Vibrational Frequencies calculated at B3PW91/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' |
3102 |
2991 |
16.27 |
|
|
|
| 2 |
A' |
1494 |
1441 |
0.98 |
|
|
|
| 3 |
A' |
1338 |
1290 |
55.56 |
|
|
|
| 4 |
A' |
1096 |
1057 |
213.90 |
|
|
|
| 5 |
A' |
636 |
613 |
74.81 |
|
|
|
| 6 |
A' |
311 |
300 |
0.47 |
|
|
|
| 7 |
A" |
3187 |
3073 |
5.17 |
|
|
|
| 8 |
A" |
1253 |
1208 |
2.65 |
|
|
|
| 9 |
A" |
938 |
904 |
0.07 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6677.2 cm
-1
Scaled (by 0.9643) Zero Point Vibrational Energy (zpe) 6438.9 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 B3PW91/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.019 |
|
|
|
| 2 |
F |
-0.185 |
|
|
|
| 3 |
Br |
-0.125 |
|
|
|
| 4 |
H |
0.145 |
|
|
|
| 5 |
H |
0.145 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.789 |
-0.648 |
0.000 |
1.903 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-29.311 |
-3.371 |
0.000 |
| y |
-3.371 |
-30.058 |
0.000 |
| z |
0.000 |
0.000 |
-29.187 |
|
| Traceless |
| | x | y | z |
| x |
0.311 |
-3.371 |
0.000 |
| y |
-3.371 |
-0.809 |
0.000 |
| z |
0.000 |
0.000 |
0.498 |
|
| Polar |
| 3z2-r2 | 0.996 |
| x2-y2 | 0.747 |
| xy | -3.371 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.569 |
-0.484 |
0.000 |
| y |
-0.484 |
6.005 |
0.000 |
| z |
0.000 |
0.000 |
3.323 |
<r2> (average value of r
2) Å
2
| <r2> |
91.516 |
| (<r2>)1/2 |
9.566 |