Vibrational Frequencies calculated at wB97X-D/CEP-121G*
| 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' |
3234 |
3234 |
2.84 |
|
|
|
| 2 |
A' |
3176 |
3176 |
10.93 |
|
|
|
| 3 |
A' |
3072 |
3072 |
10.64 |
|
|
|
| 4 |
A' |
1636 |
1636 |
2.20 |
|
|
|
| 5 |
A' |
1394 |
1394 |
6.92 |
|
|
|
| 6 |
A' |
1066 |
1066 |
9.12 |
|
|
|
| 7 |
A' |
720 |
720 |
23.44 |
|
|
|
| 8 |
A" |
924 |
924 |
100.77 |
|
|
|
| 9 |
A" |
822 |
822 |
14.16 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8021.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8021.7 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 wB97X-D/CEP-121G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.185 |
|
|
|
| 2 |
C |
-0.381 |
|
|
|
| 3 |
H |
0.190 |
|
|
|
| 4 |
H |
0.184 |
|
|
|
| 5 |
H |
0.193 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.703 |
-0.316 |
0.000 |
0.770 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.053 |
-1.280 |
0.000 |
| y |
-1.280 |
-11.004 |
0.000 |
| z |
0.000 |
0.000 |
-14.817 |
|
| Traceless |
| | x | y | z |
| x |
0.858 |
-1.280 |
0.000 |
| y |
-1.280 |
2.431 |
0.000 |
| z |
0.000 |
0.000 |
-3.289 |
|
| Polar |
| 3z2-r2 | -6.578 |
| x2-y2 | -1.049 |
| xy | -1.280 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.728 |
-0.172 |
0.000 |
| y |
-0.172 |
4.998 |
0.000 |
| z |
0.000 |
0.000 |
1.890 |
<r2> (average value of r
2) Å
2
| <r2> |
18.655 |
| (<r2>)1/2 |
4.319 |