Vibrational Frequencies calculated at B3LYPultrafine/6-31G*
| 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' |
3175 |
3041 |
8.54 |
|
|
|
| 2 |
A' |
1357 |
1300 |
25.61 |
|
|
|
| 3 |
A' |
1134 |
1086 |
189.96 |
|
|
|
| 4 |
A' |
728 |
697 |
49.02 |
|
|
|
| 5 |
A' |
450 |
431 |
2.47 |
|
|
|
| 6 |
A' |
274 |
262 |
0.21 |
|
|
|
| 7 |
A" |
1284 |
1231 |
71.30 |
|
|
|
| 8 |
A" |
768 |
735 |
277.20 |
|
|
|
| 9 |
A" |
361 |
346 |
0.10 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4764.9 cm
-1
Scaled (by 0.958) Zero Point Vibrational Energy (zpe) 4564.8 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 B3LYPultrafine/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.009 |
|
|
|
| 2 |
H |
0.230 |
|
|
|
| 3 |
F |
-0.222 |
|
|
|
| 4 |
Cl |
0.001 |
|
|
|
| 5 |
Cl |
0.001 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.115 |
0.829 |
0.000 |
1.390 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-35.543 |
-1.694 |
0.000 |
| y |
-1.694 |
-35.282 |
0.000 |
| z |
0.000 |
0.000 |
-36.567 |
|
| Traceless |
| | x | y | z |
| x |
0.381 |
-1.694 |
0.000 |
| y |
-1.694 |
0.773 |
0.000 |
| z |
0.000 |
0.000 |
-1.154 |
|
| Polar |
| 3z2-r2 | -2.308 |
| x2-y2 | -0.262 |
| xy | -1.694 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.183 |
0.143 |
0.000 |
| y |
0.143 |
4.131 |
0.000 |
| z |
0.000 |
0.000 |
6.362 |
<r2> (average value of r
2) Å
2
| <r2> |
133.272 |
| (<r2>)1/2 |
11.544 |