• Acta Physica Sinica
  • Vol. 69, Issue 10, 103101-1 (2020)
Shi-Xiong Li1、*, De-Liang Chen1, Zheng-Ping Zhang2, Zheng-Wen Long3, and Shui-Jie Qin4
Author Affiliations
  • 1School of Physics and Electronic Science, Guizhou Education University, Guiyang 550018, China
  • 2College of Big Data and Information Engineering, Guizhou University, Guiyang 550025, China
  • 3College of physics, Guizhou University, Guiyang 550025, China
  • 4Key Laboratory of Photoelectron Technology and Application, Guizhou University, Guiyang 550025, China
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    DOI: 10.7498/aps.69.20200268 Cite this Article
    Shi-Xiong Li, De-Liang Chen, Zheng-Ping Zhang, Zheng-Wen Long, Shui-Jie Qin. Study on the ground state properties and excitation properties of C18 under different external electric fields [J]. Acta Physica Sinica, 2020, 69(10): 103101-1 Copy Citation Text show less
    Optimized structure and molecular orbitals: (a) Structure observed along the z direction; (b) HOMO; (c) LUMO.
    Fig. 1. Optimized structure and molecular orbitals: (a) Structure observed along the z direction; (b) HOMO; (c) LUMO.
    Localized orbital locator calculated based on π orbitals, the isovalue is set to 0.45: (a) LOL of out-plane π orbitals; (b) LOL of in-plane π orbitals.
    Fig. 2. Localized orbital locator calculated based on π orbitals, the isovalue is set to 0.45: (a) LOL of out-plane π orbitals; (b) LOL of in-plane π orbitals.
    The energies of C18 under different external electric fields. Circle and asterisk represent the external electric fields in y and z direction, respectively.
    Fig. 3. The energies of C18 under different external electric fields. Circle and asterisk represent the external electric fields in y and z direction, respectively.
    Localized orbital locator calculated based on out-plane π orbitals under different external electric fields in the z direction, the isovalue is set to 0.38: (a) 0 a.u.; (b) 0.005 a.u.; (c) 0.01 a.u.; (d) 0.015 a.u..
    Fig. 4. Localized orbital locator calculated based on out-plane π orbitals under different external electric fields in the z direction, the isovalue is set to 0.38: (a) 0 a.u.; (b) 0.005 a.u.; (c) 0.01 a.u.; (d) 0.015 a.u..
    Electron localization function calculated based on out-plane π orbitals under different external electric fields in the z direction, the isovalue is set to 0.38: (a) 0 a.u.; (b) 0.005 a.u.; (c) 0.01 a.u.; (d) 0.015 a.u..
    Fig. 5. Electron localization function calculated based on out-plane π orbitals under different external electric fields in the z direction, the isovalue is set to 0.38: (a) 0 a.u.; (b) 0.005 a.u.; (c) 0.01 a.u.; (d) 0.015 a.u..
    LOL calculated based on out-plane π orbitals under different external electric fields in the y direction, the isovalue is set to 0.52: (a) 0 a.u.; (b) 0.015 a.u..
    Fig. 6. LOL calculated based on out-plane π orbitals under different external electric fields in the y direction, the isovalue is set to 0.52: (a) 0 a.u.; (b) 0.015 a.u..
    ELF calculated based on out-plane π orbitals under different external electric fields in the y direction, the isovalue is set to 0.61: (a) 0 a.u.; (b) 0.015 a.u..
    Fig. 7. ELF calculated based on out-plane π orbitals under different external electric fields in the y direction, the isovalue is set to 0.61: (a) 0 a.u.; (b) 0.015 a.u..
    LOL calculated based on in-plane π orbitals under different external electric fields in the z direction, the isovalue is set to 0.37: (a) 0 a.u.; (b) 0.005 a.u.; (c) 0.01 a.u.; (d) 0.015 a.u..
    Fig. 8. LOL calculated based on in-plane π orbitals under different external electric fields in the z direction, the isovalue is set to 0.37: (a) 0 a.u.; (b) 0.005 a.u.; (c) 0.01 a.u.; (d) 0.015 a.u..
    ELF calculated based on in-plane π orbitals under different external electric fields in the y direction, the isovalue is set to 0.62: (a) 0 a.u.; (b) 0.015 a.u..
    Fig. 9. ELF calculated based on in-plane π orbitals under different external electric fields in the y direction, the isovalue is set to 0.62: (a) 0 a.u.; (b) 0.015 a.u..
    Calculated infrared spectra based on different external electric fields in the z direction (left side) and y direction (right side): (a) 0 a.u.; (b) 0.005 a.u.; (c) 0.01 a.u.; (d) 0.015 a.u.; (e) 0.02 a.u.; (f) 0 a.u.; (g) 0.005 a.u.;(h) 0.01 a.u.; (i) 0.015 a.u..
    Fig. 10. Calculated infrared spectra based on different external electric fields in the z direction (left side) and y direction (right side): (a) 0 a.u.; (b) 0.005 a.u.; (c) 0.01 a.u.; (d) 0.015 a.u.; (e) 0.02 a.u.; (f) 0 a.u.; (g) 0.005 a.u.;(h) 0.01 a.u.; (i) 0.015 a.u..
    Calculated Raman spectra based on different external electric fields in the z direction (left side) and y direction (right side): (a) 0 a.u.; (b) 0.005 a.u.; (c) 0.01 a.u.; (d) 0.015 a.u.; (e) 0.02 a.u.; (f) 0 a.u.; (g) 0.005 a.u.;(h) 0.01 a.u.; (i) 0.015 a.u..
    Fig. 11. Calculated Raman spectra based on different external electric fields in the z direction (left side) and y direction (right side): (a) 0 a.u.; (b) 0.005 a.u.; (c) 0.01 a.u.; (d) 0.015 a.u.; (e) 0.02 a.u.; (f) 0 a.u.; (g) 0.005 a.u.;(h) 0.01 a.u.; (i) 0.015 a.u..
    F/a.u. EH – 3EH – 2EH – 1EHELEL + 1EL + 2EL + 3Eg/eV
    0–8.5508–8.5508–8.4485–8.4485–1.7005–1.7005–1.67541.67546.7479
    0.005z–8.5544–8.5544–8.4486–8.4486–1.7141–1.7141–1.66661.66666.7345
    0.010z–8.5650–8.5650–8.4495–8.4495–1.7392–1.73921.65471.65476.7102
    0.015z–8.5819–8.5819–8.4518–8.4518–1.7700–1.7700–1.6461–1.64616.6818
    0.020z–8.6044–8.6044–8.4562–8.4562–1.8056–1.8056–1.6415–1.64156.6505
    0.005x–8.6369–8.5205–8.4629–8.3831–1.8002–1.7217–1.6612–1.63176.5829
    0.010x–8.7048–8.5881–8.3700–8.3153–1.9358–1.8075–1.6986–1.61196.3794
    0.015x–8.7516–8.6519–8.2846–8.2518–2.0999–1.9295–1.8027–1.64936.1518
    0.050y–8.6367–8.5204–8.4630–8.3831–1.8005–1.7222–1.6609–1.63156.5825
    0.010y–8.7046–8.5879–8.3700–8.3153–1.9359–1.8075–1.6988–1.61206.3793
    0.015y–8.7527–8.6529–8.2847–8.2516–2.0992–1.9293–1.8012–1.64826.1524
    Table 1.

    The orbital energies EH, EL, EH–1, EH–2, EH–3, EL+1, EL+2, EL+3 and Eg of C18 under different external electric fields. The unit of orbital energy is hartree, the superscripts x, y and z denote thex, y and z direction, respectively.

    不同电场下的轨道能量EH, EL, EH–1, EH–2, EH–3, EL+1, EL+2, EL+3以及Eg. 轨道能量的单位是Hartree (1 Hartree = 2625.5 kJ/mol), 上标x, y, z分别表示x, y, z方向加电场

    F/a.u. zxy
    04.2534.2534.253
    0.0054.2484.2564.257
    0.0104.2324.3984.399
    0.0154.2054.6824.706
    0.0204.170
    Table 2.

    The AV1245 of C18 under different external electric fields.

    不同电场下的AV1245指数

    F/a.u. E/eV
    n = 1 267142122233536
    02.50762.63723.12853.12853.83015.65195.65195.78906.47946.4794
    0.0052.49932.62643.09783.12343.81305.63395.65585.77536.45736.4644
    0.0102.45602.57592.99333.02293.73585.57255.65645.71956.38336.4070
    0.0152.37472.46842.86212.90173.60945.46385.62325.63206.27826.3067
    Table 3.

    Excitation energy of C18 at different electric field in y direction.

    不同外电场(y方向)下C18分子部分激发态的激发能

    F/a.u. $\lambda $/nm
    n = 1 267142122233536
    0494.43470.14396.30396.30323.71219.37219.37214.17191.35191.35
    0.005496.08472.07400.24396.96325.17220.07219.21214.68192.01191.80
    0.010504.82481.32414.20410.15331.88222.49219.19216.77194.23193.51
    0.015522.11502.28433.20427.29343.51226.92220.49220.14197.48196.59
    Table 4.

    Excitation wavelength of C18 at different electric field in y direction.

    不同外电场(y方向)下C18分子部分激发态的波长

    F/a.u. f
    n = 1 267142122233536
    00.00000.00000.00300.00300.00003.02163.02160.00000.36950.3695
    0.0050.00000.00030.00250.00280.01322.96763.02220.00000.38310.3838
    0.0100.00000.00110.00140.00020.04632.80092.99730.00000.43790.4337
    0.0150.00000.00000.00030.00000.08422.49170.00002.45090.51970.5373
    Table 5.

    Oscillator strength of C18 at different electric field in y direction.

    不同外电场(y方向)下C18分子部分激发态的振子强度

    Shi-Xiong Li, De-Liang Chen, Zheng-Ping Zhang, Zheng-Wen Long, Shui-Jie Qin. Study on the ground state properties and excitation properties of C18 under different external electric fields [J]. Acta Physica Sinica, 2020, 69(10): 103101-1
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