Vibrational Frequencies calculated at ROHF/cc-pVTZ-PP
| 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' |
3357 |
3357 |
0.96 |
|
|
|
| 2 |
A' |
1322 |
1322 |
46.39 |
|
|
|
| 3 |
A' |
812 |
812 |
123.24 |
|
|
|
| 4 |
A' |
657 |
657 |
12.36 |
|
|
|
| 5 |
A' |
356 |
356 |
0.25 |
|
|
|
| 6 |
A' |
240 |
240 |
0.12 |
|
|
|
| 7 |
A" |
1361 |
1361 |
25.47 |
|
|
|
| 8 |
A" |
857 |
857 |
133.09 |
|
|
|
| 9 |
A" |
233 |
233 |
0.03 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4597.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4597.2 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 ROHF/cc-pVTZ-PP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.028 |
|
|
|
| 2 |
H |
0.174 |
|
|
|
| 3 |
Br |
-0.018 |
|
|
|
| 4 |
Cl |
-0.092 |
|
|
|
| 5 |
Cl |
-0.092 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.917 |
0.717 |
0.000 |
1.164 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-47.400 |
-0.519 |
-0.002 |
| y |
-0.519 |
-49.667 |
-0.003 |
| z |
-0.002 |
-0.003 |
-50.236 |
|
| Traceless |
| | x | y | z |
| x |
2.552 |
-0.519 |
-0.002 |
| y |
-0.519 |
-0.849 |
-0.003 |
| z |
-0.002 |
-0.003 |
-1.703 |
|
| Polar |
| 3z2-r2 | -3.406 |
| x2-y2 | 2.267 |
| xy | -0.519 |
| xz | -0.002 |
| yz | -0.003 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
212.960 |
| (<r2>)1/2 |
14.593 |