Vibrational Frequencies calculated at PBEPBEultrafine/aug-cc-pVTZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
2793 |
2762 |
80.72 |
207.09 |
0.10 |
0.19 |
| 2 |
A1 |
1759 |
1740 |
103.39 |
7.88 |
0.36 |
0.53 |
| 3 |
A1 |
1478 |
1462 |
9.36 |
8.95 |
0.42 |
0.59 |
| 4 |
B1 |
1147 |
1135 |
6.35 |
0.52 |
0.75 |
0.86 |
| 5 |
B2 |
2837 |
2805 |
138.83 |
135.14 |
0.75 |
0.86 |
| 6 |
B2 |
1217 |
1204 |
8.76 |
1.31 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 5616.1 cm
-1
Scaled (by 0.9888) Zero Point Vibrational Energy (zpe) 5553.2 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 PBEPBEultrafine/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.373 |
|
|
|
| 2 |
C |
-0.228 |
|
|
|
| 3 |
H |
0.300 |
|
|
|
| 4 |
H |
0.300 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-2.233 |
2.233 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.813 |
0.000 |
0.000 |
| y |
0.000 |
-11.795 |
0.000 |
| z |
0.000 |
0.000 |
-12.471 |
|
| Traceless |
| | x | y | z |
| x |
0.320 |
0.000 |
0.000 |
| y |
0.000 |
0.346 |
0.000 |
| z |
0.000 |
0.000 |
-0.666 |
|
| Polar |
| 3z2-r2 | -1.333 |
| x2-y2 | -0.017 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.001 |
0.000 |
0.000 |
| y |
0.000 |
2.906 |
0.000 |
| z |
0.000 |
0.000 |
3.525 |
<r2> (average value of r
2) Å
2
| <r2> |
17.206 |
| (<r2>)1/2 |
4.148 |