Vibrational Frequencies calculated at B2PLYP/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 |
Σg |
3540 |
3391 |
0.00 |
68.46 |
0.24 |
0.38 |
| 2 |
Σg |
2028 |
1942 |
0.00 |
49.59 |
0.24 |
0.39 |
| 3 |
Σu |
3447 |
3301 |
97.37 |
0.00 |
0.00 |
0.00 |
| 4 |
Πg |
601 |
576 |
0.00 |
1.33 |
0.75 |
0.86 |
| 4 |
Πg |
601 |
576 |
0.00 |
1.33 |
0.75 |
0.86 |
| 5 |
Πu |
765 |
733 |
77.25 |
0.00 |
0.00 |
0.00 |
| 5 |
Πu |
765 |
733 |
77.25 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 5874.4 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 5625.9 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 B2PLYP/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.020 |
|
|
|
| 2 |
C |
-0.020 |
|
|
|
| 3 |
H |
0.020 |
|
|
|
| 4 |
H |
0.020 |
|
|
|
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 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.374 |
0.000 |
0.000 |
| y |
0.000 |
-13.374 |
0.000 |
| z |
0.000 |
0.000 |
-6.992 |
|
| Traceless |
| | x | y | z |
| x |
-3.191 |
0.000 |
0.000 |
| y |
0.000 |
-3.191 |
0.000 |
| z |
0.000 |
0.000 |
6.382 |
|
| Polar |
| 3z2-r2 | 12.763 |
| x2-y2 | 0.000 |
| 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 |
1.401 |
0.000 |
0.000 |
| y |
0.000 |
1.401 |
0.000 |
| z |
0.000 |
0.000 |
4.301 |
<r2> (average value of r
2) Å
2
| <r2> |
17.118 |
| (<r2>)1/2 |
4.137 |