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' |
3002 |
2984 |
19.28 |
|
|
|
| 2 |
A' |
1420 |
1411 |
1.05 |
|
|
|
| 3 |
A' |
1259 |
1251 |
46.59 |
|
|
|
| 4 |
A' |
1081 |
1075 |
189.41 |
|
|
|
| 5 |
A' |
605 |
601 |
68.62 |
|
|
|
| 6 |
A' |
296 |
295 |
0.63 |
|
|
|
| 7 |
A" |
3089 |
3071 |
10.30 |
|
|
|
| 8 |
A" |
1188 |
1181 |
2.71 |
|
|
|
| 9 |
A" |
894 |
889 |
0.08 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6416.1 cm
-1
Scaled (by 0.9942) Zero Point Vibrational Energy (zpe) 6378.9 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 |
0.097 |
|
|
|
| 2 |
F |
-0.155 |
|
|
|
| 3 |
Br |
-0.110 |
|
|
|
| 4 |
H |
0.084 |
|
|
|
| 5 |
H |
0.084 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.505 |
-0.803 |
0.000 |
1.706 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-28.875 |
-2.729 |
0.000 |
| y |
-2.729 |
-29.219 |
0.000 |
| z |
0.000 |
0.000 |
-28.998 |
|
| Traceless |
| | x | y | z |
| x |
0.234 |
-2.729 |
0.000 |
| y |
-2.729 |
-0.283 |
0.000 |
| z |
0.000 |
0.000 |
0.049 |
|
| Polar |
| 3z2-r2 | 0.098 |
| x2-y2 | 0.344 |
| xy | -2.729 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.220 |
-0.499 |
0.000 |
| y |
-0.499 |
5.710 |
0.000 |
| z |
0.000 |
0.000 |
3.003 |
<r2> (average value of r
2) Å
2
| <r2> |
92.614 |
| (<r2>)1/2 |
9.624 |