Chem. J. Chinese Universities ›› 2015, Vol. 36 ›› Issue (5): 962.doi: 10.7503/cjcu20141054
• Physical Chemistry • Previous Articles Next Articles
JIN Junling1,2,*(), DING Xiang1, OU Lihui1, ZHANG Xiangyang1, SHEN Youming1, GENG Yun2, SU Zhongmin2
Received:
2014-11-28
Online:
2015-05-10
Published:
2015-04-17
Contact:
JIN Junling
E-mail:jinjl174@nenu.edu.cn
Supported by:
CLC Number:
TrendMD:
JIN Junling, DING Xiang, OU Lihui, ZHANG Xiangyang, SHEN Youming, GENG Yun, SU Zhongmin. Density Functional Theory Studies on the Photophysical Properties of N,N-Chelate Boron Complexes†[J]. Chem. J. Chinese Universities, 2015, 36(5): 962.
Fig.2 Illustration of the highest occupied molecular orbital(HOMO) and lowest unoccupied molecular orbital(LUMO) plots, the orbi-tal energy levels, and the HOMO-LUMO energy gaps for complexes 1, 1q, 2 and 2q at their optimized S0 geometries in vacuum at B3LYP/6-31G(d) levelThe molecular orbital plots were obtained with an isosurface of 0.02 a.u.
Complex | Transition | λabs/nm | Ex/eV | f | Composition | λexp./nm |
---|---|---|---|---|---|---|
1 | S0→S1 | 353.9 | 3.503 | 0.367 | HOMO→LUMO(98%) | 378 |
1q | S0→S1 | 431.8 | 2.872 | 0.207 | HOMO→LUMO(98%) | 450 |
2 | S0→S1 | 343.5 | 3.610 | 0.515 | HOMO→LUMO(99%) | 374 |
2q | S0→S1 | 419.8 | 2.954 | 0.237 | HOMO→LUMO(99%) | 446 |
Table 1 Calculated absorption wavelengths(λabs), excitation energies(Ex), oscillator strengths f, and dominant excitation character of complexes 1, 2, 1q, and 2q together with experimental results(λexp.)*
Complex | Transition | λabs/nm | Ex/eV | f | Composition | λexp./nm |
---|---|---|---|---|---|---|
1 | S0→S1 | 353.9 | 3.503 | 0.367 | HOMO→LUMO(98%) | 378 |
1q | S0→S1 | 431.8 | 2.872 | 0.207 | HOMO→LUMO(98%) | 450 |
2 | S0→S1 | 343.5 | 3.610 | 0.515 | HOMO→LUMO(99%) | 374 |
2q | S0→S1 | 419.8 | 2.954 | 0.237 | HOMO→LUMO(99%) | 446 |
Complex | Transition | λem/nm | Em/eV | f | Composition | SS/nm | kr/s-1 | knr/s-1 | Φexp. | λexp./nm |
---|---|---|---|---|---|---|---|---|---|---|
1 | S1→S0 | 410.2 | 3.022 | 0.128 | LUMO→HOMO(98%) | 56.3 | 5.10×107 | 1.02×107 | 0.29b | 516 |
1q | S1→S0 | 538.5 | 2.302 | 0.060 | LUMO→HOMO(99%) | 96.7 | 1.40×107 | 2.46×1010 | N/Ac | 578 |
2 | S1→S0 | 400.1 | 3.099 | 0.185 | LUMO→HOMO(99%) | 56.6 | 7.70×107 | 0.99×107 | 0.61b | 476 |
2q | S1→S0 | 521.9 | 2.376 | 0.080 | LUMO→HOMO(99%) | 102.1 | 2.00×107 | 2.62×1010 | N/Ac | 546 |
Table 2 Calculated emission wavelengths(λem), emission energies(Em), oscillator strengths f, dominant excitation character, Stokes shift(SS), radiative rate constants(kr) and nonradiative rate constants(knr) of complexes 1, 2, 1q, and 2q together with the reported experimental results of the emission wavelength(λexp.) and quantum yield(Φexp.)a
Complex | Transition | λem/nm | Em/eV | f | Composition | SS/nm | kr/s-1 | knr/s-1 | Φexp. | λexp./nm |
---|---|---|---|---|---|---|---|---|---|---|
1 | S1→S0 | 410.2 | 3.022 | 0.128 | LUMO→HOMO(98%) | 56.3 | 5.10×107 | 1.02×107 | 0.29b | 516 |
1q | S1→S0 | 538.5 | 2.302 | 0.060 | LUMO→HOMO(99%) | 96.7 | 1.40×107 | 2.46×1010 | N/Ac | 578 |
2 | S1→S0 | 400.1 | 3.099 | 0.185 | LUMO→HOMO(99%) | 56.6 | 7.70×107 | 0.99×107 | 0.61b | 476 |
2q | S1→S0 | 521.9 | 2.376 | 0.080 | LUMO→HOMO(99%) | 102.1 | 2.00×107 | 2.62×1010 | N/Ac | 546 |
Fig.3 Transition density matrix of the hot excitation(S0 state) for complexes 1(A, A'), 1q(B, B'), 2(C, C') and 2q(D, D') calculated by B3LYP/6-31G(2d,p) in vacuumThe unit of color scale is a.u.2, 1 a.u.=1.6×10-19 C.
Fig.4 Calculated results for the centroids of charge(C+/C-) and the charge-transfer distance(DCT) between the barycenters of density depletion(gray) and density increment(purple) zone, and the transferred charge(Δq) computed for the first electronic transitionThe calculation level is B3LYP/6-31G(2d,p) level.
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