Vibrational Frequencies calculated at B3PW91/6-31G(2df,p)
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3209 |
3085 |
15.76 |
|
|
|
| 2 |
A1 |
2242 |
2155 |
328.59 |
|
|
|
| 3 |
A1 |
1442 |
1387 |
29.76 |
|
|
|
| 4 |
A1 |
1232 |
1185 |
0.84 |
|
|
|
| 5 |
B1 |
590 |
568 |
1.19 |
|
|
|
| 6 |
B1 |
423 |
407 |
125.07 |
|
|
|
| 7 |
B2 |
3336 |
3207 |
2.86 |
|
|
|
| 8 |
B2 |
1115 |
1072 |
1.49 |
|
|
|
| 9 |
B2 |
430 |
414 |
0.49 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7009.8 cm
-1
Scaled (by 0.9614) Zero Point Vibrational Energy (zpe) 6739.2 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 B3PW91/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.418 |
|
|
|
| 2 |
N |
0.329 |
|
|
|
| 3 |
N |
-0.267 |
|
|
|
| 4 |
H |
0.178 |
|
|
|
| 5 |
H |
0.178 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-1.710 |
1.710 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-18.588 |
0.000 |
0.000 |
| y |
0.000 |
-15.178 |
0.000 |
| z |
0.000 |
0.000 |
-18.201 |
|
| Traceless |
| | x | y | z |
| x |
-1.899 |
0.000 |
0.000 |
| y |
0.000 |
3.217 |
0.000 |
| z |
0.000 |
0.000 |
-1.318 |
|
| Polar |
| 3z2-r2 | -2.636 |
| x2-y2 | -3.410 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.944 |
0.000 |
0.000 |
| y |
0.000 |
2.535 |
0.000 |
| z |
0.000 |
0.000 |
6.450 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |