Vibrational Frequencies calculated at wB97X-D/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 |
3051 |
2913 |
34.35 |
|
|
|
| 2 |
A |
3007 |
2872 |
38.82 |
|
|
|
| 3 |
A |
2930 |
2799 |
0.05 |
|
|
|
| 4 |
A |
1535 |
1466 |
4.99 |
|
|
|
| 5 |
A |
1385 |
1323 |
21.37 |
|
|
|
| 6 |
A |
1378 |
1316 |
14.61 |
|
|
|
| 7 |
A |
1135 |
1084 |
9.93 |
|
|
|
| 8 |
A |
976 |
932 |
0.80 |
|
|
|
| 9 |
A |
813 |
776 |
67.44 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8105.2 cm
-1
Scaled (by 0.955) Zero Point Vibrational Energy (zpe) 7740.4 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 wB97X-D/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.187 |
|
|
|
| 2 |
O |
-0.198 |
|
|
|
| 3 |
H |
0.149 |
|
|
|
| 4 |
H |
0.118 |
|
|
|
| 5 |
H |
0.118 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.149 |
-0.001 |
0.227 |
2.161 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.551 |
0.002 |
-0.247 |
| y |
0.002 |
-12.678 |
-0.004 |
| z |
-0.247 |
-0.004 |
-11.541 |
|
| Traceless |
| | x | y | z |
| x |
-1.442 |
0.002 |
-0.247 |
| y |
0.002 |
-0.132 |
-0.004 |
| z |
-0.247 |
-0.004 |
1.574 |
|
| Polar |
| 3z2-r2 | 3.148 |
| x2-y2 | -0.873 |
| xy | 0.002 |
| xz | -0.247 |
| yz | -0.004 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.879 |
0.000 |
-0.006 |
| y |
0.000 |
2.594 |
0.002 |
| z |
-0.006 |
0.002 |
2.240 |
<r2> (average value of r
2) Å
2
| <r2> |
20.742 |
| (<r2>)1/2 |
4.554 |