Interferometer Configurations
Fujihara Seminar
May 2009
Kentaro Somiya
Caltech
Gravitational-wave detector
LASER
Photo-detector
GW
Base line (arm) = 3~4km
Proper location of mirrors to detect GWs
= Interferometer Configuration
Detector sensitivity
• Various kinds of noise• Shot noise is one of the limiting noise sources
total
Standard Quantum Limit
Shot noise
LASER
Phase fluctuation of photons [Quantum noise]
Reduction of shot noise
1. Increase the power2. Increase the signal3. Inject squeezing
keys of good configurations
1st generation detectors; type-I
signal
power
GW
GW power recycling (power )
Fabry-Perot cavity (power + signal )
Power-recycled Fabry-Perot Michelson interferometer (LIGO, Virgo, TAMA)
Both power and signal are enhanced.
1st generation detectors; type II
signal
power
GW
GW power recycling (power )
Dual-recycledMichelson interferometer (GEO)
signal recycling (signal )
Both power and signal are enhanced.
Power/Signal recycling
Power Recycling
Signal Recycling
Power recycling
improve the floor level
Signal recycling
improve the floor level and
narrower the bandwidth
Frequency response of an interferometer is determined by the floor level and the bandwidth.
2nd generation detectors
Nevertheless….
2G detectors will accommodate all threes.
Why do we need three kinds of cavity?
resonant
resonant
anti-resonant resonant
Resonant Sideband Extraction (RSE)
signal
power
decent power recycling (power ) signal extraction
(signal )
High finesse cavity (power ) (signal )
This system changes the power balance
[Mizuno 93]
Power balance
coating substrate
~300ppm heat absorption (=0.125W)
~1W cooling capability [safety factor of 8]
400W
400kW heat transfer
High finesse + low power-recycling (RSE) is suitable for LCGT
20K 20K
Detuning
SRMirror
SR: resonantRSE: anti-resonantdetune: intermediate
SR
RSE
detune
Signal at a certain frequency resonates
Narrow-band signal enhancement
Radiation-pressure noise
1st generation detector (50W at BS, FPMI)2nd generation detector (1kW at BS, RSE)
RP noise
Shot noise Standard Quantum Limit (SQL)
High precisionHeisenberg’s principle
Back action
Reduction of shot noise (high power) Radiation pressure noise
Sensitivity of a broadband detector is limited by the SQL
Radiation pressure in a detuned detector
signal(phase) signal
(phase+amp) laser + signal (amp) [radiation pressure]
signal (phase)
rotation due to the detuning
This loop makes an optical spring and allows us to overcome the SQL
Detuning in LCGT
SQL
thermal noise
broadband
detuned (opt. for BNS)
Observable range for Binary Neutron Stars Broadband RSE : SN=10 at 185Mpc Detuned RSE : SN=10 at 242Mpc
Better sensitivity by detuning!
Variation of the signal response w/ detuning[Ballmer 07]
Broadband
BHBH
NSNS
High Freq
• Reflectivity of the mirrors is fixed• Changing the SRM location and the input power• Tunable for each GW source
total noise level of AdLIGO
3rd generation detector
PRM
SRM
Baseline 5~10km ring cavity
Detuned Sagnac interferometer with Fabry-Perot arm cavities
speed-meter
measure x back action of p measure p no back action
Overcoming the SQL in a broad frequency band
[Chen 03]
Sensitivity curve of detuned Sagnac[Mueller-Ebhardt 09]
• Overcoming the SQL in a broad frequency band• Better than other methods in the optical-loss issue
20ppm loss/arm300ppm loss/arm
End-mirror cavity[Khalili 2005]
less coatings more coatings
Configuration to reduce thermal noise
anti-reso cavity
total thermal-noise level decreases
Replacing a mirror to a cavity…
Xylophone with SPI
• Top stage: MF 10-100Hz
• Mid stage: HF 100-10kHz
• Bottom stage: LF 1-10Hz
Low mirror thermal noiseHigh power
Extremely high powerLow optical loss + squeezing
Low power + very low temperatureLow suspension thermal noise
10km
10m
(suspension-point interferometer)
Summary
1st generation detector
2nd generation detector
3rd generation detector
• Power-recycled FP Michelson configuration• Reduction of shot noise
• Broadband/detuned RSE configuration• Reaching/overcoming the SQL
• Overcoming the SQL in a broad frequency band• Any ideas being welcome