Vibrational Frequencies calculated at PBEPBEultrafine/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' |
3217 |
3181 |
0.51 |
|
|
|
| 2 |
A' |
3058 |
3023 |
2.66 |
|
|
|
| 3 |
A' |
1459 |
1443 |
24.75 |
|
|
|
| 4 |
A' |
1334 |
1319 |
25.29 |
|
|
|
| 5 |
A' |
1204 |
1190 |
15.09 |
|
|
|
| 6 |
A' |
946 |
935 |
70.92 |
|
|
|
| 7 |
A' |
524 |
518 |
0.44 |
|
|
|
| 8 |
A" |
824 |
815 |
46.02 |
|
|
|
| 9 |
A" |
649 |
642 |
10.30 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6608.0 cm
-1
Scaled (by 0.9886) Zero Point Vibrational Energy (zpe) 6532.7 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 PBEPBEultrafine/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
0.076 |
|
|
|
| 2 |
C |
-0.057 |
|
|
|
| 3 |
H |
0.143 |
|
|
|
| 4 |
H |
0.148 |
|
|
|
| 5 |
O |
-0.310 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
3.811 |
-0.382 |
0.000 |
3.830 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.841 |
-0.386 |
0.000 |
| y |
-0.386 |
-16.722 |
0.000 |
| z |
0.000 |
0.000 |
-17.530 |
|
| Traceless |
| | x | y | z |
| x |
0.285 |
-0.386 |
0.000 |
| y |
-0.386 |
0.464 |
0.000 |
| z |
0.000 |
0.000 |
-0.749 |
|
| Polar |
| 3z2-r2 | -1.498 |
| x2-y2 | -0.119 |
| xy | -0.386 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.259 |
-0.069 |
0.000 |
| y |
-0.069 |
2.661 |
0.000 |
| z |
0.000 |
0.000 |
1.801 |
<r2> (average value of r
2) Å
2
| <r2> |
38.090 |
| (<r2>)1/2 |
6.172 |