Vibrational Frequencies calculated at B1B95/aug-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 |
3171 |
3171 |
28.88 |
|
|
|
| 2 |
A1 |
1848 |
1848 |
438.38 |
|
|
|
| 3 |
A1 |
1371 |
1371 |
0.82 |
|
|
|
| 4 |
A1 |
878 |
878 |
14.79 |
|
|
|
| 5 |
B1 |
722 |
722 |
76.89 |
|
|
|
| 6 |
B1 |
433 |
433 |
7.89 |
|
|
|
| 7 |
B2 |
3255 |
3255 |
4.62 |
|
|
|
| 8 |
B2 |
924 |
924 |
0.33 |
|
|
|
| 9 |
B2 |
366 |
366 |
2.62 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6482.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 6482.8 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 B1B95/aug-cc-pV(T+d)Z
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.883 |
|
|
|
| 2 |
C |
0.220 |
|
|
|
| 3 |
S |
-0.142 |
|
|
|
| 4 |
H |
0.403 |
|
|
|
| 5 |
H |
0.403 |
|
|
|
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 |
-1.070 |
1.070 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-27.334 |
0.000 |
0.000 |
| y |
0.000 |
-23.395 |
0.000 |
| z |
0.000 |
0.000 |
-21.457 |
|
| Traceless |
| | x | y | z |
| x |
-4.908 |
0.000 |
0.000 |
| y |
0.000 |
1.001 |
0.000 |
| z |
0.000 |
0.000 |
3.907 |
|
| Polar |
| 3z2-r2 | 7.814 |
| x2-y2 | -3.939 |
| 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 |
4.987 |
0.000 |
0.000 |
| y |
0.000 |
4.910 |
0.000 |
| z |
0.000 |
0.000 |
11.439 |
<r2> (average value of r
2) Å
2
| <r2> |
66.247 |
| (<r2>)1/2 |
8.139 |