Vibrational Frequencies calculated at ROHF/Def2TZVPP
| 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' |
3356 |
3356 |
1.10 |
|
|
|
| 2 |
A' |
1324 |
1324 |
43.77 |
|
|
|
| 3 |
A' |
811 |
811 |
121.43 |
|
|
|
| 4 |
A' |
655 |
655 |
13.22 |
|
|
|
| 5 |
A' |
357 |
357 |
0.24 |
|
|
|
| 6 |
A' |
241 |
241 |
0.08 |
|
|
|
| 7 |
A" |
1364 |
1364 |
24.57 |
|
|
|
| 8 |
A" |
859 |
859 |
131.47 |
|
|
|
| 9 |
A" |
233 |
233 |
0.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4599.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4599.6 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/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.062 |
|
|
|
| 2 |
H |
0.118 |
|
|
|
| 3 |
Br |
-0.052 |
|
|
|
| 4 |
Cl |
-0.064 |
|
|
|
| 5 |
Cl |
-0.064 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.964 |
0.632 |
0.000 |
1.152 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-47.803 |
-0.571 |
-0.002 |
| y |
-0.571 |
-50.036 |
-0.003 |
| z |
-0.002 |
-0.003 |
-50.466 |
|
| Traceless |
| | x | y | z |
| x |
2.448 |
-0.571 |
-0.002 |
| y |
-0.571 |
-0.902 |
-0.003 |
| z |
-0.002 |
-0.003 |
-1.547 |
|
| Polar |
| 3z2-r2 | -3.093 |
| x2-y2 | 2.233 |
| xy | -0.571 |
| 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> |
231.931 |
| (<r2>)1/2 |
15.229 |