Vibrational Frequencies calculated at PBEPBE/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 |
A |
3592 |
3555 |
1.48 |
|
|
|
| 2 |
A |
1348 |
1335 |
26.11 |
|
|
|
| 3 |
A |
910 |
900 |
4.02 |
|
|
|
| 4 |
A |
517 |
511 |
32.74 |
|
|
|
| 5 |
A |
377 |
373 |
93.94 |
|
|
|
| 6 |
B |
3586 |
3549 |
28.29 |
|
|
|
| 7 |
B |
1355 |
1341 |
40.11 |
|
|
|
| 8 |
B |
702 |
695 |
103.29 |
|
|
|
| 9 |
B |
455 |
450 |
96.61 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6420.6 cm
-1
Scaled (by 0.9897) Zero Point Vibrational Energy (zpe) 6354.5 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 PBEPBE/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.098 |
|
|
|
| 2 |
O |
-0.263 |
|
|
|
| 3 |
O |
-0.263 |
|
|
|
| 4 |
H |
0.311 |
|
|
|
| 5 |
H |
0.311 |
|
|
|
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 |
-1.026 |
1.026 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.572 |
-4.037 |
0.000 |
| y |
-4.037 |
-16.321 |
0.000 |
| z |
0.000 |
0.000 |
-16.781 |
|
| Traceless |
| | x | y | z |
| x |
2.979 |
-4.037 |
0.000 |
| y |
-4.037 |
-1.145 |
0.000 |
| z |
0.000 |
0.000 |
-1.835 |
|
| Polar |
| 3z2-r2 | -3.669 |
| x2-y2 | 2.750 |
| xy | -4.037 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.211 |
-0.469 |
0.000 |
| y |
-0.469 |
3.610 |
0.000 |
| z |
0.000 |
0.000 |
2.003 |
<r2> (average value of r
2) Å
2
| <r2> |
40.455 |
| (<r2>)1/2 |
6.360 |