Spectroscopic determination of the doping and mobility of terahertz quantum cascade structures
J. Appl. Phys. 106, 093104 (2009); doi:10.1063/1.3247973
Published 5 November 2009
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Terahertz time-domain spectroscopy is shown to provide a convenient and rapid means to measure the conductivity of individual layers in semiconductor heterostructures such as terahertz quantum cascade lasers. By modeling the complex transmission at terahertz frequencies, the electron density and the in-plane momentum scattering time of the active regions and doped contact layers were determined for both GaAs/AlGaAs and InGaAs/InAlAs epilayers. The measured temperature dependence of the electron scattering rate revealed the significance of impurity and LO phonon scattering. The implications for laser operation at room temperature are discussed by considering the changes in absorption and resonant tunneling current with temperature.
©2009 American Institute of Physics
| History: | Received 15 September 2009; accepted 17 September 2009; published 5 November 2009 |
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http://link.aip.org/link/?JAPIAU/106/093104/1 |
KEYWORDS and PACS
PUBLICATION DATA
0021-8979 (print)
1089-7550 (online)
REFERENCES (19)
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- J. Faist, F. Capasso, D. L. Sivco, C. Sirtori, A. L. Hutchinson, and A. Y. Cho,
Science 264, 553 (1994) . - R. Kohler, A. Tredicucci, F. Beltram, H. E. Beere, E. H. Linfield, A. G. Davies, D. A. Ritchie, R. C. Iotti, and F. Rossi,
Nature (London) 417, 156 (2002) . - G. Scalari, C. Walther, M. Fischer, R. Terazzi, H. Beere, D. Ritchie, and J. Faist,
Laser Photonics Rev. 3, 45 (2009) . - M. Giehler, R. Hey, H. Kostial, S. Cronenberg, T. Ohtsuka, L. Schrottke, and H. T. Grahn, Appl. Phys. Lett. 82, 671 (2003).
- H. C. Liu, M. Wachter, D. Ban, Z. R. Wasilewski, M. Buchanan, G. C. Aers, J. C. Cao, S. L. Feng, B. S. Williams, and Q. Hu, Appl. Phys. Lett. 87, 141102 (2005).
- A. Benz, G. Fasching, A. M. Andrews, M. Martl, K. Unterrainer, T. Roch, W. Schrenk, S. Golka, and G. Strasser, Appl. Phys. Lett. 90, 101107 (2007).
- S. Kohen, B. S. Williams, and Q. Hu, J. Appl. Phys. 97, 053106 (2005).
- R. F. Kazarinov and R. A. Suris,
Sov. Phys. Semicond. 5, 707 (1971) . - M. B. Johnston, L. M. Herz, A. L. T. Khan, A. Kohler, A. G. Davies, and E. H. Linfield,
Chem. Phys. Lett. 377, 256 (2003) . - G. Scalari, M. I. Amanti, M. Fischer, R. Terazzi, C. Walther, M. Beck, and J. Faist, Appl. Phys. Lett. 94, 041114 (2009).
- The MQW structure was (from the top of the structure, with layer thicknesses in nanometers): 5.0; 85×(35.
/4.
/20.
/35.0); 35.
; 300. Here, the barrier layers (underlined) are Al0.15Ga0.85As and the wells are GaAs. Doped layers are in bold; the top and bottom contact were silicon-doped at 2×1018 cm−3, while the modulation doping in the 4 nm Al0.15Ga0.85As region was 1×1018 cm−3.
- J. Kroll, J. Darmo, and K. Unterrainer,
Opt. Express 15, 6552 (2007) . - M. Born and E. Wolf, Principles of Optics, 7th ed. (Cambridge University Press, Cambridge, 2007).
- The lifetime of the heavily doped contacts was found to be weakly frequency dependent, reducing by a factor of two across our spectral range. This frequency dependence was included in the data presented here, and will be discussed in a future publication.
- J. Lloyd-Hughes, H. E. Beere, D. A. Ritchie, and M. B. Johnston, Phys. Rev. B 77, 125322 (2008).
- P. Y. Yu and M. Cardona, Fundamentals of Semiconductors, 3rd ed. (Springer, New York, 2003).
- T. Unuma, M. Yoshita, T. Noda, H. Sakaki, and H. Akiyama, J. Appl. Phys. 93, 1586 (2003).
- N. A. Kabir, Y. Yoon, J. R. Knab, J. Y. Chen, A. G. Markelz, J. L. Reno, Y. Sadofyev, S. Johnson, Y. H. Zhang, and J. P. Bird, Appl. Phys. Lett. 89, 132109 (2006).
- C. Sirtori, F. Capasso, J. Faist, A. L. Hutchinson, D. L. Sivco, and A. Y. Cho,
IEEE J. Quantum Electron. 34, 1722 (1998) .







