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TAMA300

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Direct Measurement of Residual Gas Effect on the sensitivity ... Duct 2 x 10-8 Torr Non-baking! Chamber 1 x 10-7 Torr. 300m long vacuum duct (400mm in diameter) ... – PowerPoint PPT presentation

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Title: TAMA300


1
  • Once per 3 years (IVC15)
  • 16 parallel sessions (6days)
  • Poster sessions (3days)
  • Vacuum equipment exhibition (3days)
  • Many cancels from Japan
  • Few Japanese tourists in the street
  • My interest
  • Equipment technology
  • (TMP, MBP, IP, SRG)
  • Coating (DLC, TiN)
  • Gas dynamics

2
Direct Measurement of Residual Gas Effect on the
sensitivity in TAMA300
  • R. Takahashi, Y. Saito, M. Fukushima, M. Ando, K.
    Arai,
  • D. Tatsumi, G. Heinzel, S. Moriwaki, and T.
    Yamazaki
  • National Astronomical Observatory of Japan, KEK,
    The Univ. of Tokyo
  • Vacuum system of TAMA300
  • Residual Gas Effect
  • Experimental Setup
  • Experimental Result
  • Discussion
  • Summary

3
Specification of TAMA300
  • Location Mitaka Campus of NAOJ
  • Aimed sensitivity h 3x10-21 _at_300Hz
  • Baseline length 300m
  • Interferometer Fabry-Perot Michelson
  • Finesse of Cavity 520
  • Laser Injection-lock NdYAG
  • Output10W
  • l1,064nm
  • Recycling Gain 10
  • Vacuum System 10-6Pa

4
Vacuum System of TAMA300
5
Vacuum System of TAMA300
  • Large-scale Vacuum System
  • Volume 85m3
  • Surface 820m2
  • Technique
  • 6 stainless steel and 2 pure titanium chambers
  • ECB(Electro-chemical buffing) process
  • Gate valve(400f) with optical window
  • Pressure under operating
  • Duct 2 x 10-8 Torr Non-baking!
  • Chamber 1 x 10-7 Torr

300m long vacuum duct (400mm in diameter)
6
Residual Gas Effect 1
  • Optical path difference due to fluctuation of
    refractive index
  • Correlation function
  • Its Fourier transfer

7
Residual Gas Effect 2
  • Refractive index and Molecular density
  • Lorentz-Lorenz formula
  • Molecular density
  • Correlation function
  • Interaction time
  • Molecular velocity
  • Gaussian beam size
  • Correlation function

8
Residual Gas Effect 3
  • Resulting displacement noise in the
    interferometer
  • roundtrip in arm
  • dependent in molecular
  • We selected Xe-gas.

9
Experimental Setup
  • Measurement of pressure
  • Pressures were measured at 7 points using
    penning gauges.
  • Spinning Rotor Gauge (SRG) is suitable for this
    experiment.
  • Penning gauges were calibrated by SRG.
  • Experiment procedure
  • 1. Start ventilation
  • 2. Stop ventilation
  • 3. Wait for about 20 min.
  • 4. Measure pressure, temperature, and noise
  • 5. Repeat

10
Experimental Result 1
  • Measured spectrum
  • Most sensitive frequency was about 900Hz.

The Xe-gas pressure of 0.03Pa induced an increase
in the displacement noise of 3x10-18m/Hz1/2
11
Experimental Result 2
  • Relation between pressure and observed noise
  • Observed noise (dx2) was proportional to
    pressure.
  • This result is proving the theory.

12
Discussion
  • Correlation factor
  • Observed noise was grater than the calculation
    by factor 2.
  • This shows the correlation is larger than the
    assumption because a space is enclosed by the
    tube.
  • Acoustic effect
  • Mirrors might be directly excited by an acoustic
    emission through low vacuum.
  • Environmental acoustic noise is less than 80dB
    (0.2Pa) in TAMA300 facility.
  • Maximum 6x10-20m/Hz-1/2 _at_1Pa is predicted.
  • (even if the wall of the vacuum chamber did not
    protect any acoustic emission.)
  • This effect was negligible.

x1.8
13
Summary
  • Residual gas effect was measured directly on the
    sensitivity in TAMA300.
  • It is found that the Xe-gas pressure of 0.03Pa
    induces an increase in the displacement noise of
    3x10-18m/Hz1/2.
  • This noise level is consistent with a calculated
    optical path fluctuation due to residual-gas
    within factor 2.
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