Vibrational Frequencies calculated at wB97X-D/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' |
3459 |
3295 |
1.03 |
|
|
|
| 2 |
A' |
3146 |
2996 |
36.10 |
|
|
|
| 3 |
A' |
3037 |
2893 |
41.94 |
|
|
|
| 4 |
A' |
1747 |
1665 |
24.80 |
|
|
|
| 5 |
A' |
1485 |
1414 |
4.65 |
|
|
|
| 6 |
A' |
1378 |
1313 |
43.95 |
|
|
|
| 7 |
A' |
1080 |
1029 |
31.45 |
|
|
|
| 8 |
A" |
1175 |
1119 |
43.86 |
|
|
|
| 9 |
A" |
1095 |
1043 |
15.37 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8800.9 cm
-1
Scaled (by 0.9526) Zero Point Vibrational Energy (zpe) 8383.7 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/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.009 |
|
|
|
| 2 |
N |
-0.187 |
|
|
|
| 3 |
H |
0.037 |
|
|
|
| 4 |
H |
0.057 |
|
|
|
| 5 |
H |
0.102 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.342 |
1.326 |
0.000 |
1.887 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.427 |
1.884 |
0.000 |
| y |
1.884 |
-12.435 |
0.000 |
| z |
0.000 |
0.000 |
-13.205 |
|
| Traceless |
| | x | y | z |
| x |
1.392 |
1.884 |
0.000 |
| y |
1.884 |
-0.119 |
0.000 |
| z |
0.000 |
0.000 |
-1.274 |
|
| Polar |
| 3z2-r2 | -2.547 |
| x2-y2 | 1.007 |
| xy | 1.884 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.597 |
0.265 |
0.000 |
| y |
0.265 |
3.684 |
0.000 |
| z |
0.000 |
0.000 |
1.360 |
<r2> (average value of r
2) Å
2
| <r2> |
19.472 |
| (<r2>)1/2 |
4.413 |