Vibrational Frequencies calculated at PBEPBEultrafine/3-21G
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A' |
3179 |
3150 |
2.40 |
|
|
|
| 2 |
A' |
3078 |
3050 |
5.46 |
|
|
|
| 3 |
A' |
2982 |
2955 |
3.75 |
|
|
|
| 4 |
A' |
1621 |
1606 |
2.17 |
|
|
|
| 5 |
A' |
1410 |
1398 |
9.42 |
|
|
|
| 6 |
A' |
1061 |
1052 |
10.00 |
|
|
|
| 7 |
A' |
722 |
715 |
27.32 |
|
|
|
| 8 |
A" |
906 |
898 |
94.84 |
|
|
|
| 9 |
A" |
810 |
803 |
11.55 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7884.5 cm
-1
Scaled (by 0.9909) Zero Point Vibrational Energy (zpe) 7812.8 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/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.166 |
|
|
|
| 2 |
C |
-0.483 |
|
|
|
| 3 |
H |
0.210 |
|
|
|
| 4 |
H |
0.215 |
|
|
|
| 5 |
H |
0.223 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.632 |
-0.305 |
0.000 |
0.701 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.071 |
-1.156 |
0.000 |
| y |
-1.156 |
-10.998 |
0.000 |
| z |
0.000 |
0.000 |
-14.525 |
|
| Traceless |
| | x | y | z |
| x |
0.691 |
-1.156 |
0.000 |
| y |
-1.156 |
2.300 |
0.000 |
| z |
0.000 |
0.000 |
-2.990 |
|
| Polar |
| 3z2-r2 | -5.981 |
| x2-y2 | -1.073 |
| xy | -1.156 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.303 |
-0.244 |
0.000 |
| y |
-0.244 |
4.273 |
0.000 |
| z |
0.000 |
0.000 |
0.993 |
<r2> (average value of r
2) Å
2
| <r2> |
20.439 |
| (<r2>)1/2 |
4.521 |