Vibrational Frequencies calculated at PBEPBEultrafine/TZVP
| 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' |
3019 |
2985 |
16.23 |
|
|
|
| 2 |
A' |
1442 |
1426 |
0.63 |
|
|
|
| 3 |
A' |
1284 |
1269 |
47.50 |
|
|
|
| 4 |
A' |
1040 |
1029 |
206.72 |
|
|
|
| 5 |
A' |
606 |
599 |
75.34 |
|
|
|
| 6 |
A' |
298 |
295 |
0.48 |
|
|
|
| 7 |
A" |
3104 |
3069 |
5.99 |
|
|
|
| 8 |
A" |
1202 |
1188 |
1.89 |
|
|
|
| 9 |
A" |
903 |
893 |
0.16 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6449.4 cm
-1
Scaled (by 0.9886) Zero Point Vibrational Energy (zpe) 6375.9 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/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.030 |
|
|
|
| 2 |
F |
-0.160 |
|
|
|
| 3 |
Br |
-0.114 |
|
|
|
| 4 |
H |
0.152 |
|
|
|
| 5 |
H |
0.152 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.717 |
-0.648 |
0.000 |
1.835 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-29.528 |
-3.251 |
0.000 |
| y |
-3.251 |
-30.166 |
0.000 |
| z |
0.000 |
0.000 |
-29.451 |
|
| Traceless |
| | x | y | z |
| x |
0.281 |
-3.251 |
0.000 |
| y |
-3.251 |
-0.677 |
0.000 |
| z |
0.000 |
0.000 |
0.396 |
|
| Polar |
| 3z2-r2 | 0.792 |
| x2-y2 | 0.638 |
| xy | -3.251 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.700 |
-0.481 |
0.000 |
| y |
-0.481 |
6.314 |
0.000 |
| z |
0.000 |
0.000 |
3.442 |
<r2> (average value of r
2) Å
2
| <r2> |
93.018 |
| (<r2>)1/2 |
9.645 |