Vibrational Frequencies calculated at BLYP/6-311G*
| 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' |
3057 |
3050 |
7.90 |
|
|
|
| 2 |
A' |
1419 |
1416 |
0.26 |
|
|
|
| 3 |
A' |
1232 |
1229 |
63.05 |
|
|
|
| 4 |
A' |
657 |
656 |
115.06 |
|
|
|
| 5 |
A' |
547 |
546 |
62.43 |
|
|
|
| 6 |
A' |
214 |
213 |
0.14 |
|
|
|
| 7 |
A" |
3142 |
3134 |
0.29 |
|
|
|
| 8 |
A" |
1127 |
1124 |
0.12 |
|
|
|
| 9 |
A" |
830 |
828 |
6.46 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6113.0 cm
-1
Scaled (by 0.9975) Zero Point Vibrational Energy (zpe) 6097.7 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 BLYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.553 |
|
|
|
| 2 |
Br |
0.004 |
|
|
|
| 3 |
Cl |
-0.027 |
|
|
|
| 4 |
H |
0.288 |
|
|
|
| 5 |
H |
0.288 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.983 |
1.386 |
0.000 |
1.699 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-39.960 |
1.336 |
0.000 |
| y |
1.336 |
-35.740 |
0.000 |
| z |
0.000 |
0.000 |
-37.873 |
|
| Traceless |
| | x | y | z |
| x |
-3.153 |
1.336 |
0.000 |
| y |
1.336 |
3.176 |
0.000 |
| z |
0.000 |
0.000 |
-0.023 |
|
| Polar |
| 3z2-r2 | -0.046 |
| x2-y2 | -4.220 |
| xy | 1.336 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.277 |
-1.874 |
0.000 |
| y |
-1.874 |
5.968 |
0.000 |
| z |
0.000 |
0.000 |
3.519 |
<r2> (average value of r
2) Å
2
| <r2> |
154.501 |
| (<r2>)1/2 |
12.430 |