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 |
3728 |
3567 |
23.86 |
|
|
|
| 2 |
A |
3358 |
3212 |
18.52 |
|
|
|
| 3 |
A |
3189 |
3051 |
16.43 |
|
|
|
| 4 |
A |
1507 |
1442 |
4.40 |
|
|
|
| 5 |
A |
1362 |
1303 |
27.32 |
|
|
|
| 6 |
A |
1182 |
1131 |
89.69 |
|
|
|
| 7 |
A |
1052 |
1006 |
73.74 |
|
|
|
| 8 |
A |
538 |
514 |
185.55 |
|
|
|
| 9 |
A |
388 |
371 |
54.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8152.5 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 7798.6 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 |
-0.124 |
|
|
|
| 2 |
O |
-0.581 |
|
|
|
| 3 |
H |
0.170 |
|
|
|
| 4 |
H |
0.144 |
|
|
|
| 5 |
H |
0.392 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.175 |
1.839 |
0.115 |
1.851 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.178 |
-2.472 |
0.696 |
| y |
-2.472 |
-10.964 |
-0.037 |
| z |
0.696 |
-0.037 |
-13.964 |
|
| Traceless |
| | x | y | z |
| x |
1.286 |
-2.472 |
0.696 |
| y |
-2.472 |
1.607 |
-0.037 |
| z |
0.696 |
-0.037 |
-2.893 |
|
| Polar |
| 3z2-r2 | -5.786 |
| x2-y2 | -0.214 |
| xy | -2.472 |
| xz | 0.696 |
| yz | -0.037 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.699 |
-0.156 |
0.035 |
| y |
-0.156 |
2.116 |
-0.011 |
| z |
0.035 |
-0.011 |
0.955 |
<r2> (average value of r
2) Å
2
| <r2> |
20.766 |
| (<r2>)1/2 |
4.557 |