Einstein gravitational wave Telescope Next steps: from technology reviews to detector design Andreas Freise for the ET WG3 working group 15.10.2009, 2nd general ET workshop, Erice
Jan 16, 2016
Einstein gravitational wave Telescope
Next steps: from technology reviews to
detector design
Andreas Freisefor the ET WG3 working group
15.10.2009, 2nd general ET workshop, Erice
A. Freise A Freise, 2nd general ET workshop 15/10/2009
Slide 2
What will ET look like?
How many interferometers per site?
Quantum noise reduction
Alternative topologies
Practical considerations
Sensitivity Studies
List of reviews/reports
Discussion of trade-off study
Overview
In the ET design study we are soon reaching the milestones `Evaluation of XXX technique’ and then start the trade-off activity.
A. Freise A Freise, 2nd general ET workshop 15/10/2009
Slide 3
Detector Geometry
What will be the shape of ET?
A. Freise A Freise, 2nd general ET workshop 15/10/2009
Slide 4
Multiple Interferometers: the Triangle
Both solutions have an integrated tunnel length of 30 km, they can resolve both GW polarisations, feature redundant interferometers and have equivalent sensitivity.
The triangle reduces the number of end stations and the enclosed area!
[P Jaranowski et al, Phys Rev D 58 1998]
A. Freise A Freise, 2nd general ET workshop 15/10/2009
Slide 5
Geometry/TopologyHow Many Interferometers Arms per
Tunnel?
Picture by Jason Bacon used under a Creative Commons License
Rüdiger, Aspen 2007
A. Freise A Freise, 2nd general ET workshop 15/10/2009
Slide 6
Today's Michelsons in a Triangle
[S Hild]
A. Freise A Freise, 2nd general ET workshop 15/10/2009
Slide 7
Multiple Interferometers: a Xylophone
Low power (no thermal effects), cooled, long suspensions
High power, squeezing, LG modes, room temperature, `normal' suspensions
Maybe we can reach the target sensitivity easier by splitting the frequency range?
[S Hild et al, arXiv:0906.2655]
A. Freise A Freise, 2nd general ET workshop 15/10/2009
Slide 8
TopologyMain Driver: Reduction of Quantum Noise
[S. Hild et al, arxiv:0810.0604]
A. Freise A Freise, 2nd general ET workshop 15/10/2009
Slide 9
Quantum Noise Reduction
Optimised SR
[H. Rehbein und H. Mueller-Ebhardt, ET note ET-010-09 2009]
[S Chelkowski]
A. Freise A Freise, 2nd general ET workshop 15/10/2009
Slide 10
Quantum Noise Reduction
10dB frequency-dependentsqueezing
[H. Rehbein und H. Mueller-Ebhardt, ET note ET-010-09 2009]
[S Chelkowski]
A. Freise A Freise, 2nd general ET workshop 15/10/2009
Slide 11
Quantum Noise Reduction
Variational output and10 dB squeezing
[H. Rehbein und H. Mueller-Ebhardt, ET note ET-010-09 2009]
[S Chelkowski]
A. Freise A Freise, 2nd general ET workshop 15/10/2009
Slide 12
Quantum Noise Reduction
Sagnac with SR, variationaloutput and 10dB squeezing
[H. Rehbein und H. Mueller-Ebhardt, ET note ET-010-09 2009]
[S Chelkowski]
A. Freise A Freise, 2nd general ET workshop 15/10/2009
Slide 13
Several QND topologies seem feasible: Micheslon with SR, variational output, squeezing Sagnac or Mach Zehnder Interferometer with SR, … Optical bars, optical levers, double optical spring, …
All can be build using the L-shape form factor!
QND Topologies
Optical Lever
A. Freise A Freise, 2nd general ET workshop 15/10/2009
Slide 14
Practical considerations
New technologies introducenew technical noises which might not be thought of in the first conceptual designs and have to be studied carefully.
Two examples …
A. Freise A Freise, 2nd general ET workshop 15/10/2009
Slide 15
Additional noise couplings: For Example: The Sagnac topology
Non-zero area Sagnac Near-zero area Sagnac
A. Freise A Freise, 2nd general ET workshop 15/10/2009
Slide 16
Sagnac effect in ET
Analysis involves two effects
1.Static effects due to Earth’s rotation
Much more sensitive than current Laser gyros
2.Noise couplings• Frequency noise• Seismic noise• Beam jitter noise
[S. Chelkowski, talk at WP3 meeting 01/2009]
A. Freise A Freise, 2nd general ET workshop 15/10/2009
Slide 17
Example: Seismic noise
Non-zero area Sagnac requirements on lateral mirror motion:
Zero area Sagnac requirements:
[S. Chelkowski, talk at WP3 meeting 01/2009]
A. Freise A Freise, 2nd general ET workshop 15/10/2009
Slide 18
Practical Considerations: Example, Beam Size
A. Freise A Freise, 2nd general ET workshop 15/10/2009
Slide 19
Interferometer topology selection will be driven by the quantum noise reduction scheme
All topologies can be build as an L-shape
We can assemble 3 L-shapes efficiently as a triangle
Multiple interferometers per site are beneficial for the sensitivity, yield redundancy and robust data analysis methods (null streams)
Technical details and noise couplings need to be investigated further before a topology can be selected
Summary of the overview
A. Freise A Freise, 2nd general ET workshop 15/10/2009
Slide 20
Sensitivity Studies
One of the WG3 tasks is to provide official sensitivity curves
See main ET webpage
Please use these for your studies and ask (email) if you have
questions!
A. Freise A Freise, 2nd general ET workshop 15/10/2009
Slide 21
Sensitivity Studies
The available data (currently internal to ET science team but should be opened): Plot as pdf file Data as .txt and .mat file Polynomial fit (coming soon)
These sensitivities are: Documented, version controlled, centrally stored data Generally discussed and accepted sensitivity examples
for activities such as trade-off studies These sensitivities are NOT:
Representing proposed ET detector options Always achievable using known technologies Taking into account detector geometry (triangle,
network effects,…)
A. Freise A Freise, 2nd general ET workshop 15/10/2009
Slide 22
Technology review
Technology review documented in internal notes and papers: Quantum noise reduction Detector geometry and topology High power lasers Parametric instabilities Diffractive interferometers Squeezed light Displacement noise free interferometry
A. Freise A Freise, 2nd general ET workshop 15/10/2009
Slide 23
Trade-off studies
Problem: New technology ideas are cheap, we have to stop
evaluating those at some point Everything depends on everything (e.g. thermal noise
on beam size, on free aperture, on tunnel size on available money): it is difficult to do trade-off studies with too many options
Proposal: Identify parameters/problems which can be separated,
such as the triangular shape from the QND topology For the rest, agree on one (maybe two) complete
design as reference and compute sensitivity, noise models, costs
Discussion now. Kick-off of dedicated activities in next WG3 meeting
A. Freise A Freise, 2nd general ET workshop 15/10/2009
Slide 24
…end
A. Freise A Freise, 2nd general ET workshop 15/10/2009
Slide 25
LL
45°
Fully resolve polarizations
5 end caverns
4×L long tunnels
45° stream generated by virtual interferometry
Null stream
Redundancy
7 end caverns
6×L long tunnels
60°
L’=L/sin(60°)=1.15×L
Fully resolve polarizations by virtual interferometry
Null stream
Redundancy
3 end caverns
3.45×L long tunnels L
Equivalent to
[Ruediger et al (1985), Freise et al, Class. Quantum Grav. 26 (2009)]