Vibrational Frequencies calculated at M06-2X/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' |
3305 |
3169 |
6.21 |
|
|
|
| 2 |
A' |
3184 |
3053 |
28.40 |
|
|
|
| 3 |
A' |
3063 |
2937 |
29.81 |
|
|
|
| 4 |
A' |
1725 |
1654 |
9.29 |
|
|
|
| 5 |
A' |
1544 |
1481 |
3.29 |
|
|
|
| 6 |
A' |
1376 |
1319 |
56.36 |
|
|
|
| 7 |
A' |
1097 |
1052 |
53.99 |
|
|
|
| 8 |
A" |
1195 |
1145 |
57.97 |
|
|
|
| 9 |
A" |
1136 |
1089 |
23.76 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8812.6 cm
-1
Scaled (by 0.9587) Zero Point Vibrational Energy (zpe) 8448.7 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/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.152 |
|
|
|
| 2 |
N |
-0.503 |
|
|
|
| 3 |
H |
0.176 |
|
|
|
| 4 |
H |
0.210 |
|
|
|
| 5 |
H |
0.270 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.594 |
1.328 |
0.000 |
2.075 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.584 |
2.199 |
0.000 |
| y |
2.199 |
-12.497 |
0.000 |
| z |
0.000 |
0.000 |
-13.392 |
|
| Traceless |
| | x | y | z |
| x |
1.361 |
2.199 |
0.000 |
| y |
2.199 |
-0.009 |
0.000 |
| z |
0.000 |
0.000 |
-1.351 |
|
| Polar |
| 3z2-r2 | -2.703 |
| x2-y2 | 0.913 |
| xy | 2.199 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.289 |
0.346 |
0.000 |
| y |
0.346 |
3.391 |
0.000 |
| z |
0.000 |
0.000 |
0.873 |
<r2> (average value of r
2) Å
2
| <r2> |
19.682 |
| (<r2>)1/2 |
4.436 |