PD l l l Laser PD Bi-directional MZ Increase # of mirrors Implement many interferometers Take combination outputs cancel mirror motion Mirror motion

Example of DFI l l Two 3 -d bi-directional MZ Take combination of 4

Example of DFI l l Two 3 -d bi-directional MZ Take combination of 4 outputs Mirror motion completely cancelled GW signal remains (f 2)

Experiment (Ideal) l One bi-directional MZ Mirror motion GW Laser PD Extract GW Mirror

Experiment (Ideal) l One bi-directional MZ Mirror motion GW Laser PD Extract GW Mirror motion

Experiment (Practical) l EOM used for GW and mirror motion Simulated mirror motion Mirror

Experiment (Practical) l EOM used for GW and mirror motion Simulated mirror motion Mirror motion GW Laser ~ Simulated GW ~ Laser PD Ideal        Practical PD

Results l l Mirror motion cancels out GW signal remains Mirror motion to output

Results l l Mirror motion cancels out GW signal remains Mirror motion to output GW signal to output Difference Mirror motion    GW signal

Next step l l Implement cavity to reduce the effective frequency Demonstrate the cancellation

Next step l l Implement cavity to reduce the effective frequency Demonstrate the cancellation of the BS motion using two bi-directional MZ References l l Kawamura and Chen, PRL, 93, (2004) 211103 Chen and Kawamura, PRL, 96 (2006) 231102 Chen, Pai, Somiya, Kawamura, Sato, Kokeyama, Ward, submitted to PRL (gr-qc/0603054) Sato, Kawamura, Kokeyama, Ward, Chen, Pai, and Somiya, to be submitted to PRL

RSE

RSE

4 m RSE l l Supended mass RSE Miniature suspension system

4 m RSE l l Supended mass RSE Miniature suspension system

Previous Accomplishments l l l Tuned RSE (w/o PRM) locked Detuned RSE (w/o PRM)

Previous Accomplishments l l l Tuned RSE (w/o PRM) locked Detuned RSE (w/o PRM) locked Optical spring effect observed – Miyakawa, Somiya, Heinzel, and Kawamura, Class. and Quantum Grav. , 19 (2002) p. 1555 -1560 – Somiya, Beyersdorf, Arai, Sato, Kawamura, Miyakawa, Kawazoe, Sakata, Sekido, Mio, Appl. Opt. 44 (2005) pp. 3179 -3191

Current Activity l Try new signal extraction method – Backup for Advanced LIGO –

Current Activity l Try new signal extraction method – Backup for Advanced LIGO – Baseline for LCGT l Lock RSE (w/ PRM)

New Signal Extraction Method

New Signal Extraction Method

Signal Matrix ls ls diagonal lp orthogonal lp Black: Analytic results Red: Numerical simulation

Signal Matrix ls ls diagonal lp orthogonal lp Black: Analytic results Red: Numerical simulation using “FINESSE” Baseline Design for LCGT

Delocation l Option for LCGT - Could have potential advantages

Delocation l Option for LCGT - Could have potential advantages

Current Status l l l MZ locked only w/ PM FP Michelson locked Suspension

Current Status l l l MZ locked only w/ PM FP Michelson locked Suspension system improved

DECIGO

DECIGO

What is DECIGO? Deci-hertz Interferometer Gravitational Wave Observatory - bridges the gap between LISA

What is DECIGO? Deci-hertz Interferometer Gravitational Wave Observatory - bridges the gap between LISA and terrestrial detectors. - could attain high sensitivity because of lower confusion noise.   10 -18 Strain [Hz-1/2] LISA 10 -20 Terrestrial Detectors DECIGO 10 -22 Confusion Noise 10 -24 10 -2 100 102 Frequency [Hz] 104

Pre-conceptual Design FP-Michelson interferometer Arm length: 1000 km Laser power: 10 W Laser wavelength:

Pre-conceptual Design FP-Michelson interferometer Arm length: 1000 km Laser power: 10 W Laser wavelength: 532 nm Mirror diameter: 1 m Mirror mass: 100 kg Arm cavity Finesse: 10 Orbit and constellation: TBD Drag-free satellite PD Kawamura, et al. , CQG 23 (2006) S 125 -S 131 Laser PD Drag-free satellite Arm cavity Drag-free satellite

Drag-free and FP Cavity Displacement Signal between S/C and Mirror Local Sensor Mirror Thruster

Drag-free and FP Cavity Displacement Signal between S/C and Mirror Local Sensor Mirror Thruster Actuator Thruster Displacement signal between the two Mirrors

Requirements [Practical force noise] l 4 x 10 -17 N/ Hz per mirror [Frequency

Requirements [Practical force noise] l 4 x 10 -17 N/ Hz per mirror [Frequency Noise] @ 1 Hz l First-stage stabilization: 1 Hz/ Hz l Stabilization gain by common-mode arm length: 105 l Common-mode rejection ratio: 105

Science by DECIGO BH NS-NS (1. 4+1. 4 Msun) • z<1 (SN>26: 7200/yr) •

Science by DECIGO BH NS-NS (1. 4+1. 4 Msun) • z<1 (SN>26: 7200/yr) • z<3 (SN>12: 32000/yr) • z<5 (SN>9: 47000/yr) IMBH (1000+1000 Msun) • z<1 (SN>6000) +B H(1 @z 000 M =1 su ) n NS +N Correlation for 3 years S@ z=1

Acceleration of Expansion of the Universe Expansion +Acceleration? DECIGO GW NS-NS (z~ 1) Output

Acceleration of Expansion of the Universe Expansion +Acceleration? DECIGO GW NS-NS (z~ 1) Output Strain Template (No Acceleration) Real Signal ? Phase Delay~ 1 sec (10 years) Time Seto, Kawamura, Nakamura, PRL 87, 221103 (2001)

Roadmap for DECIGO 06 07 08 09 10 11 12 13 14 15 16

Roadmap for DECIGO 06 07 08 09 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 R&D Advanced R&D PF 1 Design & Fabrication Observation PF 2 Design & Fabrication Observation DECIGO 06 07 08 09 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24

DECIGO Pathfinder 1 Objectives l Drag-free system l Cavity locking in space l Modest

DECIGO Pathfinder 1 Objectives l Drag-free system l Cavity locking in space l Modest sensitivity at 0. 1 – 1 Hz Local Sensor Actuator Thruster

DECIGO Pathfinder 2 Objectives l DECIGO with modest specification l Cavity locking between two

DECIGO Pathfinder 2 Objectives l DECIGO with modest specification l Cavity locking between two satellites l Meaningful sensitivity Drag-free satellite Arm cavity PD Laser PD Drag-free satellite Arm cavity Drag-free satellite

DECIGO Simulator Objectives l l l 2 m Clamp Vertical Position l Continual free-fall

DECIGO Simulator Objectives l l l 2 m Clamp Vertical Position l Continual free-fall environment Clamp release Modest sensitivity down to 0. 1 Hz Possibility of long arm Release 1 sec Hold Release Hold Time

DECIGO Demonstrator Thruster Satellite A Satellite B Mirror A Mirror B Actuator Local sensor

DECIGO Demonstrator Thruster Satellite A Satellite B Mirror A Mirror B Actuator Local sensor Air-hockey table Objectives l Lock acquisition

Budget and Working Group l Will submit a budget request ($18 M for 6

Budget and Working Group l Will submit a budget request ($18 M for 6 years) this fall – R&D for DECIGO – PF 1 – w/ Pulsar Timing l DECIGO-WG: 120 members currently

MHz GW detection

MHz GW detection

Objectives and Scope l l Detect GW at MHz Develop technologies for synchronous recycling

Objectives and Scope l l Detect GW at MHz Develop technologies for synchronous recycling GW Sources at MHz l l Inspiral of mini black holes GW from inflation period

Synchronous Recycling Mirror Laser BS Photo detector Dark Fringe Drever, 1983

Synchronous Recycling Mirror Laser BS Photo detector Dark Fringe Drever, 1983

Response of Synchronous Recycling x h t y y x l Laser GW GW

Response of Synchronous Recycling x h t y y x l Laser GW GW 4 l BS Photo detector GW effect synchronously enhanced!

Plan for Table-top Experiment Integration for 1 year F 105 l 75 cm f.

Plan for Table-top Experiment Integration for 1 year F 105 l 75 cm f. GW 100 MHz h 10 -21 Hz-1/2 h 10 -26 Hz-1/2

Current Status l l Locked w/ low Finesse F 100 Noise Spectrum taken f

Current Status l l Locked w/ low Finesse F 100 Noise Spectrum taken f 1 Non 50: 50 Beam splitter 1 DOF to control EOM f 1 f GW - f 1 - BW Output

First Noise Spectrum

First Noise Spectrum

QND

QND

Objectives and Scope l l Beat SQL using ponderomotive squeezing Use FP Michelson w/

Objectives and Scope l l Beat SQL using ponderomotive squeezing Use FP Michelson w/ super light mirrors Plan 1. Observe radiation pressure noise 2. Reduce radiation pressure noise w/ homodyne detection 3. Beat SQL 4. Expand the effective frequency range

Ponderomotive Squeezing l Squeezed by phase change caused by reflection by free mass Squeezing:

Ponderomotive Squeezing l Squeezed by phase change caused by reflection by free mass Squeezing: frequency dependent Cannot beat SQL w/ RF method Laser Noise Signal Vacuum Caves, Walls & Milburn, Braginsky & Khalili, . . .

Homodyne Detection S/N can be improved by choosing appropriate homodyne phase! Signal Noise Laser

Homodyne Detection S/N can be improved by choosing appropriate homodyne phase! Signal Noise Laser Local light Homodyne phase

Quantum Noise l Radiation pressure noise can be completely cancelled at one frequency l

Quantum Noise l Radiation pressure noise can be completely cancelled at one frequency l The frequency depends on homodyne phase

Strategy l l Use super-light mirror Use high finesse – Increase radiation pressure noise

Strategy l l Use super-light mirror Use high finesse – Increase radiation pressure noise – Easier to detect l Use tuned IFO (no optical spring)

Design Parameter and Noise Estimate Laser power 200 m. W Injected power into the

Design Parameter and Noise Estimate Laser power 200 m. W Injected power into the interferometer 120 m. W Finesse 7500 Front mirror mass 200 g End mirror mass 23 mg Diameter of the end mirror 3 mm Thickness of the end mirror 1. 5 mm Beam radius on the end mirror 500 mm Q factor of substrate 105 Loss angle of coating 4× 10 -4 Temperature 300 K Length of the fiber 1 cm Thickness of silica fiber 10 mm

Current Status l l Homodyne detection method verified Vacuum tank ready Design of set-up

Current Status l l Homodyne detection method verified Vacuum tank ready Design of set-up complete Fiber of 10 m drawn successfully

The End

The End