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 |
A' |
1889 |
1814 |
381.15 |
|
|
|
| 2 |
A' |
1396 |
1341 |
294.85 |
|
|
|
| 3 |
A' |
847 |
814 |
191.23 |
|
|
|
| 4 |
A' |
812 |
780 |
30.75 |
|
|
|
| 5 |
A' |
602 |
578 |
65.13 |
|
|
|
| 6 |
A' |
464 |
445 |
13.31 |
|
|
|
| 7 |
A' |
251 |
241 |
0.16 |
|
|
|
| 8 |
A" |
757 |
727 |
15.23 |
|
|
|
| 9 |
A" |
133 |
128 |
0.52 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3575.9 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 3433.2 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 |
Cl |
0.213 |
|
|
|
| 2 |
O |
-0.311 |
|
|
|
| 3 |
N |
0.482 |
|
|
|
| 4 |
O |
-0.193 |
|
|
|
| 5 |
O |
-0.192 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.065 |
-0.159 |
0.000 |
1.077 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.844 |
-0.294 |
0.000 |
| y |
-0.294 |
-35.984 |
0.000 |
| z |
0.000 |
0.000 |
-32.591 |
|
| Traceless |
| | x | y | z |
| x |
1.444 |
-0.294 |
0.000 |
| y |
-0.294 |
-3.266 |
0.000 |
| z |
0.000 |
0.000 |
1.822 |
|
| Polar |
| 3z2-r2 | 3.645 |
| x2-y2 | 3.140 |
| xy | -0.294 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.385 |
-0.020 |
0.000 |
| y |
-0.020 |
4.012 |
0.000 |
| z |
0.000 |
0.000 |
1.810 |
<r2> (average value of r
2) Å
2
| <r2> |
131.825 |
| (<r2>)1/2 |
11.482 |