Vibrational Frequencies calculated at HSEh1PBE/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 |
A1 |
3464 |
3318 |
2.89 |
|
|
|
| 2 |
A1 |
1332 |
1276 |
22.57 |
|
|
|
| 3 |
A1 |
643 |
615 |
2.01 |
|
|
|
| 4 |
E |
3569 |
3418 |
69.90 |
|
|
|
| 4 |
E |
3569 |
3418 |
69.88 |
|
|
|
| 5 |
E |
1651 |
1581 |
32.74 |
|
|
|
| 5 |
E |
1651 |
1581 |
32.73 |
|
|
|
| 6 |
E |
854 |
818 |
27.13 |
|
|
|
| 6 |
E |
854 |
818 |
27.11 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8793.1 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 8421.2 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 HSEh1PBE/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.480 |
|
|
|
| 2 |
S |
-0.534 |
|
|
|
| 3 |
H |
0.338 |
|
|
|
| 4 |
H |
0.338 |
|
|
|
| 5 |
H |
0.338 |
|
|
|
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 |
-6.192 |
6.192 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.651 |
0.000 |
0.000 |
| y |
0.000 |
-20.651 |
0.000 |
| z |
0.000 |
0.000 |
-14.677 |
|
| Traceless |
| | x | y | z |
| x |
-2.987 |
0.000 |
0.000 |
| y |
0.000 |
-2.987 |
0.000 |
| z |
0.000 |
0.000 |
5.974 |
|
| Polar |
| 3z2-r2 | 11.948 |
| 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 |
3.176 |
0.000 |
0.000 |
| y |
0.000 |
3.175 |
-0.000 |
| z |
0.000 |
-0.000 |
4.606 |
<r2> (average value of r
2) Å
2
| <r2> |
37.437 |
| (<r2>)1/2 |
6.119 |