Vibrational Frequencies calculated at B3LYPultrafine/3-21G
| 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 |
3502 |
3379 |
7.07 |
|
|
|
| 2 |
A |
3276 |
3161 |
24.65 |
|
|
|
| 3 |
A |
3122 |
3012 |
18.20 |
|
|
|
| 4 |
A |
1516 |
1462 |
4.25 |
|
|
|
| 5 |
A |
1374 |
1325 |
32.90 |
|
|
|
| 6 |
A |
1145 |
1105 |
47.99 |
|
|
|
| 7 |
A |
1048 |
1012 |
74.62 |
|
|
|
| 8 |
A |
595 |
574 |
122.61 |
|
|
|
| 9 |
A |
434 |
419 |
82.35 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8004.7 cm
-1
Scaled (by 0.9649) Zero Point Vibrational Energy (zpe) 7723.8 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 B3LYPultrafine/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.197 |
|
|
|
| 2 |
O |
-0.516 |
|
|
|
| 3 |
H |
0.191 |
|
|
|
| 4 |
H |
0.161 |
|
|
|
| 5 |
H |
0.360 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.001 |
1.663 |
0.192 |
1.674 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.228 |
2.269 |
-0.764 |
| y |
2.269 |
-10.837 |
-0.047 |
| z |
-0.764 |
-0.047 |
-13.759 |
|
| Traceless |
| | x | y | z |
| x |
1.070 |
2.269 |
-0.764 |
| y |
2.269 |
1.656 |
-0.047 |
| z |
-0.764 |
-0.047 |
-2.726 |
|
| Polar |
| 3z2-r2 | -5.452 |
| x2-y2 | -0.391 |
| xy | 2.269 |
| xz | -0.764 |
| yz | -0.047 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.649 |
0.222 |
-0.045 |
| y |
0.222 |
2.075 |
-0.006 |
| z |
-0.045 |
-0.006 |
0.799 |
<r2> (average value of r
2) Å
2
| <r2> |
20.892 |
| (<r2>)1/2 |
4.571 |