Vibrational Frequencies calculated at B1B95/CEP-31G*
| 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 |
2311 |
2212 |
0.00 |
|
|
|
| 2 |
Σg |
773 |
740 |
0.00 |
|
|
|
| 3 |
Σu |
2467 |
2362 |
3068.29 |
|
|
|
| 4 |
Σu |
1645 |
1575 |
121.25 |
|
|
|
| 5 |
Πg |
548 |
525 |
0.00 |
|
|
|
| 5 |
Πg |
548 |
525 |
0.00 |
|
|
|
| 6 |
Πu |
576 |
551 |
76.07 |
|
|
|
| 6 |
Πu |
576 |
551 |
76.07 |
|
|
|
| 7 |
Πu |
189 |
181 |
0.26 |
|
|
|
| 7 |
Πu |
189 |
181 |
0.26 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4911.0 cm
-1
Scaled (by 0.9572) Zero Point Vibrational Energy (zpe) 4700.9 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 B1B95/CEP-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
2.032 |
|
|
|
| 2 |
C |
-1.111 |
|
|
|
| 3 |
C |
-1.111 |
|
|
|
| 4 |
O |
0.095 |
|
|
|
| 5 |
O |
0.095 |
|
|
|
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 |
-25.539 |
0.000 |
0.000 |
| y |
0.000 |
-25.539 |
0.000 |
| z |
0.000 |
0.000 |
-32.958 |
|
| Traceless |
| | x | y | z |
| x |
3.710 |
0.000 |
0.000 |
| y |
0.000 |
3.710 |
0.000 |
| z |
0.000 |
0.000 |
-7.419 |
|
| Polar |
| 3z2-r2 | -14.838 |
| 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 |
2.144 |
0.000 |
0.000 |
| y |
0.000 |
2.144 |
0.000 |
| z |
0.000 |
0.000 |
12.330 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |