Vibrational Frequencies calculated at B3LYP/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 |
A' |
3162 |
3036 |
9.38 |
|
|
|
| 2 |
A' |
3093 |
2970 |
24.54 |
|
|
|
| 3 |
A' |
3027 |
2907 |
4.19 |
|
|
|
| 4 |
A' |
1507 |
1447 |
3.52 |
|
|
|
| 5 |
A' |
1416 |
1359 |
18.63 |
|
|
|
| 6 |
A' |
1401 |
1345 |
64.01 |
|
|
|
| 7 |
A' |
1169 |
1123 |
42.34 |
|
|
|
| 8 |
A' |
1096 |
1052 |
8.98 |
|
|
|
| 9 |
A' |
836 |
803 |
0.52 |
|
|
|
| 10 |
A' |
397 |
381 |
1.98 |
|
|
|
| 11 |
A" |
3074 |
2952 |
8.78 |
|
|
|
| 12 |
A" |
1498 |
1438 |
10.24 |
|
|
|
| 13 |
A" |
1056 |
1014 |
2.05 |
|
|
|
| 14 |
A" |
772 |
742 |
14.55 |
|
|
|
| 15 |
A" |
166 |
160 |
0.23 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 11834.6 cm
-1
Scaled (by 0.9603) Zero Point Vibrational Energy (zpe) 11364.7 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 B3LYP/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.168 |
|
|
|
| 2 |
C |
-0.469 |
|
|
|
| 3 |
S |
-0.088 |
|
|
|
| 4 |
H |
0.180 |
|
|
|
| 5 |
H |
0.189 |
|
|
|
| 6 |
H |
0.178 |
|
|
|
| 7 |
H |
0.178 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.751 |
2.001 |
0.000 |
2.659 |
| CHELPG |
-1.684 |
2.076 |
0.000 |
2.673 |
| AIM |
-0.874 |
1.512 |
0.000 |
1.746 |
| ESP |
-1.723 |
2.088 |
0.000 |
2.707 |
Electric Quadrupole moment
Quadrupole components in D Å
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
74.467 |
| (<r2>)1/2 |
8.629 |