Vibrational Frequencies calculated at B3PW91/6-311G**
| 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' |
3249 |
3129 |
0.88 |
|
|
|
| 2 |
A' |
3154 |
3038 |
4.55 |
|
|
|
| 3 |
A' |
3056 |
2943 |
5.11 |
|
|
|
| 4 |
A' |
1657 |
1596 |
2.13 |
|
|
|
| 5 |
A' |
1384 |
1333 |
9.54 |
|
|
|
| 6 |
A' |
1044 |
1005 |
9.13 |
|
|
|
| 7 |
A' |
711 |
685 |
24.22 |
|
|
|
| 8 |
A" |
920 |
886 |
82.90 |
|
|
|
| 9 |
A" |
830 |
799 |
15.82 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8002.3 cm
-1
Scaled (by 0.9631) Zero Point Vibrational Energy (zpe) 7707.0 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 B3PW91/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.157 |
|
|
|
| 2 |
C |
-0.271 |
|
|
|
| 3 |
H |
0.144 |
|
|
|
| 4 |
H |
0.139 |
|
|
|
| 5 |
H |
0.145 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.622 |
-0.289 |
0.000 |
0.686 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.153 |
-1.182 |
0.000 |
| y |
-1.182 |
-11.129 |
0.000 |
| z |
0.000 |
0.000 |
-14.596 |
|
| Traceless |
| | x | y | z |
| x |
0.709 |
-1.182 |
0.000 |
| y |
-1.182 |
2.246 |
0.000 |
| z |
0.000 |
0.000 |
-2.955 |
|
| Polar |
| 3z2-r2 | -5.909 |
| x2-y2 | -1.025 |
| xy | -1.182 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.654 |
-0.177 |
0.000 |
| y |
-0.177 |
4.727 |
0.000 |
| z |
0.000 |
0.000 |
1.779 |
<r2> (average value of r
2) Å
2
| <r2> |
20.279 |
| (<r2>)1/2 |
4.503 |