Vibrational Frequencies calculated at B1B95/6-311G*
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3106 |
2978 |
13.91 |
|
|
|
| 2 |
A1 |
1306 |
1252 |
28.28 |
|
|
|
| 3 |
A1 |
552 |
529 |
2.89 |
|
|
|
| 4 |
E |
3221 |
3088 |
1.56 |
|
|
|
| 4 |
E |
3221 |
3088 |
1.56 |
|
|
|
| 5 |
E |
1482 |
1421 |
8.34 |
|
|
|
| 5 |
E |
1482 |
1421 |
8.34 |
|
|
|
| 6 |
E |
910 |
872 |
9.51 |
|
|
|
| 6 |
E |
910 |
872 |
9.51 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8095.5 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 7760.4 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 B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.823 |
|
|
|
| 2 |
I |
0.006 |
|
|
|
| 3 |
H |
0.272 |
|
|
|
| 4 |
H |
0.272 |
|
|
|
| 5 |
H |
0.272 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-1.852 |
1.852 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-36.268 |
0.000 |
0.000 |
| y |
0.000 |
-36.268 |
0.000 |
| z |
0.000 |
0.000 |
-30.781 |
|
| Traceless |
| | x | y | z |
| x |
-2.743 |
0.000 |
0.000 |
| y |
0.000 |
-2.743 |
0.000 |
| z |
0.000 |
0.000 |
5.486 |
|
| Polar |
| 3z2-r2 | 10.972 |
| x2-y2 | 0.000 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.156 |
0.000 |
0.000 |
| y |
0.000 |
4.156 |
0.000 |
| z |
0.000 |
0.000 |
7.332 |
<r2> (average value of r
2) Å
2
| <r2> |
64.152 |
| (<r2>)1/2 |
8.009 |