One- and two-axis squeezing of atomic ensembles in optical cavities

Johannes Borregaard; E.J. Davis; G.S. Bentsen; M.H. Schleier-Smith; Anders Søndberg Sørensen

doi:10.1088/1367-2630/aa8438

One- and two-axis squeezing of atomic ensembles in optical cavities

Johannes Borregaard, E.J. Davis, G.S. Bentsen, M.H. Schleier-Smith, Anders Søndberg Sørensen

12 Citationer (Scopus)

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Abstract

The strong light-matter coupling attainable in optical cavities enables the generation of highly squeezed states of atomic ensembles. It was shown by Sørensen and Mølmer (2002 Phys. Rev. A 66 022314) how an effective one-axis twisting Hamiltonian can be realized in a cavity setup. Here, we extend this work and show how an effective two-axis twisting Hamiltonian can be realized in a similar cavity setup. We compare the two schemes in order to characterize their advantages. In the absence of decoherence, the two-axis Hamiltonian leads to more squeezing than the one-axis Hamiltonian. If limited by decoherence from spontaneous emission and cavity decay, we find roughly the same level of squeezing for the two schemes scaling as where C is the single atom cooperativity and N is the total number of atoms. When compared to an ideal squeezing operation, we find that for specific initial states, a dissipative version of the one-axis scheme attains higher fidelity than the unitary one-axis scheme or the two-axis scheme. However, the unitary one-axis and two-axis schemes perform better for general initial states.

Originalsprog	Engelsk
Artikelnummer	093021
Tidsskrift	New Journal of Physics
Vol/bind	19
Antal sider	14
ISSN	1367-2630
DOI	https://doi.org/10.1088/1367-2630/aa8438
Status	Udgivet - 28 sep. 2017

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10.1088/1367-2630/aa8438

Borregaard_2017_New_J._Phys._19_093021Forlagets udgivne version, 960 KBLicens: CC BY

Citationsformater

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abstract = "The strong light-matter coupling attainable in optical cavities enables the generation of highly squeezed states of atomic ensembles. It was shown by S{\o}rensen and M{\o}lmer (2002 Phys. Rev. A 66 022314) how an effective one-axis twisting Hamiltonian can be realized in a cavity setup. Here, we extend this work and show how an effective two-axis twisting Hamiltonian can be realized in a similar cavity setup. We compare the two schemes in order to characterize their advantages. In the absence of decoherence, the two-axis Hamiltonian leads to more squeezing than the one-axis Hamiltonian. If limited by decoherence from spontaneous emission and cavity decay, we find roughly the same level of squeezing for the two schemes scaling as where C is the single atom cooperativity and N is the total number of atoms. When compared to an ideal squeezing operation, we find that for specific initial states, a dissipative version of the one-axis scheme attains higher fidelity than the unitary one-axis scheme or the two-axis scheme. However, the unitary one-axis and two-axis schemes perform better for general initial states.",

author = "Johannes Borregaard and E.J. Davis and G.S. Bentsen and M.H. Schleier-Smith and S{\o}rensen, {Anders S{\o}ndberg}",

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AU - Borregaard, Johannes

AU - Davis, E.J.

AU - Bentsen, G.S.

AU - Schleier-Smith, M.H.

AU - Sørensen, Anders Søndberg

PY - 2017/9/28

Y1 - 2017/9/28

N2 - The strong light-matter coupling attainable in optical cavities enables the generation of highly squeezed states of atomic ensembles. It was shown by Sørensen and Mølmer (2002 Phys. Rev. A 66 022314) how an effective one-axis twisting Hamiltonian can be realized in a cavity setup. Here, we extend this work and show how an effective two-axis twisting Hamiltonian can be realized in a similar cavity setup. We compare the two schemes in order to characterize their advantages. In the absence of decoherence, the two-axis Hamiltonian leads to more squeezing than the one-axis Hamiltonian. If limited by decoherence from spontaneous emission and cavity decay, we find roughly the same level of squeezing for the two schemes scaling as where C is the single atom cooperativity and N is the total number of atoms. When compared to an ideal squeezing operation, we find that for specific initial states, a dissipative version of the one-axis scheme attains higher fidelity than the unitary one-axis scheme or the two-axis scheme. However, the unitary one-axis and two-axis schemes perform better for general initial states.

AB - The strong light-matter coupling attainable in optical cavities enables the generation of highly squeezed states of atomic ensembles. It was shown by Sørensen and Mølmer (2002 Phys. Rev. A 66 022314) how an effective one-axis twisting Hamiltonian can be realized in a cavity setup. Here, we extend this work and show how an effective two-axis twisting Hamiltonian can be realized in a similar cavity setup. We compare the two schemes in order to characterize their advantages. In the absence of decoherence, the two-axis Hamiltonian leads to more squeezing than the one-axis Hamiltonian. If limited by decoherence from spontaneous emission and cavity decay, we find roughly the same level of squeezing for the two schemes scaling as where C is the single atom cooperativity and N is the total number of atoms. When compared to an ideal squeezing operation, we find that for specific initial states, a dissipative version of the one-axis scheme attains higher fidelity than the unitary one-axis scheme or the two-axis scheme. However, the unitary one-axis and two-axis schemes perform better for general initial states.

U2 - 10.1088/1367-2630/aa8438

DO - 10.1088/1367-2630/aa8438

M3 - Journal article

SN - 1367-2630

VL - 19

JO - New Journal of Physics

JF - New Journal of Physics

M1 - 093021

ER -

One- and two-axis squeezing of atomic ensembles in optical cavities

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