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The hydrogen anomaly problem in neutron Compton scattering

机译:中子康普顿散射中的氢异常问题

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摘要

Neutron Compton scattering (also called 'deep inelastic scattering of neutrons', DINS) is a method used to study momentum distributions of light atoms in solids and liquids. It has been employed extensively since the start-up of intense pulsed neutron sources about 25 years ago. The information lies primarily in the width and shape of the Compton profile and not in the absolute intensity of the Compton peaks. It was therefore not immediately recognized that the relative intensities of Compton peaks arising from scattering on different isotopes did not always agree with values expected from standard neutron cross-section tables. The discrepancies were particularly large for scattering on protons, a phenomenon that became known as 'the hydrogen anomaly problem'. The present paper is a review of the discovery, experimental tests to prove or disprove the existence of the hydrogen anomaly and discussions concerning its origin. It covers a twenty-year-long history of experimentation, theoretical treatments and discussions. The problem is of fundamental interest, since it involves quantum phenomena on the subfemtosecond time scale, which are not visible in conventional thermal neutron scattering but are important in Compton scattering where neutrons have two orders of magnitude times higher energy. Different H-containing systems show different cross-section deficiencies and when the scattering processes are followed on the femtosecond time scale the cross-section losses disappear on different characteristic time scales for each H-environment. The last section of this review reproduces results from published papers based on quantum interference in scattering on identical particles (proton or deuteron pairs or clusters), which have given a quantitative theoretical explanation both regarding the H-cross-section reduction and its time dependence. Some new explanations are added and the concluding chapter summarizes the conditions for observing the specific quantum phenomena ob
机译:中子康普顿散射(也称为“中子的深非弹性散射”,DINS)是用于研究固体和液体中的光原子的动量分布的方法。自从大约25年前激烈的脉冲中子来源启动以来,它已经广泛使用。这些信息主要位于康普顿概况的宽度和形状,而不是康普顿峰的绝对强度。因此,没有立即认识到,从不同同位素上散射产生的康普顿峰的相对强度并不总是同意预期的标准中子横截面表的价值。差异对于质子散射特别大,这是一种被称为“氢异常问题”的现象。本文是对发现,实验试验的审查,以证明或反驳存在氢异常的存在和讨论。它涵盖了二十年的实验历史,理论治疗和讨论。问题是基本兴趣,因为它涉及子交替秒的量子尺度上的量子现象,这在传统的热中子散射中不可见,但在康普顿散射中很重要,那么中子有两个更高的次数较高的能量。含有不同的H型系统显示出不同的横截面缺陷,并且当散射过程遵循FemtoSecond时间尺度时,横截面损失消失在每个H环境的不同特性时间尺度上。本综述的最后一部分基于量子干扰在相同的颗粒(质子或氘代对或簇)上的量子干扰来再现已发布的纸张的结果,这对其具有关于H形截面减少及其时间依赖性的定量理论解释。增加了一些新的解释,结束章节总结了观察特定量子现象的条件

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