Vibrational Frequencies calculated at B97D3/daug-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 |
3506 |
3506 |
15.33 |
|
|
|
| 2 |
A |
1242 |
1242 |
0.03 |
|
|
|
| 3 |
A |
936 |
936 |
8.25 |
|
|
|
| 4 |
A |
707 |
707 |
79.77 |
|
|
|
| 5 |
A |
517 |
517 |
0.23 |
|
|
|
| 6 |
B |
3506 |
3506 |
89.28 |
|
|
|
| 7 |
B |
2165 |
2165 |
564.13 |
|
|
|
| 8 |
B |
933 |
933 |
381.61 |
|
|
|
| 9 |
B |
520 |
520 |
57.42 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7015.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 7015.5 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 B97D3/daug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.113 |
|
|
|
| 2 |
N |
-0.004 |
|
|
|
| 3 |
N |
-0.004 |
|
|
|
| 4 |
H |
-0.053 |
|
|
|
| 5 |
H |
-0.053 |
|
|
|
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 |
1.906 |
1.906 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.098 |
4.006 |
0.000 |
| y |
4.006 |
-16.569 |
0.000 |
| z |
0.000 |
0.000 |
-17.598 |
|
| Traceless |
| | x | y | z |
| x |
-0.015 |
4.006 |
0.000 |
| y |
4.006 |
0.779 |
0.000 |
| z |
0.000 |
0.000 |
-0.764 |
|
| Polar |
| 3z2-r2 | -1.528 |
| x2-y2 | -0.529 |
| xy | 4.006 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.319 |
0.274 |
0.000 |
| y |
0.274 |
7.135 |
0.000 |
| z |
0.000 |
0.000 |
3.297 |
<r2> (average value of r
2) Å
2
| <r2> |
39.540 |
| (<r2>)1/2 |
6.288 |