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. 2022 Jan 18;27(3):620. doi: 10.3390/molecules27030620

Table 3.

Second-order perturbation theory analysis of Fock matrix as a basis for the NBO analysis between donor and acceptor orbitals of the studied compound.

Type Donor(i) Type Acceptor(j) E(2) Kcal/mol E(i)−E(j) (a.u) F(i,j) (a.u)
π C12-C13 π* C14-O15 28.26 0.3 0.086
π C5-C6 π* C1-C4 21.48 0.27 0.069
π C5-C6 π* C2-C3 19.66 0.29 0.068
π C38-O51 π* C32-C34 4.54 0.38 0.04
π C12-C13 σ* C6-C31 3.52 0.69 0.046
π C12-C13 σ* C31-H33 2.01 0.67 0.034
π C32-C34 σ* C31-H33 1.21 0.66 0.026
π C38-O51 π* C38-O51 1.08 0.38 0.02
π C32-C34 σ* N35-H36 0.53 0.67 0.018
σ C4-C5 σ* C1-Cl11 5.48 0.84 0.061
σ C3-H9 σ* C5-C6 4.82 1.08 0.064
σ C31-C32 σ* C34-N40 4.77 1.04 0.063
σ C32-C38 σ* C32-C34 4.29 1.27 0.066
σ C1-C2 σ* C1-C4 4.12 1.29 0.065
σ N18-H20 σ* C12-C13 4.02 1.26 0.064
σ C13-C14 σ* N16-C26 3.16 1.01 0.051
σ C12-C13 σ* C12-N18 3.11 1.16 0.054
σ N40-C41 σ* N39-C43 2.61 1.14 0.049
σ N17-C21 σ* C12-N17 2.19 1.24 0.047
σ C38-N39 σ* N39-C43 1.16 1.11 0.032
σ C5-H7 σ* C4-C5 0.64 1.09 0.024
σ C38-N39 σ* C43-H44 0.51 1.21 0.022
LP(1) N16 π* C21-O30 65.67 0.26 0.117
LP(1) N40 π* C32-C34 45.98 0.3 0.106
LP(2) O15 σ* C14-N16 28.83 0.62 0.121
LP(3) Cl11 π* C1-C4 12.11 0.33 0.062
LP(1) N40 σ* C47-H49 5.59 0.64 0.059
LP(1) O51 σ* C32-C38 2.88 1.16 0.052
LP(1) O30 σ* N17-C21 1.98 1.07 0.042
LP(2) O51 σ* C43-H44 0.91 0.67 0.023
LP(2) O51 π* C2-C3 0.62 0.27 0.012

LP—Lone pair, E(2)—Stabilization energy, E(i)−E(j)—Energy difference between the donor and acceptor NBO orbitals, F(i,j)—Fock matrix element between i and j NBO orbitals.