• Photonics Research
  • Vol. 9, Issue 11, 2296 (2021)
Shenchao Jin1, Han Bao2, Junlei Duan1, Xingda Lu1, Mingfeng Wang3, Kai-Feng Zhao4, Heng Shen5、6、7、*, and Yanhong Xiao2、8、*
Author Affiliations
  • 1Department of Physics, State Key Laboratory of Surface Physics and Key Laboratory of Micro and Nano Photonic Structures (Ministry of Education), Fudan University, Shanghai 200433, China
  • 2State Key Laboratory of Quantum Optics and Quantum Optics Devices, Institute of Laser Spectroscopy, and Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan 030006, China
  • 3Department of Physics, Wenzhou University, Wenzhou 325035, China
  • 4Applied Ion Beam Physics Laboratory, Key Laboratory of the Ministry of Education, and Institute of Modern Physics, Fudan University, Shanghai 200433, China
  • 5State Key Laboratory of Quantum Optics and Quantum Optics Devices, Institute of Opto-electronics, and Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan 030006, China
  • 6Clarendon Laboratory, University of Oxford, Oxford, OX1 3PU, UK
  • 7e-mail: hengshen@sxu.edu.cn
  • 8e-mail: yxiao@sxu.edu.cn
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    DOI: 10.1364/PRJ.413288 Cite this Article Set citation alerts
    Shenchao Jin, Han Bao, Junlei Duan, Xingda Lu, Mingfeng Wang, Kai-Feng Zhao, Heng Shen, Yanhong Xiao. Adiabaticity in state preparation for spin squeezing of large atom ensembles[J]. Photonics Research, 2021, 9(11): 2296 Copy Citation Text show less

    Abstract

    Spin-squeezed state is a many-body entangled state of great interest for precision measurements. Although the absolute sensitivity at the standard quantum limit is better for a larger atom number, the greater dominance of classical noises over atom projection noise makes it harder to achieve spin squeezing. Here, we show both theoretically and experimentally that adiabatic pulse control of the pump field in state preparation is indispensable to sufficient noise suppression, which is the prerequisite for spin squeezing. This technique is generally applicable to spin-squeezing experiments involving a large ensemble and is thus of significance for quantum metrology applications.
    dρdt+12{Γrel,ρ}=i[H,ρ]+Γexcρ,H=[00Ω1*(t)30ΔΩ2*(t)6Ω1(t)3Ω2(t)6Δ],Γrel=Diag(0,0,Γ),Γexcρ=Diag(Γ2ρ33,Γ2ρ33,0),

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    ρ11=ρ11(0)=1,ρ33=ρ33(0)=0,ρ22=ρ22(0)=0,ρ32=ρ32(0)=0.

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    ρ˙21=Γ12ρ21+iΩ2*6ρ31,ρ˙31=Γ13ρ31+iΩ26ρ21+iΩ13,

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    ρ˙21(t)=(Γ12+A22·α(t))ρ21(t)A12·α(t),

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    Γexcρ=Diag(γ5+13Γρ(2,1),(2,1)+23Γρ(2,2),(2,2),γ5+12Γρ(2,0),(2,0)+16Γρ(2,1),(2,1)+13Γρ(2,2),(2,2),γ5+12Γρ(2,1),(2,1)+12Γρ(2,1),(2,1),γ5+13Γρ(2,2),(2,2)+16Γρ(2,1),(2,1)+12Γρ(2,0),(2,0),γ5+23Γρ(2,2),(2,2)+13Γρ(2,1),(2,1),0,0,0,0,0).

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    Shenchao Jin, Han Bao, Junlei Duan, Xingda Lu, Mingfeng Wang, Kai-Feng Zhao, Heng Shen, Yanhong Xiao. Adiabaticity in state preparation for spin squeezing of large atom ensembles[J]. Photonics Research, 2021, 9(11): 2296
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