Vibrational Frequencies calculated at HF/6-31G(2df,p)
| 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 |
3281 |
2971 |
15.88 |
104.44 |
0.13 |
0.23 |
| 2 |
A1 |
1593 |
1442 |
3.22 |
3.45 |
0.74 |
0.85 |
| 3 |
A1 |
1002 |
908 |
18.89 |
54.85 |
0.22 |
0.36 |
| 4 |
B1 |
1107 |
1002 |
47.64 |
0.72 |
0.75 |
0.86 |
| 5 |
B2 |
3376 |
3057 |
0.78 |
87.76 |
0.75 |
0.86 |
| 6 |
B2 |
986 |
892 |
3.12 |
1.17 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 5672.0 cm
-1
Scaled (by 0.9055) Zero Point Vibrational Energy (zpe) 5136.0 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 HF/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.353 |
|
|
|
| 2 |
Se |
-0.047 |
|
|
|
| 3 |
H |
0.200 |
|
|
|
| 4 |
H |
0.200 |
|
|
|
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 |
-1.962 |
1.962 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.034 |
0.000 |
0.000 |
| y |
0.000 |
-26.008 |
0.000 |
| z |
0.000 |
0.000 |
-20.435 |
|
| Traceless |
| | x | y | z |
| x |
-1.812 |
0.000 |
0.000 |
| y |
0.000 |
-3.273 |
0.000 |
| z |
0.000 |
0.000 |
5.086 |
|
| Polar |
| 3z2-r2 | 10.171 |
| x2-y2 | 0.974 |
| 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 |
3.640 |
0.000 |
0.000 |
| y |
0.000 |
4.285 |
0.000 |
| z |
0.000 |
0.000 |
7.357 |
<r2> (average value of r
2) Å
2
| <r2> |
39.586 |
| (<r2>)1/2 |
6.292 |