Vibrational Frequencies calculated at B3LYPultrafine/TZVP
| 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' |
3277 |
3157 |
0.48 |
|
|
|
| 2 |
A' |
3124 |
3010 |
3.49 |
|
|
|
| 3 |
A' |
1543 |
1487 |
26.61 |
|
|
|
| 4 |
A' |
1406 |
1354 |
17.43 |
|
|
|
| 5 |
A' |
1248 |
1203 |
14.97 |
|
|
|
| 6 |
A' |
898 |
865 |
101.00 |
|
|
|
| 7 |
A' |
527 |
508 |
0.13 |
|
|
|
| 8 |
A" |
933 |
899 |
39.80 |
|
|
|
| 9 |
A" |
670 |
645 |
4.74 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6812.9 cm
-1
Scaled (by 0.9634) Zero Point Vibrational Energy (zpe) 6563.6 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 B3LYPultrafine/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
0.054 |
|
|
|
| 2 |
C |
0.014 |
|
|
|
| 3 |
H |
0.144 |
|
|
|
| 4 |
H |
0.144 |
|
|
|
| 5 |
O |
-0.356 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
4.334 |
-0.349 |
0.000 |
4.348 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.789 |
-0.534 |
0.000 |
| y |
-0.534 |
-16.698 |
0.000 |
| z |
0.000 |
0.000 |
-17.432 |
|
| Traceless |
| | x | y | z |
| x |
0.276 |
-0.534 |
0.000 |
| y |
-0.534 |
0.413 |
0.000 |
| z |
0.000 |
0.000 |
-0.688 |
|
| Polar |
| 3z2-r2 | -1.377 |
| x2-y2 | -0.091 |
| xy | -0.534 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.231 |
0.015 |
0.000 |
| y |
0.015 |
2.550 |
0.000 |
| z |
0.000 |
0.000 |
1.729 |
<r2> (average value of r
2) Å
2
| <r2> |
37.733 |
| (<r2>)1/2 |
6.143 |