首页> 外文期刊>Physical review. B, Condensed Matter And Materals Physics >High-temperature electron-hole liquid and dynamics of Fermi excitons in a In_(0.65)Al_(0.35)As/Al_(0.4)Ga_(0.6)As quantum dot array
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High-temperature electron-hole liquid and dynamics of Fermi excitons in a In_(0.65)Al_(0.35)As/Al_(0.4)Ga_(0.6)As quantum dot array

机译:In_(0.65)Al_(0.35)As / Al_(0.4)Ga_(0.6)As量子点阵列中的高温电子空穴液体和费米激子的动力学

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摘要

State-filling effects of the exciton in a In_(0.65)Al_(0.35)As/Al_(0.4)Ga_(0.6)As quantum dot array are observed by quantum dot array photoluminescence at a sample temperature of 77 K. The exciton emission at low excitation density is dominated by the radiative recombination of the states in the s shell and at high excitation density the emission mainly results from the radiative recombination of the exciton state in the p shell. The spectral interval between the states in the s and p shells is about 30-40 meV. The time resolved photoluminescence shows that the decay time of exciton states in the p shell is longer than that of exciton states in the s shell, and the emission intensity of the exciton state in the p shell is superlinearly dependent on excitation density. Furthermore, electron-hole liquid in the quantum dot array is observed at 77 K, which is a much higher temperature than that in bulk. The emission peak of the recombination of electron-hole liquid has an about 200 meV redshift from the exciton fluorescence. Two excitation density-dependent emission peaks at 1.56 and 1.59 eV are observed, respectively, which result from quantum confinement effects in QDs. The emission intensity of electron-hole liquid is directly proportional to the cubic of excitation densities and its decay time decreases significantly at the high excitation density.
机译:在77 K的样品温度下,通过量子点阵列光致发光观察了In_(0.65)Al_(0.35)As / Al_(0.4)Ga_(0.6)As量子点阵列中激子的状态填充效应。低激发密度主要由s壳态的辐射复合引起,高激发密度下的发射主要是p壳内激子态的辐射复合引起的。 s和p壳中的状态之间的光谱间隔约为30-40 meV。时间分辨的光致发光表明,p壳中的激子态的衰变时间比s壳中的激子态的衰变时间长,p壳中的激子态的发射强度与激发密度呈超线性关系。此外,在量子点阵列中观察到的电子空穴液体为77 K,该温度比整体温度高得多。电子-空穴液体复合的发射峰相对于激子荧光具有约200 meV的红移。分别在1.56和1.59 eV处观察到两个依赖于激发密度的发射峰,这是量子点中量子限制效应引起的。电子空穴液体的发射强度与激发密度的三次方成正比,在高激发密度下其衰减时间显着减少。

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