Vibrational Frequencies calculated at M06-2X/6-31G
| 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' |
3289 |
3289 |
1.26 |
|
|
|
| 2 |
A' |
3223 |
3223 |
7.67 |
|
|
|
| 3 |
A' |
3132 |
3132 |
2.11 |
|
|
|
| 4 |
A' |
1691 |
1691 |
2.80 |
|
|
|
| 5 |
A' |
1451 |
1451 |
6.50 |
|
|
|
| 6 |
A' |
1105 |
1105 |
7.14 |
|
|
|
| 7 |
A' |
760 |
760 |
19.87 |
|
|
|
| 8 |
A" |
995 |
995 |
79.80 |
|
|
|
| 9 |
A" |
894 |
894 |
30.30 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8269.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8269.7 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 M06-2X/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.116 |
|
|
|
| 2 |
C |
-0.378 |
|
|
|
| 3 |
H |
0.163 |
|
|
|
| 4 |
H |
0.162 |
|
|
|
| 5 |
H |
0.169 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.605 |
-0.224 |
0.000 |
0.645 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.082 |
-1.092 |
0.000 |
| y |
-1.092 |
-11.174 |
0.000 |
| z |
0.000 |
0.000 |
-14.399 |
|
| Traceless |
| | x | y | z |
| x |
0.705 |
-1.092 |
0.000 |
| y |
-1.092 |
2.066 |
0.000 |
| z |
0.000 |
0.000 |
-2.771 |
|
| Polar |
| 3z2-r2 | -5.542 |
| x2-y2 | -0.908 |
| xy | -1.092 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.367 |
-0.255 |
0.000 |
| y |
-0.255 |
4.407 |
0.000 |
| z |
0.000 |
0.000 |
1.137 |
<r2> (average value of r
2) Å
2
| <r2> |
20.313 |
| (<r2>)1/2 |
4.507 |