Vibrational Frequencies calculated at wB97X-D/aug-cc-pVTZ
| 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 |
3480 |
3329 |
3.68 |
|
|
|
| 2 |
A1 |
1349 |
1290 |
46.61 |
|
|
|
| 3 |
A1 |
644 |
616 |
3.15 |
|
|
|
| 4 |
E |
3579 |
3424 |
74.47 |
|
|
|
| 4 |
E |
3579 |
3424 |
74.57 |
|
|
|
| 5 |
E |
1659 |
1587 |
32.86 |
|
|
|
| 5 |
E |
1659 |
1587 |
32.94 |
|
|
|
| 6 |
E |
863 |
826 |
12.78 |
|
|
|
| 6 |
E |
863 |
826 |
12.79 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8838.0 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 8454.5 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-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
0.216 |
|
|
|
| 2 |
S |
-0.517 |
|
|
|
| 3 |
H |
0.101 |
|
|
|
| 4 |
H |
0.101 |
|
|
|
| 5 |
H |
0.101 |
|
|
|
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 |
-6.010 |
6.010 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.351 |
0.000 |
0.000 |
| y |
0.000 |
-21.351 |
0.000 |
| z |
0.000 |
0.000 |
-15.062 |
|
| Traceless |
| | x | y | z |
| x |
-3.145 |
0.000 |
0.000 |
| y |
0.000 |
-3.145 |
0.000 |
| z |
0.000 |
0.000 |
6.290 |
|
| Polar |
| 3z2-r2 | 12.579 |
| 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 |
5.437 |
0.000 |
0.000 |
| y |
0.000 |
5.443 |
-0.001 |
| z |
0.000 |
-0.001 |
6.134 |
<r2> (average value of r
2) Å
2
| <r2> |
37.949 |
| (<r2>)1/2 |
6.160 |