Vibrational Frequencies calculated at BLYP/6-311+G(3df,2p)
| 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 |
3330 |
3312 |
0.10 |
|
|
|
| 2 |
A1 |
1278 |
1271 |
19.35 |
|
|
|
| 3 |
A1 |
564 |
561 |
1.13 |
|
|
|
| 4 |
E |
3407 |
3388 |
67.04 |
|
|
|
| 4 |
E |
3407 |
3388 |
67.05 |
|
|
|
| 5 |
E |
1612 |
1603 |
29.30 |
|
|
|
| 5 |
E |
1612 |
1603 |
29.29 |
|
|
|
| 6 |
E |
800 |
796 |
13.66 |
|
|
|
| 6 |
E |
800 |
796 |
13.66 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8404.8 cm
-1
Scaled (by 0.9945) Zero Point Vibrational Energy (zpe) 8358.5 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/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.235 |
|
|
|
| 2 |
S |
-0.489 |
|
|
|
| 3 |
H |
0.241 |
|
|
|
| 4 |
H |
0.241 |
|
|
|
| 5 |
H |
0.241 |
|
|
|
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 |
-5.938 |
5.938 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.855 |
0.000 |
0.000 |
| y |
0.000 |
-21.855 |
0.000 |
| z |
0.000 |
0.000 |
-15.428 |
|
| Traceless |
| | x | y | z |
| x |
-3.213 |
0.000 |
0.000 |
| y |
0.000 |
-3.213 |
0.000 |
| z |
0.000 |
0.000 |
6.427 |
|
| Polar |
| 3z2-r2 | 12.854 |
| 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 |
5.259 |
0.000 |
0.000 |
| y |
0.000 |
5.260 |
-0.001 |
| z |
0.000 |
-0.001 |
6.310 |
<r2> (average value of r
2) Å
2
| <r2> |
39.312 |
| (<r2>)1/2 |
6.270 |