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 |
A |
3032 |
3013 |
2.16 |
|
|
|
| 2 |
A |
3011 |
2992 |
18.21 |
|
|
|
| 3 |
A |
2943 |
2924 |
2.33 |
|
|
|
| 4 |
A |
1500 |
1491 |
19.90 |
|
|
|
| 5 |
A |
1413 |
1404 |
17.49 |
|
|
|
| 6 |
A |
1359 |
1351 |
3.59 |
|
|
|
| 7 |
A |
883 |
878 |
4.49 |
|
|
|
| 8 |
A |
706 |
702 |
64.93 |
|
|
|
| 9 |
A |
665 |
660 |
0.94 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7756.7 cm
-1
Scaled (by 0.9935) Zero Point Vibrational Energy (zpe) 7706.2 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 |
C |
-0.707 |
|
|
|
| 2 |
S |
0.039 |
|
|
|
| 3 |
H |
0.228 |
|
|
|
| 4 |
H |
0.220 |
|
|
|
| 5 |
H |
0.220 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.750 |
0.000 |
0.107 |
1.753 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.287 |
-0.000 |
0.184 |
| y |
-0.000 |
-21.543 |
-0.000 |
| z |
0.184 |
-0.000 |
-19.046 |
|
| Traceless |
| | x | y | z |
| x |
1.007 |
-0.000 |
0.184 |
| y |
-0.000 |
-2.376 |
-0.000 |
| z |
0.184 |
-0.000 |
1.369 |
|
| Polar |
| 3z2-r2 | 2.738 |
| x2-y2 | 2.256 |
| xy | -0.000 |
| xz | 0.184 |
| yz | -0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
38.054 |
| (<r2>)1/2 |
6.169 |