Vibrational Frequencies calculated at mPW1PW91/aug-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' |
3122 |
2992 |
13.43 |
|
|
|
| 2 |
A' |
1460 |
1399 |
0.68 |
|
|
|
| 3 |
A' |
1317 |
1262 |
35.50 |
|
|
|
| 4 |
A' |
1086 |
1041 |
192.54 |
|
|
|
| 5 |
A' |
656 |
629 |
68.71 |
|
|
|
| 6 |
A' |
314 |
301 |
0.44 |
|
|
|
| 7 |
A" |
3217 |
3082 |
1.92 |
|
|
|
| 8 |
A" |
1235 |
1183 |
2.30 |
|
|
|
| 9 |
A" |
938 |
899 |
0.06 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6671.7 cm
-1
Scaled (by 0.9583) Zero Point Vibrational Energy (zpe) 6393.5 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 mPW1PW91/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.398 |
|
|
|
| 2 |
F |
-0.374 |
|
|
|
| 3 |
Br |
0.203 |
|
|
|
| 4 |
H |
-0.113 |
|
|
|
| 5 |
H |
-0.113 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.690 |
-0.637 |
0.000 |
1.806 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-29.466 |
-3.371 |
0.000 |
| y |
-3.371 |
-30.111 |
0.000 |
| z |
0.000 |
0.000 |
-29.302 |
|
| Traceless |
| | x | y | z |
| x |
0.241 |
-3.371 |
0.000 |
| y |
-3.371 |
-0.727 |
0.000 |
| z |
0.000 |
0.000 |
0.486 |
|
| Polar |
| 3z2-r2 | 0.972 |
| x2-y2 | 0.645 |
| xy | -3.371 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.854 |
-0.300 |
0.000 |
| y |
-0.300 |
6.745 |
0.000 |
| z |
0.000 |
0.000 |
4.587 |
<r2> (average value of r
2) Å
2
| <r2> |
90.827 |
| (<r2>)1/2 |
9.530 |