Thermal noise and thermal deformations of mirrors

Slides:



Advertisements
Similar presentations
Lattice Dynamics related to movement of atoms
Advertisements

FINESSE FINESSE Frequency Domain Interferometer Simulation Versatile simulation software for user-defined interferometer topologies. Fast, easy to use.
Gravitational Wave Astronomy Dr. Giles Hammond Institute for Gravitational Research SUPA, University of Glasgow Universität Jena, August 2010.
LIGO-G v2 Form F v1 Advanced LIGO1 SCATTERED LIGHT CONTROL in ADVANCED LIGO Michael Smith LIGO Laboratory Caltech, Pasadena, CA.
Chapter 1 Electromagnetic Fields
Reciprocity relationships for gravitational-wave interferometers Yuri Levin (Monash University) 1. Example: creep noise 2. Formalism 3. Creep noise again.
So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures.
Tine Porenta Mentor: prof. dr. Slobodan Žumer Januar 2010.
Lattice Dynamics related to movement of atoms
Transportation of Ultra-Stable Light via Optical Fiber Emily Conant Bard College, California Institute of Technology Mentors: Evan Hall, Rana Adhikari,
Thermally Deformable Mirrors: a new Adaptive Optics scheme for Advanced Gravitational Wave Interferometers Marie Kasprzack Laboratoire de l’Accélérateur.
Crystal Lattice Vibrations: Phonons
TeV Particle Astrophysics August 2006 Caltech Australian National University Universitat Hannover/AEI LIGO Scientific Collaboration MIT Corbitt, Goda,
Jaypee Institute of Information Technology University, Jaypee Institute of Information Technology University,Noida Department of Physics and materials.
LIGO-G D 1 25-May-02 Advanced LIGO Suspension Model in Mathematica Gravitational Wave Advanced Detector Workshop Elba - May 2002 Mark Barton.
Substrate mechanical loss studies Sheila Rowan (Stanford University) for: LIGO Laboratory (Caltech, MIT, LLO, LHO) LSC Partners (University of Glasgow,
23/05/06VESF School1 Gravitational Wave Interferometry Jean-Yves Vinet ARTEMIS Observatoire de la Côte d’Azur Nice (France)
Supergranulation Waves in the Subsurface Shear Layer Cristina Green Alexander Kosovichev Stanford University.
Update to End to End LSST Science Simulation Garrett Jernigan and John Peterson December, 2004 Status of the Science End-to-End Simulator: 1. Sky Models.
Micro-Resistor Beam.
What happens to the current if we: 1. add a magnetic field, 2. have an oscillating E field (e.g. light), 3. have a thermal gradient H.
Abstract Although the sine-Gordon equation was originally obtained for the description of four wave-mixing in transmission geometry, it describes self-diffraction.
Chapters: 3and 4. THREE MAIN LIGHT MATTER INTERRACTION Absorption: converts radiative energy into internal energy Emission: converts internal energy into.
Linear optical properties of dielectrics
1 AdS/CFT Calculations of Parton Energy Loss Jorge Casalderrey-Solana Lawrence Berkeley National Lab. In collaboration with D. Teaney.
Transverse Momentum Broadening of a Fast Quark in a N=4 Yang Mills Plasma Jorge Casalderrey-Solana LBNL Work in collaboration with Derek Teany.
1 Reducing Thermoelastic Noise by Reshaping the Light Beams and Test Masses Research by Vladimir Braginsky, Sergey Strigin & Sergey Vyatchanin [MSU] Erika.
Opto-mechanics with a 50 ng membrane Henning Kaufer, A. Sawadsky, R. Moghadas Nia, D.Friedrich, T. Westphal, K. Yamamoto and R. Schnabel GWADW 2012,
Thermoelastic dissipation in inhomogeneous media: loss measurements and thermal noise in coated test masses Sheila Rowan, Marty Fejer and LSC Coating collaboration.
GWADW - La Biodola 20061/20 Underground reduction of Gravity Gradient Noise. Giancarlo Cella INFN sez. Pisa/Virgo GWADW – La Biodola 2006.
Presentation for chapters 5 and 6. LIST OF CONTENTS 1.Surfaces - Emission and Absorption 2.Surfaces - Reflection 3.Radiative Transfer in the Atmosphere-Ocean.
Lattice Dynamics related to movement of atoms
The importance of Coatings for Interferometric Gravitational Wave Observatories Riccardo DeSalvo for the Coating group
17/05/2010A. Rocchi - GWADW Kyoto2 Thermal effects: a brief introduction  In TM, optical power predominantly absorbed by the HR coating and converted.
Aspen Flat Beam Profile to Depress Thermal Noise J.Agresti, R. DeSalvo LIGO-G Z.
A. Freise1 Phase and alignment noise in grating interferometers Andreas Freise QND Meeting, Hannover
AdS/CFT “Applications” Jorge Casalderrey-Solana LBNL.
Some Ideas on Coatingless all-reflective ITF Adalberto Giazotto (*) INFN- Pisa (*) Work done in collaboration with G. Cella.
Instability of optical speckle patterns in cold atomic gases ? S.E. Skipetrov CNRS/Grenoble (Part of this.
Friedrich-Schiller-University Jena Institute of Solid State Physics – Low Temperature Physics Christian Schwarz 15 th September Genoa 1 Investigation.
Electrostatic field in dielectric media When a material has no free charge carriers or very few charge carriers, it is known as dielectric. For example.
The Interaction of Light and Matter: a and n
Raman Effect The Scattering of electromagnetic radiation by matter with a change of frequency.
AP Physics Review Jeopardy.
UPB / ETTI O.DROSU Electrical Engineering 2
Deep Chatterjee IISER Kolkata Mentors: Koji Arai; Matthew Abernathy
Peter Beyersdorf TAMA300 Results from the Stanford 10m all-reflective polarization Sagnac interferometer Peter Beyersdorf TAMA300.
Chapter 1 Electromagnetic Fields
Current and future ground-based gravitational-wave detectors
Mechanical Loss in Silica substrates
Dynamical correlations & transport coefficients
Thermal noise calculations for cryogenic optics
Mechanics of Solids I Energy Method.
Review of basic EM concepts
S. Rowan, M. Fejer, E. Gustafson, R. Route, G. Zeltzer
ENE 325 Electromagnetic Fields and Waves
Homodyne or heterodyne Readout for Advanced LIGO?
Advanced LIGO Quantum noise everywhere
Quantum Optics and Macroscopic Quantum Measurement
Maxwell’s Equations and Electromagnetic Waves
Dynamical correlations & transport coefficients
Light Scattering Spectroscopies
Stability and Dynamics in Fabry-Perot cavities due to combined photothermal and radiation-pressure effects Francesco Marino1,4, Maurizio De Rosa2, Francesco.
Thermodynamic Energy Balances in Solids
Review of basic EM concepts
T3 DEVELOPMENT OF SELECTIVE READOUT SCHEMES
Advanced Optical Sensing
N.Kukhtarev, T.Kukhtareva, P.Land, J.H. Caulfield, and J.Wang
Thermo-mechanics J. Cugnoni, LMAF / EPFL 2012.
Presentation transcript:

Thermal noise and thermal deformations of mirrors Yuri Levin, Monash Fluctuation-dissipation theorem Thermo-mechanical noise; reciprocity relations; general optical readouts; gratings Thermal deformations of mirrors 4. Thermo-refractive noise; standing wave 5. Thermo-chemical noise

1. Fluctuation-dissipation theorem Callen & Welton 1951, Kubo+many others Macroscopic degree of freedom Microscopic degrees of freedom Coupling

1. Fluctuation-dissipation theorem Callen & Welton 1951, Kubo+many others dissipation Macroscopic degree of freedom Microscopic degrees of freedom Coupling

1. Fluctuation-dissipation theorem Callen & Welton 1951, Kubo+many others dissipation Macroscopic degree of freedom Microscopic degrees of freedom Coupling Thermal motion fluctuations

1. Fluctuation-dissipation theorem Callen & Welton 1951, Kubo+many others dissipation Macroscopic degree of freedom Microscopic degrees of freedom Coupling Thermal motion fluctuations

2. Thermo-mechanical noise Callen and Welton 51, Levin 98 Readout variable: Interaction 1. oscillating pressure 2. Compute/measure dissipated power 3.

Two questions: 1. How does one figure out the readout variable in a general opto-mechanical set up? Optical reciprocity Heinert + 13 2. If the dissipation is local, how does the local random stress communicate to macroscopic surface displacement? How do we quantify this communication? dissipation Elastodynamic reciprocity fluctuation

Reciprocity relations Normal computational scheme Compute all consequences of the perturbation Extract the quantity you want to know Using reciprocity relationship Identify the quantity you want to know Solve the reverse problem (often easier). Construct a map between perturbations and readout quantity. Do it once!

Opto-mechanical readout variables Question: how does the mode frequency change when dielectric interface moves? Adiabatic theorem for oscillators so Mode energy Interface displacement Optical pressure on the interface Useful for thermal noise calculations from e.g. gratings (cf. Heinert et al. 2013; correction ~25%)

Opto-mechanical readout variables Linear optical readout, e.g. phase measurements Carrier light + Perturbation Phase Form-factor

Part 6: opto-mechanics with interfaces Linear optical readout, e.g. phase measurements Photo-diode Phase Form-factor

Opto-mechanical readout variable 1. Generate imaginary beam with oscillating dipoles Photo-diode 2. Calculate induced optical pressure on the interface 3. The phase

3. Thermal deformations of mirrors Not an issue for advanced KAGRA. Major issue for LIGO & Virgo High-temperature region cf. Hello & Vinet 1990 New coordinates Basis functions: Zernike polynomials, Hermite-Gauss functions Treat this as a readout variable

Elastodynamic reciprocity relations form-factor Force density Readout variable displacement form-factor

Elastodynamic reciprocity relations form-factor Force density is invariant with respect to interchange of and Readout variable displacement form-factor

How to calculate Apply pressure to the mirror face King, Levin, Ottaway, Veitch to be submitted. Apply pressure to the mirror face Calculate trace of the induced deformation tensor Have to do it only once! Calculate the thermal deformation Young modulus Thermal expansion Temperature perturbation

Computation of scattering coefficients imaginary pressure Impressive Agreement!

Thermo-refractive noise Braginsky, Gorodetsky, & Vyatchanin 2000 medium Index of refraction: beam 3 phaseshift temperature fluctuation intensity readout variable

Thermo-refractive noise Levin 2008 Readout variable: 1. oscillating entropy injection 2. Compute/measure dissipated power, e.g. 3.

Standing waves, GEO600 beamsplitter Image credit: Prof. Nollert effective ineffective Benthem & Levin 2009

Thermochemical and Carrier-Density Noise Intensity profile effective ineffective Thermochemical noise: due to chemical impurities Benthem & Levin 2009 Carrier-density noise: due to semiconductor charge carriers Heinert et al. submitted Both seem to not threaten GW interferometry, but one has to be vigilant, especially for the ET

Conclusions Linear systems (elastic, optomechanical) feature reciprocity relations They give direct computation of readout variable non-trivial geometries, and they allow fast computations of thermal distortions and scattering coefficients Vigilance for new types of thermal noise