Vibrational Frequencies calculated at LSDA/6-31G**
Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
1 |
A1 |
2443 |
2397 |
2.26 |
|
|
|
2 |
A1 |
2196 |
2155 |
461.29 |
|
|
|
3 |
A1 |
1041 |
1022 |
11.05 |
|
|
|
4 |
A1 |
829 |
813 |
11.65 |
|
|
|
5 |
E |
2530 |
2483 |
9.63 |
|
|
|
5 |
E |
2530 |
2483 |
9.63 |
|
|
|
6 |
E |
1035 |
1015 |
1.30 |
|
|
|
6 |
E |
1035 |
1015 |
1.30 |
|
|
|
7 |
E |
759 |
745 |
11.48 |
|
|
|
7 |
E |
759 |
745 |
11.48 |
|
|
|
8 |
E |
287 |
282 |
2.11 |
|
|
|
8 |
E |
287 |
282 |
2.11 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7865.9 cm
-1
Scaled (by 0.9813) Zero Point Vibrational Energy (zpe) 7718.8 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 LSDA/6-31G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
B |
-0.352 |
|
|
|
2 |
C |
0.445 |
|
|
|
3 |
O |
-0.206 |
|
|
|
4 |
H |
0.038 |
|
|
|
5 |
H |
0.038 |
|
|
|
6 |
H |
0.038 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.000 |
0.000 |
0.997 |
0.997 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-18.176 |
0.000 |
0.000 |
y |
0.000 |
-18.176 |
0.000 |
z |
0.000 |
0.000 |
-21.657 |
|
Traceless |
| x | y | z |
x |
1.741 |
0.000 |
0.000 |
y |
0.000 |
1.741 |
0.000 |
z |
0.000 |
0.000 |
-3.481 |
|
Polar |
3z2-r2 | -6.962 |
x2-y2 | 0.000 |
xy | 0.000 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.371 |
0.000 |
0.000 |
y |
0.000 |
3.371 |
0.000 |
z |
0.000 |
0.000 |
6.218 |
<r2> (average value of r
2) Å
2
<r2> |
46.943 |
(<r2>)1/2 |
6.852 |