Vibrational Frequencies calculated at B3LYP/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' |
3435 |
3306 |
0.89 |
|
|
|
| 2 |
A' |
3111 |
2995 |
33.45 |
|
|
|
| 3 |
A' |
3015 |
2902 |
50.52 |
|
|
|
| 4 |
A' |
1713 |
1649 |
22.78 |
|
|
|
| 5 |
A' |
1493 |
1437 |
6.88 |
|
|
|
| 6 |
A' |
1370 |
1319 |
44.74 |
|
|
|
| 7 |
A' |
1075 |
1035 |
37.62 |
|
|
|
| 8 |
A" |
1166 |
1122 |
44.99 |
|
|
|
| 9 |
A" |
1102 |
1061 |
16.03 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8739.9 cm
-1
Scaled (by 0.9626) Zero Point Vibrational Energy (zpe) 8413.0 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 B3LYP/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.104 |
|
|
|
| 2 |
N |
-0.241 |
|
|
|
| 3 |
H |
0.087 |
|
|
|
| 4 |
H |
0.112 |
|
|
|
| 5 |
H |
0.147 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.376 |
1.436 |
0.000 |
1.989 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.833 |
2.026 |
0.000 |
| y |
2.026 |
-12.818 |
0.000 |
| z |
0.000 |
0.000 |
-13.664 |
|
| Traceless |
| | x | y | z |
| x |
1.409 |
2.026 |
0.000 |
| y |
2.026 |
-0.070 |
0.000 |
| z |
0.000 |
0.000 |
-1.339 |
|
| Polar |
| 3z2-r2 | -2.678 |
| x2-y2 | 0.985 |
| xy | 2.026 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.986 |
0.181 |
0.000 |
| y |
0.181 |
4.157 |
0.000 |
| z |
0.000 |
0.000 |
2.085 |
<r2> (average value of r
2) Å
2
| <r2> |
19.623 |
| (<r2>)1/2 |
4.430 |