Vibrational Frequencies calculated at M06-2X/6-31G(2df,p)
| 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 |
2718 |
2589 |
35.73 |
|
|
|
| 2 |
A1 |
2165 |
2062 |
95.95 |
|
|
|
| 3 |
A1 |
1372 |
1307 |
49.33 |
|
|
|
| 4 |
A1 |
1017 |
968 |
0.66 |
|
|
|
| 5 |
A2 |
738 |
702 |
0.00 |
|
|
|
| 6 |
B1 |
2843 |
2708 |
67.50 |
|
|
|
| 7 |
B1 |
1055 |
1005 |
0.33 |
|
|
|
| 8 |
B2 |
2026 |
1930 |
5.63 |
|
|
|
| 9 |
B2 |
700 |
667 |
0.81 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7316.9 cm
-1
Scaled (by 0.9524) Zero Point Vibrational Energy (zpe) 6968.6 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 M06-2X/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
B |
-0.288 |
|
|
|
| 2 |
H |
0.121 |
|
|
|
| 3 |
H |
0.121 |
|
|
|
| 4 |
H |
0.023 |
|
|
|
| 5 |
H |
0.023 |
|
|
|
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 |
-1.306 |
1.306 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-9.996 |
0.000 |
0.000 |
| y |
0.000 |
-9.487 |
0.000 |
| z |
0.000 |
0.000 |
-8.159 |
|
| Traceless |
| | x | y | z |
| x |
-1.173 |
0.000 |
0.000 |
| y |
0.000 |
-0.410 |
0.000 |
| z |
0.000 |
0.000 |
1.583 |
|
| Polar |
| 3z2-r2 | 3.166 |
| x2-y2 | -0.509 |
| 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 |
2.403 |
0.000 |
0.000 |
| y |
0.000 |
2.167 |
0.000 |
| z |
0.000 |
0.000 |
3.194 |
<r2> (average value of r
2) Å
2
| <r2> |
11.650 |
| (<r2>)1/2 |
3.413 |