Vibrational Frequencies calculated at wB97X-D/6-31G(2df,p)
| 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' |
3314 |
3314 |
0.27 |
|
|
|
| 2 |
A' |
3157 |
3157 |
3.08 |
|
|
|
| 3 |
A' |
1580 |
1580 |
36.69 |
|
|
|
| 4 |
A' |
1421 |
1421 |
11.40 |
|
|
|
| 5 |
A' |
1265 |
1265 |
26.67 |
|
|
|
| 6 |
A' |
1024 |
1024 |
98.27 |
|
|
|
| 7 |
A' |
548 |
548 |
0.37 |
|
|
|
| 8 |
A" |
932 |
932 |
35.28 |
|
|
|
| 9 |
A" |
699 |
699 |
2.96 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6969.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 6969.5 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 wB97X-D/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
0.110 |
|
|
|
| 2 |
C |
-0.123 |
|
|
|
| 3 |
H |
0.187 |
|
|
|
| 4 |
H |
0.190 |
|
|
|
| 5 |
O |
-0.363 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
3.945 |
-0.383 |
0.000 |
3.963 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.006 |
-0.499 |
0.000 |
| y |
-0.499 |
-15.920 |
0.000 |
| z |
0.000 |
0.000 |
-16.867 |
|
| Traceless |
| | x | y | z |
| x |
0.387 |
-0.499 |
0.000 |
| y |
-0.499 |
0.517 |
0.000 |
| z |
0.000 |
0.000 |
-0.904 |
|
| Polar |
| 3z2-r2 | -1.808 |
| x2-y2 | -0.086 |
| xy | -0.499 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.626 |
-0.072 |
0.000 |
| y |
-0.072 |
2.470 |
0.000 |
| z |
0.000 |
0.000 |
1.648 |
<r2> (average value of r
2) Å
2
| <r2> |
36.511 |
| (<r2>)1/2 |
6.042 |