Vibrational Frequencies calculated at PBEPBE/cc-pV(T+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 |
A1 |
3078 |
3056 |
26.66 |
|
|
|
| 2 |
A1 |
1790 |
1776 |
354.25 |
|
|
|
| 3 |
A1 |
1319 |
1309 |
3.70 |
|
|
|
| 4 |
A1 |
846 |
840 |
10.22 |
|
|
|
| 5 |
B1 |
651 |
647 |
81.34 |
|
|
|
| 6 |
B1 |
412 |
409 |
5.24 |
|
|
|
| 7 |
B2 |
3156 |
3132 |
4.26 |
|
|
|
| 8 |
B2 |
889 |
882 |
0.00 |
|
|
|
| 9 |
B2 |
351 |
349 |
2.85 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6246.0 cm
-1
Scaled (by 0.9926) Zero Point Vibrational Energy (zpe) 6199.8 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 PBEPBE/cc-pV(T+d)Z
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.307 |
|
|
|
| 2 |
C |
0.032 |
|
|
|
| 3 |
S |
-0.006 |
|
|
|
| 4 |
H |
0.140 |
|
|
|
| 5 |
H |
0.140 |
|
|
|
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 |
-1.020 |
1.020 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-27.275 |
0.000 |
0.000 |
| y |
0.000 |
-23.369 |
0.000 |
| z |
0.000 |
0.000 |
-21.370 |
|
| Traceless |
| | x | y | z |
| x |
-4.906 |
0.000 |
0.000 |
| y |
0.000 |
0.954 |
0.000 |
| z |
0.000 |
0.000 |
3.952 |
|
| Polar |
| 3z2-r2 | 7.904 |
| x2-y2 | -3.906 |
| 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 |
3.590 |
0.000 |
0.000 |
| y |
0.000 |
4.002 |
0.000 |
| z |
0.000 |
0.000 |
11.124 |
<r2> (average value of r
2) Å
2
| <r2> |
67.210 |
| (<r2>)1/2 |
8.198 |