This commit is contained in:
@@ -37,18 +37,15 @@ However, whether a mode is sufficiently strong to be experimentally visible
|
|||||||
|
|
||||||
// TODO: maybe it is better to assign Raman tensor to each bond, instead of atom
|
// TODO: maybe it is better to assign Raman tensor to each bond, instead of atom
|
||||||
|
|
||||||
We propose a method to estimate the magnitudes of the Raman tensors of these phonons by symmetry analysis.
|
We propose a method to estimate the magnitudes of the Raman tensors of these phonons based on symmetry analysis.
|
||||||
This method relies on the following two assumptions:
|
This approach is founded on the assumption that the change in polarizability induced by atomic displacements in 4H-SiC
|
||||||
firstly, the change of polarizability caused by the movement of the atom in different locations
|
is mainly determined by two factors: first- and second-nearest neighbors of the atom, and the symbol of charge corresponding to the atom,
|
||||||
is mainly determined by its first- and second-nearest neighbors,
|
all other factors (mass, bond length, etc.) contribute only a small value.
|
||||||
and the farther neighbors have relatively small contributions.
|
Consequently,
|
||||||
Secondly, the change of polarizability caused by Si atom and C atom is roughly connected by the reversal of the charge,
|
the phonon modes with the strongest Raman intensities can be predicted
|
||||||
other factors (mass, bond length, etc.) contribute only a small value.
|
prior to first-principles calculations and experiments,
|
||||||
Therefore, the vibration mode with the most intense Raman intensity
|
and the Raman tensors of the calculated phonon modes can be estimated without additional first-principles computations.
|
||||||
could be estimated before the first-principle calculation and experiment,
|
Further details are provided in the appendix.
|
||||||
and the Raman tensors of the calculated phonon modes could also be estimated
|
|
||||||
without further first-principle calculations.
|
|
||||||
Please see appendix for details.
|
|
||||||
|
|
||||||
The Raman tensors and frequencies of the negligible-polar phonons were calculated using first-principles methods,
|
The Raman tensors and frequencies of the negligible-polar phonons were calculated using first-principles methods,
|
||||||
and the results are compared with experiment and theory (@table-nopol).
|
and the results are compared with experiment and theory (@table-nopol).
|
||||||
|
|||||||
Reference in New Issue
Block a user