Vibrational Frequencies calculated at B97D3/TZVP
| 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' |
3069 |
3025 |
22.28 |
|
|
|
| 2 |
A' |
1290 |
1271 |
68.61 |
|
|
|
| 3 |
A' |
1062 |
1047 |
240.74 |
|
|
|
| 4 |
A' |
744 |
733 |
185.57 |
|
|
|
| 5 |
A' |
579 |
571 |
8.35 |
|
|
|
| 6 |
A' |
385 |
380 |
2.03 |
|
|
|
| 7 |
A" |
1344 |
1325 |
17.33 |
|
|
|
| 8 |
A" |
1070 |
1055 |
271.88 |
|
|
|
| 9 |
A" |
353 |
347 |
0.57 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4947.4 cm
-1
Scaled (by 0.9856) Zero Point Vibrational Energy (zpe) 4876.1 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 B97D3/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.223 |
|
|
|
| 2 |
H |
0.131 |
|
|
|
| 3 |
Cl |
-0.077 |
|
|
|
| 4 |
F |
-0.138 |
|
|
|
| 5 |
F |
-0.138 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.217 |
0.879 |
0.000 |
1.501 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.277 |
-1.060 |
0.000 |
| y |
-1.060 |
-29.240 |
0.000 |
| z |
0.000 |
0.000 |
-30.192 |
|
| Traceless |
| | x | y | z |
| x |
3.439 |
-1.060 |
0.000 |
| y |
-1.060 |
-1.006 |
0.000 |
| z |
0.000 |
0.000 |
-2.434 |
|
| Polar |
| 3z2-r2 | -4.868 |
| x2-y2 | 2.963 |
| xy | -1.060 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.136 |
0.996 |
0.000 |
| y |
0.996 |
3.785 |
0.000 |
| z |
0.000 |
0.000 |
3.151 |
<r2> (average value of r
2) Å
2
| <r2> |
93.025 |
| (<r2>)1/2 |
9.645 |