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Mechanism of spatially resolved photochemical control of the resistivity of a molecular crystalline solid

机译:空间分辨光化学控制分子晶体固体电阻率的机理

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摘要

By maintaining alpha-Ag(DM)(2) (DM = C10H8N4) around room temperature (RT) ( 155 degrees C) during ultraviolet-visible (UV-vis) irradiation, a series of photochemical products named beta was obtained. The solid beta was comprised of structurally different compounds. All of the solid beta phases share the original chemical formula of Ag(DM)(2) and exhibit semiconducting behaviour, yet they differ from each other in their XRD patterns. They are divided into two phases: beta 1 and beta 2. Compared with the XRD pattern of the alpha phase, the beta 1 phase exhibited XRD peaks at the same 2 theta-angles but with different relative intensities, while the beta 2 phase exhibited totally different XRD patterns from those of the alpha or beta 1 phases. The actual composition of a particular solid of 'beta' phase is dependent upon irradiation time, and can be controlled continuously. Around RT, the alpha phase exhibits metallic conductivity, while the beta 1 and beta 2 phases are suggested to be semiconductors. As a result, one can continuously and finely control the electrical resistivity of Ag(DM)(2) by UV irradiation to modify it into a mixture of alpha, beta 1 and/or beta 2 phases.
机译:通过在紫外可见(UV-vis)辐照期间将α-Ag(DM)(2)(DM = C10H8N4)维持在室温(RT)( 155摄氏度)附近,可以获得一系列名为β的光化学产物。固体β由结构上不同的化合物组成。所有固态β相均具有Ag(DM)(2)的原始化学式,并表现出半导体性能,但它们的XRD图谱彼此不同。它们分为两个阶段:beta 1和beta2。与alpha阶段的XRD图案相比,beta 1阶段在相同的2个θ角处显示了XRD峰,但相对强度不同,而beta 2阶段则显示了全部与α或β1相的XRD模式不同。 “β”相特定固体的实际组成取决于照射时间,并且可以连续控制。在室温附近,α相表现出金属导电性,而β1和β2相被认为是半导体。结果,人们可以通过紫外线照射连续而精细地控制Ag(DM)(2)的电阻率,以将其改性为α,β1和/或β2相的混合物。

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