Vibrational Frequencies calculated at B2PLYP=FULLultrafine/Def2TZVPP
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Σ |
3519 |
3519 |
261.30 |
31.15 |
0.22 |
0.36 |
| 2 |
Σ |
2282 |
2282 |
429.72 |
25.57 |
0.06 |
0.11 |
| 3 |
Σ |
1286 |
1286 |
97.39 |
28.92 |
0.25 |
0.40 |
| 4 |
Π |
560 |
560 |
2.81 |
0.14 |
0.75 |
0.86 |
| 4 |
Π |
560 |
560 |
2.81 |
0.14 |
0.75 |
0.86 |
| 5 |
Π |
11i |
11i |
78.54 |
5.75 |
0.75 |
0.86 |
| 5 |
Π |
11i |
11i |
78.54 |
5.75 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4092.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4092.1 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 B2PLYP=FULLultrafine/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.317 |
|
|
|
| 2 |
N |
0.347 |
|
|
|
| 3 |
C |
-0.265 |
|
|
|
| 4 |
H |
0.235 |
|
|
|
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 |
-3.084 |
3.084 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.892 |
0.000 |
0.000 |
| y |
0.000 |
-16.892 |
0.000 |
| z |
0.000 |
0.000 |
-14.095 |
|
| Traceless |
| | x | y | z |
| x |
-1.399 |
0.000 |
0.000 |
| y |
0.000 |
-1.399 |
0.000 |
| z |
0.000 |
0.000 |
2.797 |
|
| Polar |
| 3z2-r2 | 5.595 |
| x2-y2 | 0.000 |
| 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 |
1.966 |
0.000 |
0.000 |
| y |
0.000 |
1.966 |
0.000 |
| z |
0.000 |
0.000 |
6.240 |
<r2> (average value of r
2) Å
2
| <r2> |
34.517 |
| (<r2>)1/2 |
5.875 |