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首页> 外文期刊>Journal of Physics, D. Applied Physics: A Europhysics Journal >Effect of free-carrier concentration and optical injection on carrier lifetimes in undoped and iodine doped CdMgTe/CdSeTe double heterostructures grown by molecular beam epitaxy
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Effect of free-carrier concentration and optical injection on carrier lifetimes in undoped and iodine doped CdMgTe/CdSeTe double heterostructures grown by molecular beam epitaxy

机译:自由载体浓度和光学喷射对未掺杂和碘掺杂CDMGTE / CDSete双重异质结构的载体寿命的影响

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摘要

Time-resolved and time integrated photoluminescence (PL) studies are reported for undoped and doped CdMgTe/CdSeTe double heterostructures (DHs) grown by molecular beam epitaxy. Undoped DHs are studied with absorber layer thickness varying from 0.5 to 2.5 mu m. The n-type free-carrier concentration is varied similar to 7 x 10(15), 8.4 x 10(16), and 8.4 x 10(17) cm(-3) using iodine as a dopant in different absorber layer thicknesses (0.25-2.0 mu m). Optical injection is varied from 1 x 10(10) to 3 x 10(11) photons/pulse/cm(2), corresponding to the initial injection of photo-carriers up to similar to 8 x 10(15) cm(-3), to examine the effects of excess carrier concentration on the PL lifetimes. Undoped DHs exhibit an initial rapid decay followed by a slower dependence with carrier lifetimes up to similar to 485 ns. The dependence of carrier lifetimes on the thickness of the absorber layers (0.5-2.5 mu m) suggests interface recombination velocities (v(int)) similar to 1288 and 238 cm s(-1) in the initial and later decay times, respectively, corresponding to high and low photo-carrier concentrations. The Shockley-Read-Hall model is used to describe the results in which variations are observed in v(int) for undoped DHs. The lifetimes of doped DHs show a consistent trend with thickness. The v(int) similar to 80-200 cm s(-1) is estimated for doping n similar to 7 x 10(15) cm(-3) and 240-410 cm s(-1) for n similar to 8.4 x 10(16) cm(-3). The observed decrease in carrier lifetimes with increasing n is consistent with growing importance of the radiative recombination rate due to the excess carrier concentration. The effect of carrier concentration on the PL spectrum is also discussed.
机译:报告时间分辨和时间集成光致发光(PL)研究对于由分子束外延生长的未掺杂和掺杂的CDMGTE / CDSETE双异质结构(DHS)。使用0.5至2.5μm的吸收层厚度研究了未掺杂的DHS。使用碘在不同吸收层厚度的掺杂剂(0.25,类似于7×10(15),8.4×10(16)和8.4×10(17 )cm(-3)的N型自由载体浓度(0.25 -2.0 mu m)。光学喷射在1×10(10)至3×10(11)光子/脉冲/ cm(2)中,对应于初始喷射光载体的初始喷射至8×10(15)cm(-3 ),检查过量载体浓度对PL寿命的影响。未掺杂的DHS展示初始快速衰减,然后与载体寿命较慢依赖于相似的速度与485ns相似。载体寿命在吸收层(0.5-2.5μm)的厚度上的依赖性表明,在初始和后面的衰减时间中,近似衰减时的界面重组速度(V(int))显然,对应于高和低光载体浓度。 Shockley-Read-Hall模型用于描述在V(INT)中观察到未掺杂的DHS的结果。掺杂DHS的寿命显示厚度一致的趋势。类似于80-200cm S(-1)的v(int)估计类似于7×10(15)cm(-3)和240-410cm s(-1)的掺杂n,而n类似于8.4 x 10(16)厘米(-3)。随着增加的载体寿命的观察到的载体寿命的降低与由于过量的载体浓度导致辐射重组率的重要性。还讨论了载流子浓度对PL光谱的影响。

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