Vibrational Frequencies calculated at B1B95/6-31G**
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3459 |
3302 |
2.92 |
|
|
|
| 2 |
A1 |
1395 |
1332 |
19.93 |
|
|
|
| 3 |
A1 |
620 |
592 |
4.68 |
|
|
|
| 4 |
E |
3566 |
3405 |
64.30 |
|
|
|
| 4 |
E |
3566 |
3405 |
64.30 |
|
|
|
| 5 |
E |
1701 |
1624 |
38.48 |
|
|
|
| 5 |
E |
1701 |
1624 |
38.48 |
|
|
|
| 6 |
E |
871 |
832 |
47.63 |
|
|
|
| 6 |
E |
871 |
832 |
47.63 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8875.1 cm
-1
Scaled (by 0.9548) Zero Point Vibrational Energy (zpe) 8474.0 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**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.836 |
|
|
|
| 2 |
S |
-0.388 |
|
|
|
| 3 |
H |
0.408 |
|
|
|
| 4 |
H |
0.408 |
|
|
|
| 5 |
H |
0.408 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-6.440 |
6.440 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.686 |
0.000 |
0.000 |
| y |
0.000 |
-20.686 |
0.000 |
| z |
0.000 |
0.000 |
-14.489 |
|
| Traceless |
| | x | y | z |
| x |
-3.099 |
0.000 |
0.000 |
| y |
0.000 |
-3.099 |
0.000 |
| z |
0.000 |
0.000 |
6.197 |
|
| Polar |
| 3z2-r2 | 12.394 |
| x2-y2 | 0.000 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.412 |
0.000 |
0.000 |
| y |
0.000 |
2.412 |
0.000 |
| z |
0.000 |
0.000 |
4.167 |
<r2> (average value of r
2) Å
2
| <r2> |
37.968 |
| (<r2>)1/2 |
6.162 |