Vibrational Frequencies calculated at B2PLYP=FULLultrafine/cc-pVTZ
| 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 |
1855 |
1773 |
323.18 |
15.71 |
0.55 |
0.71 |
| 2 |
A1 |
568 |
543 |
18.42 |
16.34 |
0.12 |
0.21 |
| 3 |
A1 |
303 |
289 |
0.10 |
4.87 |
0.61 |
0.76 |
| 4 |
B1 |
593 |
566 |
5.66 |
0.04 |
0.75 |
0.86 |
| 5 |
B2 |
834 |
797 |
490.25 |
2.69 |
0.75 |
0.86 |
| 6 |
B2 |
441 |
421 |
1.47 |
6.45 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 2297.0 cm
-1
Scaled (by 0.9554) Zero Point Vibrational Energy (zpe) 2194.5 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 B2PLYP=FULLultrafine/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.138 |
|
|
|
| 2 |
C |
0.219 |
|
|
|
| 3 |
Cl |
-0.041 |
|
|
|
| 4 |
Cl |
-0.041 |
|
|
|
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 |
-1.125 |
1.125 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-34.823 |
0.000 |
0.000 |
| y |
0.000 |
-34.436 |
0.000 |
| z |
0.000 |
0.000 |
-38.239 |
|
| Traceless |
| | x | y | z |
| x |
1.514 |
0.000 |
0.000 |
| y |
0.000 |
2.095 |
0.000 |
| z |
0.000 |
0.000 |
-3.609 |
|
| Polar |
| 3z2-r2 | -7.218 |
| x2-y2 | -0.387 |
| 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 |
3.380 |
0.000 |
0.000 |
| y |
0.000 |
7.457 |
0.000 |
| z |
0.000 |
0.000 |
5.867 |
<r2> (average value of r
2) Å
2
| <r2> |
125.787 |
| (<r2>)1/2 |
11.215 |