Vibrational Frequencies calculated at ROHF/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 |
4191 |
70.47 |
|
|
|
| 2 |
A |
3373 |
3373 |
34.08 |
|
|
|
| 3 |
A |
3236 |
3236 |
36.75 |
|
|
|
| 4 |
A |
1609 |
1609 |
16.00 |
|
|
|
| 5 |
A |
1477 |
1477 |
49.05 |
|
|
|
| 6 |
A |
1279 |
1279 |
112.48 |
|
|
|
| 7 |
A |
1155 |
1155 |
46.53 |
|
|
|
| 8 |
A |
936 |
936 |
22.14 |
|
|
|
| 9 |
A |
408 |
408 |
118.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8832.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8832.4 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 ROHF/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.129 |
|
|
|
| 2 |
O |
-0.489 |
|
|
|
| 3 |
H |
0.149 |
|
|
|
| 4 |
H |
0.127 |
|
|
|
| 5 |
H |
0.342 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.242 |
1.465 |
0.110 |
1.488 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.378 |
2.111 |
-0.821 |
| y |
2.111 |
-10.933 |
-0.106 |
| z |
-0.821 |
-0.106 |
-13.610 |
|
| Traceless |
| | x | y | z |
| x |
0.893 |
2.111 |
-0.821 |
| y |
2.111 |
1.561 |
-0.106 |
| z |
-0.821 |
-0.106 |
-2.454 |
|
| Polar |
| 3z2-r2 | -4.909 |
| x2-y2 | -0.445 |
| xy | 2.111 |
| xz | -0.821 |
| yz | -0.106 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
20.114 |
| (<r2>)1/2 |
4.485 |