Vibrational Frequencies calculated at HF/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 |
4191 |
3795 |
72.58 |
|
|
|
| 2 |
A |
3382 |
3062 |
29.55 |
|
|
|
| 3 |
A |
3247 |
2940 |
31.09 |
|
|
|
| 4 |
A |
1607 |
1455 |
16.65 |
|
|
|
| 5 |
A |
1473 |
1334 |
50.39 |
|
|
|
| 6 |
A |
1283 |
1162 |
113.03 |
|
|
|
| 7 |
A |
1147 |
1039 |
45.83 |
|
|
|
| 8 |
A |
828 |
750 |
29.21 |
|
|
|
| 9 |
A |
406 |
368 |
113.66 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8782.8 cm
-1
Scaled (by 0.9055) Zero Point Vibrational Energy (zpe) 7952.8 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 HF/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.136 |
|
|
|
| 2 |
O |
-0.484 |
|
|
|
| 3 |
H |
0.149 |
|
|
|
| 4 |
H |
0.128 |
|
|
|
| 5 |
H |
0.343 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.229 |
1.480 |
0.115 |
1.502 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.344 |
2.107 |
-0.754 |
| y |
2.107 |
-10.881 |
-0.091 |
| z |
-0.754 |
-0.091 |
-13.634 |
|
| Traceless |
| | x | y | z |
| x |
0.914 |
2.107 |
-0.754 |
| y |
2.107 |
1.608 |
-0.091 |
| z |
-0.754 |
-0.091 |
-2.522 |
|
| Polar |
| 3z2-r2 | -5.043 |
| x2-y2 | -0.463 |
| xy | 2.107 |
| xz | -0.754 |
| yz | -0.091 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.517 |
0.130 |
-0.077 |
| y |
0.130 |
2.280 |
0.017 |
| z |
-0.077 |
0.017 |
1.459 |
<r2> (average value of r
2) Å
2
| <r2> |
20.106 |
| (<r2>)1/2 |
4.484 |