Vibrational Frequencies calculated at B3LYPultrafine/cc-pVDZ
| 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 |
3657 |
3548 |
3.29 |
|
|
|
| 2 |
A |
1381 |
1339 |
25.12 |
|
|
|
| 3 |
A |
935 |
907 |
4.31 |
|
|
|
| 4 |
A |
535 |
519 |
36.31 |
|
|
|
| 5 |
A |
372 |
361 |
113.35 |
|
|
|
| 6 |
B |
3652 |
3542 |
50.88 |
|
|
|
| 7 |
B |
1384 |
1342 |
40.66 |
|
|
|
| 8 |
B |
794 |
770 |
75.71 |
|
|
|
| 9 |
B |
429 |
416 |
106.67 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6569.0 cm
-1
Scaled (by 0.97) Zero Point Vibrational Energy (zpe) 6371.9 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 B3LYPultrafine/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.084 |
|
|
|
| 2 |
O |
-0.135 |
|
|
|
| 3 |
O |
-0.135 |
|
|
|
| 4 |
H |
0.177 |
|
|
|
| 5 |
H |
0.177 |
|
|
|
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 |
-1.094 |
1.094 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.492 |
-4.209 |
0.000 |
| y |
-4.209 |
-16.563 |
0.000 |
| z |
0.000 |
0.000 |
-16.836 |
|
| Traceless |
| | x | y | z |
| x |
3.208 |
-4.209 |
0.000 |
| y |
-4.209 |
-1.399 |
0.000 |
| z |
0.000 |
0.000 |
-1.809 |
|
| Polar |
| 3z2-r2 | -3.617 |
| x2-y2 | 3.071 |
| xy | -4.209 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.793 |
-0.472 |
0.000 |
| y |
-0.472 |
3.246 |
0.000 |
| z |
0.000 |
0.000 |
1.640 |
<r2> (average value of r
2) Å
2
| <r2> |
40.016 |
| (<r2>)1/2 |
6.326 |