Publication Type |
Journal Article |
School or College |
College of Science |
Department |
Physics |
Creator |
Mattis, Daniel C. |
Other Author |
Gallinar, J. P. |
Title |
What is the effective mass of an exciton? |
Date |
1984 |
Description |
In the effective-mass approximation, the mass M* of an exciton is just the sum of the electron and hole masses, me*+ mh*. However, the effective-mass approximation is invalid if the forces are strong. Here we derive a plausible formula for the n th bound state of the exciton: Mn*= (me* + mh*) / (1 - Kn/W), where Kn is the kinetic energy in the bound state and W is one-half the sum of the electron and hole bandwidths. For Wannier excitons, Kn/W << 1, while for Frenkel excitons, K1s/W-- 1, and the composite particle is effectively localized. |
Type |
Text |
Publisher |
American Physical Society |
Volume |
53 |
Issue |
14 |
First Page |
1391 |
Last Page |
1393 |
Subject |
Kinetic; Energy; Electron |
Language |
eng |
Bibliographic Citation |
Mattis, D. C., & Gallinar, J. P. (1984). What is the effective mass of an exciton? Physical Review Letters, 53(14), 1391-3. |
Rights Management |
(c) American Physical Society |
Format Medium |
application/pdf |
Format Extent |
223,851 bytes |
Identifier |
ir-main,5749 |
ARK |
ark:/87278/s6bg36bj |
Setname |
ir_uspace |
ID |
704521 |
Reference URL |
https://collections.lib.utah.edu/ark:/87278/s6bg36bj |