Vibrational Frequencies calculated at ROHF/aug-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' |
3358 |
3358 |
4.18 |
|
|
|
| 2 |
A' |
1338 |
1338 |
28.12 |
|
|
|
| 3 |
A' |
832 |
832 |
107.86 |
|
|
|
| 4 |
A' |
613 |
613 |
4.90 |
|
|
|
| 5 |
A' |
302 |
302 |
0.09 |
|
|
|
| 6 |
A' |
182 |
182 |
0.01 |
|
|
|
| 7 |
A" |
1298 |
1298 |
47.89 |
|
|
|
| 8 |
A" |
752 |
752 |
99.66 |
|
|
|
| 9 |
A" |
217 |
217 |
0.06 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4446.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4446.4 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/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.136 |
|
|
|
| 2 |
H |
0.274 |
|
|
|
| 3 |
Cl |
-0.197 |
|
|
|
| 4 |
Br |
0.030 |
|
|
|
| 5 |
Br |
0.030 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.935 |
0.499 |
0.000 |
1.059 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-55.199 |
-1.324 |
0.000 |
| y |
-1.324 |
-55.112 |
0.000 |
| z |
0.000 |
0.000 |
-55.592 |
|
| Traceless |
| | x | y | z |
| x |
0.153 |
-1.324 |
0.000 |
| y |
-1.324 |
0.283 |
0.000 |
| z |
0.000 |
0.000 |
-0.437 |
|
| Polar |
| 3z2-r2 | -0.873 |
| x2-y2 | -0.087 |
| xy | -1.324 |
| xz | 0.000 |
| yz | 0.000 |
|
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> |
0.000 |
| (<r2>)1/2 |
0.000 |