Vibrational Frequencies calculated at mPW1PW91/6-31+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 |
A' |
3294 |
3135 |
0.92 |
|
|
|
| 2 |
A' |
3209 |
3055 |
2.82 |
|
|
|
| 3 |
A' |
3105 |
2956 |
4.02 |
|
|
|
| 4 |
A' |
1673 |
1592 |
2.49 |
|
|
|
| 5 |
A' |
1399 |
1332 |
7.50 |
|
|
|
| 6 |
A' |
1060 |
1009 |
7.30 |
|
|
|
| 7 |
A' |
723 |
688 |
23.22 |
|
|
|
| 8 |
A" |
932 |
887 |
96.17 |
|
|
|
| 9 |
A" |
835 |
794 |
17.35 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8114.4 cm
-1
Scaled (by 0.9518) Zero Point Vibrational Energy (zpe) 7723.3 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 mPW1PW91/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.178 |
|
|
|
| 2 |
C |
-0.344 |
|
|
|
| 3 |
H |
0.173 |
|
|
|
| 4 |
H |
0.171 |
|
|
|
| 5 |
H |
0.178 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.694 |
-0.324 |
0.000 |
0.766 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.335 |
-1.288 |
0.000 |
| y |
-1.288 |
-11.298 |
0.000 |
| z |
0.000 |
0.000 |
-15.030 |
|
| Traceless |
| | x | y | z |
| x |
0.829 |
-1.288 |
0.000 |
| y |
-1.288 |
2.384 |
0.000 |
| z |
0.000 |
0.000 |
-3.213 |
|
| Polar |
| 3z2-r2 | -6.426 |
| x2-y2 | -1.037 |
| xy | -1.288 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.741 |
-0.081 |
-0.001 |
| y |
-0.081 |
5.020 |
0.001 |
| z |
-0.001 |
0.001 |
2.400 |
<r2> (average value of r
2) Å
2
| <r2> |
20.491 |
| (<r2>)1/2 |
4.527 |