Vibrational Frequencies calculated at wB97X-D/cc-pVQZ
| 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' |
3149 |
3149 |
3.15 |
|
|
|
| 2 |
A' |
1464 |
1464 |
0.19 |
|
|
|
| 3 |
A' |
1256 |
1256 |
48.57 |
|
|
|
| 4 |
A' |
759 |
759 |
96.65 |
|
|
|
| 5 |
A' |
633 |
633 |
23.07 |
|
|
|
| 6 |
A' |
230 |
230 |
0.24 |
|
|
|
| 7 |
A" |
3231 |
3231 |
0.95 |
|
|
|
| 8 |
A" |
1153 |
1153 |
0.00 |
|
|
|
| 9 |
A" |
869 |
869 |
2.50 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6372.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 6372.2 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-pVQZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.100 |
|
|
|
| 2 |
Br |
-0.046 |
|
|
|
| 3 |
Cl |
-0.055 |
|
|
|
| 4 |
H |
0.101 |
|
|
|
| 5 |
H |
0.101 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.856 |
1.359 |
0.000 |
1.606 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-39.106 |
1.312 |
0.000 |
| y |
1.312 |
-35.092 |
0.000 |
| z |
0.000 |
0.000 |
-37.109 |
|
| Traceless |
| | x | y | z |
| x |
-3.006 |
1.312 |
0.000 |
| y |
1.312 |
3.015 |
0.000 |
| z |
0.000 |
0.000 |
-0.010 |
|
| Polar |
| 3z2-r2 | -0.019 |
| x2-y2 | -4.014 |
| xy | 1.312 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.111 |
-1.458 |
0.000 |
| y |
-1.458 |
7.129 |
0.000 |
| z |
0.000 |
0.000 |
5.320 |
<r2> (average value of r
2) Å
2
| <r2> |
146.600 |
| (<r2>)1/2 |
12.108 |