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Introduction to Optomechanics
Klemens Hammerer
IMPRS Lecture Week – Mardorf -- 19
Centre for Quantum Engineering and Space-Time Research
Leibniz University Hannover Institute for Theoretical Physics
Institute for Gravitational Physics (AEI)
Optomechanics • Cavity Optomechanics: Mechanical degree of freedom coupled to a cavity mode
thermal force
radiation pressure force
Can be used to cool the mirror:
Mean energy in thermal equilibrium:
“Quantum Optomechanics”
Can it be used to observe quantum effects with macroscopic systems?
Optomechanical Systems
LIGO – Laser Interferometer Gravitational Wave Observatory
D. Bowmeester, Santa Barbara/Leiden
Optomechanical Systems
Aspelmeyer (Vienna) Heidmann (Paris) Bouwmeester (St Barbara, Leiden)
Kippenberg (MPQ) Weig (LMU) Vahala (Caltech) Bowen (UQ)
Harris (Yale) Kimble (Caltech) Treutlein (Basel)
Micromembranes Micromirrors Microtoroids
Optomechanical Systems
Optomechanical Crystals
Painter (Caltech) Tang (Yale)
Optomechanics with BEC
Esslinger (Caltech) Stamper-Kurn (Berkeley)
Theory: Chang (Caltech) Romero-Isart (MPQ, ICFO) Experiment: Raizen (Austin)
Levitated Nanoobjects
Mechanical Systems Coupled to Light
Quantum Optomechanics M. Aspelmeyer, F. Marquardt, T. Kippenberg, RMP, arXiv:1303.0733 Macroscopic Quantum Mechanics: Theory and Experimental Concepts of Optomechanics Y. Chen arXiv:1302.1924
Quantum MECHANICAL Tests of the Superposition Principle
Marshall Bouwmeester Penrose PRL 2003
Quantum Mechanical Tests of the Superposition Principle
• “Ramsey – Approach”
• in matter wave interferometry
Evolution: Schrödinger Equ. & ?? Create superposition Measure
K Hornberger, S Gerlich, P Haslinger, S Nimmrichter, M Arndt RMP 84, 157 (2012)
Quantum Mechanical Tests of the Superposition Principle
• “Ramsey – Approach”
• in matter wave interferometry
Create superposition Measure
H Müntinga W Schleich E Rasel et al. PRL 110 093602 (2013)
Evolution: Schrödinger Equ. & ??
Quantum Mechanical Tests of the Superposition Principle
• “Ramsey – Approach”
• in optomechanics with nanospheres
Create superposition Measure
Romero-Isart et al. PRL 107, 020405 (2011)
Evolution: Schrödinger Equ. & ??
Quantum Mechanical Tests of the Superposition Principle
• Tests based on Continuous Measurements
• idea: – use continuous (precision) measurement to simultaneously prepare and measure
superposition states
– compare predictions according to (stochastic) Schrödinger equation with prediction from (Schrödinger equation & nonstandard model)
• goal: create and monitor pure quantum states (superposition states) of mechanical oscillators via continuous measurements
Macroscopic Quantum Mechanics: Theory and Experimental Concepts of Optomechanics
Y. Chen, arXiv:1302.1924
This talk
• Quantum Nondemolition Measurements of Mechanical Oscillators
• Continuous Measurement: measurement sensitivity & purity of conditional quantum state
• Quantum control via time continuous teleportation
tomorrow’s talk: • Nonclassical superposition states via nonlinear dynamics
• Quantum control of optomechanical systems via coupling to atomic systems
Quantum Description
• Mechanical oscillator creation/annihilation operator Hamiltonian quadrature operators physical position and momentum
• Cavity creation/annihilation operator Hamiltonian cavity frequency Length depends on mirror
position!
Quantum Description
• cavity frequency for moving mirror
• Optomechanical Hamiltonian
• Coupling rate in a Fabry-Perot microcavity
for 1ng and 1MHz oscillator
Equations of motion
• Hamiltonian
• Equations of motion cavity slowly varying variable
decay drive vacuum noise
cavity resonance
laser detuning from cavity resonance
Equations of motion
• Hamiltonian
• Equations of motion cavity mechanical oscillator
decay drive vacuum noise
decay thermal force
cavity resonance
Equations of motion
• Quantum equations of motion
• Classical equations of motion
no vacuum fluctuations
classical random force
Equations of motion
• Classical equations of motion at zero temperature: (deterministic)
Equations describe nonlinear, highly nontrivial physics: multistability, self induced oscillations, chaos… Assume stable steady state solution exist with mean values • We want to analyze the quantum dynamics around these mean values due to
classical random forces and quantum noise on mirror and cavity: Introduce fluctuation operators:
no classical random force
F. Marquardt, M. Ludwig
Equations of motion
• Fluctuations evolve according to
coupling strength of order:
for large intracavity amplitude drop small, nonlinear terms
Equations of motion
• Quantum fluctuations evolve according to linearized equations of motion
• Classical description: replace operators by C-numbers, drop vacuum noise
Equations of motion
• Quantum fluctuations evolve according to linearized equations of motion
• Equations of motion in terms of quadratures:
Equations of motion
• Quantum fluctuations evolve according to linearized equations of motion
• Equations of motion in terms of amplitude (creation/annihilation) operators:
Corresponds to effective optomechanical interaction Hamiltonian
RWA for noise: Valid for high Q Large T
compare to:
Radiation Pressure Interactions in Optomechanics
• (linearized) radiation pressure interaction in optomechanical systems
Squeezing via Quantum Non Demolition Measurement
in
Squeezing via Quantum Non Demolition Measurement
out in
Squeezing via Quantum Non Demolition Measurement
squeezed state!
conditioned on measurement
out in final
Squeezing via Quantum Non Demolition Measurement
• QND Hamiltonian
• Heisenberg picture
• conditional atomic variance
projection noise level
KH, A.S. Sorensen, E.S. Polzik, RMP. 82, 1041 (2010);
QND Measurement with Short Pulses
• linearized radiation pressure interaction for short pulses
• relevant decoherence rate of oscillator requires
– short pulses compatible with cavity – optimization of pulse profile – matching of LO profile to compensate
for pulse distortion – good cavity design…
M. Vanner et al. PNAS 108, 16182 (2011)
Mechanical Squeezing via QND Measurement
• Application: Cooling via successive QND measurements
• Application: Improved position/force sensing in pulsed or stroboscopic measurements
1st measurement 2nd measurement free evolution for
quarter period
Braginsky, Khalili…
M. Vanner, KH, et al. PNAS 108, 16182 (2011)
Experiment with musec pulses: M. Vanner et al. quant-ph/1211.7036
Continuous Measurement and Back Action
• Full dynamics is not of QND type
• cavity phase quadrate reads out position position evolves freely momentum couples to amplitude quadrature (radiation pressure) Amplitude noise couples via mechanics into phase quadrature: back action of light
+ cavity decay + vacuum noise
+ decay + thermal noise
Continuous Measurement Sensitivity
• phase quadrature in frequency domain
• noise spectral density referred to signal strength on resonance :
shot noise (phase noise)
back action noise (amplitude noise)
signal
…mechanical susceptibility
sensitivity
Continuous Measurement Sensitivity
• sensitivity
• standard quantum limit: shot noise = back action noise achieved for power such that
• back action larger than thermal noise achieved for power such that “strong optomechanical cooperativity”
thermal noise
~ Power se
nsiti
vity
Introduction to Quantum Noise, Measurement and Amplification Clerk, et al, RMP 82, 1155 (2010)
power
Strong Optomechanical Cooperativity
• Back action noise recently observed with micromechanical oscillators for the first time
• optomechanical ground state cooling also requires
Purdy, Peterson, Regal, Science 339, 801 (2013) [observed before with atomic oscillators Murch, Stamper-Kurn, Nat. Phys. 4, 561 (2008)]
Chan, et al., Nature 478, 89 (2011). Teufel, et al., Nature 475, 359 (2011).
Marquardt, Wilson-Rae
Strong Optomechanical Cooperativity
• Back action noise recently observed with micromechanical oscillators for the first time
• optomechanical cooperativity per single photon
(linearized vs single photon coupling )
M. Aspelmeyer, F. Marquardt, T. Kippenberg, RMP, arXiv:1303.0733
Purdy, Peterson, Regal, Science 339, 801 (2013) [observed before with atomic oscillators Murch, Stamper-Kurn, Nat. Phys. 4, 561 (2008)]
Conditional Quantum State
• Conditional quantum state according to stochastic master equation solution: Monte Carlo
• For linearized interaction and homodyne detection of light: Gaussian states and dynamics Stochastic Master Equation is equivalent to
– stochastic evolution of first moments
– deterministic evolution of second moments
Quantum Measurement and Control (2009) Wiseman, Milburn
unconditional dynamics conditional dynamics
Conditional Quantum State
• covariance matrix obeys Ricatti equation:
• stochastic (but known) mean values and deterministic covariance matrix fully determine quantum state, e.g. Wigner function etc purity of state uncertainty product
drift matrix diffusion matrix measurement term (nonlinear!)
uncondtional dynamics conditional dynamics
Belavkin et al, arXiv:0506018 Genoni et al., PRA 87 042333 (2013)
Vasilyev, Muschik, KH, PRA, arXiv:1303.5888
Quantum Optics in Phase Space W. Schleich
pure state! even for
Continuous Preparation and Monitoring of Pure Quantum States
• the conditional state is pure, Gaussian
• position and momentum are effectively probed with equal sensitivity if in this case the conditional quantum state will be a coherent state
• a squeezed state is generated if per single photon
arXiv:1303.0733
Universal Quantum Control via Measurement and Feedback
• idea: (superposition) state engineering via continuous quantum teleportation
• drive optomechanical system on upper sideband entangling interaction between light & oscillator
• perform Bell measurement on light
• linear feedback transfers quantum statistics of light on oscillator: non-Gaussian statistics of light generates non-Gaussian state of oscillator pulsed teleportation protocols: (here: cw!)
Romero-Isart, Pflanzer, Cirac , PRA 83, 013803 (2011) Hofer et al PRA 84, 052327 (2011)
Continuous Bell measurement with Gaussian Input Field
• linear interaction of arbitrary system with light field
• conditional master equation for system under continuous Bell measurement
• linear feedback with “forces”
• unconditional feedback master equation
measurement terms depend on
Hofer, Vasilyev, Aspelmeyer, KH, arXiv:1303.4976
mechanical squeezing
Continuous Quantum Teleportation
• select an entangling interaction by tuning to the upper sideband
• feedback master equation (ideally) with jump operator such that
• including thermal noise & counterrotating terms:
Hofer, Vasilyev, Aspelmeyer, KH, arXiv:1303.4976
i.e.
input squeezing - 6dB
Continuous Quantum Teleportation & Entanglement Swapping
• more general (non Gaussian) states: use field emitted from a second, source system and transfer to target system field emitted by an cavity QED is a (continuos) Matrix Product State of the contiunuous 1D EM field:
• if both systems have an entangling interaction with light: time continuous entanglement swapping generates EPR state of oscillators generates entangled state of micromechanical oscillators in steady state
• entangled states with EPR squeezing superposition size scaling as
source
target
Barrett, KH et al. PRL 110, 090501 (2013)
Hofer, Vasilyev, Aspelmeyer, KH, arXiv:1303.4976
Continuous Quantum Teleportation & Entanglement Swapping
• can also be applied to spins for correct feedback steady state is
• including tramsmision losses
Continuous Quantum Teleportation & Entanglement Swapping
• setup is similar to a GWD Michelson interferometer: entangled state of mirror test masses predicted in
• continuous test of quantum mechanics with macroscopic objects:
– parametrize how the dynamics of the object
would deviate from standard quantum mechanics (for a given collapse model)
– monitor true dynamics and exclude parameters
Müller-Ebhardt, Rehbein, Schnabel, Danzmann, Chen, PRL 100 013601 (2008) Miao, PRA 81 012114 (2010)
Macroscopic Quantum Mechanics: Theory and Experimental Concepts of Optomechanics Y. Chen, arXiv:1302.1924
Requirements & Summary
• Experiments need to have a strong optomechanical cooperativity
• the conditional state predicted by the stochastic master equation has to be reconstructed from measured photocurrent via Kalman/Wiener–filtering applied to optomechanical system in free space
• continuous measurement at the quantum limit is
– getting feasible in state of the art optomechanical systems
– toolbox for universal quantum state engineering
– detector of non-standard physics based on macroscopic superposition states
(alternative to Ramsey-like approaches)
Furusawa et al 1305.0066
Gaussian States and Interactions
• The optomechanical toolbox
– linearized interaction:
– homodyne detection of light: measurement of
– injection of squeezed, coherent (Gaussian) light
preserves Gaussian character of states.
• We can select the dominant interaction by choosing the detuning
red
cooling, state exchange
blue
entanglement
resonant
displacement detection QND measurement
Non Gaussian States and Interactions
• How can we leave the Gaussian world?
• The Non Gaussian toolbox
– inject Non-Gaussian light
– photon counting (instead of homodyne detection)
– non-bilinear Hamiltonians
radiation pressure interaction is fundamentally nonlinear, but notoriously weak:
F.Khalili, S.Danilishin, H.Miao, H.Muller-Ebhardt, H.Yang, Y.Chen, arxiv:1001.3738 U. Akram, N. Kiesel, M. Aspelmeyer, G. J. Milburn, arxiv:1002.1517
can be engineered with micromembranes
Marshall, C.Simon, R.Penrose, D.Bouwmeester, PRL 91, 130401 (2003)
Quantum Optomechanics
• Radiation pressure Hamiltonian is nonlinear For sufficiently strong coupling per single photon g0 the dynamics will be Non-Gaussian.
• Do Non-Gaussian features persist in steady state? Negative Wigner Functions? Master Equation
thermal contact
cavity decay driving field
Steady State
• Solve master equation for steady state for (rather extreme) parameters
• Wigner function
detuning
Qian, Clerk, KH, Marquardt PRL 109, 253601, 2012
A
Steady State
• Solve master equation for steady state for (rather extreme) parameters
• Wigner function
detuning
Qian, Clerk, KH, Marquardt PRL 109, 253601, 2012
B
Steady State
• Solve master equation for steady state for (rather extreme) parameters
• Wigner function
detuning
C
Qian, Clerk, KH, Marquardt PRL 109, 253601, 2012
Steady State
• Solve master equation for steady state for (rather extreme) parameters
• Wigner function
detuning
Qian, Clerk, KH, Marquardt PRL 109, 253601, 2012
D
Steady State
• Wigner functions
• Phonon number and Fano factor Negative Wigner
functions
cooling heating
Qian, Clerk, KH, Marquardt PRL 109, 253601, 2012
Limit Cycles
• Quantum equations of motion
• limit cycles are classical nonlinear dynamics
+ noise
+ noise
Marquardt, Ludwig… RMP, arXiv:1303.0733
Limit Cycles
• Classical equations of motion
• slowly varying amplitude solution intensity
Marquardt, Ludwig… RMP, arXiv:1303.0733
off resonant terms
Limit Cycles
• mechanical amplitude
• nonlinear optical damping
o no limit cycles for Δ > 0 ! o negative Wigner functions?
Marquardt, Ludwig… RMP, arXiv:1303.0733
Conditional state
• Conditional state as calculated from one trajectory of Monte-Carlo simulation
Loerch, KH, in prep
Albert Einstein Institute
Institute for Theoretical Physics
Centre for Quantum Engineering and Space-
Time Research Group: Sebastian Hofer Denis Vasilyev Niels Loerch Sergey Tarabrin
Collaborators: M. Aspelmeyer & company M.S. Kim, G.J. Milburn, C. Brukner, I. Pikovski T. Osborne, S. Harrison, S. Barrett, T. Northup C. Muschik
Thank you!
Support through: DFG (QUEST), EC (MALICIA, iQUOEMS)
Winter School on Rydberg Physics and Quantum Information Obergurgl Feb 10-14 1013 www.rqi.uni-hannover.de
arXiv:1303.4976