Vibrational Frequencies calculated at PBEPBE/daug-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 |
A' |
3335 |
3335 |
1.99 |
|
|
|
| 2 |
A' |
3032 |
3032 |
30.31 |
|
|
|
| 3 |
A' |
2933 |
2933 |
58.67 |
|
|
|
| 4 |
A' |
1655 |
1655 |
19.96 |
|
|
|
| 5 |
A' |
1440 |
1440 |
4.55 |
|
|
|
| 6 |
A' |
1323 |
1323 |
39.64 |
|
|
|
| 7 |
A' |
1036 |
1036 |
33.97 |
|
|
|
| 8 |
A" |
1130 |
1130 |
40.94 |
|
|
|
| 9 |
A" |
1054 |
1054 |
17.55 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8468.0 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8468.0 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 PBEPBE/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.524 |
|
|
|
| 2 |
N |
-0.828 |
|
|
|
| 3 |
H |
0.548 |
|
|
|
| 4 |
H |
0.558 |
|
|
|
| 5 |
H |
0.247 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.319 |
1.419 |
0.000 |
1.937 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.921 |
2.047 |
0.000 |
| y |
2.047 |
-12.996 |
0.000 |
| z |
0.000 |
0.000 |
-13.812 |
|
| Traceless |
| | x | y | z |
| x |
1.483 |
2.047 |
0.000 |
| y |
2.047 |
-0.129 |
0.000 |
| z |
0.000 |
0.000 |
-1.354 |
|
| Polar |
| 3z2-r2 | -2.707 |
| x2-y2 | 1.075 |
| xy | 2.047 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.492 |
0.086 |
0.000 |
| y |
0.086 |
4.547 |
0.000 |
| z |
0.000 |
0.000 |
2.655 |
<r2> (average value of r
2) Å
2
| <r2> |
19.887 |
| (<r2>)1/2 |
4.460 |