Vibrational Frequencies calculated at wB97X-D/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' |
3285 |
3130 |
1.12 |
|
|
|
| 2 |
A' |
3204 |
3052 |
3.65 |
|
|
|
| 3 |
A' |
3103 |
2956 |
4.35 |
|
|
|
| 4 |
A' |
1678 |
1598 |
2.74 |
|
|
|
| 5 |
A' |
1401 |
1334 |
7.67 |
|
|
|
| 6 |
A' |
1067 |
1017 |
7.72 |
|
|
|
| 7 |
A' |
731 |
696 |
22.95 |
|
|
|
| 8 |
A" |
939 |
894 |
94.27 |
|
|
|
| 9 |
A" |
842 |
802 |
21.28 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8124.8 cm
-1
Scaled (by 0.9526) Zero Point Vibrational Energy (zpe) 7739.7 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/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.183 |
|
|
|
| 2 |
C |
-0.324 |
|
|
|
| 3 |
H |
0.170 |
|
|
|
| 4 |
H |
0.164 |
|
|
|
| 5 |
H |
0.173 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.713 |
-0.343 |
0.000 |
0.791 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.313 |
-1.306 |
0.000 |
| y |
-1.306 |
-11.319 |
0.000 |
| z |
0.000 |
0.000 |
-15.025 |
|
| Traceless |
| | x | y | z |
| x |
0.859 |
-1.306 |
0.000 |
| y |
-1.306 |
2.350 |
0.000 |
| z |
0.000 |
0.000 |
-3.209 |
|
| Polar |
| 3z2-r2 | -6.419 |
| x2-y2 | -0.994 |
| xy | -1.306 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.639 |
-0.235 |
0.000 |
| y |
-0.235 |
4.661 |
0.000 |
| z |
0.000 |
0.000 |
1.577 |
<r2> (average value of r
2) Å
2
| <r2> |
20.487 |
| (<r2>)1/2 |
4.526 |