Vibrational Frequencies calculated at B1B95/6-311G*
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
1245 |
1193 |
549.50 |
0.49 |
0.48 |
0.65 |
| 2 |
A1 |
703 |
674 |
38.37 |
3.98 |
0.10 |
0.18 |
| 3 |
A1 |
427 |
410 |
7.40 |
1.49 |
0.57 |
0.73 |
| 4 |
B1 |
595 |
571 |
53.71 |
1.49 |
0.75 |
0.86 |
| 5 |
B2 |
1443 |
1384 |
351.51 |
0.00 |
0.75 |
0.86 |
| 6 |
B2 |
342 |
328 |
3.43 |
1.94 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 2377.9 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 2279.4 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 B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
B |
0.443 |
|
|
|
| 2 |
Cl |
-0.151 |
|
|
|
| 3 |
F |
-0.146 |
|
|
|
| 4 |
F |
-0.146 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-0.012 |
0.012 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.987 |
0.000 |
0.000 |
| y |
0.000 |
-29.512 |
0.000 |
| z |
0.000 |
0.000 |
-28.686 |
|
| Traceless |
| | x | y | z |
| x |
3.112 |
0.000 |
0.000 |
| y |
0.000 |
-2.176 |
0.000 |
| z |
0.000 |
0.000 |
-0.937 |
|
| Polar |
| 3z2-r2 | -1.873 |
| x2-y2 | 3.525 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.100 |
0.000 |
0.000 |
| y |
0.000 |
2.741 |
0.000 |
| z |
0.000 |
0.000 |
4.262 |
<r2> (average value of r
2) Å
2
| <r2> |
91.995 |
| (<r2>)1/2 |
9.591 |