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. 2021 Jul 9;7(7):e07529. doi: 10.1016/j.heliyon.2021.e07529

Table 2.

Observed and calculated vibrational frequency of 2-chloroquinoline-3-carboxaldehyde at B3LYP with 6–311++G (d,p) basis set.

SI.
No
Experimental
Theoretical
IR
Raman
Raman
Intensity
c(IRaman)
dAssignments
Frequency (cm−1)
Frequencies (cm−1)
Intensity
Activity
FT-IR FT-Raman Unscaled ascaled bRelative Absolute cRelative Absolute
1 3107(w) 3062 (vs) 3203 3078 5 1 202 57 0.399 ʋCH(95)
2 3058(w) 3040 (vw) 3192 3067 13 3 216 61 0.433 ʋCH(100)
3 3041(m) 3176 3052 7 2 115 32 0.235 ʋCH(88)
4 2928(m) 3020 (vw) 3167 3043 2 0 56 16 0.116 ʋCH(90)
5 2870(s) 2873(s) 3153 3030 4 1 65 18 0.137 ʋCH(99)
6 2750 (vw) 2767(m) 2869 2757 108 30 137 39 0.411 ʋCH(100)
7 1685(s) 1682 (vs) 1786 1717 367 100 212 60 2.952 ʋOC(90)
8 1612(s) 1661(m) 1654 1590 79 21 106 30 1.831 ʋCC(57)
9 1577 (vs) 1612 (vs) 1625 1561 165 45 42 12 0.764 ʋNC(18)+ʋCC(32)+βHCC(13)
10 1489(s) 1579 (vs) 1593 1530 80 22 46 13 0.878 ʋNC(13)+ʋCC(23)+βCCC(10)
11 1454(m) 1490(s) 1522 1463 19 5 10 3 0.222 ʋCC(11)+βHCC(11)
12 1456(m) 1485 1427 12 3 7 2 0.158 ʋNC(11)+ʋCC(10)+βHCC(36)
13 1370(s) 1413(w) 1450 1394 8 2 40 11 0.987 βHCO(57)
14 1332(s) 1383 (vs) 1423 1367 41 11 355 100 9.278 ʋCC(10)+ʋNC(11)+βHCO(10)+βCCC(11)
15 1329(m) 1383 1329 15 4 36 10 1.000 ʋCC(19)+βHCO(16)
16 1370 1317 39 11 39 11 1.134 ʋNC(22)+ʋCC(33)+βHCC(16)
17 1212(m) 1218(w) 1331 1279 4 1 15 4 0.465 ʋCC(14)+ʋNC(13)+βHCC(20)
18 1167(m) 1274 1224 4 1 2 1 0.084 ʋCC(11)+βHCC(38)
19 1165 (vs) 1143(m) 1247 1198 10 3 4 1 0.141 ʋCC(26)+ʋNC(20)+βHCC(12)
20 1131(s) 1192 1146 44 12 27 8 1.111 ʋCC(14)+βHCC(38)
21 1171 1125 6 2 11 3 0.479 βHCC(56)
22 1045 (vs) 1156 1111 31 9 3 1 0.115 βHCC(51)
23 970(m) 1016(s) 1060 1019 152 41 2 1 0.116 ʋCC(10)+ʋClC(11)+βCNC(21)
24 939(m) 1037 996 0 0 30 9 1.789 ʋCC(54)+βHCC(13)
25 1018 979 2 0 4 1 0.230 τHCCC(49)+τOCCC(33)
26 911(s) 950 (vw) 1007 968 0 0 0 0 0.013 τHCCC(81)+τCCCC(11)
27 981 943 3 1 0 0 0.024 τHCCC(78)
28 872(w) 900 (vw) 935 899 14 4 0 0 0.005 τHCCC(76)
29 909 874 7 2 1 0 0.070 ʋCC(11)+ʋNC(10)+βCCC(38)
30 806(m) 808(s) 879 845 5 1 0 0 0.005 τHCCC(80)
31 776(w) 750(s) 809 778 14 4 33 9 3.483 βCCC(23)
32 760(s) 784 753 25 7 0 0 0.008 τHCCC(16)+τCNCC(20)+τCCCC(35)+ωNCCC(12)
33 769 739 66 18 8 2 0.980 βOCC(27)+βCCC(15)
34 767 738 38 10 0 0 0.014 τHCCC(51)+τCCCC(11)
35 678(m) 640 (vw) 696 669 1 0 0 0 0.072 τCCCC(32)+τClCNC(24)
36 621(w) 600 (vw) 671 644 14 4 5 1 0.794 ʋClC(11)+βCNC(13)+βCCC(20)+βNCC(13)
37 592(w) 621 596 15 4 2 0 0.304 βCCC(48)
38 550 (vw) 599 576 2 0 3 1 0.653 ʋClC(15)+βCCC(34)
39 543 522 1 0 0 0 0.052 τHCCC(21)+τCNCC(12)+τCCCC(11)+ωClCNC(19)
40 486(w) 476(w) 492 473 5 1 0 0 0.001 τCCCC(11)+ωNCCC(17)+ωCCCC(36)
41 450(w) 456 439 11 3 4 1 1.435 βOCC(11)+βCCC(26)+βClCN(17)
42 410(w) 424 407 1 0 2 1 0.825 τCCCC(41)+ωClCNC(10)+ωCCCC(19)
43 320(s) 378 363 3 1 18 5 10.85 ʋClC(18)
44 348 335 3 1 5 1 3.733 ʋCC(14)+ʋClC(24)+βOCC(16)
45 250(w) 298 286 0 0 0 0 0.422 τHCCC(13)+ωClCNC(21)+ωCCCC(38)
46 240(w) 271 260 0 0 1 0 0.680 τCNCC(16)+τCCCC(47)
47 200(m) 227 218 0 0 1 0 1.728 βNCC(20)+βClCN(47)
48 194 187 5 1 0 0 0.177 βOCC(12)+βCCC(60)
49 110(s) 145 140 9 3 1 0 3.242 τHCCC(12)+τOCCC(26)+τCCCC(22)+ωCCCC(16)
50 80(s) 98 94 0 0 0 0 4.771 τCCCC(36)+ωNCCC(25)
51 48 46 3 1 2 1 100.0 τOCCC(20)+τCNCC(18)+τCCCC(10)+ωCCCC(17)
a

Scaling factor: 0.961 for B3LYP/6–311++G (d,p).

b

Relative absorption intensities normalized with higher peak absorption equal to 100.

c

Relative Raman activities normalized to 100. Relative Raman intensities calculated by Eq. (1) and normalized to 100.

d

ʋ-Stretching β-in plane bending ω-out plane pending τ-torsion.