all you need is squeezing! - fuw.edu.pl

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All you need is squeezing! optimal schemes for realistic quantum metrology R. Demkowicz-Dobrzański 1 , K. Banaszek 1 , J. Kołodyński 1 , M. Jarzyna 1 , M. Guta 2 , R. Schnabel 3 1 Faculty of Physics, Warsaw University, Poland 2 School of Mathematical Sciences, University of Nottingham, United Kingdom 3 Max-Planck-Institut fur Gravitationsphysik, Hannover, Germany

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Page 1: All you need is squeezing! - fuw.edu.pl

All you need is squeezing! optimal schemes for realistic quantum metrology

R. Demkowicz-Dobrzański1, K. Banaszek1, J. Kołodyński1, M. Jarzyna1, M. Guta2, R. Schnabel3

1Faculty of Physics, Warsaw University, Poland 2 School of Mathematical Sciences, University of Nottingham, United Kingdom

3 Max-Planck-Institut fur Gravitationsphysik, Hannover, Germany

Page 2: All you need is squeezing! - fuw.edu.pl

,,Classical’’ interferometry

the best estimator

Page 3: All you need is squeezing! - fuw.edu.pl

Poisson statistics

classical (standard) scaling

„Classical” interferometry

the best estimator

Each photon interferes only with itself!

Page 4: All you need is squeezing! - fuw.edu.pl

Quantum enhancement thanks to the squeezed states

Coherent state

Precision enhancement thanks to subpoissonian fluctuations of n1- n2!

simple estimator based on n1- n2:

Squeezed vacuum

Page 5: All you need is squeezing! - fuw.edu.pl

Optimal strategy?

General two-mode N photon state

general quantum measurement

estimator

single parameter quantum channel estimation

Page 6: All you need is squeezing! - fuw.edu.pl

Quantum Cramer-Rao bound and the optimal N photon state

estimator

Heisenberg limit NOON states

1

2

Good estimation possible only for states with high ∆n1

Page 7: All you need is squeezing! - fuw.edu.pl

Other „Heisenberg limits”

estimator

1

2

In a Bayesian approach

no a priori knowledge about the phase

Optimal state:

D. W. Berry and H. M. Wiseman, Phys. Rev. Lett. 85, 5098 (2000).

Covariant measurements are optimal:

Page 8: All you need is squeezing! - fuw.edu.pl

Other „Heisenberg limits”

estimator

1

2

For states with indefinite photon number

So in principle we can have

H. Hoffman, Phys. Rev. A 79, 033822 (2009) And beat the ``naive’’ Heisenberg limit:

P.M. Anisimov, et al., Phys. Rev. Lett. 104, 103602 (2010) Sub Heisenberg strategies are ineffective V. Giovannetti, L. Maccone, Phys. Rev. Lett 108, 210404 (2012)

Page 9: All you need is squeezing! - fuw.edu.pl

Complicated….

How to saturate the bounds?

a priori knowledge? beating Heisenberg limit?

Page 10: All you need is squeezing! - fuw.edu.pl

then God added decoherence…

and everything became… simpler

Page 11: All you need is squeezing! - fuw.edu.pl

Quantum interferometry in the presence of loss

estimator

J. Kolodyński, R. Demkowicz-Dobrzański, PRA 82,053804 (2010) – Bayesian approach S. Knysh, V. Smelyanskiy, G. Durkin , PRA 83, (2011) – Fisher information approach

Heisenberg scaling is lost! also valid if N replaced with ⟨N⟩

B. M. Escher, R. L. de Matos Filho, L. Davidovich, Nat. Phys. 7, 406 (2011)

Page 12: All you need is squeezing! - fuw.edu.pl

R. Demkowicz-Dobrzański, J. Kolodyński, M. Guta, Nat. Commun. 3, 1063 (2012)

Quantum metrology with decoherence

Page 13: All you need is squeezing! - fuw.edu.pl

Saturating the fundamental bound is simple!

Weak squezing + simple measurement + simple estimator = optimal strategy! (thanks to decoherence)

Fundamental bound

Simple estimator based on n1- n2 measurement

C. Caves, Phys. Rev D 23, 1693 (1981)

For strong beams:

Page 14: All you need is squeezing! - fuw.edu.pl

Optimality of the squeezed vacuum+coherent state strategy

Page 15: All you need is squeezing! - fuw.edu.pl

Quantum precision enhancement in the GEO600 interferometer

Page 16: All you need is squeezing! - fuw.edu.pl

Quantum precision enhancement in the GEO600 interferometer

Can the precision be improved by using better quantum states and better measurements?

Page 17: All you need is squeezing! - fuw.edu.pl

Quantum optical model

U

up to irrelevant phase factors and assuming no transition to higher order sidebands

If recycling cavity is tuned to the central frequency:

Effectively two modes:

Page 18: All you need is squeezing! - fuw.edu.pl

Equivalent quantum model

the problem reduced Mach-Zehnder interferometry!

Page 19: All you need is squeezing! - fuw.edu.pl

GEO600 interferometer at the fundamental quantum bound

+10dB squeezed coherent light

fundamental bound

R. Demkowicz-Dobrzanski, K. Banaszek, R. Schnabel, arxiv:1302????

Gravitational wave strain sensitivity:

detectable mirror oscilation amplitude

Page 20: All you need is squeezing! - fuw.edu.pl

Ramsey interferometry Atomic clocks calibration, N two level atoms

cavity vs atom transition detuning

Taking into account dephasing:

For large N using spin-squeezed states: Fundamental bound!

precision improved thanks to squeezing

S. Huelga et al. Phys. Rev. Lett 79, 3865 (1997)

Page 21: All you need is squeezing! - fuw.edu.pl

Matrix product state with bond dimension D

Matrix product states and metrology?

No need to entangle large number of probes

M.Jarzyna, R. Demkowicz-Dobrzanski, arxiv:1301.4246

Low bond dimension matrix product states are sufficient.

D=1 D=2 D=3

Page 22: All you need is squeezing! - fuw.edu.pl

Summary • Heisenberg scaling asymptotically destroyed

• Simple schemes saturate the fundamental bounds

• GEO600 optimal

• The same applies to atoms with loss/dephasing – spin squeezed states + Ramsey interferometry optimal

• Matrix product states and metrology…. ?

• Translate results to quantum oracle algortihms with noise? R. Demkowicz-Dobrzański, J. Kolodyński, M. Guta, Nat. Commun. 3, 1063 (2012)

R. Demkowicz-Dobrzanski, K. Banaszek, R. Schnabel, arxiv:1302???? M.Jarzyna, R. Demkowicz-Dobrzanski, arxiv:1301.4246