Vibrational Frequencies calculated at B3LYP/TZVP
| 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 |
3137 |
3029 |
12.07 |
|
|
|
| 2 |
A1 |
2841 |
2742 |
18.27 |
|
|
|
| 3 |
A1 |
1515 |
1462 |
57.75 |
|
|
|
| 4 |
A1 |
1279 |
1235 |
7.83 |
|
|
|
| 5 |
B1 |
740 |
715 |
98.95 |
|
|
|
| 6 |
B1 |
647 |
624 |
1.87 |
|
|
|
| 7 |
B2 |
3198 |
3087 |
1.62 |
|
|
|
| 8 |
B2 |
922 |
890 |
52.18 |
|
|
|
| 9 |
B2 |
427 |
412 |
2.70 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7352.7 cm
-1
Scaled (by 0.9654) Zero Point Vibrational Energy (zpe) 7098.3 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 B3LYP/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.477 |
|
|
|
| 2 |
B |
0.217 |
|
|
|
| 3 |
H |
0.139 |
|
|
|
| 4 |
H |
0.139 |
|
|
|
| 5 |
H |
-0.018 |
|
|
|
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 |
-0.573 |
0.573 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.369 |
0.000 |
0.000 |
| y |
0.000 |
-11.722 |
0.000 |
| z |
0.000 |
0.000 |
-11.705 |
|
| Traceless |
| | x | y | z |
| x |
-4.656 |
0.000 |
0.000 |
| y |
0.000 |
2.315 |
0.000 |
| z |
0.000 |
0.000 |
2.341 |
|
| Polar |
| 3z2-r2 | 4.681 |
| x2-y2 | -4.647 |
| 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 |
3.378 |
0.000 |
0.000 |
| y |
0.000 |
2.816 |
0.000 |
| z |
0.000 |
0.000 |
5.723 |
<r2> (average value of r
2) Å
2
| <r2> |
21.722 |
| (<r2>)1/2 |
4.661 |