Mode |
Computed Frequencies |
Observed Freq. |
PEDs |
Mode Assignment |
Unscaled |
Scaled |
Raman |
IR |
ν1 |
3835(75,134)0.23 |
3662 |
- |
3430# |
ν(O23-H24)(100) |
ν(O23-H24) |
ν2 |
3576(24,51)0.75 |
3415 |
- |
- |
νasym(NH2)(100) |
νasym(NH2) |
ν3 |
3507(12,94)0.13 |
3349 |
- |
- |
νsym(NH2)(90)-ν(O21-H22)(10) |
νsym(NH2) |
ν4 |
3481(251,115)0.07 |
3324 |
3207# |
3207 |
ν(O21-H22)(89)+ ν(N16-H18)(7) |
ν(O21-H22) |
ν5 |
3194(4,144)0.22 |
3050 |
3061# |
3041, 3068# |
ν(C6-H10)(94) |
ν(CH) |
ν6 |
3166(9,135)0.16 |
3024 |
3042# |
3025, 3042# |
ν(C3-H8)(65)+ ν(C2-H7)(33) |
ν(CH) |
ν7 |
3160(8,48)0.51 |
3018 |
3027# |
3024# |
ν(C5-H9)(92) |
ν(CH) |
ν8 |
3149(16,64)0.61 |
3007 |
3014# |
3014# |
ν(C2-H7)(66)-ν(C3-H8)(33) |
ν(CH) |
ν9 |
3090(6,50)0.41 |
2951 |
2950# |
2960, 2962# |
νasym(CH2)(98) |
νasym(CH2) |
ν10 |
3043(23,25)0.21 |
2906 |
2923# |
2931, 2928# |
νsym(CH2)(60)- ν(C12-H15)(39) |
νsym(CH2) |
ν11 |
3032(5,116)0.10 |
2896 |
2863# |
2894, 2864# |
ν(C12-H15)(59)+ νsym(CH2)(40) |
ν(C12-H15) |
ν12 |
1835(374,15)0.27 |
1752 |
- |
1630# |
ν(C19-O20)(78) |
ν(C19-O20) |
ν13 |
1663(29,5)0.74 |
1588 |
1587, 1590# |
1582, 1589# |
d(NH2)(95) |
d(NH2) |
ν14 |
1653(49,56)0.52 |
1579 |
1567 |
1579 |
ν(C5-C6)(20)+ ν(C2-C3)(18)-ν(C1-C6)(10)-ν(C3-C4)(10)+ α2(R)(11)+β(C3-H8)(6) |
ν(R) |
ν15 |
1629(15,5)0.72 |
1556 |
1551, 1531# |
1572, 1532# |
ν(C1-C2)(24)+ ν(C4-C5)(17)-ν(C1-C6)(16)-ν(C3-C4)(10)- α3(R)(8) |
ν(R) |
ν16 |
1543(105,2)0.70 |
1474 |
1481, 1463# |
1453, 1454# |
ν(C1-C6)(10)-ν(C3-C4)(10)+ν(C1-C2)(9)-ν(C4-C5)(7)-β(C6-H10)(10)+β(C2-H7)(14)+β(C3-H8)(12)-β(C5-H9)(13)-ν(C1-O23)(8) |
β(CH) |
ν17 |
1489(6,6)0.73 |
1422 |
1419, 1414# |
1435, 1438# |
d(CH2)(89) |
d(CH2) |
ν18 |
1466(13,0)0.75 |
1400 |
- |
1417, 1416# |
ν(C5-C6)(17)+ν(C2-C3)(16)+ν(C4-C5)(6)+β(C6-H10)(12)+β(C2-H7)(9)-β(C3-H8)(7)- α(C1-O23-H24)(8) |
ν(R) |
ν19 |
1412(433,6)0.61 |
1348 |
1365, 1368# |
1363, 1367# |
α(C19-O21-H22)(65)- ν(C1-C6)(15) |
α(C19-O21-H22) |
ν20 |
1376(14,21)0.40 |
1314 |
1327, 1328# |
1332, 1328# |
α(C11-C12-H15) (23)- w(CH2)(23)- r(CH2)(11)- ν(C11-C12)(6) |
α(C11-C12-H15) |
ν21 |
1361(30,1)0.58 |
1300 |
- |
- |
β(C5-H9)(11)+β(C3-H8)(10)- α(C1-O23-H24)(11)- α(N16-C12-H15)(10)+ ν(C2-C3)(9)-ν(C1-C2)(8)-ν(C5-C6)(7)-ν(C3-C4)(6) ν(C3-C4)(6)+ν(C1-C6)(6)+ w(CH2)(6) |
β(CH) |
ν22 |
1358(19,9)0.32 |
1297 |
- |
1286# |
α(N16-C12-H15) (27)- w(CH2)(25)+ β(C5-H9)(7) |
α(N16-C12-H15) |
ν23 |
1344(3,4)0.46 |
1284 |
1284, 1286# |
1267 |
α(C11-C12-H15)(14)+ ν(C3-C4)(9)-ν(C4-C5)(8)+ν(C5-C6)(5)+ β(C2-H7)(8)+ β(C6-H10)(8) + α(N16-C12-H15) (8)+ r(CH2)(6) |
ν(R) |
ν24 |
1292(4,1)0.67 |
1234 |
- |
1247, 1246# |
w(CH2)(22)+ r(NH2) (21)+ α(N16-C12-H15) (12)+ α(C11-C12-H15) (11) |
w(CH2) |
ν25 |
1288(4,14)0.25 |
1230 |
1249, 1247# |
1243 |
α(N16-C12-H15) (24)- r(CH2)(16)+ α(C11-C12-H15)(14)- r(NH2)(11) |
r(CH2) |
ν26 |
1280(115,12)0.03 |
1222 |
1214, 1212# |
1214, 1213# |
ν(C1-O23)(47)- α1(R)(9)-ν(C2-C3)(8)+ β(C2-H7)(8) |
ν(C1-O23) |
ν27 |
1225(2,27)0.09 |
1170 |
1164, 1178# |
1176, 1177# |
ν(C4-C11)(39)- α1(R)(13)- ν(C2-C3)(6)-ν(C3-C4)(6)-ν(C4-C5)(6) |
ν(R) |
ν28 |
1210(18,7)0.73 |
1156 |
1156, 1150# |
1155, 1153# |
ν(C19-O21)(33)- ν(C12-C19)(16)+ r(CH2)(13)+α(C19-O21-H22)(8)- d(COOH)(6)+ r(COOH) (6)+ w(NH2)(6) |
ν(C19-O21) |
ν29 |
1195(3,4)0.31 |
1141 |
- |
- |
β(C2-H7)(26)- β(C3-H8)(18)-β(C6-H10)(17)- β(C5-H9)(16)+ ν(C2-C3)(7) |
β(CH) |
ν30 |
1187(207,12)0.11 |
1134 |
1114, 1113# |
1113, 1112# |
α(C1-O23-H24)(48)+ ν(C1-C6)(15)+ β(C6-H10)(8)- ν(C1-O23)(7)- ν(C1-C2)(6) |
α(C-OH)/OH |
ν31 |
1160(10,3)0.44 |
1108 |
1100, 1098# |
- |
r(NH2)(19)- r(CH2)(18)- α(C11-C12-H15) (17)+ ν(C19-O21)(6) |
r(NH2) |
ν32 |
1120(20,1)0.66 |
1070 |
- |
1099, 1099# |
β(C6-H10)(12)- β(C5-H9)(10)+ β(C2-H7)(9)- β(C3-H8)(7)+ ν(C2-C3)(10)- ν(C5-C6)(9)+ ν(C12-N16)(8) |
β(CH) |
ν33 |
1097(14,12)0.54 |
1048 |
1045, 1046# |
1042, 1046# |
ν(C12-N16)(39)- ν(C11-C12)(15)+ r(CH2)(7)- β(C12-C19)(6) |
ν(C11-C12) |
ν34 |
1029(0,0)0.04 |
983 |
- |
- |
α1(R)(49)+ ν(C1-C6)(11)+ ν(C1-C2)(10)- ν(C3-C4)(7)- ν(C4-C5)(7) |
α1(R) |
ν35 |
979(48,6)0.29 |
958 |
986, 985# |
986, 988# |
τ(CH2)(15)- γ(C5-H9)(14)+ w(NH2) (10)+ γ(C6-H10)(8)- r(NH2)(6)- w(NH2)(6) |
τ(CH2) |
ν36 |
973(15,2)0.35 |
952 |
967# |
939, 939# |
γ(C5-H9)(37)- γ(C6-H10)(26)+ τ(CH2)(6) |
γ(CH) |
ν37 |
948(48,2)0.57 |
928 |
935, 938# |
929# |
w(NH2) (24)- ν(C11-C12)(23)+ γ(C3-H8)(14)+ ν(C12-C19)(7) |
ν(C12-C19) |
ν38 |
942(7,1)0.74 |
922 |
894, 897# |
- |
γ(C3-H8)(43)- γ(C2-H7)(16)- Φ1(R)(13) |
γ(CH) |
ν39 |
887(22,16)0.02 |
868 |
878 |
896, 899# |
γ(C6-H10)(10)+ α(C4-C11-C12)(10)+ w(NH2) (10)+ γ(C2-H7)(9)+ w(COOH)(7)- γ(C4-C11)(6) |
w(NH2) |
ν40 |
874(46,1)0.52 |
855 |
855# |
878, 878# |
τ(C19-O21)(33)+ τ(CH2)(13)- ν(C12-N16)(13)- w(NH2) (10)- ν(C11-C12)(8) |
ν(C12-N16) |
ν41 |
855(51,12)0.14 |
837 |
845, 846# |
842, 842# |
τ(C19-O21)(36)+ w(NH2)(9)- τ(CH2)(7)- α2(R)(7)+ ν(C12-N16)(6) |
τ(C19-O21) |
ν42 |
846(20,11)0.04 |
828 |
828, 829# |
829, 830# |
w(NH2) (21)+ τ(C19-O21)(13)- ν(C12-C19)(10)+ α3(R)(8)+ ν(C1-O23)(7)+ ν(C1-C6)(6) |
ν(R) |
ν43 |
837(29,2)0.09 |
819 |
808 |
803, 808# |
γ(C6-H10)(40)+γ(C5-H9)(28)- γ(C1-O23)(8) |
γ(CH) |
ν44 |
815(25,1)0.17 |
798 |
796, 797# |
793, 799# |
γ(C2-H7)(56)+γ(C3-H8)(22)- γ(C1-O23)(7) |
γ(CH) |
ν45 |
792(14,8)0.09 |
775 |
741, 738# |
741, 739# |
α1(R)(17)-ν(C12-C19)(12)-ν(C1-O23)(10)- d(COOH)(10) + ν(C4-C11)(9)+ w(COOH) (8)- ν(C19-O21)(6) |
w(COOH) |
ν46 |
730(2,2)0.72 |
714 |
- |
- |
Φ1(R)(60)+γ(C4-C11)(12)-γ(C1-O23)(12)- w(COOH) (6) |
Φ1(R) |
ν47 |
702(12,6)0.05 |
687 |
714, 714# |
713, 715# |
w(COOH) (24)+ Φ1(R)(16)- ν(C4-C11)(10)- d(COOH)(8)- ν(C11-C12)(7)- α1(R)(7) |
ν(C4-C11) |
ν48 |
657(3,2)0.66 |
643 |
- |
646# |
d(COOH)(34)+w(NH2)(22)+Φ1(R)(10)+w(COOH) (10) |
d(COOH) |
ν49 |
655(1,5)0.75 |
641 |
641, 642# |
651 |
α3(R)(79) |
α3(R) |
ν50 |
565(11,2)0.46 |
553 |
574, 574# |
576, 575# |
ρ(COOH)(16)+γ(C1-O23)(11)+w(NH2)(11)+α(C11-C12-N16) (10)- Φ2(R)(8)- α(C4-C11-C12)(6)- α2(R)(6) |
r(COOH) |
ν51 |
526(14,1)0.33 |
515 |
528, 534# |
530, 535# |
γ(C1-O23)(27) + γ(C4-C11)(13)- Φ2(R)(25)+ d(COOH)(7) - ρ(COOH) (7) |
Φ2(R) |
ν52 |
492(9,3)0.40 |
481 |
492, 496# |
495, 499# |
α2(R)(39)+ γ(C1-O23)(11)- Φ2(R)(10) |
α2(R) |
ν53 |
428(11,0)0.59 |
419 |
- |
434, 435# |
β(C1-O23)(46)- α3(R)(16)+ β(C4-C11)(13)+ Φ3(R)(11) |
β(C1-O23) |
ν54 |
423(3,0)0.35 |
414 |
- |
408# |
Φ3(R)(76) |
Φ3(R) |
ν55 |
409(4,3)0.32 |
400 |
380, 386# |
388# |
α(C11-C12-N16) (37)+ w(COOH)(7)- Φ1(R)(6) |
α(N16-C12-C11) |
ν56 |
347(7,3)0.58 |
340 |
338# |
340# |
α(C11-C12-N16) (22)+ Φ1(R)(16)- γ(C4-C11)(10)+ γ(C1-O23)(10) |
γ(C1-O23) |
ν57 |
340(8,2)0.28 |
333 |
336, 331# |
327# |
α(N16-C12-C19) (40)- ρ(COOH) (29) |
α(N16-C12-C19) |
ν58 |
310(96,1)0.71 |
303 |
311, 313# |
313# |
τ(C1-O23)(89) |
τ(C1-O23) |
ν59 |
307(15,0)0.74 |
300 |
-- |
-- |
τ(C12-N16)(41)- τ(C19-O21)(20)- β(C4-C11)(13) |
β(C4-C11) |
ν60 |
296(27,0)0.73 |
290 |
- |
294# |
τ(C12-N16)(41)+β(C4-C11)(16)-τ(C19-O21)(8)-β(C12-C19)(7) |
τ(C12-N16) |
ν61 |
186(0,1)0.13 |
182 |
196# |
- |
Φ2(R)(24)- α(C11-C12-C19) (16)- α(C4-C11-C12)(14)- ν(C4-C11)(6)- γ(C4-C11)(6)- γ(C12-C19)(6) |
α(C4-C11-C12) |
ν62 |
169(9,1)0.66 |
165 |
167# |
-- |
α(C11-C12-C19) (34)+ Φ2(R)(32)+γ(C12-C19)(7)- α(C4-C11-C12)(7) |
α(C11-C12-C19) |
ν63 |
83(1,1)0.75 |
81 |
-- |
-- |
τ(C12-C19)(58)- τ(C12-N16)(14)- τ(C19-O21)(10) |
τ(C12-C19) |
ν64 |
63(1,1)0.71 |
62 |
-- |
-- |
τ(C12-C19)(31)-γ(C4-C11)(14)-α(C4-C11-C12)(12)-Φ2(R)(9)-τ(C12-N16)(9)+α(C11-C12-C19) (7)-τ(C19-O21)(6) |
γ(C4-C11) |
ν65 |
46(3,1)0.75 |
45 |
-- |
-- |
τ(C11-C12)(46)+ τ(C12-C19)(20)- τ(C12-N16)(7) |
τ(R’’) |
ν66 |
40(1,4)0.75 |
39 |
-- |
-- |
τ(C4-C11)(57)+ τ(C12-C19)(18)- τ(C12-N16)(9) |
τ(R’) |
The number before the modes are the % potential energy calculated using normal coordinate analysis. The modes contributing with ≤ 5% have been omitted. The
abbreviations ν, δ, α(R), Φ1(R), ν(R), β, γ, α(A-B-C), ω, ρ, τ asym and sym have been used for stretching, scissoring, ring planar deformation, ring non-planar deformation,
ring stretching, in plane bending, out of plane bending, angle bending, wagging, rocking, torsion, anti-symmetric and symmetric respectively.
Calculated wave numbers up to 1000 cm-1 were scaled by the scale factor 0.9786 and those above 1000 cm-1 by the scale factor 0.9550 for larger wave numbers.
Number outside bracket is frequency in cm-1 unit, numbers within the bracket are IR intensity (approximate) and Raman activity (approximate) and number outside bracket
is depolarization ratio. The values superscripted with # are taken from literature Ref.-[6] |