Vibrational Frequencies calculated at wB97X-D/6-31G*
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3247 |
3080 |
13.25 |
|
|
|
| 2 |
A1 |
2258 |
2142 |
398.15 |
|
|
|
| 3 |
A1 |
1486 |
1410 |
32.56 |
|
|
|
| 4 |
A1 |
1251 |
1187 |
1.17 |
|
|
|
| 5 |
B1 |
595 |
565 |
1.57 |
|
|
|
| 6 |
B1 |
470 |
446 |
159.74 |
|
|
|
| 7 |
B2 |
3371 |
3197 |
1.09 |
|
|
|
| 8 |
B2 |
1148 |
1089 |
1.54 |
|
|
|
| 9 |
B2 |
431 |
409 |
0.48 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7128.5 cm
-1
Scaled (by 0.9485) Zero Point Vibrational Energy (zpe) 6761.4 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 wB97X-D/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.402 |
|
|
|
| 2 |
N |
0.197 |
|
|
|
| 3 |
N |
-0.223 |
|
|
|
| 4 |
H |
0.214 |
|
|
|
| 5 |
H |
0.214 |
|
|
|
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 |
-1.718 |
1.718 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-18.725 |
0.000 |
0.000 |
| y |
0.000 |
-15.167 |
0.000 |
| z |
0.000 |
0.000 |
-18.353 |
|
| Traceless |
| | x | y | z |
| x |
-1.965 |
0.000 |
0.000 |
| y |
0.000 |
3.372 |
0.000 |
| z |
0.000 |
0.000 |
-1.407 |
|
| Polar |
| 3z2-r2 | -2.814 |
| x2-y2 | -3.558 |
| 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 |
1.535 |
0.000 |
0.000 |
| y |
0.000 |
2.236 |
0.000 |
| z |
0.000 |
0.000 |
6.474 |
<r2> (average value of r
2) Å
2
| <r2> |
37.720 |
| (<r2>)1/2 |
6.142 |