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Mirror Qs and thermal noise in the TNI with ring dampers

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Parametric Oscillations in Fabry-Perot Cavities. Cavity length determines field inside. Mirror mechanical oscillations affect ... contact of mirror with barn. ... – PowerPoint PPT presentation

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Title: Mirror Qs and thermal noise in the TNI with ring dampers


1
Mirror Qs and thermal noisein the TNIwith ring
dampers
  • Akira Villar
  • OWG Telecon
  • April 28, 2006
  • Eric D. Black, Kenneth G. Libbrecht

2
Coupling Between Light and Sound Acousto-Optic
Effect
3
Parametric Oscillations in Fabry-Perot Cavities
Cavity length determines field inside. Mirror
mechanical oscillations affect cavity length. If
radiation pressure can drive mechanical
oscillations, feedback will occur.
Spatial overlap between optical and mechanical
modes complicates the picture, rings up multiple
mechanical and optical modes and bleeds power out
of the TEM00 mode. b) Mirror mechanical mode c)
Associated optical mode (from Zhao, et al.,
PRL 94, 121102 (2005).)
4
Potential Problem for AdLIGO
  • David Blair group observe parametric damping of
    mechanical modes in bar detector transducers
  • Phys. Rev. Lett. 74, 1908-1911 (1995)
  • Braginsky, et al. point out that acousto-optic
    feedback can ring up body modes in a F-P cavity,
    bleeding power out of the TEM00 mode - parametric
    amplification.
  • Phys. Lett. A 287, 331-338 (2001)
  • Vahalas group observes radiation-pressure-driven
    oscillations in microcavities
  • Optics Express 13, 5293-5301 (24 June, 2005)
  • Phys. Rev. Lett. 95, 033901 (2005)
  • N. Mavalvala observes the effect in a macroscopic
    cavity with suspended mirrors
  • LIGO-P050045-00-R (Oct. 27, 2005)

5
Instability Condition Rgt1
Ju, et al. G050325-00 who got it from Braginsky,
et al. Phys. Lett. A 305, 111 (2002)
6
Reducing Qswithout affecting thermal noise
(much)
7
Ring Damper
Idea Lossy ring around mirror barrel could
suppress mechanical Qs of many modes, without
affecting thermal noise on the face (much)
8
FEA Model 1
Gras, et al. preprint Test Mass Ring Dampers with
Minimum Thermal Noise
9
FEA Model 2
D. Coyne, T050173-00
10
Ring Dampers
  • 4x 4 fused silica mirrors.
  • Ring dampers only on SAC output mirror.
  • Two ring dampers 1/8 thick located 1 on either
    side of the midpoint.
  • Dampers are made of buna.

11
Thermal Noise Interferometer
  • Fundamental-noise limited interferometer (thermal
    and shot).
  • Test Cavities
  • Fused silica substrates
  • Titanium doped silica tantala coatings
  • Ring dampers around SAC output
  • Measurement made as relevant to AdLIGO as
    possible in a small interferometer.
  • Lowest noise levels practical
  • Low-mechanical-loss substrates
  • Largest practical spot size

12
TNI Total Noise
13
Effect of damper on Qs
14
Effect of damper on Qs
15
Effect of damper on Qs
16
Effect on Broadband Thermal Noise (NAC)
17
Effect on Broadband Thermal Noise (SAC)
18
Servo Block Diagram
19
Noise Breakdown
20
Mirror Floats Freely
21
Error Signal Scales with Power
22
Error Signal Scales with Modulation Depth
23
What can be said about the bump?
  • It is only in SAC.
  • It is not due to
  • servo electronic noise.
  • laser frequency noise.
  • pendulum thermal noise.
  • shot noise.
  • contact of mirror with barn.
  • It scales with power and modulation depth in a
    way that is consistent with length noise.
  • It is stable and reproducible.

24
What Next?
  • A model that accounts for the change in the
    broadband noise and indicates how to avoid it.

25
Dennis Coynes FEA Modal Analysis
  • Dennis Coyne did a rough FEA modal analysis and
    found mechanical modes at a few kilohertz (wiggle
    modes of a square o-ring).
  • Riccardo and Phil independently showed that low-Q
    modes at a few kilohertz could lead to the
    shelf observed in our broadband noise floor.
  • Precise calculation would require detailed
    knowledge of o-ring shape when stretched, as well
    as contact area with the mirror.

26
Riccardos fit
  • Gaussian peak combined with fit to TNI before
    noise curve.
  • Thermal noise peak really should be Lorentzian,
    but Gaussian ought to be a reasonable
    approximation.
  • Quantitatively reproduces shelf behavior.

27
Phils model
  • Simple harmonic oscillator with low-Q viscous
    damping.
  • Physical model, as opposed to fit to data.
  • Qualitatively reproduces shelf appearance
  • (y-axis is noise, x-axis is frequency)

28
Conclusions I
  • Parametric instabilities are expected to be a
    problem for AdLIGO.
  • Ring dampers have been proposed to avoid them.
  • Ring dampers were installed at the TNI.
  • Observed a drastic reduction in Qs.
  • Observed an increase in broadband thermal noise.

29
Conclusions II
  • Models indicate that the increase in the
    broadband noise floor is probably due to a
    mechanical mode (wiggle mode) of the o-ring.
  • Need something flat to get around this.
  • Riccardo suggests a thin aluminum ring, shrunk to
    fit.
  • David Blair has proposed a strip of optical
    coating around the barrel.
  • We are trying Kapton tape now.
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