Vibrational Frequencies calculated at PBE1PBE/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' |
3103 |
2982 |
16.05 |
|
|
|
| 2 |
A' |
1495 |
1437 |
0.64 |
|
|
|
| 3 |
A' |
1336 |
1284 |
42.13 |
|
|
|
| 4 |
A' |
1126 |
1082 |
191.50 |
|
|
|
| 5 |
A' |
657 |
631 |
66.07 |
|
|
|
| 6 |
A' |
317 |
304 |
0.42 |
|
|
|
| 7 |
A" |
3185 |
3061 |
4.73 |
|
|
|
| 8 |
A" |
1256 |
1207 |
2.64 |
|
|
|
| 9 |
A" |
946 |
910 |
0.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6710.7 cm
-1
Scaled (by 0.961) Zero Point Vibrational Energy (zpe) 6448.9 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 PBE1PBE/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.122 |
|
|
|
| 2 |
F |
-0.175 |
|
|
|
| 3 |
Br |
-0.123 |
|
|
|
| 4 |
H |
0.088 |
|
|
|
| 5 |
H |
0.088 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.616 |
-0.727 |
0.000 |
1.772 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-29.194 |
-3.029 |
0.000 |
| y |
-3.029 |
-29.767 |
0.000 |
| z |
0.000 |
0.000 |
-29.154 |
|
| Traceless |
| | x | y | z |
| x |
0.266 |
-3.029 |
0.000 |
| y |
-3.029 |
-0.593 |
0.000 |
| z |
0.000 |
0.000 |
0.327 |
|
| Polar |
| 3z2-r2 | 0.654 |
| x2-y2 | 0.572 |
| xy | -3.029 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.943 |
-0.438 |
0.000 |
| y |
-0.438 |
6.139 |
0.000 |
| z |
0.000 |
0.000 |
3.717 |
<r2> (average value of r
2) Å
2
| <r2> |
90.340 |
| (<r2>)1/2 |
9.505 |