Vibrational Frequencies calculated at B97D3/6-311G*
| 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' |
3237 |
3237 |
2.33 |
|
|
|
| 2 |
A' |
3074 |
3074 |
1.08 |
|
|
|
| 3 |
A' |
1468 |
1468 |
17.84 |
|
|
|
| 4 |
A' |
1338 |
1338 |
24.58 |
|
|
|
| 5 |
A' |
1222 |
1222 |
16.42 |
|
|
|
| 6 |
A' |
947 |
947 |
66.97 |
|
|
|
| 7 |
A' |
534 |
534 |
0.52 |
|
|
|
| 8 |
A" |
799 |
799 |
40.13 |
|
|
|
| 9 |
A" |
650 |
650 |
11.76 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6634.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 6634.5 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 B97D3/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
0.017 |
|
|
|
| 2 |
C |
-0.169 |
|
|
|
| 3 |
H |
0.218 |
|
|
|
| 4 |
H |
0.228 |
|
|
|
| 5 |
O |
-0.295 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
3.669 |
-0.367 |
0.000 |
3.688 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.370 |
-0.376 |
0.000 |
| y |
-0.376 |
-16.378 |
0.000 |
| z |
0.000 |
0.000 |
-17.223 |
|
| Traceless |
| | x | y | z |
| x |
0.430 |
-0.376 |
0.000 |
| y |
-0.376 |
0.419 |
0.000 |
| z |
0.000 |
0.000 |
-0.849 |
|
| Polar |
| 3z2-r2 | -1.699 |
| x2-y2 | 0.007 |
| xy | -0.376 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.767 |
-0.060 |
0.000 |
| y |
-0.060 |
2.411 |
0.000 |
| z |
0.000 |
0.000 |
1.451 |
<r2> (average value of r
2) Å
2
| <r2> |
37.679 |
| (<r2>)1/2 |
6.138 |