towards observation of quantum radiation pressure ... · towards observation of quantum radiation...
TRANSCRIPT
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Towards observation of quantum radiation pressure fluctuation acting on a massive torsion pendulum
Middle presentation in Ando laboratory
D2 Kentaro Komori
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ContentsØ Motivation
Ø Super-detailed noise estimation and design
Ø Future plan
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MotivationObservation of quantum radiation pressure fluctuation
R&D for GW detectors Tests of quantum mechanics
Ø radiation pressure noiseØ observation and reduction
on the table ahead
ü No precedent ever with a massive pendulum over wide frequency range
Ø opto-mechanics experimentØ toward superposition of
macroscopic objects
Torsion pendulum
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Torsion pendulum as test massØ two triangle cavities at both edgesØ read out differential signal (torsional
mode)
• small effective mass• low resonant frequency resulting in
suspension thermal noise• common mode rejection with one
test mass
Advantages𝜙 = 3𝜇𝑚l = 1𝑐𝑚
𝐿 = 15𝑚𝑚ℎ = 1.5𝑚𝑚𝑡 = 0.2𝑚𝑚
𝑚 = 9.9𝑚𝑔𝜔42𝜋 = 0.12𝐻𝑧
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ParameterØ finesse : 2000Ø each input power : 20 mWØ resonant frequency : 0.12 HzØ Q of rotational mode : 2000Ø Q of pendulum mode : 1×109Ø air pressure : 1×10:; PaØ frequency stabilization : 100/f Hz/ Hz (below SQL)Ø intensity stabilization : 1×10:> / Hz (2 times shot noise)Ø cavity round trip length : 11 cmØ common mode rejection rate : 10Ø on a platform suspended from intermediate mass
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MirrorsØ torsion pendulum (prepared)• dimension : 1.5 mm * 15 mm * 0.2 or 0.3 mm• reflectivity : R>99.99% (1064 nm, p-pol, 42º)• curvature : flatØ controlled mirror (prepared)• dimension : 0.5 inch covered with holders (𝜙=35mm)• reflectivity : R>99.98% (1064 nm, 0º)• curvature : 500 mm
20 mW
~15 W
Ø fixed mirror (ordered)• dimension : 0.5 inch, t=3 mm• reflectivity : R>99.8% (1064 nm, p-pol, 43º)• curvature : flat
all mirrors are made of fused silica
Designedℱ~2800 , @AB @⁄ ~0.9
1 cm
5 cm
ℱ~2000, 𝑃EFGE~10 W in the previous 5-mg experiment
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Radiation pressure𝑆IGJ(𝜔) =
ℱ cos𝛽 16ℏ𝜔E𝑃FS𝜋𝑐(1 + 𝛿V)
12𝑚𝜔V
ℱ = 2000𝛽 = 42.6°𝑃FS = 20mW𝛿 = 0𝑚 = 9.9 mg𝑃EFGE~15W
1×10:Z9 m/√Hz@100 Hz
Ø SQL frequency ~ 4 kHz
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Radiation pressureℱ = 2000𝛽 = 42.6°𝑃FS = 20mW𝛿 = 0𝑚 = 9.9 mg𝑃EFGE~10W
1×10:Z9 m/√Hz@100 Hz
0.2 mm 4 mm 3 μmachieved →
stabilized →
suspended →achieved →9 W
← achieved
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Suspension thermal
𝑆G](𝜔) =4𝑘_𝑇ab𝑚𝜔GcaV
𝑄Gca𝜔12
𝑚𝜔V
𝑓Gca = 0.12 Hz, 𝑓JfSg = 𝑓h = 5 Hz
𝑆J](𝜔) =4𝑘_𝑇ab𝑚𝜔JfSgV
𝑄JfSg𝜔𝑟jhkk𝑚𝜔V
𝑆4](𝜔) =4𝑘_𝑇ab𝑀𝜔hV
𝑄h𝜔1
𝑀𝜔V 𝑄Gca = 2000𝑄JfSg = 109𝑄h = 10V
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Suspension thermal𝑄Gca = 2000𝑄JfSg = 109𝑄h = 10V
← achieved with 3um wire and various bars← achieved with 3um wire← easy
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Residual gas𝑆m,op](𝜔) = 4𝑃pFG𝑆 𝑚4cq𝑘_𝑇ab
𝑃pFG = 1×10:; Pa𝑆 = 15 mm × 1.5 mmmolecule : H2O
𝑆op](𝜔) = r 4𝑃pFG 𝑚4cq𝑘_𝑇ab𝑙𝑥V𝑑𝑥v/V
:v/V𝐿𝐼𝜔V
= 4𝑃pFG𝑆 𝑚4cq𝑘_𝑇ab ZV
4yz
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Residual gas𝑆m,op](𝜔) = 4𝑃pFG𝑆 𝑚4cq𝑘_𝑇ab
𝑃pFG = 1×10:; Pa𝑆 = 15 mm × 1.5 mmmolecule : H2O
𝑆op](𝜔) = r 4𝑃pFG 𝑚4cq𝑘_𝑇ab𝑙𝑥V𝑑𝑥v/V
:v/V𝐿𝐼𝜔V
= 4𝑃pFG𝑆 𝑚4cq𝑘_𝑇ab ZV
4yz
← achieved (< 2×10:; Pa with some parts)
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Mirror and bar thermal
𝑆4FG(𝜔) =4𝑘_𝑇ab𝜋𝑤|
1 − 𝜈]V
𝑌]𝜙fmm𝜔
𝜙] = 1×10:9 : SiO2
𝜙Z = 1×10:; : SiO2
𝜙V = 4×10:; : Ta2O5
𝑤| = 0.21 mm
𝜙fmm = 𝜙] +1𝜋𝑤|
𝑑Z𝜙Z𝑌Z𝑌]+𝑌]𝑌Z
+𝑑V𝜙V𝑌V𝑌]+𝑌]𝑌V
𝑆�pG(𝜔) =4𝑘_𝑇ab𝑚𝜔�pGV
𝜙fmm𝜔
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Mirror and bar thermal
𝜙fmm = 𝜙] +1𝜋𝑤|
𝑑Z𝜙Z𝑌Z𝑌]+𝑌]𝑌Z
+𝑑V𝜙V𝑌V𝑌]+𝑌]𝑌V
𝑆�pG(𝜔) =4𝑘_𝑇ab𝑚𝜔�pGV
𝜙fmm𝜔
5.3 kHz 14 kHz1×10:96×10:�
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Frequency and Intensityachieved
but not yet with the turbo pomp on
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VIS
X
xs
xfxs
xixm
mm mi
mf
ms
li
lfkm
kr
Γm
Γr
X
x1x
x3x2m2 m3
m1
k2
k1
Γm
Γ1
k3
vertical20 cm
20 cm platform : Al 1.5 kgrubber viton
intermediate : Cu 2.2 kg damping :
Fe 4.9 kgneodymium
springhorizontal
spring
rubberrubber
common (Q~20)
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Seismic
vertical and horizontal coupling : 1/50
measured by Shimoda-kun
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Lock acquisition𝑣G4] <
�����hℱ
= 2×10:� m/s
𝐹pEa = 1×10:� N 𝐻pEa = 1×10:; N/V
𝑓JfSg = 5 Hz 𝑥G4] < 7×10:> m
𝑥G4] =𝜔JfSg𝑄JfSg
2 𝑥Jqpa(𝜔JfSg)
𝑥Jqpa 𝜔JfSg < 8×10:ZZ m/√Hz
𝑥Jqpa/𝑥]fF] 𝜔JfSg < 1/50
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Lock acquisition𝑥Jqpa/𝑥]fF] 𝜔JfSg < 1/50
0.006 (cleared)
Ø One arm can be locked easily.
𝑣pG4 = 6𝐹Gpg𝑥g/𝑚
𝐹Gpg =2cos 𝛽𝑐(1 + 𝛿V)
ℱ𝑃FS𝜋
𝛿 = 2, 𝑃FS = 1mW
𝑣G4] < 2×10:� m/s
= 2×10:� 𝑥g/10:> m/s
𝑥G4] < 1×10:> m𝑥JfSg = 2×10:> m not bad
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Total noise
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Matters of concernØ Almost nothing
Ø Scattering ?
Ø Other fluctuation of the cavity length at initial lock
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Current statusØ finish to design the set up for the main cavity and to order
short parts (maybe)Ø change the set up of the platform for stabilization system
RC
in loop
out of loop
RC
out of loopin loop
20 cm
5 cm
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Future plan
Ø ultra-super lucky case
Month 4 8 12 4 8
Ø wonderful case
Ø likely case
Ø garbage case
ordering short parts and recovering stabilization system
constructing system for main cavity
lockingimproving the sensitivity and observing QRPF