• Laser & Optoelectronics Progress
  • Vol. 58, Issue 1, 127002 (2021)
Peng Yonggang*
Author Affiliations
  • Department of Applied Physics, College of Science, Nanjing University of Posts and Telecommunications, Nanjing 210003, China
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    DOI: 10.3788/LOP202158.0127002 Cite this Article Set citation alerts
    Peng Yonggang. Optimal Pulse Sequence of Quantum Controlled Not-Gates via Nuclear Magnetic Resonance Realization[J]. Laser & Optoelectronics Progress, 2021, 58(1): 127002 Copy Citation Text show less
    Q1 and Q2 versus time step obtained by executing CCNOT111 when k=1
    Fig. 1. Q1 and Q2 versus time step obtained by executing CCNOT111 when k=1
    Q1 and Q2 versus time step obtained by executing CCNOT211 when k=1
    Fig. 2. Q1 and Q2 versus time step obtained by executing CCNOT211 when k=1
    Q1 and Q2 versus time step obtained by executing CCNOT311 when k=1
    Fig. 3. Q1 and Q2 versus time step obtained by executing CCNOT311 when k=1
    Q1 and Q2 versus time step obtained by executing CCNOT411 when k=1
    Fig. 4. Q1 and Q2 versus time step obtained by executing CCNOT411 when k=1
    Q1 and Q2 versus time step obtained by executing CCNOT111 when k=32
    Fig. 5. Q1 and Q2 versus time step obtained by executing CCNOT111 when k=32
    Q1 and Q2 versus time step obtained by executing CCNOT211 when k=32
    Fig. 6. Q1 and Q2 versus time step obtained by executing CCNOT211 when k=32
    Q1 and Q2 versus time step obtained by executing CCNOT311 when k=32
    Fig. 7. Q1 and Q2 versus time step obtained by executing CCNOT311 when k=32
    Q1 and Q2 versus time step obtained by executing CCNOT411 when k=32
    Fig. 8. Q1 and Q2 versus time step obtained by executing CCNOT411 when k=32
    ParameterY1X1'Y¯1X2'Y¯2I12'Y2
    J12z-4.3×10-7-4.3×10-7-4.3×10-7-4.3×10-7-4.3×10-7-4.3×10-7-4.3×10-7
    h1z1111111
    h2z0.250.250.250.250.250.250.25
    h˜1x3.125×10-25.596×10-2-3.125×10-24.451×10-2-7.812×10-307.812×10-3
    h˜2x7.812×10-31.399×10-2-7.813×10-31.113×10-2-1.953×10-301.953×10-3
    f1x1.001.001.000.250.2500.25
    f2x1.001.001.000.250.2500.25
    h˜1y3.125×10-25.595×10-2-3.125×10-24.451×10-2-7.812×10-307.812×10-3
    h˜2y7.812×10-31.398×10-2-7.812×10-31.112×10-2-1.953×10-301.953×10-3
    f1y1.001.001.000.250.2500.25
    f2y1.001.001.000.250.2500.25
    Table 1. Parameters J,
    OperationY1X1'Y¯1X2'Y¯2I12'Y2
    Value8.008.008.00128.001281.16×106128.00
    Table 2. Parameter execution time of NMR pulse sequence under different operation when k =1 unit: 4
    ParameterY1X1'Y¯1X2'Y¯2I12'Y2
    τδm88.00×10-210088.00×10-210088.00×10-21001281.281001281.281001.162×1061.162×10611281.28100
    Table 3. Execution time, time step and number of execution steps of NMR pulse sequence under different operation when k =1 unit:
    Operationk=1k=2k=4k=8k=32
    Q1Q2Q1Q2Q1Q2Q1Q2Q1Q2
    CCNOT1110.99901.00001.00001.00001.0000
    CCNOT2110.74500.93100.98200.99601.0000
    CCNOT3110.74400.93100.98200.99601.0000
    CCNOT4110.72900.92700.98100.99501.0000
    Table 4. Expectation values of Q1 and Q2 under four different operation when k=1,2,4,8,32
    Peng Yonggang. Optimal Pulse Sequence of Quantum Controlled Not-Gates via Nuclear Magnetic Resonance Realization[J]. Laser & Optoelectronics Progress, 2021, 58(1): 127002
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