• Laser & Optoelectronics Progress
  • Vol. 59, Issue 1, 0136001 (2022)
Zhe Meng*, Xue Guo*, Xiaoxiao Chen*, Jiazhi Yang*, Jian Li*, Mairikena Aili*, and Anning Zhang*
Author Affiliations
  • [in Chinese]
  • show less
    DOI: 10.3788/LOP202259.0136001 Cite this Article Set citation alerts
    Zhe Meng, Xue Guo, Xiaoxiao Chen, Jiazhi Yang, Jian Li, Mairikena Aili, Anning Zhang. [J]. Laser & Optoelectronics Progress, 2022, 59(1): 0136001 Copy Citation Text show less
    Experimental setup. (a) Single-photon source preparation; (b) three parts are initial state preparation, evolution, and final state measurement from left to right in sequence
    Fig. 1. Experimental setup. (a) Single-photon source preparation; (b) three parts are initial state preparation, evolution, and final state measurement from left to right in sequence
    Final state density matrix theoretical value
    Fig. 2. Final state density matrix theoretical value
    Final state density matrix experimental value from quantum state tomography
    Fig. 3. Final state density matrix experimental value from quantum state tomography
    Experimental observation of the breaking of the PT-symmetry (real part of eigenvalue E+ decreases when 0aa>1)
    Fig. 4. Experimental observation of the breaking of the PT-symmetry (real part of eigenvalue E+ decreases when 0<a<1 and equals zero when a>1)
    Experimental observation of the breaking of the PT-symmetry (imaginary part of eigenvalue E+ equals zero when 0aa>1)
    Fig. 5. Experimental observation of the breaking of the PT-symmetry (imaginary part of eigenvalue E+ equals zero when 0<a<1 and increases when a>1)
    Zhe Meng, Xue Guo, Xiaoxiao Chen, Jiazhi Yang, Jian Li, Mairikena Aili, Anning Zhang. [J]. Laser & Optoelectronics Progress, 2022, 59(1): 0136001
    Download Citation