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The Physics of Spallation Processes

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Chapter 2Research with NeutronsA neutron is an uncharged (electrically neutral) subatomic particle with mass 1,839 timesthat <strong>of</strong> the electron. Neutrons are stable when bound in an atomic nucleus, whilst havinga mean lifetime <strong>of</strong> approximately 900 seconds as a free particle, decaying through the weakinteraction into a proton, an electron, and an antineutrino. <strong>The</strong> neutron (like the proton)is the ground state <strong>of</strong> a three-quark system and consists <strong>of</strong> one “up” and two “down”quarks with spin 1/2 and baryon number 1. QCD allows the calculation <strong>of</strong> particle massesand magnetic moments; predictions, 939 MeV and -1.86 nuclear magneton, compare wellwith measured values, 939.6 MeV and -1.913 nuclear magneton. <strong>The</strong> neutron and theproton form nearly the entire mass <strong>of</strong> atomic nuclei, so they are both called nucleons.<strong>The</strong>y interact through the nuclear, weak, electromagnetic and gravitational forces.At the end <strong>of</strong> the second World War researchers in the USA gained access to the largeneutron fluxes that even relatively modest nuclear reactors were capable <strong>of</strong> delivering.For more than a decade (Nobel Prize in physics to Sir James Chadwick in 1935 for theneutron discovery in 1932) neutrons had then been known as building blocks in the atomicnucleus. Enrico Fermi showed in 1942 that neutrons from fission <strong>of</strong> the uranium nucleuscould support a controlled chain reaction. He had earlier made the important discoverythat slowed-down or thermal neutrons show a much greater inclination to react than fastones do (Nobel Prize for this discovery, among others, to Fermi in 1938). <strong>The</strong> specialproperties <strong>of</strong> these slow neutrons make them suitable for detecting the positions andmovements <strong>of</strong> atoms. Even before the entry <strong>of</strong> the nuclear reactors into the researcharena, results <strong>of</strong> using simple neutron sources had indicated that neutron beams could beused for studying solid bodies and liquids (condensed matter). However, there were manydifficulties to overcome before these possibilities could be realized. <strong>The</strong> 1994 Nobel Prizein <strong>Physics</strong> was awarded to Bertram Brockhouse and Clifford Shull for their pioneeringcontributions to the development <strong>of</strong> neutron scattering techniques (neutron diffractionand neutron spectroscopy) for studies <strong>of</strong> condensed matter. In simple terms, they helpedanswer the questions <strong>of</strong> where atoms ”are” and <strong>of</strong> what atoms ”do”.Neutrons are an ideal probe for investigation <strong>of</strong> the structural and dynamical properties<strong>of</strong> matter. <strong>The</strong>ir electrical neutrality enables them to penetrate deep into matter anddue to the low energy the matter can be studied without being destroyed. <strong>The</strong> magneticmoment enables neutrons to explore microscopic magnetic structures and study magneticfluctuations. <strong>The</strong> energies <strong>of</strong> thermal neutrons are similar to the energies <strong>of</strong> elementaryexcitations in solids and consequently molecular vibrations, lattice modes and the dynamics<strong>of</strong> atomic motions can be probed. Very much the same is true for the wavelengths <strong>of</strong>5

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