Author Affiliations
1School of Physics and Electronic Science, Guizhou Education University, Guiyang 550018, China2College of Big Data and Information Engineering, Guizhou University, Guiyang 550025, China3College of physics, Guizhou University, Guiyang 550025, China4Key Laboratory of Photoelectron Technology and Application, Guizhou University, Guiyang 550025, Chinashow less
Fig. 1. Optimized structure and molecular orbitals: (a) Structure observed along the z direction; (b) HOMO; (c) LUMO.
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.
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.
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..
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..
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..
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..
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..
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..
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..
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 – 3 | EH – 2 | EH – 1 | EH | EL | EL + 1 | EL + 2 | EL + 3 | Eg/eV
| 0 | –8.5508 | –8.5508 | –8.4485 | –8.4485 | –1.7005 | –1.7005 | –1.6754 | 1.6754 | 6.7479 | 0.005z | –8.5544 | –8.5544 | –8.4486 | –8.4486 | –1.7141 | –1.7141 | –1.6666 | 1.6666 | 6.7345 | 0.010z | –8.5650 | –8.5650 | –8.4495 | –8.4495 | –1.7392 | –1.7392 | 1.6547 | 1.6547 | 6.7102 | 0.015z | –8.5819 | –8.5819 | –8.4518 | –8.4518 | –1.7700 | –1.7700 | –1.6461 | –1.6461 | 6.6818 | 0.020z | –8.6044 | –8.6044 | –8.4562 | –8.4562 | –1.8056 | –1.8056 | –1.6415 | –1.6415 | 6.6505 | 0.005x | –8.6369 | –8.5205 | –8.4629 | –8.3831 | –1.8002 | –1.7217 | –1.6612 | –1.6317 | 6.5829 | 0.010x | –8.7048 | –8.5881 | –8.3700 | –8.3153 | –1.9358 | –1.8075 | –1.6986 | –1.6119 | 6.3794 | 0.015x | –8.7516 | –8.6519 | –8.2846 | –8.2518 | –2.0999 | –1.9295 | –1.8027 | –1.6493 | 6.1518 | 0.050y | –8.6367 | –8.5204 | –8.4630 | –8.3831 | –1.8005 | –1.7222 | –1.6609 | –1.6315 | 6.5825 | 0.010y | –8.7046 | –8.5879 | –8.3700 | –8.3153 | –1.9359 | –1.8075 | –1.6988 | –1.6120 | 6.3793 | 0.015y | –8.7527 | –8.6529 | –8.2847 | –8.2516 | –2.0992 | –1.9293 | –1.8012 | –1.6482 | 6.1524 |
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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.
| z | x | y | 0 | 4.253 | 4.253 | 4.253 | 0.005 | 4.248 | 4.256 | 4.257 | 0.010 | 4.232 | 4.398 | 4.399 | 0.015 | 4.205 | 4.682 | 4.706 | 0.020 | 4.170 | | |
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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
| 2 | 6 | 7 | 14 | 21 | 22 | 23 | 35 | 36 | 0 | 2.5076 | 2.6372 | 3.1285 | 3.1285 | 3.8301 | 5.6519 | 5.6519 | 5.7890 | 6.4794 | 6.4794 | 0.005 | 2.4993 | 2.6264 | 3.0978 | 3.1234 | 3.8130 | 5.6339 | 5.6558 | 5.7753 | 6.4573 | 6.4644 | 0.010 | 2.4560 | 2.5759 | 2.9933 | 3.0229 | 3.7358 | 5.5725 | 5.6564 | 5.7195 | 6.3833 | 6.4070 | 0.015 | 2.3747 | 2.4684 | 2.8621 | 2.9017 | 3.6094 | 5.4638 | 5.6232 | 5.6320 | 6.2782 | 6.3067 |
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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
| 2 | 6 | 7 | 14 | 21 | 22 | 23 | 35 | 36 | 0 | 494.43 | 470.14 | 396.30 | 396.30 | 323.71 | 219.37 | 219.37 | 214.17 | 191.35 | 191.35 | 0.005 | 496.08 | 472.07 | 400.24 | 396.96 | 325.17 | 220.07 | 219.21 | 214.68 | 192.01 | 191.80 | 0.010 | 504.82 | 481.32 | 414.20 | 410.15 | 331.88 | 222.49 | 219.19 | 216.77 | 194.23 | 193.51 | 0.015 | 522.11 | 502.28 | 433.20 | 427.29 | 343.51 | 226.92 | 220.49 | 220.14 | 197.48 | 196.59 |
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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
| 2 | 6 | 7 | 14 | 21 | 22 | 23 | 35 | 36 | 0 | 0.0000 | 0.0000 | 0.0030 | 0.0030 | 0.0000 | 3.0216 | 3.0216 | 0.0000 | 0.3695 | 0.3695 | 0.005 | 0.0000 | 0.0003 | 0.0025 | 0.0028 | 0.0132 | 2.9676 | 3.0222 | 0.0000 | 0.3831 | 0.3838 | 0.010 | 0.0000 | 0.0011 | 0.0014 | 0.0002 | 0.0463 | 2.8009 | 2.9973 | 0.0000 | 0.4379 | 0.4337 | 0.015 | 0.0000 | 0.0000 | 0.0003 | 0.0000 | 0.0842 | 2.4917 | 0.0000 | 2.4509 | 0.5197 | 0.5373 |
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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