Title: Silica Research in Glasgow
1Silica Research in Glasgow
- Gianpietro Cagnoli IGR - University of Glasgow
- GEO Collaboration
- Ginzton Lab, Stanford
- Caltech
2Summary
- Silica suspensions in GEO600
- Direct Measurement of Thermal Noise
- Coating Losses
- Non-Linear Thermoelastic Effect
3Silica suspensions in GEO600GEO600 Collaboration
- Two monolithic silica suspensions have been
installed in GEO600 (middle of June) - GEO600 is the first interferometer to use such
suspension to reduce thermal noise - Some numbers
- fibres length 285 mm
- vertical freq. 16 Hz
- mirror mass 5.6 kg
4Silica suspensions in GEO600
- Features
- 4 fibres welded on ears
- 2 silicate bonded ears each mass
- Selective damping of violin modes with teflon
coating on fibres - Masses are hold in a rigid frame during the
welding and transportation inside the tank - Once the stage is suspended the holding frame
becomes a catcher
5Silica suspensions in GEO600
Coating
Cutting
6Silica suspensions in GEO600
Welding (test)
7Direct measurement of thermal noise GEO600
Collaboration
- During the last year the 10m interferometer in
Glasgow have been upgraded - A sensitivity limit lower than 10 18 m/Hz ½
has been achieved above 500 Hz (blue curve at
right) - Shot noise 210 19 m/Hz ½
- Damping of the internal modes of one mass was
increased by spreading 3 strips of grease on the
barrel and noise was again measured (red curve)
8Direct measurement of thermal noise
- Q of several modes were measured
- Q 1800 for greased mass
- Q 1.210 5 for clean masses
- Thermal noise estimation
- - semi-infinite mass
- - homogeneous structural damping (Levin Yu.,
Phys.Rev. D, 57 (2), 659-663) - Results
- Fluctuation-Dissipation Theorem has been
verified experimentally -
3 masses Q 120000 1 mass Q 1800
4 masses Q 120000
9Coating losses Glasgow and Stanford Collaboration
Identify and measure the coating loss from Q
measurements on silica cylinders
- Sample
- - Corning 7980
- - 127 mm diameter, 100 mm length
- - IR coating on front faces and barrel
- Measurements
- - ring down method, 7 modes measured
- - 15 different sample suspensions tested
- Finite elements analysis
- - used for energy ratios (surface to bulk)
- - convergence with N. of points checked
- - agreement to a few with measured
- frequencies
10Coating losses
- Two parameters model
-
- Cff is the front face to bulk energy ratio
- Results comments
- - all modes but 1st asymmetric are lined up
- - low loss measurement is not accidental
- - 1st symmetric mode loss too high?
- - but then the linear fitting is not good
then another source of loss is significant
11Coating losses
- Results comments
- - apart for the 1st symmetric mode (high loss)
the other points are aligned
- other sources of loss are currently under
- investigation to justify the high value
- measured for the 1st symmetric mode
Coating losses could be a serious limit to the
next generation interferometers
12Non-linear thermoelastic effect Glasgow and
Caltech Collaboration
13Non-linear thermoelastic effect
In non-linear thermoelastic effect thermal
fluctuations are transformed in strain
fluctuations through the thermoelastic
coefficient b 1/EdE/dT
This second order effect becomes relevant due to
the large longitudinal static stress so in the
suspension fibre
P
14Non-linear thermoelastic effect
An article will be submitted soon to Phys. Rev. D
by Cagnoli G. and Willems P.