Vibrational Frequencies calculated at BLYP/6-31+G**
| 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 |
3037 |
3021 |
1.46 |
|
|
|
| 2 |
A |
3014 |
2998 |
19.22 |
|
|
|
| 3 |
A |
2941 |
2925 |
4.46 |
|
|
|
| 4 |
A |
1438 |
1430 |
19.03 |
|
|
|
| 5 |
A |
1330 |
1323 |
12.50 |
|
|
|
| 6 |
A |
1304 |
1297 |
5.37 |
|
|
|
| 7 |
A |
840 |
835 |
1.93 |
|
|
|
| 8 |
A |
675 |
672 |
1.00 |
|
|
|
| 9 |
A |
613 |
610 |
58.92 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7595.3 cm
-1
Scaled (by 0.9947) Zero Point Vibrational Energy (zpe) 7555.0 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 BLYP/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.551 |
|
|
|
| 2 |
S |
-0.016 |
|
|
|
| 3 |
H |
0.191 |
|
|
|
| 4 |
H |
0.188 |
|
|
|
| 5 |
H |
0.188 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.850 |
0.000 |
0.092 |
1.853 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.943 |
-0.000 |
0.178 |
| y |
-0.000 |
-22.225 |
-0.000 |
| z |
0.178 |
-0.000 |
-19.445 |
|
| Traceless |
| | x | y | z |
| x |
0.892 |
-0.000 |
0.178 |
| y |
-0.000 |
-2.530 |
-0.000 |
| z |
0.178 |
-0.000 |
1.639 |
|
| Polar |
| 3z2-r2 | 3.277 |
| x2-y2 | 2.281 |
| xy | -0.000 |
| xz | 0.178 |
| yz | -0.000 |
|
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> |
38.319 |
| (<r2>)1/2 |
6.190 |