Vibrational Frequencies calculated at HF/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' |
3375 |
3067 |
0.54 |
|
|
|
| 2 |
A' |
3320 |
3016 |
6.09 |
|
|
|
| 3 |
A' |
3226 |
2931 |
6.21 |
|
|
|
| 4 |
A' |
1618 |
1470 |
4.00 |
|
|
|
| 5 |
A' |
1407 |
1278 |
4.02 |
|
|
|
| 6 |
A' |
1176 |
1068 |
7.72 |
|
|
|
| 7 |
A' |
815 |
741 |
12.87 |
|
|
|
| 8 |
A" |
977 |
888 |
73.90 |
|
|
|
| 9 |
A" |
901 |
819 |
11.89 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8407.4 cm
-1
Scaled (by 0.9086) Zero Point Vibrational Energy (zpe) 7638.9 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 HF/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.255 |
|
|
|
| 2 |
C |
-0.178 |
|
|
|
| 3 |
H |
0.165 |
|
|
|
| 4 |
H |
0.132 |
|
|
|
| 5 |
H |
0.136 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.572 |
-0.278 |
0.000 |
0.636 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.341 |
-1.099 |
0.000 |
| y |
-1.099 |
-11.505 |
0.000 |
| z |
0.000 |
0.000 |
-15.065 |
|
| Traceless |
| | x | y | z |
| x |
0.944 |
-1.099 |
0.000 |
| y |
-1.099 |
2.197 |
0.000 |
| z |
0.000 |
0.000 |
-3.142 |
|
| Polar |
| 3z2-r2 | -6.283 |
| x2-y2 | -0.835 |
| xy | -1.099 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.114 |
-0.133 |
0.000 |
| y |
-0.133 |
4.690 |
0.000 |
| z |
0.000 |
0.000 |
2.987 |
<r2> (average value of r
2) Å
2
| <r2> |
20.456 |
| (<r2>)1/2 |
4.523 |