Vibrational Frequencies calculated at B97D3/3-21G*
| 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' |
3168 |
3168 |
30.32 |
|
|
|
| 2 |
A' |
3063 |
3063 |
41.61 |
|
|
|
| 3 |
A' |
2933 |
2933 |
68.08 |
|
|
|
| 4 |
A' |
1647 |
1647 |
6.16 |
|
|
|
| 5 |
A' |
1495 |
1495 |
0.61 |
|
|
|
| 6 |
A' |
1341 |
1341 |
63.86 |
|
|
|
| 7 |
A' |
1078 |
1078 |
46.49 |
|
|
|
| 8 |
A" |
1159 |
1159 |
52.08 |
|
|
|
| 9 |
A" |
1074 |
1074 |
21.87 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8478.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8478.2 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 B97D3/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.154 |
|
|
|
| 2 |
N |
-0.482 |
|
|
|
| 3 |
H |
0.170 |
|
|
|
| 4 |
H |
0.207 |
|
|
|
| 5 |
H |
0.259 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.475 |
1.228 |
0.000 |
1.919 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.521 |
2.110 |
0.000 |
| y |
2.110 |
-12.497 |
0.000 |
| z |
0.000 |
0.000 |
-13.287 |
|
| Traceless |
| | x | y | z |
| x |
1.371 |
2.110 |
0.000 |
| y |
2.110 |
-0.093 |
0.000 |
| z |
0.000 |
0.000 |
-1.278 |
|
| Polar |
| 3z2-r2 | -2.557 |
| x2-y2 | 0.976 |
| xy | 2.110 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.426 |
0.320 |
0.000 |
| y |
0.320 |
3.512 |
0.000 |
| z |
0.000 |
0.000 |
0.908 |
<r2> (average value of r
2) Å
2
| <r2> |
19.833 |
| (<r2>)1/2 |
4.453 |