Vibrational Frequencies calculated at B3LYP/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' |
3236 |
3139 |
1.31 |
|
|
|
| 2 |
A' |
3151 |
3057 |
3.95 |
|
|
|
| 3 |
A' |
3047 |
2956 |
3.79 |
|
|
|
| 4 |
A' |
1660 |
1610 |
1.55 |
|
|
|
| 5 |
A' |
1365 |
1324 |
8.23 |
|
|
|
| 6 |
A' |
1040 |
1009 |
10.45 |
|
|
|
| 7 |
A' |
703 |
682 |
23.37 |
|
|
|
| 8 |
A" |
909 |
881 |
64.20 |
|
|
|
| 9 |
A" |
804 |
779 |
11.49 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7957.2 cm
-1
Scaled (by 0.97) Zero Point Vibrational Energy (zpe) 7718.5 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 B3LYP/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.110 |
|
|
|
| 2 |
C |
-0.026 |
|
|
|
| 3 |
H |
0.045 |
|
|
|
| 4 |
H |
0.044 |
|
|
|
| 5 |
H |
0.047 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.570 |
-0.267 |
0.000 |
0.629 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.225 |
-1.090 |
0.000 |
| y |
-1.090 |
-11.227 |
0.000 |
| z |
0.000 |
0.000 |
-14.410 |
|
| Traceless |
| | x | y | z |
| x |
0.593 |
-1.090 |
0.000 |
| y |
-1.090 |
2.091 |
0.000 |
| z |
0.000 |
0.000 |
-2.684 |
|
| Polar |
| 3z2-r2 | -5.368 |
| x2-y2 | -0.998 |
| xy | -1.090 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.686 |
-0.242 |
-0.002 |
| y |
-0.242 |
4.693 |
0.000 |
| z |
-0.002 |
0.000 |
1.569 |
<r2> (average value of r
2) Å
2
| <r2> |
20.445 |
| (<r2>)1/2 |
4.522 |