Vibrational Frequencies calculated at wB97X-D/LANL2DZ
| 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 |
3185 |
3185 |
9.62 |
|
|
|
| 2 |
A1 |
2870 |
2870 |
25.53 |
|
|
|
| 3 |
A1 |
1521 |
1521 |
75.36 |
|
|
|
| 4 |
A1 |
1320 |
1320 |
7.87 |
|
|
|
| 5 |
B1 |
826 |
826 |
154.75 |
|
|
|
| 6 |
B1 |
698 |
698 |
3.77 |
|
|
|
| 7 |
B2 |
3273 |
3273 |
0.46 |
|
|
|
| 8 |
B2 |
930 |
930 |
64.40 |
|
|
|
| 9 |
B2 |
490 |
490 |
5.66 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7555.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 7555.9 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 wB97X-D/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.586 |
|
|
|
| 2 |
B |
0.007 |
|
|
|
| 3 |
H |
0.223 |
|
|
|
| 4 |
H |
0.223 |
|
|
|
| 5 |
H |
0.134 |
|
|
|
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 |
-0.502 |
0.502 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.248 |
0.000 |
0.000 |
| y |
0.000 |
-11.382 |
0.000 |
| z |
0.000 |
0.000 |
-10.994 |
|
| Traceless |
| | x | y | z |
| x |
-5.060 |
0.000 |
0.000 |
| y |
0.000 |
2.239 |
0.000 |
| z |
0.000 |
0.000 |
2.821 |
|
| Polar |
| 3z2-r2 | 5.641 |
| x2-y2 | -4.866 |
| 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 |
2.202 |
0.000 |
0.000 |
| y |
0.000 |
2.427 |
0.000 |
| z |
0.000 |
0.000 |
5.268 |
<r2> (average value of r
2) Å
2
| <r2> |
21.713 |
| (<r2>)1/2 |
4.660 |