Vibrational Frequencies calculated at B3LYPultrafine/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 |
3591 |
3472 |
23.51 |
|
|
|
| 2 |
A |
1288 |
1245 |
0.00 |
|
|
|
| 3 |
A |
927 |
896 |
12.66 |
|
|
|
| 4 |
A |
725 |
701 |
92.15 |
|
|
|
| 5 |
A |
544 |
526 |
0.26 |
|
|
|
| 6 |
B |
3589 |
3469 |
124.38 |
|
|
|
| 7 |
B |
2229 |
2154 |
622.12 |
|
|
|
| 8 |
B |
925 |
895 |
439.98 |
|
|
|
| 9 |
B |
546 |
528 |
73.87 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7181.9 cm
-1
Scaled (by 0.9667) Zero Point Vibrational Energy (zpe) 6942.7 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 B3LYPultrafine/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.150 |
|
|
|
| 2 |
N |
-0.256 |
|
|
|
| 3 |
N |
-0.256 |
|
|
|
| 4 |
H |
0.181 |
|
|
|
| 5 |
H |
0.181 |
|
|
|
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 |
2.007 |
2.007 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.803 |
4.052 |
0.000 |
| y |
4.052 |
-16.236 |
0.000 |
| z |
0.000 |
0.000 |
-17.308 |
|
| Traceless |
| | x | y | z |
| x |
-0.031 |
4.052 |
0.000 |
| y |
4.052 |
0.820 |
0.000 |
| z |
0.000 |
0.000 |
-0.789 |
|
| Polar |
| 3z2-r2 | -1.577 |
| x2-y2 | -0.568 |
| xy | 4.052 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.486 |
0.315 |
0.000 |
| y |
0.315 |
6.220 |
0.000 |
| z |
0.000 |
0.000 |
2.458 |
<r2> (average value of r
2) Å
2
| <r2> |
38.730 |
| (<r2>)1/2 |
6.223 |