首页> 外文期刊>Journal of Vacuum Science & Technology. B, Microelectronics and Nanometer Structure >Recombination dynamics of localized excitons in cubic In_xGa_(1-x)N/GaN multiple quantum wells grown by radio frequency molecular beam epitaxy on 3C-SiC substrate
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Recombination dynamics of localized excitons in cubic In_xGa_(1-x)N/GaN multiple quantum wells grown by radio frequency molecular beam epitaxy on 3C-SiC substrate

机译:射频分子束外延在3C-SiC衬底上生长的立方In_xGa_(1-x)N / GaN多量子阱中局部激子的复合动力学

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Recombination dynamics of localized excitons in strained cubic (c-)In_xGa_(1-x)N/GaN multiple quantum wells (MQWs) grown on 3C-SiC (001) were summarized in terms of well thickness L, InN molar fraction x, and temperature T. Photoluminescence (PL) peak energy of c-In_(0.1)Ga_(0.9)N/GaN MQWs showed a moderate blueshift as L decreased, and the low-temperature PL lifetime did not change remarkably by changing L. These results proved that the quantum-confined Stark effect due either to spontaneous or piezoelectric polarization was inactive in cubic polytypes. Consequently, time-resolved PL (TRPL) data of c-InGaN MQWs reflect the intrinsic exciton dynamics. The TRPL signal showed stretched exponential decay and spectral redshift with time after excitation up to 300 K. The results are fingerprints that the spontaneous emission is due to the radiative recombination of excitons localized in disordered quantum nanostructures forming extended and localized states. Effective localization depth increased with the increase in x, which gave rise to fast exciton localization. However, nonradiative lifetime in the free or extended states decreased more rapidly with the increase in x and T, giving the emission efficiency maximum at particular x around 0.1.
机译:总结了生长在3C-SiC(001)上的应变立方(c-)In_xGa_(1-x)N / GaN多量子阱(MQWs)中的局部激子的重组动力学,包括阱厚度L,InN摩尔分数x和c-In_(0.1)Ga_(0.9)N / GaN MQW的光致发光(PL)峰值能量随着L的降低显示出适度的蓝移,并且通过改变L,低温PL寿命没有显着改变。这些结果证明了认为由于自发极化或压电极化引起的量子限制斯塔克效应在立方多型体中是无效的。因此,c-InGaN MQW的时间分辨PL(TRPL)数据反映了本征激子动力学。 TRPL信号在激发到300 K之后显示出随时间变化的拉伸指数衰减和光谱红移。结果是指纹图谱,表明自发发射是由于激子在局部无序形成的量子态纳米结构中的辐射复合而形成的。有效定位深度随x的增加而增加,这导致快速激子定位。然而,随着x和T的增加,自由或扩展状态下的非辐射寿命下降得更快,特定的x处的发射效率最大值约为0.1。

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