Vibrational Frequencies calculated at M06-2X/6-311G*
| 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' |
3475 |
3475 |
1.19 |
|
|
|
| 2 |
A' |
3168 |
3168 |
36.28 |
|
|
|
| 3 |
A' |
3068 |
3068 |
41.51 |
|
|
|
| 4 |
A' |
1761 |
1761 |
26.11 |
|
|
|
| 5 |
A' |
1519 |
1519 |
6.76 |
|
|
|
| 6 |
A' |
1399 |
1399 |
39.00 |
|
|
|
| 7 |
A' |
1095 |
1095 |
35.87 |
|
|
|
| 8 |
A" |
1191 |
1191 |
55.22 |
|
|
|
| 9 |
A" |
1112 |
1112 |
17.37 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8893.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8893.7 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 M06-2X/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.247 |
|
|
|
| 2 |
N |
-0.454 |
|
|
|
| 3 |
H |
0.194 |
|
|
|
| 4 |
H |
0.219 |
|
|
|
| 5 |
H |
0.288 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.487 |
1.452 |
0.000 |
2.078 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.527 |
2.056 |
0.000 |
| y |
2.056 |
-12.677 |
0.000 |
| z |
0.000 |
0.000 |
-13.612 |
|
| Traceless |
| | x | y | z |
| x |
1.617 |
2.056 |
0.000 |
| y |
2.056 |
-0.107 |
0.000 |
| z |
0.000 |
0.000 |
-1.510 |
|
| Polar |
| 3z2-r2 | -3.020 |
| x2-y2 | 1.150 |
| xy | 2.056 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.576 |
0.236 |
0.000 |
| y |
0.236 |
3.732 |
0.000 |
| z |
0.000 |
0.000 |
1.427 |
<r2> (average value of r
2) Å
2
| <r2> |
19.497 |
| (<r2>)1/2 |
4.415 |