Vibrational Frequencies calculated at HSEh1PBE/3-21G*
| 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' |
1518 |
1457 |
140.04 |
|
|
|
| 2 |
A' |
1151 |
1105 |
260.85 |
|
|
|
| 3 |
A' |
797 |
765 |
149.16 |
|
|
|
| 4 |
A' |
764 |
733 |
0.46 |
|
|
|
| 5 |
A' |
593 |
569 |
11.51 |
|
|
|
| 6 |
A' |
389 |
373 |
0.02 |
|
|
|
| 7 |
A' |
210 |
201 |
0.15 |
|
|
|
| 8 |
A" |
651 |
625 |
11.89 |
|
|
|
| 9 |
A" |
127 |
122 |
0.51 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3099.0 cm
-1
Scaled (by 0.9599) Zero Point Vibrational Energy (zpe) 2974.7 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/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Br |
0.208 |
|
|
|
| 2 |
O |
-0.260 |
|
|
|
| 3 |
N |
0.543 |
|
|
|
| 4 |
O |
-0.239 |
|
|
|
| 5 |
O |
-0.253 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.179 |
-0.967 |
0.000 |
1.525 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-38.596 |
1.214 |
0.000 |
| y |
1.214 |
-40.624 |
0.000 |
| z |
0.000 |
0.000 |
-37.797 |
|
| Traceless |
| | x | y | z |
| x |
0.615 |
1.214 |
0.000 |
| y |
1.214 |
-2.427 |
0.000 |
| z |
0.000 |
0.000 |
1.813 |
|
| Polar |
| 3z2-r2 | 3.625 |
| x2-y2 | 2.028 |
| xy | 1.214 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.416 |
1.817 |
0.000 |
| y |
1.817 |
5.260 |
0.000 |
| z |
0.000 |
0.000 |
2.048 |
<r2> (average value of r
2) Å
2
| <r2> |
185.837 |
| (<r2>)1/2 |
13.632 |