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' |
3445 |
3262 |
1.67 |
|
|
|
| 2 |
A' |
3190 |
3021 |
37.06 |
|
|
|
| 3 |
A' |
3096 |
2932 |
35.97 |
|
|
|
| 4 |
A' |
1773 |
1679 |
27.95 |
|
|
|
| 5 |
A' |
1523 |
1442 |
4.44 |
|
|
|
| 6 |
A' |
1389 |
1316 |
41.03 |
|
|
|
| 7 |
A' |
1084 |
1027 |
37.18 |
|
|
|
| 8 |
A" |
1185 |
1122 |
51.51 |
|
|
|
| 9 |
A" |
1113 |
1054 |
15.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8899.4 cm
-1
Scaled (by 0.947) Zero Point Vibrational Energy (zpe) 8427.7 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/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.134 |
|
|
|
| 2 |
N |
-0.491 |
|
|
|
| 3 |
H |
0.147 |
|
|
|
| 4 |
H |
0.169 |
|
|
|
| 5 |
H |
0.309 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.470 |
1.417 |
0.000 |
2.042 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.491 |
2.020 |
0.000 |
| y |
2.020 |
-12.528 |
0.000 |
| z |
0.000 |
0.000 |
-13.374 |
|
| Traceless |
| | x | y | z |
| x |
1.460 |
2.020 |
0.000 |
| y |
2.020 |
-0.095 |
0.000 |
| z |
0.000 |
0.000 |
-1.365 |
|
| Polar |
| 3z2-r2 | -2.730 |
| x2-y2 | 1.037 |
| xy | 2.020 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.568 |
0.271 |
0.000 |
| y |
0.271 |
3.626 |
0.000 |
| z |
0.000 |
0.000 |
1.154 |
<r2> (average value of r
2) Å
2
| <r2> |
19.461 |
| (<r2>)1/2 |
4.411 |