Vibrational Frequencies calculated at PBEPBE/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 |
A' |
3338 |
3298 |
2.66 |
|
|
|
| 2 |
A' |
3035 |
2998 |
34.56 |
|
|
|
| 3 |
A' |
2934 |
2899 |
57.22 |
|
|
|
| 4 |
A' |
1660 |
1640 |
19.60 |
|
|
|
| 5 |
A' |
1444 |
1426 |
4.00 |
|
|
|
| 6 |
A' |
1327 |
1310 |
42.36 |
|
|
|
| 7 |
A' |
1038 |
1026 |
36.07 |
|
|
|
| 8 |
A" |
1134 |
1120 |
42.43 |
|
|
|
| 9 |
A" |
1056 |
1043 |
16.60 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8483.1 cm
-1
Scaled (by 0.9879) Zero Point Vibrational Energy (zpe) 8380.4 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/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.096 |
|
|
|
| 2 |
N |
-0.242 |
|
|
|
| 3 |
H |
0.077 |
|
|
|
| 4 |
H |
0.102 |
|
|
|
| 5 |
H |
0.159 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.332 |
1.361 |
0.000 |
1.905 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.831 |
1.987 |
0.000 |
| y |
1.987 |
-12.877 |
0.000 |
| z |
0.000 |
0.000 |
-13.672 |
|
| Traceless |
| | x | y | z |
| x |
1.443 |
1.987 |
0.000 |
| y |
1.987 |
-0.126 |
0.000 |
| z |
0.000 |
0.000 |
-1.317 |
|
| Polar |
| 3z2-r2 | -2.635 |
| x2-y2 | 1.046 |
| xy | 1.987 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.122 |
0.175 |
0.000 |
| y |
0.175 |
4.256 |
0.000 |
| z |
0.000 |
0.000 |
2.114 |
<r2> (average value of r
2) Å
2
| <r2> |
19.811 |
| (<r2>)1/2 |
4.451 |