Vibrational Frequencies calculated at PBEPBE/Def2TZVPP
| 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 |
3728 |
3683 |
46.22 |
|
|
|
| 2 |
A |
3209 |
3170 |
11.63 |
|
|
|
| 3 |
A |
3067 |
3029 |
18.43 |
|
|
|
| 4 |
A |
1433 |
1415 |
6.10 |
|
|
|
| 5 |
A |
1327 |
1311 |
24.01 |
|
|
|
| 6 |
A |
1178 |
1164 |
87.15 |
|
|
|
| 7 |
A |
1022 |
1009 |
46.71 |
|
|
|
| 8 |
A |
513 |
507 |
125.76 |
|
|
|
| 9 |
A |
411 |
406 |
23.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7943.6 cm
-1
Scaled (by 0.9879) Zero Point Vibrational Energy (zpe) 7847.5 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/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.157 |
|
|
|
| 2 |
O |
-0.241 |
|
|
|
| 3 |
H |
0.100 |
|
|
|
| 4 |
H |
0.087 |
|
|
|
| 5 |
H |
0.211 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.168 |
1.439 |
0.256 |
1.471 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.830 |
2.089 |
-0.595 |
| y |
2.089 |
-11.157 |
-0.017 |
| z |
-0.595 |
-0.017 |
-14.542 |
|
| Traceless |
| | x | y | z |
| x |
1.020 |
2.089 |
-0.595 |
| y |
2.089 |
2.028 |
-0.017 |
| z |
-0.595 |
-0.017 |
-3.048 |
|
| Polar |
| 3z2-r2 | -6.096 |
| x2-y2 | -0.672 |
| xy | 2.089 |
| xz | -0.595 |
| yz | -0.017 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.315 |
0.092 |
-0.001 |
| y |
0.092 |
2.765 |
-0.010 |
| z |
-0.001 |
-0.010 |
2.331 |
<r2> (average value of r
2) Å
2
| <r2> |
20.822 |
| (<r2>)1/2 |
4.563 |