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Molecular beam epitaxy of II‐VI compounds

机译:II连字符;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 mgr;m, and the continuously adjustable refractive index offered by their ternary alloys. Films of waveguide thickness (1/2–2 mgr;m) 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 mgr;m/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 mgr;m/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 byinsituLEED. 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‐mgr;m‐thick films being smooth to tens of angstroms. The following system is recommended for integrated 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化合物因其高电连字符光学系数、从可见光到10&mgr;m以上的宽透明度范围以及三元合金提供的连续可调折射率而成为集成光学器件的理想选择。通过在超高真空下将组成元素(Zn、Cd、Se、Te)从单独的液体&连字符&氮&连字符;笼罩的石墨 Knudsen 细胞蒸发到温度&连字符;受化学机械抛光的单连字符-晶体基板上,在这里生长波导厚度 (1/2–2 &mgr;m) 的薄膜。以一种新的方式使用在生长温度下工作的石英晶体沉积监测仪,通过测量沉积速率作为撞击速率比的函数,确定将产生化学计量薄膜的组&连字符;VI/II冲击速率比。生长膜的解离再蒸发设定了生长温度的上限;计算出在400 °C下,镉和镉的再蒸发速率为470 °C,锌Se的再蒸发速率为570 °C。在相当于约1 &mgr;m/h的撞击速率下,ZnSe在低于该点的125 °C时停止沉积,而其他三种化合物在低于该点的50 °C下停止沉积。在低于沉积停止的50°C范围内,通过原位LEED测定了所有II‐VI化合物的外延。通过Nomarski差分&连字符;干涉&连字符;对比显微镜检查胶片表面形貌。晶体学质量略有不同,表面光滑度很大程度上取决于衬底取向,质量从低到低依次为:(1)GaAs(100);(2)砷化镓(110);(3)CdS(0001)、CdSe(0001)。在砷化镓上,ZnTe和Zn(SeTe)薄膜比ZnSe薄膜光滑得多,1‐&mgr;m‐厚薄膜光滑到几十埃。对于集成光学器件,建议使用以下系统:Zn(SeTe)上的ZnTe波导,用于将波导与高&连字符;折射率基板进行光学隔离,InAs(100)用于0.6%晶格常数失配。

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