Vibrational Frequencies calculated at PBEPBE/cc-pV(D+d)Z
| 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 |
2559 |
2559 |
1.31 |
|
|
|
| 2 |
A |
832 |
832 |
0.42 |
|
|
|
| 3 |
A |
472 |
472 |
0.15 |
|
|
|
| 4 |
A |
337 |
337 |
22.96 |
|
|
|
| 5 |
A |
199 |
199 |
0.03 |
|
|
|
| 6 |
B |
2556 |
2556 |
8.15 |
|
|
|
| 7 |
B |
818 |
818 |
11.07 |
|
|
|
| 8 |
B |
439 |
439 |
36.67 |
|
|
|
| 9 |
B |
355 |
355 |
18.40 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4283.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4283.2 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 PBEPBE/cc-pV(D+d)Z
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
-0.068 |
|
|
|
| 2 |
S |
-0.076 |
|
|
|
| 3 |
S |
-0.076 |
|
|
|
| 4 |
H |
0.110 |
|
|
|
| 5 |
H |
0.110 |
|
|
|
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 |
-0.631 |
0.631 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-37.003 |
-3.876 |
0.000 |
| y |
-3.876 |
-38.594 |
0.000 |
| z |
0.000 |
0.000 |
-40.933 |
|
| Traceless |
| | x | y | z |
| x |
2.761 |
-3.876 |
0.000 |
| y |
-3.876 |
0.374 |
0.000 |
| z |
0.000 |
0.000 |
-3.134 |
|
| Polar |
| 3z2-r2 | -6.269 |
| x2-y2 | 1.591 |
| xy | -3.876 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.693 |
-0.865 |
0.000 |
| y |
-0.865 |
11.586 |
0.000 |
| z |
0.000 |
0.000 |
5.715 |
<r2> (average value of r
2) Å
2
| <r2> |
142.510 |
| (<r2>)1/2 |
11.938 |