Vibrational Frequencies calculated at B3LYP/cc-pV(T+d)Z
| 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 |
3176 |
3066 |
0.28 |
|
|
|
| 2 |
A1 |
664 |
641 |
4.82 |
|
|
|
| 3 |
A1 |
362 |
349 |
0.21 |
|
|
|
| 4 |
E |
1235 |
1193 |
21.07 |
|
|
|
| 4 |
E |
1235 |
1193 |
21.07 |
|
|
|
| 5 |
E |
728 |
703 |
167.71 |
|
|
|
| 5 |
E |
728 |
703 |
167.66 |
|
|
|
| 6 |
E |
256 |
247 |
0.00 |
|
|
|
| 6 |
E |
256 |
247 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4320.0 cm
-1
Scaled (by 0.9654) Zero Point Vibrational Energy (zpe) 4170.5 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 B3LYP/cc-pV(T+d)Z
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.031 |
|
|
|
| 2 |
H |
0.168 |
|
|
|
| 3 |
Cl |
-0.067 |
|
|
|
| 4 |
Cl |
-0.067 |
|
|
|
| 5 |
Cl |
-0.067 |
|
|
|
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 |
1.102 |
1.102 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-44.146 |
0.000 |
0.000 |
| y |
0.000 |
-44.146 |
0.000 |
| z |
0.000 |
0.000 |
-42.000 |
|
| Traceless |
| | x | y | z |
| x |
-1.073 |
0.000 |
0.000 |
| y |
0.000 |
-1.073 |
0.000 |
| z |
0.000 |
0.000 |
2.146 |
|
| Polar |
| 3z2-r2 | 4.291 |
| 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 |
8.095 |
0.000 |
0.000 |
| y |
0.000 |
8.095 |
0.000 |
| z |
0.000 |
0.000 |
5.034 |
<r2> (average value of r
2) Å
2
| <r2> |
177.432 |
| (<r2>)1/2 |
13.320 |