Differences between revisions 47 and 52 (spanning 5 versions)
Revision 47 as of 2013-10-06 19:28:54
Size: 2279
Comment:
Revision 52 as of 2013-10-07 00:42:57
Size: 2835
Comment:
Deletions are marked like this. Additions are marked like this.
Line 5: Line 5:
To correct for the modal frequency shifts in the FP arm cavity that arise from the spatial inhomogeneities on the mirror surface. This will be done by imaging heat patterns on the ETM surface. The thermoelastic deformations created on the mirror surface introduces phase shifts to the cavity modes. The green ALS system will be used to mode scan the cavity continuously. A feedback control system will actively correct for the frequency shifts based on the cavity mode scan information. To correct for the modal frequency shifts in the FP arm cavity that arise from the spatial inhomogeneities on the mirror surface (We are not looking to suppress the higher order modes). This will be done by imaging heat patterns on the ETM surface. The thermoelastic deformations created on the mirror surface introduces phase shifts to the cavity modes. The green ALS system will be used to mode scan the cavity continuously. A feedback control system will actively correct for the frequency shifts based on the cavity mode scan information.
Line 25: Line 25:
we can conclude that '''the amplitude of the beatnote as a function of the end-green laser frequency (or the local oscillator frequency) will hold the information about the cavity resonance frequencies and hence the effect of the mirror distortions created by various heat patterns can be mapped'''. we can conclude that the amplitude of the beatnote as a function of the end-green laser frequency (or the local oscillator frequency) will hold the information about the cavity resonance frequencies and hence the effect of the mirror distortions created by various heat patterns can be mapped.
Line 29: Line 29:
==== SIS ====  1. Using SIS find the resonance frequencies of the various transverse modes: Using the phase map measurements made for the ITM and ETM, we will estimate the modal content of the arm cavity.
Line 31: Line 31:
 1.  2. COMSOL model various heat patterns on the ETM : Model thermal deformations on the ETM: core heating, ring heating, core+ring heating for various pixel sizes and various deformation depths on the mirror and generate phase maps.

 3. Analyze the effect of deformed mirror cavity and analyze the cavity fields using SIS.

 4.

Tuning Fabry-Perot cavity modal frequencies using controlled thermoelastic deformations on mirror surface

Goal

To correct for the modal frequency shifts in the FP arm cavity that arise from the spatial inhomogeneities on the mirror surface (We are not looking to suppress the higher order modes). This will be done by imaging heat patterns on the ETM surface. The thermoelastic deformations created on the mirror surface introduces phase shifts to the cavity modes. The green ALS system will be used to mode scan the cavity continuously. A feedback control system will actively correct for the frequency shifts based on the cavity mode scan information.

The lessons learned from this exercise will help in designing/implementing a similar kind of system for the folding mirrors in the signal recycling cavity.

System Overview

CTD.pdf

alt text

Description

The PSL laser is locked to the arm cavity using the PDH error signal. The green laser is injected from the ETM side of the arm. The relative phase between the two lasers is kept constant using a phase-locked-loop (PLL) servo. The transmitted end-green from the arm interferes with the frequency-doubled PSL and produces a beatnote.

Taking into account the following:

  1. The amplitude of the beatnote depends on the intensity of the transmitted green.
  2. Changing the frequency of the end-green laser (using the PLL local oscillator) will affect it's resonance conditions in the arm cavity and excite the various transverse modes.
  3. The frequencies at which the various transverse mode resonances occur depend on the spatial inhomogeneities on the mirror surface.

we can conclude that the amplitude of the beatnote as a function of the end-green laser frequency (or the local oscillator frequency) will hold the information about the cavity resonance frequencies and hence the effect of the mirror distortions created by various heat patterns can be mapped.

Simulation/Modelling

  1. Using SIS find the resonance frequencies of the various transverse modes: Using the phase map measurements made for the ITM and ETM, we will estimate the modal content of the arm cavity.
  2. COMSOL model various heat patterns on the ETM : Model thermal deformations on the ETM: core heating, ring heating, core+ring heating for various pixel sizes and various deformation depths on the mirror and generate phase maps.
  3. Analyze the effect of deformed mirror cavity and analyze the cavity fields using SIS.

Design and construction

  1. Heater array
  2. Heater electronics
  3. Telescope components
  4. Apertures
  5. PLL for green laser
  6. Inversion matrix
  7. Front ends

Tasks/Timeline

Advanced_Techniques/Adaptive_Thermal_Compensation (last edited 2013-11-16 13:50:04 by ManasadevithirugnanasambandamATligoDOTorg)