Quantum Effects of Neutron Scattering on Indistinguishable Particles

Q4 Physics and Astronomy
E. Karlsson
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Abstract

A recent paper by Matsumoto et. al [1] revitalizes the discussion of neutron scattering on indistinguishable particles, started in 2000 by Karlsson and Lovesey [2]. In a QENS measurement, Matsumoto et al. showed that the proton entanglement created in scattering on SiH2 (deposited on Si-surfaces) changes the conditions for vibrational excitations of the SiH2 “molecules”; the second scissor mode at 226 meV was strongly reduced compared to the first one at 113 meV. The present note will discuss the selection rules for vibrational excitations when the proton pairs are quantum entangled during scattering, and relate them to the reduced Compton cross-sections for such proton pairs, first discussed theoretically in [2]. It is well known that in the collision of two particles of the same kind, like in electron-electron scattering, their space and spin states become entangled, which leads to interference terms in the cross-section (see Schiff [3], Ch. 6). But the same is valid also for two or more identical particles of any kind which are interacting coherently with a neutron or an X-ray photon in scattering experiments (measurement-induced entanglement). In QNES as well as in Compton scattering, the coherence volume Vcoh = lx × ly × lz contains more than one particle if the energy resolution (determining lz) is high and the detector solid angles (determining lx and ly) are small enough. For the simplest case of only two particles a and b within Vcoh, the initial state of the scattering system can be taken as [[2],
不可区分粒子上中子散射的量子效应
Matsumoto等人[1]最近的一篇论文振兴了Karlsson和Lovesey于2000年开始的关于中子在不可区分粒子上散射的讨论[2]。在QENS测量中,Matsumoto等人表明,在SiH2(沉积在Si表面)上的散射中产生的质子纠缠改变了SiH2“分子”振动激发的条件;226meV的第二剪式模式与113meV的第一剪式模式相比显著降低。本注释将讨论当质子对在散射过程中量子纠缠时振动激发的选择规则,并将其与[2]中首次从理论上讨论的这种质子对的简化康普顿截面联系起来。众所周知,在两个同类粒子的碰撞中,就像在电子-电子散射中一样,它们的空间和自旋态会纠缠在一起,这会导致横截面中的干涉项(见Schiff[3],第6章)。但这同样适用于散射实验中与中子或X射线光子相干相互作用的两个或多个任何类型的相同粒子(测量诱导纠缠)。在QNES和康普顿散射中,如果能量分辨率(确定lz)高并且探测器立体角(确定lx和ly)足够小,相干体积Vcoh=lx×ly×lz包含一个以上的粒子。对于Vcoh内只有两个粒子a和b的最简单情况,散射系统的初始状态可以取为[[2],
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
Neutron News
Neutron News Physics and Astronomy-Nuclear and High Energy Physics
CiteScore
0.30
自引率
0.00%
发文量
36
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