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

Table 4. Calculated Dominant Vertical Excitation Energies (TD-DFT/B3LYP/aug-cc-pVDZ) and Oscillator Strengths of C2H5NO2, Compared Where Possible with the Corresponding Experimental Data and Other Work in the Literature (Energies in eV)a.

nitroethane (C2H5NO2)
   
state E (eV) fL dominant excitations Eexp. (eV)b cross-section (Mb)
1A′          
2 1A″ 4.605 0.00006 π*(5a← n̅OCN(15a) (99%) 4.550 0.04
2 1A′ 6.789 0.11079 π*(5a π(4a) (86%) 6.256 16.10
5 1A′ 7.480 0.06883 π*(5a nOCH(3a) (70%) + 3s(17a← n̅OCN(15a) (20%) 7.847 7.76
7 1A′ 8.087 0.02867 3s(19a← n̅O(16a) (74%) + 3s(18a) ← OCN(15a) (20%) 8.271 11.48
12 1A′ 9.129 0.01501 4s/3py/3pz(20a) ← O (16a) (81%) 8.725 18.60
17 1A′ 9.664 0.05147 π*(5a″ π(2a) (29%) + 3s(17a) ← O/σCC(14a) (49%) 9.44(6) 22.54
19 1A′ 9.754 0.14702 3s(17a← n̅OCC(14a) (48%) + π*(5a) ← π(2a) (24%) + 4s(21a← n̅OCN(15a) (11%) 9.54(5) 22.87
a

See text for details.

b

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