Vibrational Frequencies calculated at HF/LANL2DZ
| 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 |
1228 |
1105 |
565.69 |
0.70 |
0.35 |
0.51 |
| 2 |
A1 |
662 |
596 |
39.97 |
4.41 |
0.13 |
0.23 |
| 3 |
A1 |
408 |
367 |
18.97 |
1.93 |
0.58 |
0.73 |
| 4 |
B1 |
609 |
548 |
125.66 |
1.91 |
0.75 |
0.86 |
| 5 |
B2 |
1425 |
1283 |
452.75 |
0.04 |
0.75 |
0.86 |
| 6 |
B2 |
336 |
302 |
11.60 |
2.79 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 2334.0 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 2100.4 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 HF/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
B |
0.699 |
|
|
|
| 2 |
Cl |
-0.072 |
|
|
|
| 3 |
F |
-0.314 |
|
|
|
| 4 |
F |
-0.314 |
|
|
|
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 |
0.284 |
0.284 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.384 |
0.000 |
0.000 |
| y |
0.000 |
-31.541 |
0.000 |
| z |
0.000 |
0.000 |
-31.217 |
|
| Traceless |
| | x | y | z |
| x |
5.995 |
0.000 |
0.000 |
| y |
0.000 |
-3.240 |
0.000 |
| z |
0.000 |
0.000 |
-2.755 |
|
| Polar |
| 3z2-r2 | -5.509 |
| x2-y2 | 6.157 |
| 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 |
1.229 |
0.000 |
0.000 |
| y |
0.000 |
1.852 |
0.000 |
| z |
0.000 |
0.000 |
3.334 |
<r2> (average value of r
2) Å
2
| <r2> |
78.324 |
| (<r2>)1/2 |
8.850 |