Vibrational Frequencies calculated at B2PLYP/6-31G**
| 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' |
3300 |
3300 |
2.00 |
|
|
|
| 2 |
A' |
3223 |
3223 |
5.92 |
|
|
|
| 3 |
A' |
3120 |
3120 |
4.26 |
|
|
|
| 4 |
A' |
1706 |
1706 |
1.64 |
|
|
|
| 5 |
A' |
1428 |
1428 |
5.54 |
|
|
|
| 6 |
A' |
1087 |
1087 |
9.66 |
|
|
|
| 7 |
A' |
741 |
741 |
20.00 |
|
|
|
| 8 |
A" |
940 |
940 |
71.60 |
|
|
|
| 9 |
A" |
831 |
831 |
7.37 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8187.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8187.7 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 B2PLYP/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.113 |
|
|
|
| 2 |
C |
-0.265 |
|
|
|
| 3 |
H |
0.128 |
|
|
|
| 4 |
H |
0.122 |
|
|
|
| 5 |
H |
0.127 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.575 |
-0.245 |
0.000 |
0.625 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.047 |
-1.047 |
0.000 |
| y |
-1.047 |
-11.118 |
0.000 |
| z |
0.000 |
0.000 |
-14.245 |
|
| Traceless |
| | x | y | z |
| x |
0.635 |
-1.047 |
0.000 |
| y |
-1.047 |
2.027 |
0.000 |
| z |
0.000 |
0.000 |
-2.663 |
|
| Polar |
| 3z2-r2 | -5.325 |
| x2-y2 | -0.928 |
| xy | -1.047 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.460 |
-0.257 |
0.000 |
| y |
-0.257 |
4.385 |
0.000 |
| z |
0.000 |
0.000 |
1.308 |
<r2> (average value of r
2) Å
2
| <r2> |
20.197 |
| (<r2>)1/2 |
4.494 |