Vibrational Frequencies calculated at PBEPBEultrafine/cc-pVDZ
| 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' |
3047 |
3029 |
4.79 |
|
|
|
| 2 |
A' |
1367 |
1359 |
0.01 |
|
|
|
| 3 |
A' |
1182 |
1175 |
48.64 |
|
|
|
| 4 |
A' |
710 |
706 |
109.92 |
|
|
|
| 5 |
A' |
584 |
580 |
44.02 |
|
|
|
| 6 |
A' |
219 |
218 |
0.18 |
|
|
|
| 7 |
A" |
3138 |
3120 |
0.14 |
|
|
|
| 8 |
A" |
1088 |
1082 |
0.00 |
|
|
|
| 9 |
A" |
815 |
810 |
3.64 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6075.2 cm
-1
Scaled (by 0.9942) Zero Point Vibrational Energy (zpe) 6039.9 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 PBEPBEultrafine/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.159 |
|
|
|
| 2 |
Br |
-0.043 |
|
|
|
| 3 |
Cl |
-0.058 |
|
|
|
| 4 |
H |
0.130 |
|
|
|
| 5 |
H |
0.130 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.811 |
1.299 |
0.000 |
1.531 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-38.505 |
1.103 |
0.000 |
| y |
1.103 |
-34.827 |
0.000 |
| z |
0.000 |
0.000 |
-36.876 |
|
| Traceless |
| | x | y | z |
| x |
-2.653 |
1.103 |
0.000 |
| y |
1.103 |
2.863 |
0.000 |
| z |
0.000 |
0.000 |
-0.210 |
|
| Polar |
| 3z2-r2 | -0.420 |
| x2-y2 | -3.678 |
| xy | 1.103 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.688 |
-1.630 |
0.000 |
| y |
-1.630 |
5.722 |
0.000 |
| z |
0.000 |
0.000 |
3.493 |
<r2> (average value of r
2) Å
2
| <r2> |
150.291 |
| (<r2>)1/2 |
12.259 |