Vibrational Frequencies calculated at B3LYPultrafine/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' |
1810 |
1755 |
285.93 |
|
|
|
| 2 |
A' |
1352 |
1311 |
294.42 |
|
|
|
| 3 |
A' |
821 |
796 |
209.59 |
|
|
|
| 4 |
A' |
744 |
721 |
0.27 |
|
|
|
| 5 |
A' |
556 |
539 |
75.10 |
|
|
|
| 6 |
A' |
395 |
383 |
1.34 |
|
|
|
| 7 |
A' |
206 |
200 |
0.02 |
|
|
|
| 8 |
A" |
733 |
711 |
14.92 |
|
|
|
| 9 |
A" |
121 |
118 |
0.51 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3368.1 cm
-1
Scaled (by 0.97) Zero Point Vibrational Energy (zpe) 3267.0 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 B3LYPultrafine/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Br |
0.220 |
|
|
|
| 2 |
O |
-0.297 |
|
|
|
| 3 |
N |
0.412 |
|
|
|
| 4 |
O |
-0.164 |
|
|
|
| 5 |
O |
-0.171 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.215 |
-1.030 |
0.000 |
1.593 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-39.017 |
1.429 |
0.000 |
| y |
1.429 |
-40.434 |
0.000 |
| z |
0.000 |
0.000 |
-37.916 |
|
| Traceless |
| | x | y | z |
| x |
0.158 |
1.429 |
0.000 |
| y |
1.429 |
-1.968 |
0.000 |
| z |
0.000 |
0.000 |
1.809 |
|
| Polar |
| 3z2-r2 | 3.619 |
| x2-y2 | 1.417 |
| xy | 1.429 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.437 |
2.021 |
0.000 |
| y |
2.021 |
5.767 |
0.000 |
| z |
0.000 |
0.000 |
2.320 |
<r2> (average value of r
2) Å
2
| <r2> |
187.154 |
| (<r2>)1/2 |
13.680 |