Vibrational Frequencies calculated at B3PW91/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' |
1815 |
1745 |
346.17 |
|
|
|
| 2 |
A' |
1357 |
1305 |
291.93 |
|
|
|
| 3 |
A' |
831 |
799 |
211.45 |
|
|
|
| 4 |
A' |
769 |
740 |
6.32 |
|
|
|
| 5 |
A' |
581 |
558 |
92.09 |
|
|
|
| 6 |
A' |
410 |
395 |
1.77 |
|
|
|
| 7 |
A' |
211 |
203 |
0.00 |
|
|
|
| 8 |
A" |
758 |
729 |
11.93 |
|
|
|
| 9 |
A" |
128 |
123 |
0.24 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3429.8 cm
-1
Scaled (by 0.9616) Zero Point Vibrational Energy (zpe) 3298.1 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 B3PW91/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Br |
0.190 |
|
|
|
| 2 |
O |
-0.261 |
|
|
|
| 3 |
N |
0.481 |
|
|
|
| 4 |
O |
-0.204 |
|
|
|
| 5 |
O |
-0.206 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.280 |
-0.914 |
0.000 |
1.573 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-39.568 |
1.207 |
0.000 |
| y |
1.207 |
-40.646 |
0.000 |
| z |
0.000 |
0.000 |
-38.147 |
|
| Traceless |
| | x | y | z |
| x |
-0.171 |
1.207 |
0.000 |
| y |
1.207 |
-1.789 |
0.000 |
| z |
0.000 |
0.000 |
1.960 |
|
| Polar |
| 3z2-r2 | 3.920 |
| x2-y2 | 1.079 |
| xy | 1.207 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.217 |
1.827 |
0.000 |
| y |
1.827 |
6.379 |
0.000 |
| z |
0.000 |
0.000 |
3.370 |
<r2> (average value of r
2) Å
2
| <r2> |
182.348 |
| (<r2>)1/2 |
13.504 |