Vibrational Frequencies calculated at M06-2X/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 |
A' |
3423 |
3423 |
6.91 |
|
|
|
| 2 |
A' |
3227 |
3227 |
32.76 |
|
|
|
| 3 |
A' |
3103 |
3103 |
31.90 |
|
|
|
| 4 |
A' |
1744 |
1744 |
17.71 |
|
|
|
| 5 |
A' |
1538 |
1538 |
6.31 |
|
|
|
| 6 |
A' |
1368 |
1368 |
45.40 |
|
|
|
| 7 |
A' |
1082 |
1082 |
55.74 |
|
|
|
| 8 |
A" |
1191 |
1191 |
64.98 |
|
|
|
| 9 |
A" |
1139 |
1139 |
25.74 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8906.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8906.9 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/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.139 |
|
|
|
| 2 |
N |
-0.447 |
|
|
|
| 3 |
H |
0.139 |
|
|
|
| 4 |
H |
0.169 |
|
|
|
| 5 |
H |
0.279 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.716 |
1.457 |
0.000 |
2.251 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.719 |
2.372 |
0.000 |
| y |
2.372 |
-12.629 |
0.000 |
| z |
0.000 |
0.000 |
-13.447 |
|
| Traceless |
| | x | y | z |
| x |
1.319 |
2.372 |
0.000 |
| y |
2.372 |
-0.046 |
0.000 |
| z |
0.000 |
0.000 |
-1.273 |
|
| Polar |
| 3z2-r2 | -2.547 |
| x2-y2 | 0.910 |
| xy | 2.372 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.467 |
0.297 |
0.000 |
| y |
0.297 |
3.728 |
0.000 |
| z |
0.000 |
0.000 |
1.013 |
<r2> (average value of r
2) Å
2
| <r2> |
19.743 |
| (<r2>)1/2 |
4.443 |