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硅(100)和硅(111)衬底生长的GaAs/AlGaAs核壳纳米线中光生载流子的动力学

Dynamics of Optically-Generated Carriers in Si (100) and Si (111) Substrate-Grown GaAs/AlGaAs Core-Shell Nanowires.

作者信息

Delos Santos Ramon, Ibañes Jasher John, Balgos Maria Herminia, Jaculbia Rafael, Afalla Jessica Pauline, Bailon-Somintac Michelle, Estacio Elmer, Salvador Arnel, Somintac Armando, Que Christopher, Tsuzuki Satoshi, Yamamoto Kohji, Tani Masahiko

机构信息

National Institute of Physics, University of the Philippines, Diliman, Quezon City, Philippines,

出版信息

Nanoscale Res Lett. 2015 Dec;10(1):1050. doi: 10.1186/s11671-015-1050-9. Epub 2015 Aug 21.

Abstract

GaAs/Al0.1Ga0.9As core-shell nanowires (CSNWs), with average lateral size of 125 nm, were grown on gold nanoparticle-activated Si (100) and Si (111) substrates via molecular beam epitaxy. Room temperature-photoluminescence (RT-PL) from the samples showed bulk-like GaAs and Al0.1Ga0.9As bandgap emission peaks at 1.43 and 1.56 eV, respectively. Higher PL emission intensity of the sample on Si (111) compared to that on Si (100) is attributed to uniform Al0.1Ga0.9As shell passivation of surface states on Si (111)-grown CSNWs. Carrier dynamics in two different temporal regimes were studied. In the sub-nanosecond time scale (300-500 ps), time-resolved radiative recombination efficiency of carriers was examined. In the 0-4 ps range, surface field-driven ballistic transport of carriers was probed in terms of the radiated terahertz (THz) waves. Time-resolved PL measurements at 300 K revealed that the carrier recombination lifetime of the GaAs core on Si (100)-grown CSNWs is 333 ps while that on Si (111)-grown sample is 500 ps. Ultrafast photoexcitation of GaAs core on the two samples generated a negligible difference in the intensity and bandwidth of emitted THz radiation. This result is ascribed to the fact that the deposited GaAs material on both substrates produced samples with comparable NW densities and similar GaAs core average diameter of about 75 nm. The samples' difference in GaAs core's carrier recombination lifetime did not influence THz emission since the two processes involve distinct mechanisms. The THz spectrum of CSNWs grown on Si (111) exhibited Fabry-Perot modes that originated from multiple reflections of THz waves within the Si substrate.

摘要

通过分子束外延在金纳米颗粒活化的硅(100)和硅(111)衬底上生长了平均横向尺寸为125纳米的砷化镓/铝0.1镓0.9砷核壳纳米线(CSNWs)。样品的室温光致发光(RT-PL)显示,块状砷化镓和铝0.1镓0.9砷的带隙发射峰分别位于1.43和1.56电子伏特。与在硅(100)上的样品相比,在硅(111)上的样品具有更高的光致发光发射强度,这归因于在硅(111)上生长的CSNWs表面态的铝0.1镓0.9砷壳层均匀钝化。研究了两种不同时间尺度下的载流子动力学。在亚纳秒时间尺度(300 - 500皮秒)内,研究了载流子的时间分辨辐射复合效率。在0 - 4皮秒范围内,根据辐射的太赫兹(THz)波探测了表面场驱动的载流子弹道输运。300K下的时间分辨光致发光测量表明,在硅(100)上生长的CSNWs上砷化镓核的载流子复合寿命为333皮秒,而在硅(111)上生长的样品中为500皮秒。对两个样品上的砷化镓核进行超快光激发,在发射的太赫兹辐射的强度和带宽上产生的差异可忽略不计。这一结果归因于两个衬底上沉积的砷化镓材料产生了具有可比纳米线密度和约75纳米相似砷化镓核平均直径的样品。样品在砷化镓核载流子复合寿命上的差异并未影响太赫兹发射,因为这两个过程涉及不同的机制。在硅(111)上生长的CSNWs的太赫兹光谱表现出法布里 - 珀罗模式,该模式源于太赫兹波在硅衬底内的多次反射。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2bf5/4545763/200de572a9ad/11671_2015_1050_Fig1_HTML.jpg

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