Acta Physica Sinica, Volume. 69, Issue 18, 180301-1(2020)

Research progress of Rydberg many-body interaction

Zheng-Yuan Zhang, Tian-Yi Zhang, Zong-Kai Liu, Dong-Sheng Ding*, and Bao-Sen Shi
Author Affiliations
  • CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei 230026, China
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    Figures & Tables(14)
    Energy level of two-atoms system excited by one laser.
    Schematic of binary Rydberg energy with detuning: (a) The energy of a pair of atoms with and ; (b) the energy of a pair of atoms with different detuning and potentials[19].
    Spatially ordered components of the many-body states[3]: (a) Directly imaging result; (b) accumulative result of many measurements; (c) predicted result.
    (a) Tensor network form of the partition function for 1D Ising model; (b) tensor element for the partition function of 2D Ising model; (c) tensor network form of the partition function for 2D Ising model[26]
    Relationship between the specific heat and the reciprocal of the temperature[27].
    Parameters of single-photon source: (a) as a function of effective principle quantum number[30]. Coincidence count as a function of time decay is showed in the inset[30]; (b) normalized coincidence count as a function of time decay using quantum dots[28]; (c) normalized coincidence count of Hong-Ou-Mandel interference as a function of time decay with parallel and cross polarization respectively using quantum dots[28].
    Properties of quantum storage with different number of input photons Nin[47]: (a) Storage efficiency as a function of storage time; (b) storage efficiency as a function of Rydberg states.
    Schematic of energy levels combined exciting state with ground state[4]: (a) Procedure of writing; (b) storage in the ground state; (c) procedure of read.
    Scheme of imaging process and simulated results[6]: (a) Scheme of single-atom imaging process; (b) absorption of probe light without control light; (c) absorption of probe light with control light.
    (a) Number of retrial gate photons as a function of number of stored gate photons with different number of source photons [7]; (b) contrast of optimal efficiency of subtraction[7].
    phase diagram[10] and self-organized behaviors[64]: (a) Phase diagram of density of Rydberg atom; (b) EIT phase diagram without control light; (c) evolution in the self-organized process; (d) regulation of self-organized stationary states.
    Quantum simulation in two dimensions[63]: (a) Collective Rabi oscillation with different number of atoms; (c) Rydberg fraction of the systems with 20 atoms; (d) Rydberg fraction of the systems with 28 atoms.
    Many-atom quantum simulation in one dimension[9]: (a) Predicted results of evolution with different interaction; (b) experimental results of evolution with different interaction; (c) ground-state probability as a function of system size; (d) number of states with identical number of occurrences.
    • Table 1. Relation between the properties of Rydberg atom and its principal quantum number[11].

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      Table 1. Relation between the properties of Rydberg atom and its principal quantum number[11].

      性质与主量子数关系Na(10 d)
      束缚能n–20.14 eV
      相邻n态间的能量差 n–30.023 eV
      轨道半径n2147a0
      几何截面n468000 $a_0^2$
      偶极矩 $\left\langle {nd\left| {er} \right|\left. {nf} \right\rangle } \right.$n2143ea0
      极化率n70.21 MHz·cm2·V–2
      辐射寿命n31.0 μs
      精细结构间隔n–3–92 MHz
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    Zheng-Yuan Zhang, Tian-Yi Zhang, Zong-Kai Liu, Dong-Sheng Ding, Bao-Sen Shi. Research progress of Rydberg many-body interaction[J]. Acta Physica Sinica, 2020, 69(18): 180301-1

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    Paper Information

    Received: May. 2, 2020

    Accepted: --

    Published Online: Jan. 5, 2021

    The Author Email:

    DOI:10.7498/aps.69.20200649

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