Vibrational Frequencies calculated at LSDA/aug-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 |
A1 |
3073 |
3044 |
29.71 |
|
|
|
| 2 |
A1 |
2765 |
2739 |
10.90 |
|
|
|
| 3 |
A1 |
1497 |
1483 |
59.96 |
|
|
|
| 4 |
A1 |
1192 |
1181 |
21.23 |
|
|
|
| 5 |
B1 |
673 |
667 |
79.57 |
|
|
|
| 6 |
B1 |
619 |
613 |
6.93 |
|
|
|
| 7 |
B2 |
3138 |
3108 |
10.38 |
|
|
|
| 8 |
B2 |
869 |
861 |
31.05 |
|
|
|
| 9 |
B2 |
333 |
330 |
4.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7079.9 cm
-1
Scaled (by 0.9906) Zero Point Vibrational Energy (zpe) 7013.3 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/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.635 |
|
|
|
| 2 |
B |
-0.125 |
|
|
|
| 3 |
H |
0.368 |
|
|
|
| 4 |
H |
0.368 |
|
|
|
| 5 |
H |
0.024 |
|
|
|
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 |
-0.430 |
0.430 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.293 |
0.000 |
0.000 |
| y |
0.000 |
-11.888 |
0.000 |
| z |
0.000 |
0.000 |
-11.503 |
|
| Traceless |
| | x | y | z |
| x |
-4.598 |
0.000 |
0.000 |
| y |
0.000 |
2.010 |
0.000 |
| z |
0.000 |
0.000 |
2.588 |
|
| Polar |
| 3z2-r2 | 5.175 |
| x2-y2 | -4.405 |
| 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 |
4.311 |
0.000 |
0.000 |
| y |
0.000 |
3.824 |
0.000 |
| z |
0.000 |
0.000 |
6.010 |
<r2> (average value of r
2) Å
2
| <r2> |
21.708 |
| (<r2>)1/2 |
4.659 |