Vibrational Frequencies calculated at B3PW91/6-31G*
| 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 |
3181 |
3044 |
23.70 |
|
|
|
| 2 |
A1 |
1857 |
1777 |
361.39 |
|
|
|
| 3 |
A1 |
1391 |
1331 |
0.95 |
|
|
|
| 4 |
A1 |
869 |
831 |
17.16 |
|
|
|
| 5 |
B1 |
708 |
678 |
97.79 |
|
|
|
| 6 |
B1 |
427 |
408 |
1.81 |
|
|
|
| 7 |
B2 |
3263 |
3122 |
3.73 |
|
|
|
| 8 |
B2 |
941 |
900 |
0.33 |
|
|
|
| 9 |
B2 |
362 |
346 |
1.70 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6499.6 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 6218.1 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 B3PW91/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.520 |
|
|
|
| 2 |
C |
0.103 |
|
|
|
| 3 |
S |
-0.025 |
|
|
|
| 4 |
H |
0.221 |
|
|
|
| 5 |
H |
0.221 |
|
|
|
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 |
-1.369 |
1.369 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.966 |
0.000 |
0.000 |
| y |
0.000 |
-22.920 |
0.000 |
| z |
0.000 |
0.000 |
-21.191 |
|
| Traceless |
| | x | y | z |
| x |
-4.911 |
0.000 |
0.000 |
| y |
0.000 |
1.159 |
0.000 |
| z |
0.000 |
0.000 |
3.752 |
|
| Polar |
| 3z2-r2 | 7.503 |
| x2-y2 | -4.046 |
| 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 |
2.442 |
0.000 |
0.000 |
| y |
0.000 |
3.226 |
0.000 |
| z |
0.000 |
0.000 |
10.253 |
<r2> (average value of r
2) Å
2
| <r2> |
66.915 |
| (<r2>)1/2 |
8.180 |