Vibrational Frequencies calculated at HF/daug-cc-pVTZ
| 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' |
3335 |
3016 |
1.71 |
|
|
|
| 2 |
A' |
1474 |
1333 |
19.97 |
|
|
|
| 3 |
A' |
1237 |
1119 |
200.39 |
|
|
|
| 4 |
A' |
795 |
719 |
43.30 |
|
|
|
| 5 |
A' |
496 |
449 |
1.56 |
|
|
|
| 6 |
A' |
297 |
269 |
0.12 |
|
|
|
| 7 |
A" |
1384 |
1252 |
71.14 |
|
|
|
| 8 |
A" |
886 |
802 |
248.89 |
|
|
|
| 9 |
A" |
402 |
364 |
0.41 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5153.0 cm
-1
Scaled (by 0.9046) Zero Point Vibrational Energy (zpe) 4661.4 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/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
1.032 |
|
|
|
| 2 |
H |
0.565 |
|
|
|
| 3 |
F |
-0.702 |
|
|
|
| 4 |
Cl |
-0.448 |
|
|
|
| 5 |
Cl |
-0.448 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.233 |
0.646 |
0.000 |
1.392 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-36.282 |
-2.162 |
0.000 |
| y |
-2.162 |
-35.872 |
0.000 |
| z |
0.000 |
0.000 |
-36.701 |
|
| Traceless |
| | x | y | z |
| x |
0.005 |
-2.162 |
0.000 |
| y |
-2.162 |
0.620 |
0.000 |
| z |
0.000 |
0.000 |
-0.624 |
|
| Polar |
| 3z2-r2 | -1.249 |
| x2-y2 | -0.410 |
| xy | -2.162 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.090 |
0.125 |
0.000 |
| y |
0.125 |
5.648 |
0.000 |
| z |
0.000 |
0.000 |
7.514 |
<r2> (average value of r
2) Å
2
| <r2> |
129.815 |
| (<r2>)1/2 |
11.394 |