Vibrational Frequencies calculated at B97D3/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' |
3025 |
2979 |
23.58 |
|
|
|
| 2 |
A' |
1463 |
1441 |
0.18 |
|
|
|
| 3 |
A' |
1334 |
1314 |
27.18 |
|
|
|
| 4 |
A' |
1028 |
1012 |
173.67 |
|
|
|
| 5 |
A' |
694 |
683 |
109.92 |
|
|
|
| 6 |
A' |
367 |
361 |
0.80 |
|
|
|
| 7 |
A" |
3102 |
3055 |
8.39 |
|
|
|
| 8 |
A" |
1221 |
1202 |
2.16 |
|
|
|
| 9 |
A" |
983 |
968 |
0.25 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6608.0 cm
-1
Scaled (by 0.9847) Zero Point Vibrational Energy (zpe) 6506.9 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/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.150 |
|
|
|
| 2 |
F |
-0.357 |
|
|
|
| 3 |
Cl |
-0.185 |
|
|
|
| 4 |
H |
0.196 |
|
|
|
| 5 |
H |
0.196 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.894 |
1.563 |
0.000 |
1.801 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.499 |
-1.385 |
0.000 |
| y |
-1.385 |
-22.478 |
0.000 |
| z |
0.000 |
0.000 |
-23.378 |
|
| Traceless |
| | x | y | z |
| x |
-3.571 |
-1.385 |
0.000 |
| y |
-1.385 |
2.461 |
0.000 |
| z |
0.000 |
0.000 |
1.110 |
|
| Polar |
| 3z2-r2 | 2.220 |
| x2-y2 | -4.021 |
| xy | -1.385 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.693 |
0.651 |
0.000 |
| y |
0.651 |
5.384 |
0.000 |
| z |
0.000 |
0.000 |
4.058 |
<r2> (average value of r
2) Å
2
| <r2> |
66.845 |
| (<r2>)1/2 |
8.176 |