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作 者:唐晓萍[1] 纪英露[2] 胡雅洁[1] 吴晓春[2]
机构地区:[1]北京出入境检验检疫局检验检疫技术中心,北京100026 [2]国家纳米科学中心中国科学院纳米标准与检测重点实验室,北京1001901
出 处:《分析试验室》2016年第4期414-417,共4页Chinese Journal of Analysis Laboratory
基 金:北京国检局科技计划课题资金资助项目(2015BK012)资助
摘 要:采用金纳米棒吸收光谱法测定水中Hg(Ⅱ)的浓度。研究表明,金纳米棒比金纳米球具有更高的长波等离激元共振峰(LSPR)位移,不同长径比的金纳米棒对LSPR位移影响不大;当p H<7时,溶液中p H越小LSPR位移越小,当p H>7时,LSPR位移基本不变。LSPR位移在Hg(Ⅱ)浓度为3μmol/L前后表现出两度线性关系,Hg(Ⅱ)浓度大于20μmol/L时金纳米棒与汞完全形成合金,测定Hg(Ⅱ)的检出限为41 nmol/L。The concentration of mercury( II) in water was determined by the optical absorption spectra of gold nanorods. The results showed that the longitudinal plasmon resonance( LSPR) shifts of the gold nanorods were more clear than that of the gold nanospheres and the LSPR shifts were hardly affected by aspect ratio. At the lower p H,the more the LSPR shifted when the p H 〉7,while the LSPR shifts were almost the same when p H〈 7. When the concentration of mercury( II) was near or lower than 3 μmol / L,the LSPR shift was linear with the concentration of mercury( II). When the concentration of mercury( II) was higher than 20 μmol / L,the gold nanorods completely formed amalgam. Only Pb( II) could result in negative interference at the determination of Mercury( II) and the limit of detection was 41 nmol / L.
关 键 词:金纳米棒 Hg(Ⅱ) 吸收光谱法 长波等离激元共振峰
分 类 号:X830.2[环境科学与工程—环境工程]
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