Vibrational Frequencies calculated at B2PLYP/daug-cc-pVTZ
| 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' |
3459 |
3459 |
1.02 |
|
|
|
| 2 |
A' |
3154 |
3154 |
25.58 |
|
|
|
| 3 |
A' |
3053 |
3053 |
45.86 |
|
|
|
| 4 |
A' |
1689 |
1689 |
17.50 |
|
|
|
| 5 |
A' |
1492 |
1492 |
7.27 |
|
|
|
| 6 |
A' |
1374 |
1374 |
40.46 |
|
|
|
| 7 |
A' |
1076 |
1076 |
35.71 |
|
|
|
| 8 |
A" |
1165 |
1165 |
43.84 |
|
|
|
| 9 |
A" |
1101 |
1101 |
15.39 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8781.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8781.3 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 B2PLYP/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.957 |
|
|
|
| 2 |
N |
-0.915 |
|
|
|
| 3 |
H |
0.707 |
|
|
|
| 4 |
H |
0.817 |
|
|
|
| 5 |
H |
0.348 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.364 |
1.518 |
0.000 |
2.041 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.885 |
2.077 |
0.000 |
| y |
2.077 |
-12.914 |
0.000 |
| z |
0.000 |
0.000 |
-13.822 |
|
| Traceless |
| | x | y | z |
| x |
1.483 |
2.077 |
0.000 |
| y |
2.077 |
-0.060 |
0.000 |
| z |
0.000 |
0.000 |
-1.423 |
|
| Polar |
| 3z2-r2 | -2.846 |
| x2-y2 | 1.029 |
| xy | 2.077 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.285 |
0.101 |
0.000 |
| y |
0.101 |
4.333 |
0.000 |
| z |
0.000 |
0.000 |
2.578 |
<r2> (average value of r
2) Å
2
| <r2> |
19.711 |
| (<r2>)1/2 |
4.440 |