Vibrational Frequencies calculated at BLYP/3-21G
| 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 |
3246 |
3228 |
0.88 |
|
|
|
| 2 |
A1 |
1265 |
1258 |
30.56 |
|
|
|
| 3 |
A1 |
560 |
557 |
2.52 |
|
|
|
| 4 |
E |
3338 |
3319 |
36.04 |
|
|
|
| 4 |
E |
3338 |
3319 |
36.04 |
|
|
|
| 5 |
E |
1679 |
1670 |
39.42 |
|
|
|
| 5 |
E |
1679 |
1670 |
39.42 |
|
|
|
| 6 |
E |
776 |
772 |
56.63 |
|
|
|
| 6 |
E |
776 |
772 |
56.63 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8329.2 cm
-1
Scaled (by 0.9945) Zero Point Vibrational Energy (zpe) 8283.4 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 BLYP/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.676 |
|
|
|
| 2 |
S |
-0.386 |
|
|
|
| 3 |
H |
0.354 |
|
|
|
| 4 |
H |
0.354 |
|
|
|
| 5 |
H |
0.354 |
|
|
|
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 |
-6.630 |
6.630 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.641 |
0.000 |
0.000 |
| y |
0.000 |
-20.641 |
0.000 |
| z |
0.000 |
0.000 |
-14.356 |
|
| Traceless |
| | x | y | z |
| x |
-3.142 |
0.000 |
0.000 |
| y |
0.000 |
-3.142 |
0.000 |
| z |
0.000 |
0.000 |
6.284 |
|
| Polar |
| 3z2-r2 | 12.569 |
| 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 |
1.723 |
0.000 |
0.000 |
| y |
0.000 |
1.723 |
0.000 |
| z |
0.000 |
0.000 |
3.895 |
<r2> (average value of r
2) Å
2
| <r2> |
40.584 |
| (<r2>)1/2 |
6.371 |