Vibrational Frequencies calculated at B2PLYP/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 |
1232 |
1232 |
536.69 |
0.57 |
0.45 |
0.62 |
| 2 |
A1 |
697 |
697 |
39.08 |
4.25 |
0.10 |
0.18 |
| 3 |
A1 |
429 |
429 |
7.26 |
1.63 |
0.56 |
0.72 |
| 4 |
B1 |
602 |
602 |
55.21 |
1.50 |
0.75 |
0.86 |
| 5 |
B2 |
1430 |
1430 |
343.96 |
0.00 |
0.75 |
0.86 |
| 6 |
B2 |
345 |
345 |
3.65 |
2.05 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 2366.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 2366.9 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 B2PLYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
B |
0.464 |
|
|
|
| 2 |
Cl |
-0.154 |
|
|
|
| 3 |
F |
-0.155 |
|
|
|
| 4 |
F |
-0.155 |
|
|
|
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 |
-0.046 |
0.046 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.221 |
0.000 |
0.000 |
| y |
0.000 |
-29.854 |
0.000 |
| z |
0.000 |
0.000 |
-29.063 |
|
| Traceless |
| | x | y | z |
| x |
3.238 |
0.000 |
0.000 |
| y |
0.000 |
-2.212 |
0.000 |
| z |
0.000 |
0.000 |
-1.026 |
|
| Polar |
| 3z2-r2 | -2.051 |
| x2-y2 | 3.633 |
| 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 |
2.094 |
0.000 |
0.000 |
| y |
0.000 |
2.755 |
0.000 |
| z |
0.000 |
0.000 |
4.285 |
<r2> (average value of r
2) Å
2
| <r2> |
92.777 |
| (<r2>)1/2 |
9.632 |