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Exploiting charge-transfer complexation for selective measurement of gas-phase olefins with nanoparticle-coated chemiresistors

机译:利用电荷转移络合物选择性测量带有纳米颗粒涂层化学电阻的气相烯烃

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Charge-transfer-mediated olefin-selective sensing by use of chemiresistors (CR) coated with composite films of n-octanethiolate-monolayer-protected gold nanoparticles (C8-MPN) and each of several square-planar PtCl2(olefin)(pyridine) coordination complexes is described. Where the gas-phase olefin analyte differs from that initially coordinated to Pt, olefin substitution occurs and is accompanied by a persistent shift in the composite film resistance. Commensurate changes in film mass are also observed with a similarly coated thickness shear mode resonator. Regeneration is possible by exposure to the initially complexed olefin gas or vapor. If the olefin analyte is the same as that initially coordinated to Pt, then a reversible charge-transfer interaction occurs that is accompanied by a decrease in film resistance (increase in film mass), which recovers spontaneously after removal of the olefin from the atmosphere above the sensor. This behavior differs from that of MPN-coated CRs lacking such Pt complexes, which invariably yield resistance increases upon exposure to nonpolar vapors. Red shifts in the UV-vis absorbance spectra of the PtCl2(olefin)(pyridine) complexes in solution upon addition of free olefin support the hypothesis that Pt-olefin coordination in the composite films creates temporary low-resistance pathways that compete effectively with the concurrent increase in tunneling resistance associated with swelling-induced separation of C8-MPN cores. Structurally analogous non-olefins produce only increases in film resistance. Selective measurement of styrene, ethylene, 1-octene, and 1,3-butadiene is illustrated. Olefin detection limits are reduced as much as 23 000-fold by inclusion of the corresponding Pt complex in the CR interface film. Composite films suffer a gradual loss of selectivity from decomposition of the Pt-olefin complex, apparently facilitated by a Au-Pt charge transfer.
机译:描述了使用涂有正辛硫代单层保护金纳米颗粒(C8-MPN)复合膜的化学电阻器(CR)和几种方形平面PtCl2(烯烃)(吡啶)配位配合物中的每一种的化学电阻器(CR)进行电荷转移介导的烯烃选择性传感。当气相烯烃分析物与最初配位于Pt的分析物不同时,就会发生烯烃取代,并伴随着复合膜电阻的持续变化。使用类似涂层的厚度剪切模式谐振器也可以观察到薄膜质量的相应变化。通过暴露于最初络合的烯烃气体或蒸气中可以再生。如果烯烃分析物与最初配位于Pt的分析物相同,则发生可逆的电荷转移相互作用,伴随着薄膜电阻的降低(薄膜质量的增加),在从传感器上方的大气中去除烯烃后,烯烃会自发恢复。这种行为与缺乏这种 Pt 配合物的 MPN 包被的 CR 不同,后者在暴露于非极性蒸气时总是会产生阻力增加。加入游离烯烃后,溶液中PtCl2(烯烃)(吡啶)配合物的紫外-可见光吸光度光谱的红移支持了以下假设:复合薄膜中的Pt-烯烃配位产生了暂时的低电阻途径,该途径与与溶胀诱导的C8-MPN核心分离相关的隧穿阻力同时增加有效竞争。结构相似的非烯烃只会增加薄膜电阻。图示了苯乙烯、乙烯、1-辛烯和1,3-丁二烯的选择性测量。通过在CR界面膜中加入相应的Pt复合物,烯烃的检测限降低了23 000倍。复合薄膜因 Pt-烯烃配合物的分解而逐渐失去选择性,这显然是由 Au-Pt 电荷转移促进的。

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