Vibrational Frequencies calculated at BLYP/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' |
3151 |
3156 |
1.85 |
|
|
|
| 2 |
A' |
3057 |
3062 |
5.43 |
|
|
|
| 3 |
A' |
2947 |
2951 |
6.58 |
|
|
|
| 4 |
A' |
1607 |
1610 |
1.31 |
|
|
|
| 5 |
A' |
1325 |
1327 |
7.50 |
|
|
|
| 6 |
A' |
1007 |
1009 |
10.45 |
|
|
|
| 7 |
A' |
677 |
679 |
24.69 |
|
|
|
| 8 |
A" |
870 |
871 |
61.03 |
|
|
|
| 9 |
A" |
757 |
758 |
8.27 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7699.3 cm
-1
Scaled (by 1.0016) Zero Point Vibrational Energy (zpe) 7711.7 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 BLYP/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.094 |
|
|
|
| 2 |
C |
0.004 |
|
|
|
| 3 |
H |
0.028 |
|
|
|
| 4 |
H |
0.030 |
|
|
|
| 5 |
H |
0.032 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.554 |
-0.282 |
0.000 |
0.621 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.322 |
-1.074 |
0.000 |
| y |
-1.074 |
-11.330 |
0.000 |
| z |
0.000 |
0.000 |
-14.375 |
|
| Traceless |
| | x | y | z |
| x |
0.530 |
-1.074 |
0.000 |
| y |
-1.074 |
2.019 |
0.000 |
| z |
0.000 |
0.000 |
-2.549 |
|
| Polar |
| 3z2-r2 | -5.098 |
| x2-y2 | -0.992 |
| xy | -1.074 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.781 |
-0.246 |
-0.001 |
| y |
-0.246 |
4.804 |
-0.000 |
| z |
-0.001 |
-0.000 |
1.581 |
<r2> (average value of r
2) Å
2
| <r2> |
20.648 |
| (<r2>)1/2 |
4.544 |