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 |
3062 |
3045 |
0.16 |
|
|
|
| 2 |
A |
3056 |
3040 |
12.80 |
|
|
|
| 3 |
A |
2977 |
2961 |
1.97 |
|
|
|
| 4 |
A |
1494 |
1485 |
19.51 |
|
|
|
| 5 |
A |
1384 |
1376 |
19.69 |
|
|
|
| 6 |
A |
1335 |
1328 |
3.15 |
|
|
|
| 7 |
A |
874 |
869 |
3.02 |
|
|
|
| 8 |
A |
608 |
605 |
0.59 |
|
|
|
| 9 |
A |
379 |
377 |
95.73 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7584.9 cm
-1
Scaled (by 0.9945) Zero Point Vibrational Energy (zpe) 7543.2 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 |
-0.771 |
|
|
|
| 2 |
S |
0.080 |
|
|
|
| 3 |
H |
0.234 |
|
|
|
| 4 |
H |
0.229 |
|
|
|
| 5 |
H |
0.229 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.865 |
-0.000 |
0.086 |
1.867 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.699 |
-0.000 |
0.150 |
| y |
-0.000 |
-21.650 |
-0.000 |
| z |
0.150 |
-0.000 |
-19.058 |
|
| Traceless |
| | x | y | z |
| x |
0.655 |
-0.000 |
0.150 |
| y |
-0.000 |
-2.272 |
-0.000 |
| z |
0.150 |
-0.000 |
1.617 |
|
| Polar |
| 3z2-r2 | 3.234 |
| x2-y2 | 1.951 |
| xy | -0.000 |
| xz | 0.150 |
| 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> |
39.627 |
| (<r2>)1/2 |
6.295 |