1999
DOI: 10.1088/0268-1242/14/10/311
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Enhanced drift velocity of photoelectrons in a semiconductor with ultrafast carrier recombination

Abstract: It is shown by Monte Carlo simulations that the electron velocity overshoot phenomenon in the transient response causes a significant enhancement of the steady-state electron drift velocity in semiconductors in which the electron recombination time is of the same order as the time of the electron transient response. The effect can take place in GaAs layers grown by molecular beam epitaxy at low temperatures.

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Cited by 16 publications
(13 citation statements)
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“…This value is consistent with the slope of the linear portion of transient drift velocity curve obtained from MonteCarlo calculations [18]. The corresponding effective mass for holes is m h = 0.106m 0 .…”
supporting
confidence: 87%
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“…This value is consistent with the slope of the linear portion of transient drift velocity curve obtained from MonteCarlo calculations [18]. The corresponding effective mass for holes is m h = 0.106m 0 .…”
supporting
confidence: 87%
“…When coupled with velocity overshoot phenomenon reported in many photoconductor materials [12,16,17,18,19,20], t tr of majority of carriers is reduced to < 1 ps, i.e., t tr ≤ f −1 . For efficient use of SPPs, it is desirable to have thin (∼10 nm) normal metal lines with subwavelength features distributed throughout the active volume (Fig 1a) in a manner that would collectively enhance the optical field intensity in the vicinity of the metal lines.…”
mentioning
confidence: 93%
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“…This effect of electron velocity overshoot [32] is the additional proof of fast electron trapping by QDs. Structures with fewer QD layers would saturate at lower PCA biases, due to the correspondingly lower number of dots and capture sites.…”
Section: Thz Generation In Qd Based Devicesmentioning
confidence: 84%
“…At such short times, the transport of non-thermalized carriers might be expected 8 , 29 due to considerable contribution of the light holes with a large non-degenerate diffusion coefficient. Moreover, ballistic-like spreading of short-living holes dragged by more mobile electrons might be also important for the enhancement of the effective hole diffusion coefficient within the initial few picoseconds after short-pulse excitation, similar to the phenomenon causing the velocity overshoot in low-temperature GaAs 30 .…”
Section: Resultsmentioning
confidence: 99%