Vibrational Frequencies calculated at B3LYPultrafine/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' |
3129 |
3027 |
2.78 |
|
|
|
| 2 |
A' |
1449 |
1402 |
0.04 |
|
|
|
| 3 |
A' |
1249 |
1208 |
51.25 |
|
|
|
| 4 |
A' |
713 |
690 |
100.55 |
|
|
|
| 5 |
A' |
595 |
575 |
37.90 |
|
|
|
| 6 |
A' |
222 |
215 |
0.18 |
|
|
|
| 7 |
A" |
3209 |
3105 |
1.24 |
|
|
|
| 8 |
A" |
1146 |
1109 |
0.00 |
|
|
|
| 9 |
A" |
854 |
826 |
2.33 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6283.0 cm
-1
Scaled (by 0.9675) Zero Point Vibrational Energy (zpe) 6078.8 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 B3LYPultrafine/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.318 |
|
|
|
| 2 |
Br |
0.024 |
|
|
|
| 3 |
Cl |
-0.154 |
|
|
|
| 4 |
H |
0.224 |
|
|
|
| 5 |
H |
0.224 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.814 |
1.355 |
0.000 |
1.581 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-39.523 |
1.353 |
0.000 |
| y |
1.353 |
-35.553 |
0.000 |
| z |
0.000 |
0.000 |
-37.541 |
|
| Traceless |
| | x | y | z |
| x |
-2.976 |
1.353 |
0.000 |
| y |
1.353 |
2.979 |
0.000 |
| z |
0.000 |
0.000 |
-0.003 |
|
| Polar |
| 3z2-r2 | -0.006 |
| x2-y2 | -3.970 |
| xy | 1.353 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.932 |
-1.522 |
0.000 |
| y |
-1.522 |
7.900 |
0.000 |
| z |
0.000 |
0.000 |
6.170 |
<r2> (average value of r
2) Å
2
| <r2> |
149.562 |
| (<r2>)1/2 |
12.230 |