Vibrational Frequencies calculated at wB97X-D/aug-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' |
3144 |
3008 |
10.35 |
|
|
|
| 2 |
A' |
1320 |
1262 |
58.87 |
|
|
|
| 3 |
A' |
1131 |
1082 |
229.89 |
|
|
|
| 4 |
A' |
808 |
773 |
155.25 |
|
|
|
| 5 |
A' |
605 |
579 |
6.41 |
|
|
|
| 6 |
A' |
413 |
395 |
0.10 |
|
|
|
| 7 |
A" |
1390 |
1330 |
12.34 |
|
|
|
| 8 |
A" |
1150 |
1100 |
235.92 |
|
|
|
| 9 |
A" |
367 |
351 |
0.43 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5164.5 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 4940.4 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 wB97X-D/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.503 |
|
|
|
| 2 |
H |
0.282 |
|
|
|
| 3 |
Cl |
-0.139 |
|
|
|
| 4 |
F |
-0.323 |
|
|
|
| 5 |
F |
-0.323 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.148 |
0.883 |
0.000 |
1.449 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.149 |
-0.994 |
0.000 |
| y |
-0.994 |
-29.183 |
0.000 |
| z |
0.000 |
0.000 |
-30.088 |
|
| Traceless |
| | x | y | z |
| x |
3.486 |
-0.994 |
0.000 |
| y |
-0.994 |
-1.064 |
0.000 |
| z |
0.000 |
0.000 |
-2.422 |
|
| Polar |
| 3z2-r2 | -4.844 |
| x2-y2 | 3.033 |
| xy | -0.994 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.887 |
0.703 |
0.000 |
| y |
0.703 |
4.697 |
0.000 |
| z |
0.000 |
0.000 |
4.278 |
<r2> (average value of r
2) Å
2
| <r2> |
90.667 |
| (<r2>)1/2 |
9.522 |