advanced virgo optical design: arm cavities with adjustable finesse
DESCRIPTION
Advanced Virgo optical design: Arm cavities with adjustable Finesse. Stefan Hild , Andreas Freise, Simon Chelkowski University of Birmingham Roland Schilling, Jerome Degallaix AEI Hannover Maddalena Mantovani EGO, Cascina March 2008, GEO-simulation WS. Overview. - PowerPoint PPT PresentationTRANSCRIPT
Stefan Hild, Andreas Freise, Simon ChelkowskiUniversity of Birmingham
Roland Schilling, Jerome DegallaixAEI Hannover
Maddalena MantovaniEGO, Cascina
March 2008, GEO-simulation WS
Advanced Virgo optical design:Arm cavities with adjustable Finesse
Stefan Hild GEO Simulation WS, March 2008 Slide 2
Overview
Requirements for Advanced Virgo arm cavities: Etalon effect vs wedges.
New concept for advanced GW detectors that combines wedges and etalon effect.
Performance of an ideal etalon
Example of optical system design: Influence of etalon imperfections Numerical simulations Analytical approximations Influence onto alignment signals Higher-order mode buildup
Stefan Hild GEO Simulation WS, March 2008 Slide 3
Motivation: Input mirror without wedge
Initial Virgo has no wedges in the input mirrors
The etalon effect could be used for adjusting the cavity finesse (compensating for differential losses)
If etalon effect is not controlled it might cause problems
Stefan Hild GEO Simulation WS, March 2008 Slide 4
Motivation: Input mirror featuring a wedge
Used by initial LIGO
Reflected beams from AR coating can be separated from main beam => pick-off beams provide additional ports for generation of control signals.
No etalon effect available.
Stefan Hild GEO Simulation WS, March 2008 Slide 5
What to use for Advanced VIRGO?Etalon or Wedges ??
For AdV possibility to adjust cavity finesse gets more important (higher cavity finesse, DC-readout).
For AdV possibility to create more and better control signals seem desirable.
Is there a possibilty to have both for Advanced Virgo ??
Stefan Hild GEO Simulation WS, March 2008 Slide 6
Advanced Virgo: symmetric beam geometry
Increase beam size at mirrors => reduce thermal noise contribution of the test masses.
Move beam waist away from input test mass
Is there still an etalon effect in the (flat/curved) input mirror ?
Stefan Hild GEO Simulation WS, March 2008 Slide 7
Etalon effect:flat/flat vs curved/flat
Flat/flat etalon: Perfect overlap of wavefronts
Curved/flat etalon: Mismatch of wavefront curvature Fortunately mirror curvature of a few km
is not so far from “flat”. Simulations show: a reduced etalon effect
in curved/flat input mirror is still present
Stefan Hild GEO Simulation WS, March 2008 Slide 8
Etalon effect:flat/flat vs curved/flat
Flat/flat etalon: Perfect overlap of wavefronts
Curved/flat etalon: Mismatch of wavefront curvature Fortunately mirror curvature of a few km
are not so far “flat”. Simulations show: a reduced etalon effect
in curved/flat input mirror is still presentStill
we have to choose:
either wegde in input m
irror (P
ick-off beams available)
or no wedge in input mirro
r (Etalon effect available)
Stefan Hild GEO Simulation WS, March 2008 Slide 9
Overview
Requirements for Advanced Virgo arm cavities: Etalon effect vs wedges.
New concept for advanced GW detectors that combines wedges and etalon effect.
Performance of an ideal etalon
Example of optical system design: Influence of etalon imperfections Numerical simulations Analytical approximations Influence onto alignment signals Higher order mode buildup
Stefan Hild GEO Simulation WS, March 2008 Slide 10
IDEA: Wedges at input mirrors and etalon effect at end mirrors
Wedge at input mirrors: Allows for additional pick-off beams (Concentrate on compensating thermal lensing in input mirror)
Use etalon effect at end test mass Replace AR-coating by a coating of about 10% reflectivity. Ideally use a curved back surface (same curvature as front). End mirror behaves similarly to flat/flat etalon.
Stefan Hild GEO Simulation WS, March 2008 Slide 11
Now let’s have a look
at numbers for
Advanced Virgo
Stefan Hild GEO Simulation WS, March 2008 Slide 12
Overview
Requirements for Advanced Virgo arm cavities: Etalon effect vs wedges.
New concept for advanced GW detectors that combines wedges and etalon effect.
Performance of an ideal etalon
Example of optical system design: Influence of etalon imperfections Numerical simulations Analytical approximations Influence onto alignment signals Higher order mode buildup
Stefan Hild GEO Simulation WS, March 2008 Slide 13
Starting with a single AdV arm cavity
Using a single AdV arm cavity (no IFO).
Parameters used:IM trans = 0.007IM loss = 50 ppmEM trans = 50 ppmEM loss = 50 ppmAR coatings = 0ppmIM curvature = 1910mEM curvature = 1910mInput = 1W
Figure of merrit = intra cavity power, i.e. loss compensation.
Parameters taken from these 2 documents:
Stefan Hild GEO Simulation WS, March 2008 Slide 14
Influence of losses inside the cavity
Imperfection of optics (surface + coatings) might cause different losses in the arm cavities := differential losses.
What are the expected differential losses of AdV ? 5ppm? 50ppm?
A differential loss of 15ppm corresponds to a change of 2W intra cavity power in this example.
Stefan Hild GEO Simulation WS, March 2008 Slide 15
End mirror as curved etalon (optimal solution)
Simulation done with Finesse.
Back surface of end mirror curved (1910m).
AR coating replaced by coating of 10% or 20% reflectivity.
R=0.1 allows adjustment range of 10W (65ppm)
R=0.2 allows adjustment range of 16W (95ppm)
Stefan Hild GEO Simulation WS, March 2008 Slide 16
Optimal solution: curved Etalon
Alternative figures of merrit: Transmittance of end mirror (etalon) Finesse of arm cavity
Stefan Hild GEO Simulation WS, March 2008 Slide 17
Etalon changes optical phase
When changing the etalon tuning the optical-phase changes as well. (noise!)
The two etalon surfaces build a compound mirror, whose apparent position depends on the etalon tuning.
Stefan Hild GEO Simulation WS, March 2008 Slide 18
Requirement for temperature stability of etalon substrate
Can calculate require-ment for temperature stability for Advanced Virgo etalon
Using ‘worst case’: 1.22pm/deg
dn/dT = 1.09e-5/K Substrate thickness =
10cm
Example @100Hz: 4e-11K/sqrt(Hz)
This requirement is still 2 orders of magnitude above (safer) than temperature stability required from dL/dT of the substrates.
Stefan Hild GEO Simulation WS, March 2008 Slide 19
Everything fine as long
Etalon matches the
specs…
… but what if not ??
=> need to check !!
Stefan Hild GEO Simulation WS, March 2008 Slide 20
Overview
Requirements for Advanced Virgo arm cavities: Etalon effect vs wedges.
New concept for advanced GW detectors that combines wedges and etalon effect.
Performance of an ideal etalon
Example of optical system design: Influence of etalon imperfections Numerical simulations Analytical approximations Influence onto alignment signals Higher order mode buildup
Stefan Hild GEO Simulation WS, March 2008 Slide 21
Optical design: Check system integrity for deviations from specs
A deviation in the reflectivity of the etalon coating: Only changes tuning range
(no problem)
A deviation in the relative misalignment (parallelism) and relative curvature of the two etalon surfaces: Imperfect wave front overlap… Reduces tuning range … Beam shape distortions …
Stefan Hild GEO Simulation WS, March 2008 Slide 22
FFT-simulation of a non-perfect etalon
Using R. Schilling’s WaveProp, (http://www.rzg.mpg.de/~ros/WaveProp/)
Parameters: Field: 256x256 Computing 3000 roundtrips End mirror front:
50ppm transmission R_c = 1910m
End mirror back: Varying three parameters Reflectance Misalignment (parallelism) Curvature
Stefan Hild GEO Simulation WS, March 2008 Slide 23
Analytic Approximations using Higher-Order Modes
For small misalignments the coupling coefficients knmnm can be approximated. The amount of light which remains in a TEM00 mode is given by:
(q is the Gaussian beam parameter of the light at the mirror)
Reflection at a (slightly) misaligned component can be characterised by scattering into higher order TEM modes
This model is valid for misalignments below half the diffraction angle (paraxial approximation)
The amplitude in the outgoing fields is given by coupling coefficients knmnm
Stefan Hild GEO Simulation WS, March 2008 Slide 24
Misalignment of etalon back surface
Strong influence of relative alignment of etalon surfaces.
Question: What accuracy can state of the art manufacturing provide?
Example: Initial Virgo input mirrors (flat/flat) = 1urad
Stefan Hild GEO Simulation WS, March 2008 Slide 25
Curvature deviation of etalon back surface
Curvature mismatch has only moderate influence to tuning range of the etalon.
Stefan Hild GEO Simulation WS, March 2008 Slide 26
!!! KEEP IN MIND !!!For this example…
Numerical simulations and analytical approximation: Can used to understand optics Are used to derive specifications Both do not necessarily represent the reality in all
cases
Optimal solution (if feasible): Test concept in a prototype experiment
Stefan Hild GEO Simulation WS, March 2008 Slide 27
Investigating alignment signals for Advanced Virgo with etalons
Aim: Checking influence of perfect and non-perfect etalon to alignment signals
Performed FINESSE simulation
Investigating Ward and Anderson techniques
Stefan Hild GEO Simulation WS, March 2008 Slide 28
Alignment signals for perfect etalon
Sig
nal i
n tr
ansm
issi
on:
An
der
son
tec
hniq
ue
Sig
nal i
n re
flect
ion:
War
d t
echn
ique
150 %variation
10 %variation
Stefan Hild GEO Simulation WS, March 2008 Slide 29
Non perfect etalon: TEM01-buildup in the arm cavity
Misalignment of etalon back surface induces 1st order modes inside the arm cavities.
TEM01 from etalon imperfection is negligible compared to misalignment of the whole end test mass.
Stefan Hild GEO Simulation WS, March 2008 Slide 30
Summary Advanced Virgo CAN feature
wedges in the input mirrors AND use the etalon effect at the end mirrors.
Proposed concept allows us to build ‘arm cavities with adjustable losses’.
A curved/curved etalon would be ideal.
Evaluated and quantified the influence of etalon imperfections using numerical simulations and analytical approximations (tuning range, alignment signals)
Stefan Hild GEO Simulation WS, March 2008 Slide 31
OutlookPotential issues to be investigated:
Need a control system for etalon tuning (error signal + actuator).
Need a value for the expected differential losses in Advanced Virgo in order to choose the reflectivity of the etalon.
More details can soon be found in …
Stefan Hild GEO Simulation WS, March 2008 Slide 32
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