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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 velence C_(10)H_8N_4) around room temperature (RT) (l55 deg 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:通过在紫外线(UV-vis)照射期间在室温(RT)( 155摄氏度)附近维持α-Ag(DM)_2(DM活性C_(10)H_8N_4),一系列名为b的光化学产品获得。固体β由结构上不同的化合物组成。所有的固态β相都具有原始的Ag(DM)_2化学分子式,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beta_2。与α相的XRD图谱相比,β_1相在相同的两个θ角处表现出XRD峰,但相对强度不同,而β_2相则与α相或β_1相表现出完全不同的XRD图谱。 “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β_1和β_2相则被认为是半导体。结果,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,β_1和/或β_2相的混合物。

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