Vibrational Frequencies calculated at B1B95/6-31G(2df,p)
Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
1 |
A |
3734 |
3576 |
32.73 |
|
|
|
2 |
A |
3675 |
3519 |
33.16 |
|
|
|
3 |
A |
3612 |
3459 |
20.57 |
|
|
|
4 |
A |
3156 |
3023 |
17.61 |
|
|
|
5 |
A |
3141 |
3008 |
23.51 |
|
|
|
6 |
A |
3060 |
2931 |
16.94 |
|
|
|
7 |
A |
3040 |
2912 |
25.80 |
|
|
|
8 |
A |
2998 |
2872 |
45.02 |
|
|
|
9 |
A |
1838 |
1761 |
461.66 |
|
|
|
10 |
A |
1616 |
1548 |
161.02 |
|
|
|
11 |
A |
1530 |
1465 |
3.40 |
|
|
|
12 |
A |
1499 |
1435 |
2.40 |
|
|
|
13 |
A |
1486 |
1423 |
6.18 |
|
|
|
14 |
A |
1456 |
1394 |
213.22 |
|
|
|
15 |
A |
1445 |
1384 |
58.88 |
|
|
|
16 |
A |
1403 |
1344 |
10.62 |
|
|
|
17 |
A |
1353 |
1296 |
16.73 |
|
|
|
18 |
A |
1298 |
1243 |
0.62 |
|
|
|
19 |
A |
1215 |
1164 |
19.47 |
|
|
|
20 |
A |
1169 |
1120 |
1.14 |
|
|
|
21 |
A |
1127 |
1079 |
17.29 |
|
|
|
22 |
A |
1072 |
1027 |
14.36 |
|
|
|
23 |
A |
1003 |
961 |
1.64 |
|
|
|
24 |
A |
901 |
863 |
2.32 |
|
|
|
25 |
A |
819 |
784 |
0.55 |
|
|
|
26 |
A |
784 |
751 |
45.78 |
|
|
|
27 |
A |
583 |
558 |
49.08 |
|
|
|
28 |
A |
554 |
530 |
48.52 |
|
|
|
29 |
A |
540 |
517 |
86.02 |
|
|
|
30 |
A |
474 |
454 |
25.46 |
|
|
|
31 |
A |
377 |
361 |
93.25 |
|
|
|
32 |
A |
354 |
339 |
1.81 |
|
|
|
33 |
A |
265 |
254 |
3.53 |
|
|
|
34 |
A |
191 |
183 |
3.26 |
|
|
|
35 |
A |
100 |
96 |
5.92 |
|
|
|
36 |
A |
57 |
55 |
0.86 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 26463.3 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 25343.9 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.429 |
|
|
|
2 |
H |
0.142 |
|
|
|
3 |
H |
0.140 |
|
|
|
4 |
H |
0.142 |
|
|
|
5 |
C |
-0.137 |
|
|
|
6 |
H |
0.114 |
|
|
|
7 |
H |
0.131 |
|
|
|
8 |
N |
-0.372 |
|
|
|
9 |
H |
0.262 |
|
|
|
10 |
N |
-0.588 |
|
|
|
11 |
H |
0.273 |
|
|
|
12 |
H |
0.261 |
|
|
|
13 |
C |
0.476 |
|
|
|
14 |
O |
-0.416 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-3.048 |
2.496 |
-0.668 |
3.996 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-37.588 |
6.708 |
-1.316 |
y |
6.708 |
-34.265 |
-1.473 |
z |
-1.316 |
-1.473 |
-37.179 |
|
Traceless |
| x | y | z |
x |
-1.866 |
6.708 |
-1.316 |
y |
6.708 |
3.119 |
-1.473 |
z |
-1.316 |
-1.473 |
-1.253 |
|
Polar |
3z2-r2 | -2.506 |
x2-y2 | -3.323 |
xy | 6.708 |
xz | -1.316 |
yz | -1.473 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
9.391 |
-0.100 |
0.158 |
y |
-0.100 |
7.660 |
-0.080 |
z |
0.158 |
-0.080 |
5.342 |
<r2> (average value of r
2) Å
2
<r2> |
200.073 |
(<r2>)1/2 |
14.145 |