Vibrational Frequencies calculated at HSEh1PBE/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' |
1824 |
1751 |
386.81 |
|
|
|
| 2 |
A' |
1370 |
1315 |
314.16 |
|
|
|
| 3 |
A' |
843 |
809 |
233.48 |
|
|
|
| 4 |
A' |
773 |
742 |
3.99 |
|
|
|
| 5 |
A' |
590 |
566 |
99.88 |
|
|
|
| 6 |
A' |
408 |
392 |
1.47 |
|
|
|
| 7 |
A' |
211 |
203 |
0.00 |
|
|
|
| 8 |
A" |
754 |
724 |
11.65 |
|
|
|
| 9 |
A" |
123 |
119 |
0.46 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3447.8 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 3310.3 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 HSEh1PBE/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Br |
0.172 |
|
|
|
| 2 |
O |
-0.192 |
|
|
|
| 3 |
N |
0.242 |
|
|
|
| 4 |
O |
-0.114 |
|
|
|
| 5 |
O |
-0.108 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.464 |
-1.108 |
0.000 |
1.836 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-40.083 |
1.406 |
0.000 |
| y |
1.406 |
-41.299 |
0.000 |
| z |
0.000 |
0.000 |
-38.491 |
|
| Traceless |
| | x | y | z |
| x |
-0.188 |
1.406 |
0.000 |
| y |
1.406 |
-2.012 |
0.000 |
| z |
0.000 |
0.000 |
2.200 |
|
| Polar |
| 3z2-r2 | 4.400 |
| x2-y2 | 1.216 |
| xy | 1.406 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.950 |
1.991 |
0.000 |
| y |
1.991 |
6.320 |
0.000 |
| z |
0.000 |
0.000 |
2.823 |
<r2> (average value of r
2) Å
2
| <r2> |
183.624 |
| (<r2>)1/2 |
13.551 |