Vibrational Frequencies calculated at mPW1PW91/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 |
A' |
3198 |
3068 |
1.28 |
|
|
|
| 2 |
A' |
1201 |
1152 |
31.99 |
|
|
|
| 3 |
A' |
734 |
704 |
127.06 |
|
|
|
| 4 |
A' |
614 |
589 |
22.89 |
|
|
|
| 5 |
A' |
334 |
320 |
0.19 |
|
|
|
| 6 |
A' |
222 |
213 |
0.01 |
|
|
|
| 7 |
A" |
1241 |
1190 |
17.10 |
|
|
|
| 8 |
A" |
775 |
743 |
147.37 |
|
|
|
| 9 |
A" |
215 |
206 |
0.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4266.3 cm
-1
Scaled (by 0.9592) Zero Point Vibrational Energy (zpe) 4092.2 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 mPW1PW91/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.036 |
|
|
|
| 2 |
H |
0.156 |
|
|
|
| 3 |
Br |
-0.015 |
|
|
|
| 4 |
Cl |
-0.053 |
|
|
|
| 5 |
Cl |
-0.053 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.881 |
0.581 |
0.000 |
1.055 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-47.269 |
-0.407 |
0.000 |
| y |
-0.407 |
-49.246 |
0.000 |
| z |
0.000 |
0.000 |
-49.643 |
|
| Traceless |
| | x | y | z |
| x |
2.175 |
-0.407 |
0.000 |
| y |
-0.407 |
-0.790 |
0.000 |
| z |
0.000 |
0.000 |
-1.385 |
|
| Polar |
| 3z2-r2 | -2.771 |
| x2-y2 | 1.977 |
| xy | -0.407 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.876 |
1.868 |
0.000 |
| y |
1.868 |
8.293 |
0.000 |
| z |
0.000 |
0.000 |
8.527 |
<r2> (average value of r
2) Å
2
| <r2> |
232.526 |
| (<r2>)1/2 |
15.249 |