Vibrational Frequencies calculated at B97D3/6-311+G(3df,2p)
| 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 |
2915 |
2877 |
36.58 |
|
|
|
| 2 |
A |
2873 |
2835 |
47.39 |
|
|
|
| 3 |
A |
2799 |
2763 |
0.67 |
|
|
|
| 4 |
A |
1481 |
1461 |
6.00 |
|
|
|
| 5 |
A |
1317 |
1300 |
30.62 |
|
|
|
| 6 |
A |
1303 |
1286 |
15.18 |
|
|
|
| 7 |
A |
1087 |
1073 |
8.73 |
|
|
|
| 8 |
A |
936 |
924 |
0.51 |
|
|
|
| 9 |
A |
536 |
529 |
100.98 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7623.3 cm
-1
Scaled (by 0.987) Zero Point Vibrational Energy (zpe) 7524.2 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 B97D3/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.085 |
|
|
|
| 2 |
O |
-0.432 |
|
|
|
| 3 |
H |
0.129 |
|
|
|
| 4 |
H |
0.109 |
|
|
|
| 5 |
H |
0.109 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.101 |
-0.002 |
0.228 |
2.113 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.714 |
0.002 |
-0.270 |
| y |
0.002 |
-12.836 |
-0.002 |
| z |
-0.270 |
-0.002 |
-11.675 |
|
| Traceless |
| | x | y | z |
| x |
-1.458 |
0.002 |
-0.270 |
| y |
0.002 |
-0.142 |
-0.002 |
| z |
-0.270 |
-0.002 |
1.600 |
|
| Polar |
| 3z2-r2 | 3.201 |
| x2-y2 | -0.877 |
| xy | 0.002 |
| xz | -0.270 |
| yz | -0.002 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.599 |
0.001 |
-0.044 |
| y |
0.001 |
3.076 |
0.002 |
| z |
-0.044 |
0.002 |
2.617 |
<r2> (average value of r
2) Å
2
| <r2> |
20.881 |
| (<r2>)1/2 |
4.570 |