Vibrational Frequencies calculated at BLYP/6-311+G(3df,2p)
| 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' |
3162 |
3145 |
0.43 |
|
|
|
| 2 |
A' |
3045 |
3028 |
3.31 |
|
|
|
| 3 |
A' |
2945 |
2929 |
6.37 |
|
|
|
| 4 |
A' |
1601 |
1592 |
2.08 |
|
|
|
| 5 |
A' |
1360 |
1353 |
8.47 |
|
|
|
| 6 |
A' |
1015 |
1010 |
8.01 |
|
|
|
| 7 |
A' |
687 |
683 |
23.58 |
|
|
|
| 8 |
A" |
890 |
885 |
71.39 |
|
|
|
| 9 |
A" |
777 |
773 |
17.46 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7741.1 cm
-1
Scaled (by 0.9945) Zero Point Vibrational Energy (zpe) 7698.5 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 BLYP/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.226 |
|
|
|
| 2 |
C |
-0.280 |
|
|
|
| 3 |
H |
0.191 |
|
|
|
| 4 |
H |
0.152 |
|
|
|
| 5 |
H |
0.164 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.619 |
-0.362 |
0.000 |
0.717 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.734 |
-1.232 |
0.000 |
| y |
-1.232 |
-11.631 |
0.000 |
| z |
0.000 |
0.000 |
-15.079 |
|
| Traceless |
| | x | y | z |
| x |
0.620 |
-1.232 |
0.000 |
| y |
-1.232 |
2.276 |
0.000 |
| z |
0.000 |
0.000 |
-2.896 |
|
| Polar |
| 3z2-r2 | -5.792 |
| x2-y2 | -1.103 |
| xy | -1.232 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.525 |
-0.022 |
0.000 |
| y |
-0.022 |
5.345 |
0.000 |
| z |
0.000 |
0.000 |
3.222 |
<r2> (average value of r
2) Å
2
| <r2> |
20.713 |
| (<r2>)1/2 |
4.551 |