Vibrational Frequencies calculated at B2PLYP/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' |
3280 |
3280 |
2.23 |
|
|
|
| 2 |
A' |
3191 |
3191 |
5.45 |
|
|
|
| 3 |
A' |
3095 |
3095 |
3.01 |
|
|
|
| 4 |
A' |
1687 |
1687 |
2.50 |
|
|
|
| 5 |
A' |
1480 |
1480 |
7.31 |
|
|
|
| 6 |
A' |
1124 |
1124 |
9.44 |
|
|
|
| 7 |
A' |
772 |
772 |
22.68 |
|
|
|
| 8 |
A" |
972 |
972 |
84.50 |
|
|
|
| 9 |
A" |
869 |
869 |
17.64 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8235.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8235.2 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 B2PLYP/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.162 |
|
|
|
| 2 |
C |
-0.457 |
|
|
|
| 3 |
H |
0.205 |
|
|
|
| 4 |
H |
0.203 |
|
|
|
| 5 |
H |
0.211 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.612 |
-0.263 |
0.000 |
0.666 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.190 |
-1.095 |
0.000 |
| y |
-1.095 |
-11.220 |
0.000 |
| z |
0.000 |
0.000 |
-14.544 |
|
| Traceless |
| | x | y | z |
| x |
0.691 |
-1.095 |
0.000 |
| y |
-1.095 |
2.147 |
0.000 |
| z |
0.000 |
0.000 |
-2.839 |
|
| Polar |
| 3z2-r2 | -5.677 |
| x2-y2 | -0.970 |
| xy | -1.095 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.220 |
-0.259 |
0.000 |
| y |
-0.259 |
4.148 |
0.000 |
| z |
0.000 |
0.000 |
0.941 |
<r2> (average value of r
2) Å
2
| <r2> |
20.327 |
| (<r2>)1/2 |
4.509 |