Vibrational Frequencies calculated at BLYP/aug-cc-pVDZ
| 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' |
3160 |
3154 |
0.56 |
|
|
|
| 2 |
A' |
3065 |
3059 |
4.06 |
|
|
|
| 3 |
A' |
2955 |
2950 |
6.67 |
|
|
|
| 4 |
A' |
1596 |
1593 |
1.69 |
|
|
|
| 5 |
A' |
1340 |
1338 |
8.55 |
|
|
|
| 6 |
A' |
1009 |
1008 |
8.74 |
|
|
|
| 7 |
A' |
681 |
680 |
22.10 |
|
|
|
| 8 |
A" |
897 |
895 |
70.43 |
|
|
|
| 9 |
A" |
751 |
750 |
18.35 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7727.6 cm
-1
Scaled (by 0.9981) Zero Point Vibrational Energy (zpe) 7712.9 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 BLYP/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.402 |
|
|
|
| 2 |
C |
1.045 |
|
|
|
| 3 |
H |
-0.576 |
|
|
|
| 4 |
H |
-0.469 |
|
|
|
| 5 |
H |
-0.402 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.612 |
-0.353 |
0.000 |
0.707 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.771 |
-1.237 |
0.000 |
| y |
-1.237 |
-11.802 |
0.000 |
| z |
0.000 |
0.000 |
-15.069 |
|
| Traceless |
| | x | y | z |
| x |
0.665 |
-1.237 |
0.000 |
| y |
-1.237 |
2.118 |
0.000 |
| z |
0.000 |
0.000 |
-2.783 |
|
| Polar |
| 3z2-r2 | -5.565 |
| x2-y2 | -0.968 |
| xy | -1.237 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.700 |
-0.048 |
0.000 |
| y |
-0.048 |
5.582 |
0.000 |
| z |
0.000 |
0.000 |
3.292 |
<r2> (average value of r
2) Å
2
| <r2> |
20.967 |
| (<r2>)1/2 |
4.579 |