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Molecular beam epitaxy of II‐VI compounds

机译:II-VI化合物的分子束外延

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The II‐VI compounds are desirable for integrated optics due to their high electro‐optic coefficients, wide transparency range from the visible to beyond 10 μm, and the continuously adjustable refractive index offered by their ternary alloys. Films of waveguide thickness (1/2–2 μm) were grown here by evaporation, under ultrahigh vacuum, of the constituent elements (Zn, Cd, Se, Te) from separately liquid‐nitrogen‐shrouded graphite Knudsen cells onto temperature‐controlled chemomechanically polished single‐crystal substrates. A quartz‐crystal deposition monitor operating at the growth temperature was used in a novel way to determine the group‐VI/II impingement rate ratio which would produce stoichiometric films, by measuring deposition rate as a function of the impingement rate ratio. Dissociative reevaporation of growing films sets an upper limit to growth temperature; 1 μm/h reevaporation rates were calculated to be reached at 400 °C for CdTe, 470 °C for ZnTe and CdSe, and 570 °C for ZnSe. At impingement rates corresponding to about 1 μm/h, ZnSe ceased to deposit at 125 °C below that point and the other three compounds at 50 °C below that point. Over a 50 °C range below the cessation of deposition, epitaxy was obtained for all II‐VI compounds, as determined by in situ LEED. Film surface topography was examined by Nomarski differential‐interference‐contrast microscopy. Crystallographic quality depended slightly and surface smoothness depended very strongly on substrate orientation in the following decreasing order of quality: (1) GaAs(100); (2) GaAs(110); (3) CdS(0001), CdSe(0001). On GaAs, ZnTe and Zn(SeTe) films were much smoother than ZnSe films, 1‐μm‐thick films being smooth to tens of angstroms. The following system is recommended for i-nntegrated optics: ZnTe waveguide on Zn(SeTe) to optically isolate the waveguide from the high‐index substrate, InAs(100) for 0.6% lattice constant mismatch.
机译:II-VI化合物因其高电光系数,从可见光到超过10μm的宽透明度范围以及其三元合金提供的可连续调节的折射率而非常适合集成光学。在超高真空下,通过将液氮包裹的石墨Knudsen细胞中的组成元素(Zn,Cd,Se,Te)蒸发(在超高真空下),在化学控制下进行化学控制,从而生长出波导厚度(1 / 2–2μm)的薄膜抛光的单晶衬底。通过以一种新的方式使用在生长温度下运行的石英晶体沉积监测器,通过测量沉积速率与碰撞速率比的函数,来确定将产生化学计量膜的VI / II组碰撞速率比。生长膜的解离性再蒸发为生长温度设定了上限;计算得出,CdTe在400 C,ZnTe和CdSe在470 C,ZnSe在570 C达到1μm/ h的再蒸发速率。在相当于约1μm/ h的撞击速率下,ZnSe在低于该点的125 C处停止沉积,而其他三种化合物在低于该点的50 C处停止沉积。在低于停止沉积的50 C范围内,所有II-VI化合物均获得了外延,这是通过原位LEED确定的。膜表面形貌通过Nomarski微分干涉对比显微镜检查。晶体学质量略有变化,表面光滑度在很大程度上取决于衬底的取向,其质量降序如下:(1)GaAs(100); (2)砷化镓(110); (3)CdS(0001),CdSe(0001)。在GaAs上,ZnTe和Zn(SeTe)薄膜比ZnSe薄膜光滑得多,厚度为1 µm的薄膜光滑到几十埃。对于i集成光学器件,建议使用以下系统:Zn(SeTe)上的ZnTe波导可将波导与高折射率衬底InAs(100)光学隔离,以实现0.6%的晶格常数失配。

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    《Journal of Applied Physics 》 |1975年第6期| P.2366-2374| 共9页
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  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
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