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Re: [abinit-forum] electron phonon analysis of a semiconductor


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  • From: Matthieu Verstraete <mjv500@york.ac.uk>
  • To: forum@abinit.org
  • Subject: Re: [abinit-forum] electron phonon analysis of a semiconductor
  • Date: Sat, 16 Feb 2008 00:47:15 +0000 (GMT)


the matrix element. If I understand correctly, the matrix element is
calculated through the ground state wavefunction at least for getting
the lamda (e-p constant).
yes: these are matrix elements of the GS wfct from the phonon run. Any temperature or energy window you select are post-hoc and concern 0K GS states.

So if the system is excited by a laser pulse, can the matrix element be the same? I mean, since the screen potential is from the fact that the electrons react to contribute to the effective potential. Wouldn't this effective potential change when the electrons are excited in terms of non-zero electron temperatures, temperature dependent?
Yes, but it depends which time scales you are looking at. In a first approximation, immediately after the pulse, the electrons are excited in a really unequilibrated way. Then (normally) electronic processes allow thermalization of the electron population and the distribution of the states should be fermi-like. Later, the e-p coupling kicks in and the heat is progressively (sometimes quite quickly!) transferred or shared with the lattice.


This sounds that one has to do calculation of
the wavefunctions at conditions of non-zero electron temperatures.
Yes, but it's always more complex
1) your distribution of hot electrons will not be spatially homogeneous
2) the distribution of energies will not be a simple fermi one. All of the standard distributions correspond to thermodynamic potentials with a given equilibrium and ensemble. You should be completely out of equilibrium, and the time scale analysis above presumes you will go rapidly to a sequence of pseudo equilibrium states with thermalized electrons then phonons etc...


And here comes another questions while I was reading your previous email about the physical electron temperature tphysel and the laser paper by CEA group PRL 2006. I assume that they specify the value of tphysel to be 6eV in abinit?
tphysel is probably not necessary. To my knowledge they used just a fermi distribution. tphysel is for intermediate physical temperatures, when the physical smearing is not enough to improve your kpoint convergence. Then you can add a second (rapidly decaying) smearing function in order to improve your k convergence without destroying your electronic temperature dependence.

BTW, the umklapp processes is included in the calculations of matrix element?
hmmmm. I'm not sure I know the answer to that one. You mean for q vectors out of the first BZ? I'll ponder that some more. Anyone have an idea?


Matthieu




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