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. 2023 Feb 2;127(6):1445–1457. doi: 10.1021/acs.jpca.2c08023

Table 1. Calculated Dominant Vertical Excitation Energies (TD-DFT/B3LYP/aug-cc-pVDZ) and Oscillator Strengths of CH3NO2, Compared Where Possible with the Corresponding Experimental Data and Other Work in the Literature (Energies in eV)a.

nitromethane (CH3NO2)
       
state E (eV) fL dominant excitations Eexp. (eV)b cross-section (Mb) E (eV)1 E (eV)3
1A′              
2 1A″ 4.605 0.00002 π*(4a← n̅O/σCN(12a′) (100%) 4.550 0.04 4.5  
2 1A′ 6.879 0.15459 π*(4a π(3a) (90%) 6.271 17.74 6.25 6.27
3 1A′ 7.100 0.00037 3s(14a← n̅O(13a) (95%) 7.637 2.59 7.44 7.531
4 1A′ 7.510 0.03627 3s(14a← n̅OCN(12a) (97%) 8.38(3)(s) 12.13 8.07 8.257
6 1A′ 8.223 0.02625 3px/σ(16a) ← O(13a) (72%) + 3py(15a← n̅O(13a) (22%) 7.92(5) 5.98 7.8 7.974
9 1A′ 8.851 0.10584 π*(4a) ← πNO(2a) (70%) + 3px/σ(16a← n̅OCN(12a) (21%) 8.803 16.33 8.3 8.531
12 1A′ 9.702 0.20343 σCN*(17a← n̅OCN(12a) (79%) + 4s/4py(19a← n̅O(13a) (14%) 9.450 27.35   9.368
19 1A′ 10.696 0.03473 4s/5pz(20a← n̅OCN(12a) (93%) 10.315 23.63   10.347
18 1A″ 10.960 0.02397 4s*(20a← n̅OCN(12a) (90%) 10.739 22.32   10.798
a

See text for details.

b

The last decimal of the energy value is given in parentheses for these less-resolved features.