Vibrational Frequencies calculated at B97D3/aug-cc-pVDZ
| 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' |
3183 |
3183 |
1.30 |
|
|
|
| 2 |
A' |
3096 |
3096 |
6.45 |
|
|
|
| 3 |
A' |
2992 |
2992 |
8.26 |
|
|
|
| 4 |
A' |
1613 |
1613 |
1.41 |
|
|
|
| 5 |
A' |
1350 |
1350 |
8.28 |
|
|
|
| 6 |
A' |
1020 |
1020 |
9.70 |
|
|
|
| 7 |
A' |
692 |
692 |
20.72 |
|
|
|
| 8 |
A" |
896 |
896 |
72.57 |
|
|
|
| 9 |
A" |
761 |
761 |
16.86 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7801.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 7801.5 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 B97D3/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.291 |
|
|
|
| 2 |
C |
0.781 |
|
|
|
| 3 |
H |
-0.446 |
|
|
|
| 4 |
H |
-0.343 |
|
|
|
| 5 |
H |
-0.283 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.601 |
-0.340 |
0.000 |
0.690 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.504 |
-1.201 |
0.000 |
| y |
-1.201 |
-11.556 |
0.000 |
| z |
0.000 |
0.000 |
-14.920 |
|
| Traceless |
| | x | y | z |
| x |
0.734 |
-1.201 |
0.000 |
| y |
-1.201 |
2.155 |
0.000 |
| z |
0.000 |
0.000 |
-2.890 |
|
| Polar |
| 3z2-r2 | -5.779 |
| x2-y2 | -0.947 |
| xy | -1.201 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.615 |
-0.065 |
0.000 |
| y |
-0.065 |
5.444 |
0.000 |
| z |
0.000 |
0.000 |
3.291 |
<r2> (average value of r
2) Å
2
| <r2> |
20.765 |
| (<r2>)1/2 |
4.557 |