Discover
/
Article

Thermodynamics of excitons in semiconductors

MAR 01, 1982
Groups of photoexcited electrons and holes in silicon and germanium, observed through spectroscopy and imaging techniques, show thermodynamic behavior much like that of atomic and molecular gases and liquids.
James P. Wolfe

During the few microseconds between its laser‐induced creation in a pure semiconductor crystal and its destruction by recombination, a bound electron–hole pair, or exciton, is very active. Like the negative and positive charge carriers from which it forms, the exciton exhibits great mobility, whether it is coaxed by an applied force or simply moves under its own thermal energy. And like an atom in free space, it is bound by Coulomb forces, has discrete energy levels and may combine with other excitons into molecules or even condense into a liquid‐like state. In a semiconductor crystal such as silicon, all of this occurs at temperatures below about 30 K, for these weakly bound neutral particles ionize easily into electrons and holes at higher temperatures. The study of these particles and their products has occupied many physicists over the last couple of decades, and the investigations continue to uncover interesting new phenomena.

This article is only available in PDF format

References

  1. 1. See, for example, W. A. Harrison, Electronic Structure and the Properties of Solids, Freeman, San Francisco (1980).

  2. 2. See, for example, D. L. Dexter, R. S. Knox, Excitons, Wiley, New York (1965).

  3. 3. S. Nikitine in Excitons at High Density, Springer, New York (1975).
    Also, E. F. Gross, Nuovo Cimento Suppl. 3, 672 (1956).https://doi.org/NUCUAF

  4. 4. P. L. Gourley, J. P. Wolfe, Phys. Rev. B20, 3319 (1979); https://doi.org/PRBMDO
    P. L. Gourley, J. P. Wolfe, Phys. Rev. Lett. 40, 526 (1978); https://doi.org/PRLTAO
    P. L. Gourley, J. P. Wolfe, Phys. Rev. B 24, 5970 (1981).https://doi.org/PRBMDO

  5. 5. M. A. Tamor, J. P. Wolfe, Phys. Rev. Lett. 44, 1703 (1980).https://doi.org/PRLTAO

  6. 6. R. S. Markiewicz, J. P. Wolfe, C. D. Jeffries, Phys. Rev. B15, 1988 (1977).https://doi.org/PLRBAQ

  7. 7. M. A. Lampert, Phys. Rev. Lett. 1, 450 (1958).https://doi.org/PRLTAO

  8. 8. See, for example, the review articles by T. M. Rice, and by J. C. Hensel, T. G. Phillips, G. A. Thomas, Solid State Physics, Vol. 32, Academic, New York (1977).
    Also, C. D. Jeffries, Science 189, 955 (1975).https://doi.org/SCIEAS

  9. 9. G. A. Thomas, V. B. Timofeev in Optical Properties of Solids, Handbook on Semiconductors, Vol. 2, M. Balkanski, ed., North‐Holland, Amsterdam (1980).

  10. 10. J. Shah, M. Combescot, A. H. Dayem, Phys. Rev. Lett. 38, 1497 (1977).https://doi.org/PRLTAO

  11. 11. M. Greenstein, J. P. Wolfe, Phys. Rev. Lett. 41, 715 (1978); https://doi.org/PRLTAO
    M. Greenstein, J. P. Wolfe, Phys. Rev. B 24, 3318 (1981).https://doi.org/PRBMDO

  12. 12. R. S. Markiewcz, M. Greenstein, J. P. Wolfe, Sol. St. Comm. 35, 339 (1980).https://doi.org/SSCOA4

  13. 13. N. F. Mott, Metal Insulator Transitions, Barnes and Noble, New York (1974).

  14. 14. E. Hanamura, H. Haug, Physics Lett. C 33, 209 (1977).https://doi.org/PRPLCM

  15. 15. A. Mysyrowicz, J. Physique 41, C7‐281 (1980).

  16. 16. D. Hulin, A. Mysyrowicz, C. Benoit a la Guillaume, Phys. Rev. Lett. 45, 190 (1980). https://doi.org/PRLTAO
    L. L. Chase, N. Peyghambarian, G. Grynberg, A. Mysyrowicz, Phys. Rev. Lett. 42, 1231 (1979); https://doi.org/PRLTAO
    also, E. Hanamura, in reference 3.

  17. 17. See D. C. Reynolds, T. C. Collins, Excitons: Their Properties and Uses, Academic, New York (1981), page 252, and references therein.

More about the authors

James P. Wolfe, University of Illinois, Urbana–Champaign.

Related content
/
Article
A half century after the discovery of Hawking radiation, we are still dealing with the quantum puzzle it exposed.
/
Article
Since the discovery was first reported in 1999, researchers have uncovered many aspects of the chiral-induced spin selectivity effect, but its underlying mechanisms remain unclear.
/
Article
Metrologists are using fundamental physics to define units of measure. Now NIST has developed new quantum sensors to measure and realize the pascal.
/
Article
Nanoscale, topologically protected whirlpools of spins have the potential to move from applications in spintronics into quantum science.
This Content Appeared In
pt-cover_1982_03.jpeg

Volume 35, Number 3

Get PT newsletters in your inbox

pt_newsletter_card_blue.png
PT The Week in Physics

A collection of PT's content from the previous week delivered every Monday.

pt_newsletter_card_darkblue.png
PT New Issue Alert

Be notified about the new issue with links to highlights and the full TOC.

pt_newsletter_card_pink.png
PT Webinars & White Papers

The latest webinars, white papers and other informational resources.

By signing up you agree to allow AIP to send you email newsletters. You further agree to our privacy policy and terms of service.