Vibrational Frequencies calculated at M06-2X/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 |
3750 |
3551 |
147.11 |
|
|
|
| 2 |
A |
1326 |
1255 |
131.96 |
|
|
|
| 3 |
A |
1155 |
1093 |
103.92 |
|
|
|
| 4 |
A |
1126 |
1066 |
62.36 |
|
|
|
| 5 |
A |
803 |
761 |
160.93 |
|
|
|
| 6 |
A |
528 |
500 |
46.55 |
|
|
|
| 7 |
A |
424 |
401 |
18.37 |
|
|
|
| 8 |
A |
414 |
392 |
34.71 |
|
|
|
| 9 |
A |
271 |
257 |
113.52 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4897.3 cm
-1
Scaled (by 0.947) Zero Point Vibrational Energy (zpe) 4637.7 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 M06-2X/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
1.121 |
|
|
|
| 2 |
O |
-0.646 |
|
|
|
| 3 |
O |
-0.492 |
|
|
|
| 4 |
O |
-0.448 |
|
|
|
| 5 |
H |
0.465 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.564 |
-0.305 |
0.997 |
2.767 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.167 |
-1.911 |
-0.948 |
| y |
-1.911 |
-33.449 |
0.328 |
| z |
-0.948 |
0.328 |
-27.330 |
|
| Traceless |
| | x | y | z |
| x |
4.223 |
-1.911 |
-0.948 |
| y |
-1.911 |
-6.701 |
0.328 |
| z |
-0.948 |
0.328 |
2.478 |
|
| Polar |
| 3z2-r2 | 4.956 |
| x2-y2 | 7.283 |
| xy | -1.911 |
| xz | -0.948 |
| yz | 0.328 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.648 |
0.376 |
0.052 |
| y |
0.376 |
4.203 |
-0.059 |
| z |
0.052 |
-0.059 |
2.542 |
<r2> (average value of r
2) Å
2
| <r2> |
74.338 |
| (<r2>)1/2 |
8.622 |