Abstract
The electron-hole droplet nucleation in highly excited direct gap semiconductors is a non-equilibrium phase transition of second order. Within the framework of a Fokker - Planck approximation modifications of the thermodynamic phase diagram and the cluster distribution function are calculated. Due to the short lifetime of the electronic excitations only very small electron - hole clusters can be formed.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.