Vibrational Frequencies calculated at LSDA/aug-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 |
A1 |
3087 |
3052 |
28.15 |
|
|
|
| 2 |
A1 |
2772 |
2741 |
10.83 |
|
|
|
| 3 |
A1 |
1492 |
1475 |
59.46 |
|
|
|
| 4 |
A1 |
1178 |
1165 |
21.89 |
|
|
|
| 5 |
B1 |
672 |
665 |
80.56 |
|
|
|
| 6 |
B1 |
606 |
599 |
8.82 |
|
|
|
| 7 |
B2 |
3162 |
3126 |
9.22 |
|
|
|
| 8 |
B2 |
864 |
854 |
27.62 |
|
|
|
| 9 |
B2 |
335 |
332 |
3.48 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7083.7 cm
-1
Scaled (by 0.9887) Zero Point Vibrational Energy (zpe) 7003.7 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-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.738 |
|
|
|
| 2 |
B |
-0.568 |
|
|
|
| 3 |
H |
-0.334 |
|
|
|
| 4 |
H |
-0.334 |
|
|
|
| 5 |
H |
0.499 |
|
|
|
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 |
-0.459 |
0.459 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.434 |
0.000 |
0.000 |
| y |
0.000 |
-11.902 |
0.000 |
| z |
0.000 |
0.000 |
-11.598 |
|
| Traceless |
| | x | y | z |
| x |
-4.683 |
0.000 |
0.000 |
| y |
0.000 |
2.114 |
0.000 |
| z |
0.000 |
0.000 |
2.570 |
|
| Polar |
| 3z2-r2 | 5.140 |
| x2-y2 | -4.531 |
| 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 |
3.801 |
0.000 |
| z |
0.000 |
0.000 |
6.107 |
<r2> (average value of r
2) Å
2
| <r2> |
21.959 |
| (<r2>)1/2 |
4.686 |