Vibrational Frequencies calculated at B2PLYP/Def2TZVPP
| 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' |
3270 |
3270 |
0.67 |
|
|
|
| 2 |
A' |
3183 |
3183 |
2.44 |
|
|
|
| 3 |
A' |
3082 |
3082 |
3.17 |
|
|
|
| 4 |
A' |
1672 |
1672 |
2.27 |
|
|
|
| 5 |
A' |
1408 |
1408 |
8.00 |
|
|
|
| 6 |
A' |
1064 |
1064 |
7.99 |
|
|
|
| 7 |
A' |
720 |
720 |
20.72 |
|
|
|
| 8 |
A" |
937 |
937 |
75.62 |
|
|
|
| 9 |
A" |
830 |
830 |
17.44 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8082.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8082.7 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 B2PLYP/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.155 |
|
|
|
| 2 |
C |
-0.184 |
|
|
|
| 3 |
H |
0.128 |
|
|
|
| 4 |
H |
0.102 |
|
|
|
| 5 |
H |
0.110 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.623 |
-0.311 |
0.000 |
0.696 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.485 |
-1.189 |
0.000 |
| y |
-1.189 |
-11.444 |
0.000 |
| z |
0.000 |
0.000 |
-14.910 |
|
| Traceless |
| | x | y | z |
| x |
0.692 |
-1.189 |
0.000 |
| y |
-1.189 |
2.253 |
0.000 |
| z |
0.000 |
0.000 |
-2.945 |
|
| Polar |
| 3z2-r2 | -5.890 |
| x2-y2 | -1.040 |
| xy | -1.189 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.030 |
-0.125 |
0.000 |
| y |
-0.125 |
5.005 |
0.000 |
| z |
0.000 |
0.000 |
2.542 |
<r2> (average value of r
2) Å
2
| <r2> |
20.412 |
| (<r2>)1/2 |
4.518 |