Vibrational Frequencies calculated at HSEh1PBE/aug-cc-pVDZ
| 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' |
3316 |
3191 |
0.71 |
|
|
|
| 2 |
A' |
3149 |
3030 |
3.92 |
|
|
|
| 3 |
A' |
1554 |
1495 |
41.20 |
|
|
|
| 4 |
A' |
1399 |
1346 |
13.20 |
|
|
|
| 5 |
A' |
1241 |
1194 |
26.24 |
|
|
|
| 6 |
A' |
980 |
943 |
114.79 |
|
|
|
| 7 |
A' |
542 |
521 |
0.08 |
|
|
|
| 8 |
A" |
943 |
907 |
33.94 |
|
|
|
| 9 |
A" |
685 |
660 |
5.14 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6904.8 cm
-1
Scaled (by 0.9622) Zero Point Vibrational Energy (zpe) 6643.8 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/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
0.017 |
|
|
|
| 2 |
C |
0.788 |
|
|
|
| 3 |
H |
-0.136 |
|
|
|
| 4 |
H |
-0.196 |
|
|
|
| 5 |
O |
-0.473 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
4.209 |
-0.397 |
0.000 |
4.227 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.820 |
-0.510 |
0.000 |
| y |
-0.510 |
-16.628 |
0.000 |
| z |
0.000 |
0.000 |
-17.579 |
|
| Traceless |
| | x | y | z |
| x |
0.283 |
-0.510 |
0.000 |
| y |
-0.510 |
0.571 |
0.000 |
| z |
0.000 |
0.000 |
-0.854 |
|
| Polar |
| 3z2-r2 | -1.709 |
| x2-y2 | -0.192 |
| xy | -0.510 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.686 |
-0.080 |
0.000 |
| y |
-0.080 |
3.123 |
0.000 |
| z |
0.000 |
0.000 |
2.445 |
<r2> (average value of r
2) Å
2
| <r2> |
37.219 |
| (<r2>)1/2 |
6.101 |