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 |
3895 |
3717 |
45.24 |
|
|
|
| 2 |
A |
3296 |
3145 |
21.76 |
|
|
|
| 3 |
A |
3149 |
3005 |
24.43 |
|
|
|
| 4 |
A |
1505 |
1436 |
11.00 |
|
|
|
| 5 |
A |
1374 |
1312 |
31.39 |
|
|
|
| 6 |
A |
1250 |
1192 |
96.82 |
|
|
|
| 7 |
A |
1068 |
1019 |
51.06 |
|
|
|
| 8 |
A |
641 |
612 |
67.95 |
|
|
|
| 9 |
A |
434 |
414 |
96.04 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8306.1 cm
-1
Scaled (by 0.9543) Zero Point Vibrational Energy (zpe) 7926.5 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 |
-0.103 |
|
|
|
| 2 |
O |
-0.473 |
|
|
|
| 3 |
H |
0.132 |
|
|
|
| 4 |
H |
0.109 |
|
|
|
| 5 |
H |
0.335 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.030 |
1.532 |
0.188 |
1.544 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.313 |
-2.130 |
0.698 |
| y |
-2.130 |
-10.800 |
-0.058 |
| z |
0.698 |
-0.058 |
-13.763 |
|
| Traceless |
| | x | y | z |
| x |
0.969 |
-2.130 |
0.698 |
| y |
-2.130 |
1.738 |
-0.058 |
| z |
0.698 |
-0.058 |
-2.707 |
|
| Polar |
| 3z2-r2 | -5.414 |
| x2-y2 | -0.513 |
| xy | -2.130 |
| xz | 0.698 |
| yz | -0.058 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.685 |
-0.147 |
0.058 |
| y |
-0.147 |
2.275 |
0.009 |
| z |
0.058 |
0.009 |
1.208 |
<r2> (average value of r
2) Å
2
| <r2> |
20.296 |
| (<r2>)1/2 |
4.505 |