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183W nuclear dipole moment determined by gas-phase NMR spectroscopy
Chemical Physics ( IF 2.3 ) Pub Date : 2017-10-10 , DOI: 10.1016/j.chemphys.2017.10.003
Piotr Garbacz , Włodzimierz Makulski

The magnetic dipole moment of the tungsten-183 nucleus, µ(183W), is determined from measurements of gas-phase 183W nuclear magnetic resonance of tungsten hexafluoride dissolved in CF4. The tungsten-183 resonance frequency combined with recently reported computations of the magnetic shielding of the 183W nucleus in WF6 [K. Ruud, T. B. Demissie, M. Jaszuński, J. Chem. Phys., 140 (2014) 194308] yields μ(183W) = 0.116953(18) μN. Moreover, it is found that the gas-to-liquid shifts of nuclear shielding for WF6 are ΔσGL(19F) = -6.9 ppm and ΔσGL(183W) = -18.4 ppm. The spin-spin coupling 1J(183W,19F) is 43.75(24) Hz for liquid WF6.

中文翻译:

气相NMR光谱法测定183 W核偶极矩

钨183原子核的磁偶极矩μ(183 W)由溶解在CF 4中的六氟化钨的气相183 W核磁共振测量确定。钨183共振频率与最近报道的WF 6中183 W核磁屏蔽的计算[K. Ruud,TB Demissie,M。Jaszuński,J。Chem。物理 ,140(2014)194308]的产率μ(183 W)= 0.116953(18)μ Ñ。此外,据发现,核屏蔽的对WF的气体-液体转变6是Δσ GL19 F)= -6.9 ppm的和Δσ GL183 W)= -18.4 ppm。对于液体WF 6,自旋-自旋耦合器1 J183 W,19 F)为43.75(24)Hz 。
更新日期:2017-10-10
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