Vibrational Frequencies calculated at wB97X-D/aug-cc-pVDZ
| 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 |
3474 |
3326 |
4.03 |
|
|
|
| 2 |
A1 |
1325 |
1269 |
43.45 |
|
|
|
| 3 |
A1 |
639 |
611 |
3.36 |
|
|
|
| 4 |
E |
3588 |
3435 |
73.35 |
|
|
|
| 4 |
E |
3588 |
3435 |
73.44 |
|
|
|
| 5 |
E |
1626 |
1556 |
32.81 |
|
|
|
| 5 |
E |
1626 |
1556 |
32.88 |
|
|
|
| 6 |
E |
847 |
811 |
16.66 |
|
|
|
| 6 |
E |
847 |
811 |
16.68 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8779.6 cm
-1
Scaled (by 0.9573) Zero Point Vibrational Energy (zpe) 8404.8 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 wB97X-D/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.179 |
|
|
|
| 2 |
S |
-0.176 |
|
|
|
| 3 |
H |
0.118 |
|
|
|
| 4 |
H |
0.118 |
|
|
|
| 5 |
H |
0.118 |
|
|
|
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 |
-6.064 |
6.064 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.440 |
0.000 |
0.000 |
| y |
0.000 |
-21.440 |
0.000 |
| z |
0.000 |
0.000 |
-15.054 |
|
| Traceless |
| | x | y | z |
| x |
-3.193 |
0.000 |
0.000 |
| y |
0.000 |
-3.193 |
0.000 |
| z |
0.000 |
0.000 |
6.385 |
|
| Polar |
| 3z2-r2 | 12.771 |
| 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 |
4.930 |
0.000 |
0.000 |
| y |
0.000 |
4.933 |
-0.000 |
| z |
0.000 |
-0.000 |
6.088 |
<r2> (average value of r
2) Å
2
| <r2> |
38.391 |
| (<r2>)1/2 |
6.196 |