Vibrational Frequencies calculated at mPW1PW91/6-31G**
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A' |
3850 |
3663 |
101.19 |
|
|
|
| 2 |
A' |
3537 |
3365 |
91.37 |
|
|
|
| 3 |
A' |
2329 |
2216 |
119.29 |
|
|
|
| 4 |
A' |
1256 |
1195 |
100.52 |
|
|
|
| 5 |
A' |
1117 |
1063 |
92.38 |
|
|
|
| 6 |
A' |
645 |
614 |
46.09 |
|
|
|
| 7 |
A' |
392 |
373 |
11.48 |
|
|
|
| 8 |
A" |
544 |
518 |
48.37 |
|
|
|
| 9 |
A" |
432 |
411 |
15.59 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7050.2 cm
-1
Scaled (by 0.9515) Zero Point Vibrational Energy (zpe) 6708.2 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 mPW1PW91/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.133 |
|
|
|
| 2 |
C |
-0.121 |
|
|
|
| 3 |
O |
-0.553 |
|
|
|
| 4 |
H |
0.183 |
|
|
|
| 5 |
H |
0.358 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.585 |
-0.872 |
0.000 |
1.809 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.875 |
-2.365 |
0.000 |
| y |
-2.365 |
-11.429 |
0.000 |
| z |
0.000 |
0.000 |
-18.106 |
|
| Traceless |
| | x | y | z |
| x |
-2.108 |
-2.365 |
0.000 |
| y |
-2.365 |
6.062 |
0.000 |
| z |
0.000 |
0.000 |
-3.954 |
|
| Polar |
| 3z2-r2 | -7.909 |
| x2-y2 | -5.446 |
| xy | -2.365 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.737 |
0.222 |
0.000 |
| y |
0.222 |
5.332 |
0.000 |
| z |
0.000 |
0.000 |
1.470 |
<r2> (average value of r
2) Å
2
| <r2> |
40.364 |
| (<r2>)1/2 |
6.353 |