Terrestrial Detector for Low Frequency GW Based on Full ...
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Hyung Mok Lee Department of Physics and Astronomy, Seoul National University
Collaborators: H. Paik, Vol Moody, Cornelius Griggs, Ettore Majorana, Jan Harms, C. Kim, A. Nielsen
KCK Meeting, Dec. 14, 2015 Beijing
Terrestrial Detector for Low Frequency GW Based on Full Tensor
Measurement
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2015 KCK, Dec. 14-16, Beijing HMLee
Gravitational Waves in Wide Spectral Range
http://rhcole.com/apps/GWplotter by Moore, Cole & Berry
}
There is a gap here (0.1 - 10 Hz)
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2015 KCK, Dec. 14-16, Beijing HMLee
Terrestrial Detector Concepts for Low Frequencies
• Astrophyiscal requirement for detectors at ~ 0.1 Hz: should be better than 10-20 Hz-1/2 (Harms et al. 2013)
• Following Detector Concepts have been considered 1. Atom-laser interferometer 2. Torsional bar with laser interferometer (TOBA)
3. Michelson interferometer
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2015 KCK, Dec. 14-16, Beijing HMLee
Gravity Gradiometer as a GW Detecror
•Geodesic deviation equation:
• In weak field limit
• Strain Amplitude
d
2x
i
dt
2= �R
i0j0x
j
Ri0j0 ⇡ @
2�
@x
i@x
j
Ri0j0 = �1
2
@2hij
@t2⇡ 1
2!2hij
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2015 KCK, Dec. 14-16, Beijing HMLee
• Truncated icosahedral gravitational wave antenna (Johnson & Merkowitz 1993)
• Omni-directional
• Measure direction and polarization
• Spherical Resonant Detectors
• MiniGRAIL (Leiden)
• Schenberg (Sao Paulo)
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Full Tensor Detectors
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2015 KCK, Dec. 14-16, Beijing HMLee
Tunable Free Mass GW Detector (Wagoner et al. 1979)• The relative motion of two masses induces driving emf of
resonant L-C circuit • The relative momentum is determined by the current in the
circuits • Can be tuned over a wide frequency range
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2015 KCK, Dec. 14-16, Beijing HMLee
Superconducting Tensor Gravity Gradiometer (Univ. of Maryland)
Test masses are magnetically suspend (fDM ~ 0.01 Hz). 100x higher sensitivity
Six test masses mounted a cube form a tensor gradiometer.
Test masses are levitated by a current induced along a tube.
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2015 KCK, Dec. 14-16, Beijing HMLee
Superconducting tensor GW Detector
• Superconducting Omni-directional Gravitational Radiation Observatory (SOGRO)
• By detecting all six components of Riemann tensor, the source direction and the polarization can be determined
hii(t) =1
L
[x+ii(t)� x�ii(t)]
hij(t) =1
L
{[x+ij(t)� x�ij(t)]� [x�ji(t)� x+ji(t)]}
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2015 KCK, Dec. 14-16, Beijing HMLee
Requirements and Philosophy
• Extremely low detector noise is required • Low temperature, high Q and quantum limited detector
• Test mass suspension frequency should be lowered to below the signal bandwidth (0.1 - 10 Hz) • Almost free test masses by magnetic levitation
• Seismic noise is more difficult to isolate at low frequencies • High CM rejection in a superconducting differential
accelerometer • Newtonian noise increases sharply below 10 Hz
• Tensor detector which can discriminate against the near-field gravity
hij ⇠1
!
2
@
2�
@x
i@x
j
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2015 KCK, Dec. 14-16, Beijing HMLee
Basic Design of SOGRO
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2015 KCK, Dec. 14-16, Beijing HMLee
Suspension• Go underground to reduce seismic and gravity gradient
noise
• Nodal support in order to suppress the odd harmonics
• 25m pendulum gives fp=0.1 Hz for two horizontal modes and fr <0.001 Hz for three angular modes
• passive isolation for high frequencies
• Triangulate with thin wall tubes to make the platform rigid
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2015 KCK, Dec. 14-16, Beijing HMLee
Magnetic Levitation• Field required to levitate 5 ton mass:
• The biggest challenges: • To obtain symmetry, vertical DM resonance frequencies
must also reduced to 0.01 Hz. • Employ “push-pull levitation”
B2
2µ0A = Mg, B =
✓2µ0Mg
A
◆1/2
⇡ 0.16T
(Moody, Chan and Paik, JAP, 1986)
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2015 KCK, Dec. 14-16, Beijing HMLee
Tuned Capacity-Bridge Transducer
•Capacitor bridge coupled to a near quantum-limited SQUID thru S/C transformer.
•LC resonance increases energy coupling β by Qp .
•Oscillator noise is rejected by the bridge balance. • Maintain precise
balance by feedback.
EN (f) =kBT!D
QD+
|!2 � !2D|
!p
✓1 +
1
�2
◆1/2
kBTN
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2015 KCK, Dec. 14-16, Beijing HMLee
Achievable detector noiseFor CW signal impedance matched bridge transducer
Parameter SOGRO 1 SOGRO 2 Method Employed (SOGRO 1 / 2)Each mass M 5 ton 5 ton Nb square tubeSeparation L 30 m 100 m Over “rigid” mounting platformAntenna temp T 1.5 K 0.1 K Superfluid He / dilution refrigeratorDM frequency fD 0.01 Hz 0.01 Hz Magnetic levitation w/ negative springDM quality factor QD 108 109 Surface polished pure NbSignal frequency f 0.1-10 Hz 0.1-10 Hz Detector noise computed at 1 HzPump frequency fp 50 kHz 50 kHz Tuned capacitor bridge transducerAmplifier noise no. n 200 10 Near-quantum-limited SQUIDDetector noise S 1/2(f )
h 2×10�20 Hz�1/2 2×10�21 Hz�1/2 Two phase development
Sh(!) =8
ML2!4
(kB!D
QD+
|!2 � !2D|
!p
✓1 +
1
�2
◆1/2
kBTN
), kBTN = n!p
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2015 KCK, Dec. 14-16, Beijing HMLee
Seismic noise
Seismic noise of underground sites
▪ 20-m pendulum with nodal support ⇒ Passive isolation for f > 0.1 Hz. ▪ 110 dB reduction by combining passive
and active isolation with CM rejection of the detector.
Seismic background
Active isolation
Axis alignment and scale factor match
Error compensation
Paik 14
SOGRO 1 sensitivity
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Major challenges: ▪ Large-scale cryogenics. ▪ Mitigation of Newtonian noise. 13
Sensitivity goals of SOGRO
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2015 KCK, Dec. 14-16, Beijing HMLee
Newtonian gravity noise (NN)▪ Seismic and atmospheric density modulations cause
Newtonian gravity gradient noise. ▪ GWs are transverse and do not have longitudinal
components whereas the Newtonian gradient does.In GW frame,with the wave traveling along the 3rd axis,
GW could be distinguished from near-field Newtonian
gravity.
h0(!) =
0
@h+(!) + h0
NG,11(!) h⇥(!) + h0NG,12(!) h0
NG,13(!)h⇥(!) + h0
NG,12(!) �h+(!) + h0NG,22(!) h0
NG,23(!)h0NG,13(!) h0
NG,23(!) h0NG,33(!)
1
A
By combining tensor components, we get
Similar expression can be found for hx(ω).
h+(!) = h011(!)� 2 cot ✓h0
13(!) + csc
2 ✓2⇡G⇢0
!
�RcR
exp
✓!
cRz
◆X
i
⇠(!)
+ csc
2 ✓4⇡G
!2
X
i
�⇢i(!) sin2 #i exp
✓!
cISz sin#i
◆
Due to Rayleigh Waves
Due to Infrasound waves
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2015 KCK, Dec. 14-16, Beijing HMLee
Removal of Newtonian noise
Tensor + 8 microphones 100 m ( 100m, SNR 105)
Harms and Paik, PRD (2015)
Tensor + ver CM (0 noise)
Ω
Meets sensitivity goal of SOGRO 1.
Tensor + ver CM (SNR 106
+7 seisemometers (5km, SNR 103)
Tensor + 15 microphones(0, 0.6, 1 km, SNR 104)
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2015 KCK, Dec. 14-16, Beijing HMLee
Summary
Maximum distances to detect IMBH- IMBH binary merger (SOGRO 2)
▪ SOGRO would fill in the missing signal band between eLISA and aLIGO/Virgo/KAGRA, 0.1 – 10 Hz.
▪ SOGRO is a tensor detector with all-sky coverage and with the ability to locate the source and determine wave polarization.
▪ SOGRO, a full-tensor detector, has an advantage in rejecting NN. ▪ Technical details have to be further studied.
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