Vibrational Frequencies calculated at B3LYP/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 |
3065 |
2943 |
0.00 |
|
|
|
2 |
A1 |
2041 |
1960 |
167.50 |
|
|
|
3 |
A1 |
1374 |
1319 |
18.91 |
|
|
|
4 |
A1 |
818 |
785 |
0.07 |
|
|
|
5 |
E |
3139 |
3014 |
1.66 |
|
|
|
5 |
E |
3139 |
3014 |
1.66 |
|
|
|
6 |
E |
1491 |
1432 |
6.74 |
|
|
|
6 |
E |
1491 |
1432 |
6.74 |
|
|
|
7 |
E |
929 |
892 |
27.01 |
|
|
|
7 |
E |
929 |
892 |
27.00 |
|
|
|
8 |
E |
356 |
341 |
9.36 |
|
|
|
8 |
E |
356 |
341 |
9.36 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 9562.5 cm
-1
Scaled (by 0.9603) Zero Point Vibrational Energy (zpe) 9182.9 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 B3LYP/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.627 |
|
|
|
2 |
B |
0.348 |
|
|
|
3 |
O |
-0.312 |
|
|
|
4 |
H |
0.197 |
|
|
|
5 |
H |
0.197 |
|
|
|
6 |
H |
0.197 |
|
|
|
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 |
-3.392 |
3.392 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-16.674 |
0.000 |
0.000 |
y |
0.000 |
-16.674 |
0.000 |
z |
0.000 |
0.000 |
-20.588 |
|
Traceless |
| x | y | z |
x |
1.957 |
0.000 |
0.000 |
y |
0.000 |
1.957 |
0.000 |
z |
0.000 |
0.000 |
-3.914 |
|
Polar |
3z2-r2 | -7.828 |
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 |
2.724 |
0.000 |
0.000 |
y |
0.000 |
2.724 |
0.000 |
z |
0.000 |
0.000 |
4.385 |
<r2> (average value of r
2) Å
2
<r2> |
50.118 |
(<r2>)1/2 |
7.079 |