Vibrational Frequencies calculated at wB97X-D/cc-pVDZ
| 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' |
3188 |
3037 |
2.32 |
|
|
|
| 2 |
A' |
1335 |
1271 |
17.36 |
|
|
|
| 3 |
A' |
1115 |
1062 |
220.69 |
|
|
|
| 4 |
A' |
751 |
715 |
46.83 |
|
|
|
| 5 |
A' |
464 |
442 |
1.65 |
|
|
|
| 6 |
A' |
285 |
272 |
0.09 |
|
|
|
| 7 |
A" |
1295 |
1234 |
65.69 |
|
|
|
| 8 |
A" |
821 |
782 |
262.39 |
|
|
|
| 9 |
A" |
371 |
354 |
0.29 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4812.4 cm
-1
Scaled (by 0.9526) Zero Point Vibrational Energy (zpe) 4584.3 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 wB97X-D/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.173 |
|
|
|
| 2 |
H |
0.238 |
|
|
|
| 3 |
F |
-0.183 |
|
|
|
| 4 |
Cl |
0.059 |
|
|
|
| 5 |
Cl |
0.059 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.309 |
0.619 |
0.000 |
1.448 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-36.257 |
-2.154 |
0.000 |
| y |
-2.154 |
-35.942 |
0.000 |
| z |
0.000 |
0.000 |
-36.605 |
|
| Traceless |
| | x | y | z |
| x |
0.016 |
-2.154 |
0.000 |
| y |
-2.154 |
0.489 |
0.000 |
| z |
0.000 |
0.000 |
-0.506 |
|
| Polar |
| 3z2-r2 | -1.012 |
| x2-y2 | -0.315 |
| xy | -2.154 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.155 |
0.164 |
0.000 |
| y |
0.164 |
4.906 |
0.000 |
| z |
0.000 |
0.000 |
6.881 |
<r2> (average value of r
2) Å
2
| <r2> |
131.917 |
| (<r2>)1/2 |
11.486 |