Vibrational Frequencies calculated at TPSSh/6-311G*
| 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' |
3435 |
3309 |
0.33 |
222.17 |
0.34 |
0.51 |
| 2 |
A' |
3051 |
2939 |
42.33 |
129.49 |
0.42 |
0.60 |
| 3 |
A' |
2639 |
2542 |
0.21 |
114.81 |
0.33 |
0.50 |
| 4 |
A' |
1652 |
1591 |
170.55 |
12.98 |
0.23 |
0.37 |
| 5 |
A' |
1398 |
1347 |
26.70 |
6.12 |
0.12 |
0.21 |
| 6 |
A' |
1215 |
1170 |
27.50 |
14.00 |
0.62 |
0.77 |
| 7 |
A' |
935 |
900 |
55.77 |
5.15 |
0.50 |
0.67 |
| 8 |
A' |
697 |
671 |
78.38 |
5.68 |
0.25 |
0.40 |
| 9 |
A' |
423 |
407 |
17.48 |
3.36 |
0.49 |
0.66 |
| 10 |
A" |
1054 |
1016 |
3.38 |
0.47 |
0.75 |
0.86 |
| 11 |
A" |
733 |
706 |
85.34 |
3.49 |
0.75 |
0.86 |
| 12 |
A" |
406 |
391 |
46.46 |
4.30 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 8818.2 cm
-1
Scaled (by 0.9632) Zero Point Vibrational Energy (zpe) 8493.7 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 TPSSh/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.476 |
|
|
|
| 2 |
C |
-0.143 |
|
|
|
| 3 |
S |
-0.062 |
|
|
|
| 4 |
H |
0.284 |
|
|
|
| 5 |
H |
0.217 |
|
|
|
| 6 |
H |
0.179 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.601 |
1.253 |
0.000 |
1.390 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.003 |
1.326 |
0.000 |
| y |
1.326 |
6.745 |
0.000 |
| z |
0.000 |
0.000 |
2.608 |
<r2> (average value of r
2) Å
2
| <r2> |
67.761 |
| (<r2>)1/2 |
8.232 |