Vibrational Frequencies calculated at B3PW91/6-31G(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' |
3812 |
3665 |
101.14 |
|
|
|
| 2 |
A' |
3521 |
3385 |
93.71 |
|
|
|
| 3 |
A' |
2316 |
2227 |
117.14 |
|
|
|
| 4 |
A' |
1252 |
1204 |
86.45 |
|
|
|
| 5 |
A' |
1105 |
1062 |
89.28 |
|
|
|
| 6 |
A' |
629 |
605 |
48.36 |
|
|
|
| 7 |
A' |
407 |
392 |
9.72 |
|
|
|
| 8 |
A" |
533 |
512 |
42.05 |
|
|
|
| 9 |
A" |
428 |
412 |
21.84 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7001.8 cm
-1
Scaled (by 0.9614) Zero Point Vibrational Energy (zpe) 6731.5 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 B3PW91/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.229 |
|
|
|
| 2 |
C |
-0.368 |
|
|
|
| 3 |
O |
-0.422 |
|
|
|
| 4 |
H |
0.217 |
|
|
|
| 5 |
H |
0.344 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.475 |
-0.864 |
0.000 |
1.710 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.636 |
-2.436 |
0.000 |
| y |
-2.436 |
-11.588 |
0.000 |
| z |
0.000 |
0.000 |
-18.071 |
|
| Traceless |
| | x | y | z |
| x |
-1.807 |
-2.436 |
0.000 |
| y |
-2.436 |
5.766 |
0.000 |
| z |
0.000 |
0.000 |
-3.959 |
|
| Polar |
| 3z2-r2 | -7.918 |
| x2-y2 | -5.049 |
| xy | -2.436 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.118 |
0.032 |
0.000 |
| y |
0.032 |
5.412 |
0.000 |
| z |
0.000 |
0.000 |
1.926 |
<r2> (average value of r
2) Å
2
| <r2> |
40.189 |
| (<r2>)1/2 |
6.339 |