Vibrational Frequencies calculated at B3LYPultrafine/6-31+G**
| 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 |
3440 |
3312 |
9.03 |
|
|
|
| 2 |
A1 |
1357 |
1306 |
18.47 |
|
|
|
| 3 |
A1 |
581 |
559 |
8.40 |
|
|
|
| 4 |
E |
3543 |
3410 |
86.13 |
|
|
|
| 4 |
E |
3543 |
3410 |
86.13 |
|
|
|
| 5 |
E |
1656 |
1595 |
35.21 |
|
|
|
| 5 |
E |
1656 |
1595 |
35.21 |
|
|
|
| 6 |
E |
835 |
804 |
32.02 |
|
|
|
| 6 |
E |
835 |
804 |
32.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8723.0 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 8397.6 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/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.759 |
|
|
|
| 2 |
S |
-0.374 |
|
|
|
| 3 |
H |
0.378 |
|
|
|
| 4 |
H |
0.378 |
|
|
|
| 5 |
H |
0.378 |
|
|
|
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 |
-6.342 |
6.342 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.778 |
0.000 |
0.000 |
| y |
0.000 |
-21.778 |
0.000 |
| z |
0.000 |
0.000 |
-15.071 |
|
| Traceless |
| | x | y | z |
| x |
-3.353 |
0.000 |
0.000 |
| y |
0.000 |
-3.353 |
0.000 |
| z |
0.000 |
0.000 |
6.707 |
|
| Polar |
| 3z2-r2 | 13.414 |
| x2-y2 | 0.000 |
| 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 |
3.863 |
0.000 |
0.000 |
| y |
0.000 |
3.863 |
0.000 |
| z |
0.000 |
0.000 |
5.424 |
<r2> (average value of r
2) Å
2
| <r2> |
39.293 |
| (<r2>)1/2 |
6.268 |