Vibrational Frequencies calculated at HF/6-311G*
| 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 |
3980 |
3599 |
35.89 |
|
|
|
| 2 |
A |
3849 |
3481 |
40.38 |
|
|
|
| 3 |
A |
3277 |
2964 |
43.69 |
|
|
|
| 4 |
A |
3256 |
2944 |
46.01 |
|
|
|
| 5 |
A |
3209 |
2902 |
23.22 |
|
|
|
| 6 |
A |
3196 |
2891 |
31.85 |
|
|
|
| 7 |
A |
3179 |
2875 |
36.99 |
|
|
|
| 8 |
A |
1962 |
1774 |
411.36 |
|
|
|
| 9 |
A |
1809 |
1636 |
120.43 |
|
|
|
| 10 |
A |
1634 |
1478 |
11.83 |
|
|
|
| 11 |
A |
1626 |
1471 |
5.75 |
|
|
|
| 12 |
A |
1606 |
1453 |
5.44 |
|
|
|
| 13 |
A |
1563 |
1414 |
20.13 |
|
|
|
| 14 |
A |
1539 |
1392 |
56.94 |
|
|
|
| 15 |
A |
1409 |
1274 |
0.10 |
|
|
|
| 16 |
A |
1391 |
1258 |
155.04 |
|
|
|
| 17 |
A |
1230 |
1113 |
4.48 |
|
|
|
| 18 |
A |
1210 |
1094 |
0.86 |
|
|
|
| 19 |
A |
1153 |
1043 |
9.62 |
|
|
|
| 20 |
A |
1075 |
972 |
2.26 |
|
|
|
| 21 |
A |
888 |
803 |
11.88 |
|
|
|
| 22 |
A |
856 |
774 |
1.75 |
|
|
|
| 23 |
A |
676 |
611 |
13.04 |
|
|
|
| 24 |
A |
655 |
592 |
20.34 |
|
|
|
| 25 |
A |
536 |
485 |
5.61 |
|
|
|
| 26 |
A |
476 |
430 |
4.43 |
|
|
|
| 27 |
A |
275 |
249 |
10.19 |
|
|
|
| 28 |
A |
234 |
212 |
6.89 |
|
|
|
| 29 |
A |
218 |
197 |
282.99 |
|
|
|
| 30 |
A |
34 |
31 |
0.36 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 24000.2 cm
-1
Scaled (by 0.9044) Zero Point Vibrational Energy (zpe) 21705.8 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 HF/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
H |
0.379 |
0.459 |
|
0.464 |
| 2 |
H |
0.375 |
0.416 |
|
0.417 |
| 3 |
N |
-0.897 |
-1.104 |
|
-1.107 |
| 4 |
O |
-0.477 |
-0.640 |
|
-0.626 |
| 5 |
C |
0.654 |
0.874 |
|
0.849 |
| 6 |
H |
0.226 |
0.005 |
|
0.016 |
| 7 |
H |
0.226 |
0.022 |
|
0.032 |
| 8 |
C |
-0.541 |
0.001 |
|
0.007 |
| 9 |
H |
0.205 |
0.050 |
|
0.076 |
| 10 |
H |
0.221 |
0.051 |
|
0.082 |
| 11 |
H |
0.227 |
0.051 |
|
0.081 |
| 12 |
C |
-0.596 |
-0.183 |
|
-0.289 |
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.803 |
-3.775 |
0.390 |
3.879 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
-0.776 |
-3.761 |
0.416 |
3.863 |
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.879 |
2.439 |
-0.790 |
| y |
2.439 |
-33.460 |
-0.481 |
| z |
-0.790 |
-0.481 |
-31.438 |
|
| Traceless |
| | x | y | z |
| x |
6.570 |
2.439 |
-0.790 |
| y |
2.439 |
-4.801 |
-0.481 |
| z |
-0.790 |
-0.481 |
-1.768 |
|
| Polar |
| 3z2-r2 | -3.537 |
| x2-y2 | 7.581 |
| xy | 2.439 |
| xz | -0.790 |
| yz | -0.481 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.514 |
0.281 |
0.017 |
| y |
0.281 |
6.321 |
-0.002 |
| z |
0.017 |
-0.002 |
4.523 |
<r2> (average value of r
2) Å
2
| <r2> |
127.367 |
| (<r2>)1/2 |
11.286 |