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混合表面活性剂体系合成锆掺杂介孔分子筛

在水热体系中研究了以阳离子表面活性剂为主,阴离子表面活性剂、非离子表面活性剂、中性伯胺等为辅的混合表面活性剂对合成锆掺杂介孔分子筛的影响,考察了水/SiO_2摩尔比、晶化温度、晶化时间及混合表面活性剂/SiO_2摩尔比对所制分子筛结构的影响,对优化条件下合成的样品进行了表征.结果表明,锆掺杂介孔分子筛的最佳合成体系为阴阳离子表面活性剂混合体系,最佳合成配方为水/SiO_2摩尔比58,混合表面活性剂/SiO_2摩尔比0.15,100℃下晶化48h.最佳条件下合成的样品在小角区域有一个明显的衍射峰,表明其具有一定的长程有序性,晶面间距d=9.71nm,平均孔径为5.55nm,壁厚4.16nm,具有三维蠕虫状孔道结构,吸附亚甲基蓝、罗丹明B与甲基橙的混合溶液时,对亚甲基蓝的吸附选择性较好,吸附率达90.24%

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JUNO Sensitivity on Proton Decay p→νˉK+p\to \bar\nu K^+ Searches

The Jiangmen Underground Neutrino Observatory (JUNO) is a large liquid scintillator detector designed to explore many topics in fundamental physics. In this paper, the potential on searching for proton decay in $p\to \bar\nu K^+$ mode with JUNO is investigated.The kaon and its decay particles feature a clear three-fold coincidence signature that results in a high efficiency for identification. Moreover, the excellent energy resolution of JUNO permits to suppress the sizable background caused by other delayed signals. Based on these advantages, the detection efficiency for the proton decay via $p\to \bar\nu K^+$ is 36.9% with a background level of 0.2 events after 10 years of data taking. The estimated sensitivity based on 200 kton-years exposure is $9.6 \times 10^{33}$ years, competitive with the current best limits on the proton lifetime in this channel

JUNO sensitivity on proton decay p → ν K + searches*

The Jiangmen Underground Neutrino Observatory (JUNO) is a large liquid scintillator detector designed to explore many topics in fundamental physics. In this study, the potential of searching for proton decay in the $p\to \bar{\nu} K^+$ mode with JUNO is investigated. The kaon and its decay particles feature a clear three-fold coincidence signature that results in a high efficiency for identification. Moreover, the excellent energy resolution of JUNO permits suppression of the sizable background caused by other delayed signals. Based on these advantages, the detection efficiency for the proton decay via $p\to \bar{\nu} K^+$ is 36.9% ± 4.9% with a background level of $0.2\pm 0.05({\rm syst})\pm$$0.2({\rm stat})$ events after 10 years of data collection. The estimated sensitivity based on 200 kton-years of exposure is $9.6 \times 10^{33}$ years, which is competitive with the current best limits on the proton lifetime in this channel and complements the use of different detection technologies