Vibrational Frequencies calculated at PBE1PBE/daug-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' |
3473 |
3473 |
0.88 |
|
|
|
| 2 |
A' |
3152 |
3152 |
28.35 |
|
|
|
| 3 |
A' |
3044 |
3044 |
46.77 |
|
|
|
| 4 |
A' |
1730 |
1730 |
23.74 |
|
|
|
| 5 |
A' |
1478 |
1478 |
6.55 |
|
|
|
| 6 |
A' |
1365 |
1365 |
40.11 |
|
|
|
| 7 |
A' |
1067 |
1067 |
33.21 |
|
|
|
| 8 |
A" |
1161 |
1161 |
46.56 |
|
|
|
| 9 |
A" |
1102 |
1102 |
15.70 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8785.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8785.5 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 PBE1PBE/daug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.727 |
|
|
|
| 2 |
N |
0.087 |
|
|
|
| 3 |
H |
-0.435 |
|
|
|
| 4 |
H |
-0.369 |
|
|
|
| 5 |
H |
-0.010 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.358 |
1.505 |
0.000 |
2.027 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.747 |
2.056 |
0.000 |
| y |
2.056 |
-12.840 |
0.000 |
| z |
0.000 |
0.000 |
-13.767 |
|
| Traceless |
| | x | y | z |
| x |
1.557 |
2.056 |
0.000 |
| y |
2.056 |
-0.083 |
0.000 |
| z |
0.000 |
0.000 |
-1.474 |
|
| Polar |
| 3z2-r2 | -2.948 |
| x2-y2 | 1.093 |
| xy | 2.056 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.311 |
0.110 |
0.000 |
| y |
0.110 |
4.370 |
0.000 |
| z |
0.000 |
0.000 |
2.566 |
<r2> (average value of r
2) Å
2
| <r2> |
19.719 |
| (<r2>)1/2 |
4.441 |