首页 | 本学科首页   官方微博 | 高级检索  
     


Nuclear spin relaxation in beryllium metal
Affiliation:1. Department of Integrative Medicine, Zhongshan Hospital, and Laboratory of Neurology, Institute of Integrative Medicine, Fudan University, Shanghai 200032, China;2. Department of Diagnostic Radiology, Xiehe Hospital, Fujian Medical University, Fujian 350001, China;1. Department of Physics and Astronomy, University of Bologna, Italy;2. Centro Fermi-Museo Storico della Fisica e Centro Studi e Ricerche “Enrico Fermi”, Roma, Italy;3. Department DICAM, University of Bologna, Italy;4. MacDiarmid Institute for Advanced Materials and Nanotechnology, School of Chemical and Physical Sciences, Victoria University of Wellington, New Zealand;1. Department of Chemistry, Columbia University, New York, NY 10027, United States;2. New York Structural Biology Center, New York, NY 10027, United States;1. Institute of Molecular Physics, Polish Academy of Sciences, M. Smoluchowskiego 17, 60-179 Poznan, Poland;2. Faculty of Chemical Technology, Poznan University of Technology, Berdychowo 4, 60-965 Poznan, Poland
Abstract:The quadrupole-split NMR spectrum of Be9 nuclei (I = 32 role=presentation style=font-size: 90%; display: inline-block; position: relative;>32) in pure Be metal has been studied by pulse methods. The free induction decay (FID) is modulated: the frequency of modulation gives a new measurement of the quadrupole coupling constant e2qQh= 57 ± 1 kHz role=presentation style=font-size: 90%; display: inline-block; position: relative;>e2qQh= 57 ± 1 kHz. Analysis of the FID shows also that the central line and satellites are non-gaussian. Their second moments agree with the dipolar values in an annealed sample. If the sample is not annealed the satellites are broadened. The width of the distribution of the electric field gradient has been deduced. The spin echo envelope is also modulated. Previous calculations of echoes in quadrupole-split systems are verified for this particular case.Spin lattice relaxation time T1, measurements show that T1T is constant from 1.5 to 300°K. The value of this constant depends of the state of annealing of the sample. This observation shows that the electronic structure of Be is very sensitive to slight changes of the crystal structure. After a long anneal T1T= (1·85 ±0·10) × 104sec °K.
Keywords:
本文献已被 ScienceDirect 等数据库收录!
设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号