Vibrational Frequencies calculated at HSEh1PBE/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' |
3764 |
3579 |
93.45 |
|
|
|
| 2 |
A' |
3536 |
3362 |
84.67 |
|
|
|
| 3 |
A' |
2327 |
2213 |
116.10 |
|
|
|
| 4 |
A' |
1273 |
1210 |
108.17 |
|
|
|
| 5 |
A' |
1116 |
1061 |
84.75 |
|
|
|
| 6 |
A' |
638 |
606 |
45.80 |
|
|
|
| 7 |
A' |
385 |
366 |
11.15 |
|
|
|
| 8 |
A" |
538 |
512 |
45.71 |
|
|
|
| 9 |
A" |
424 |
403 |
17.18 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6999.4 cm
-1
Scaled (by 0.951) Zero Point Vibrational Energy (zpe) 6656.4 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 HSEh1PBE/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.123 |
|
|
|
| 2 |
C |
-0.173 |
|
|
|
| 3 |
O |
-0.620 |
|
|
|
| 4 |
H |
0.218 |
|
|
|
| 5 |
H |
0.452 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.635 |
-0.823 |
0.000 |
1.831 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.796 |
-2.531 |
0.000 |
| y |
-2.531 |
-11.523 |
0.000 |
| z |
0.000 |
0.000 |
-18.181 |
|
| Traceless |
| | x | y | z |
| x |
-1.944 |
-2.531 |
0.000 |
| y |
-2.531 |
5.965 |
0.000 |
| z |
0.000 |
0.000 |
-4.021 |
|
| Polar |
| 3z2-r2 | -8.042 |
| x2-y2 | -5.272 |
| xy | -2.531 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.714 |
0.119 |
0.000 |
| y |
0.119 |
5.324 |
0.000 |
| z |
0.000 |
0.000 |
1.454 |
<r2> (average value of r
2) Å
2
| <r2> |
40.441 |
| (<r2>)1/2 |
6.359 |