Vibrational Frequencies calculated at LSDA/6-31+G**
| 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 |
2255 |
2221 |
0.00 |
|
|
|
| 2 |
Σg |
778 |
766 |
0.00 |
|
|
|
| 3 |
Σu |
2431 |
2395 |
2319.64 |
|
|
|
| 4 |
Σu |
1628 |
1604 |
99.64 |
|
|
|
| 5 |
Πg |
575 |
566 |
0.00 |
|
|
|
| 5 |
Πg |
575 |
566 |
0.00 |
|
|
|
| 6 |
Πu |
736 |
725 |
44.34 |
|
|
|
| 6 |
Πu |
736 |
725 |
44.34 |
|
|
|
| 7 |
Πu |
177 |
174 |
1.53 |
|
|
|
| 7 |
Πu |
177 |
174 |
1.53 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5032.6 cm
-1
Scaled (by 0.985) Zero Point Vibrational Energy (zpe) 4957.1 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 LSDA/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
1.621 |
|
|
|
| 2 |
C |
-0.323 |
|
|
|
| 3 |
C |
-0.323 |
|
|
|
| 4 |
O |
-0.488 |
|
|
|
| 5 |
O |
-0.488 |
|
|
|
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 |
-26.023 |
0.000 |
0.000 |
| y |
0.000 |
-26.023 |
0.000 |
| z |
0.000 |
0.000 |
-33.854 |
|
| Traceless |
| | x | y | z |
| x |
3.915 |
0.000 |
0.000 |
| y |
0.000 |
3.915 |
0.000 |
| z |
0.000 |
0.000 |
-7.831 |
|
| Polar |
| 3z2-r2 | -15.662 |
| 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 |
2.580 |
0.000 |
0.000 |
| y |
0.000 |
2.580 |
0.000 |
| z |
0.000 |
0.000 |
12.814 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |