Vibrational Frequencies calculated at ROHF/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 |
A1 |
2761 |
2508 |
39.62 |
|
|
|
| 2 |
A1 |
2126 |
1931 |
120.58 |
|
|
|
| 3 |
A1 |
1332 |
1210 |
60.65 |
|
|
|
| 4 |
A1 |
725 |
659 |
38.50 |
|
|
|
| 5 |
A2 |
954 |
866 |
0.00 |
|
|
|
| 6 |
B1 |
2876 |
2613 |
105.67 |
|
|
|
| 7 |
B1 |
1144 |
1040 |
3.53 |
|
|
|
| 8 |
B2 |
2043 |
1856 |
8.80 |
|
|
|
| 9 |
B2 |
850 |
772 |
0.69 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7405.6 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 6728.0 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 ROHF/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
B |
-0.133 |
|
|
|
| 2 |
H |
0.054 |
|
|
|
| 3 |
H |
0.054 |
|
|
|
| 4 |
H |
0.013 |
|
|
|
| 5 |
H |
0.013 |
|
|
|
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 |
-1.176 |
1.176 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.695 |
0.000 |
0.000 |
| y |
0.000 |
-10.005 |
0.000 |
| z |
0.000 |
0.000 |
-8.996 |
|
| Traceless |
| | x | y | z |
| x |
-1.194 |
0.000 |
0.000 |
| y |
0.000 |
-0.160 |
0.000 |
| z |
0.000 |
0.000 |
1.353 |
|
| Polar |
| 3z2-r2 | 2.707 |
| x2-y2 | -0.689 |
| 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 |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
12.084 |
| (<r2>)1/2 |
3.476 |