Vibrational Frequencies calculated at BLYP/6-311G**
| 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 |
3601 |
3587 |
84.57 |
|
|
|
| 2 |
A |
1154 |
1150 |
97.86 |
|
|
|
| 3 |
A |
1031 |
1027 |
77.28 |
|
|
|
| 4 |
A |
971 |
967 |
49.46 |
|
|
|
| 5 |
A |
596 |
594 |
121.25 |
|
|
|
| 6 |
A |
462 |
460 |
27.90 |
|
|
|
| 7 |
A |
363 |
361 |
25.44 |
|
|
|
| 8 |
A |
358 |
356 |
21.40 |
|
|
|
| 9 |
A |
242 |
241 |
89.46 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4388.7 cm
-1
Scaled (by 0.9961) Zero Point Vibrational Energy (zpe) 4371.6 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/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.917 |
|
|
|
| 2 |
O |
-0.422 |
|
|
|
| 3 |
O |
-0.407 |
|
|
|
| 4 |
O |
-0.372 |
|
|
|
| 5 |
H |
0.285 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.251 |
0.651 |
1.116 |
2.596 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.583 |
0.949 |
-0.586 |
| y |
0.949 |
-34.438 |
0.088 |
| z |
-0.586 |
0.088 |
-27.818 |
|
| Traceless |
| | x | y | z |
| x |
4.545 |
0.949 |
-0.586 |
| y |
0.949 |
-7.237 |
0.088 |
| z |
-0.586 |
0.088 |
2.692 |
|
| Polar |
| 3z2-r2 | 5.385 |
| x2-y2 | 7.855 |
| xy | 0.949 |
| xz | -0.586 |
| yz | 0.088 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.246 |
0.301 |
0.014 |
| y |
0.301 |
5.037 |
-0.013 |
| z |
0.014 |
-0.013 |
2.597 |
<r2> (average value of r
2) Å
2
| <r2> |
78.680 |
| (<r2>)1/2 |
8.870 |