Vibrational Frequencies calculated at PBEPBEultrafine/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 |
3082 |
3063 |
15.66 |
|
|
|
| 2 |
A1 |
2771 |
2754 |
17.04 |
|
|
|
| 3 |
A1 |
1468 |
1459 |
53.00 |
|
|
|
| 4 |
A1 |
1211 |
1203 |
12.68 |
|
|
|
| 5 |
B1 |
690 |
686 |
77.31 |
|
|
|
| 6 |
B1 |
592 |
588 |
4.09 |
|
|
|
| 7 |
B2 |
3155 |
3136 |
2.75 |
|
|
|
| 8 |
B2 |
879 |
874 |
28.67 |
|
|
|
| 9 |
B2 |
378 |
376 |
1.62 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7112.9 cm
-1
Scaled (by 0.9939) Zero Point Vibrational Energy (zpe) 7069.5 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 PBEPBEultrafine/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.641 |
|
|
|
| 2 |
B |
-0.510 |
|
|
|
| 3 |
H |
-0.344 |
|
|
|
| 4 |
H |
-0.344 |
|
|
|
| 5 |
H |
0.557 |
|
|
|
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 |
-0.496 |
0.496 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.426 |
0.000 |
0.000 |
| y |
0.000 |
-11.901 |
0.000 |
| z |
0.000 |
0.000 |
-11.751 |
|
| Traceless |
| | x | y | z |
| x |
-4.601 |
0.000 |
0.000 |
| y |
0.000 |
2.188 |
0.000 |
| z |
0.000 |
0.000 |
2.413 |
|
| Polar |
| 3z2-r2 | 4.826 |
| x2-y2 | -4.526 |
| 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 |
4.394 |
0.000 |
0.000 |
| y |
0.000 |
3.771 |
0.000 |
| z |
0.000 |
0.000 |
6.151 |
<r2> (average value of r
2) Å
2
| <r2> |
22.093 |
| (<r2>)1/2 |
4.700 |