Vibrational Frequencies calculated at ROHF/TZVP
| 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' |
3391 |
3391 |
0.49 |
|
|
|
| 2 |
A' |
3341 |
3341 |
6.82 |
|
|
|
| 3 |
A' |
3255 |
3255 |
4.70 |
|
|
|
| 4 |
A' |
1780 |
1780 |
2.83 |
|
|
|
| 5 |
A' |
1512 |
1512 |
7.20 |
|
|
|
| 6 |
A' |
1200 |
1200 |
7.42 |
|
|
|
| 7 |
A' |
827 |
827 |
13.43 |
|
|
|
| 8 |
A" |
1058 |
1058 |
75.82 |
|
|
|
| 9 |
A" |
966 |
966 |
34.38 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8664.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8664.7 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 ROHF/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.108 |
|
|
|
| 2 |
C |
-0.244 |
|
|
|
| 3 |
H |
0.122 |
|
|
|
| 4 |
H |
0.111 |
|
|
|
| 5 |
H |
0.120 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.634 |
-0.248 |
0.000 |
0.680 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.306 |
-1.148 |
0.001 |
| y |
-1.148 |
-11.473 |
-0.001 |
| z |
0.001 |
-0.001 |
-15.101 |
|
| Traceless |
| | x | y | z |
| x |
0.981 |
-1.148 |
0.001 |
| y |
-1.148 |
2.231 |
-0.001 |
| z |
0.001 |
-0.001 |
-3.212 |
|
| Polar |
| 3z2-r2 | -6.424 |
| x2-y2 | -0.833 |
| xy | -1.148 |
| xz | 0.001 |
| yz | -0.001 |
|
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> |
20.236 |
| (<r2>)1/2 |
4.498 |