Editing Neutron scattering

{{Short description|Physical phenomenon}}
{{More citations needed|date=November 2019}}
{{Use American English|date = April 2019}}
{{Use mdy dates|date = April 2019}}
{{Science with neutrons}}

'''Neutron scattering''', the irregular dispersal of free [[neutron]]s by matter, can refer to either the naturally occurring physical process itself or to the man-made experimental techniques that use the natural process for investigating materials. The natural/physical phenomenon is of elemental importance in [[nuclear engineering]] and the nuclear sciences. Regarding the experimental technique, understanding and manipulating neutron scattering is fundamental to the applications used in [[crystallography]], [[physics]], [[physical chemistry]], [[biophysics]], and [[materials research]].

Neutron scattering is practiced at [[research reactor]]s and [[spallation]] neutron sources that provide [[neutron radiation]] of varying [[neutron flux|intensities]]. [[Neutron diffraction]] ([[elastic scattering]]) techniques are used for analyzing structures; where '''inelastic neutron scattering''' is used in studying atomic [[phonon|vibration]]s and other [[excited state|excitations]].

== Scattering of fast neutrons ==
{{See also|Neutron temperature|neutron moderator}}

"Fast neutrons" (see [[neutron temperature]]) have a kinetic energy above 1&nbsp;[[Electronvolt|MeV]]. They can be scattered by condensed matter—nuclei having kinetic energies far below 1&nbsp;eV—as a valid experimental approximation of an [[elastic collision]] with a particle at rest. With each collision, the fast neutron transfers a significant part of its kinetic energy to the scattering nucleus (condensed matter), the more so the lighter the nucleus. And with each collision, the "fast" neutron is slowed  until it reaches thermal equilibrium with the material in which it is scattered.

[[Neutron moderator]]s are used to produce [[thermal neutrons]], which have kinetic energies below 1&nbsp;eV (T < 500K).<ref name=ibach>
{{cite book
|last=Lüth
|first=Harald Ibach, Hans
|title=Solid-state physics : an introduction to principles of materials science
|year=2009
|publisher=Springer
|location=Berlin
|isbn=978-3-540-93803-3
|edition=4th extensively updated and enlarged
}}
</ref> Thermal neutrons are used to maintain a nuclear chain reaction in a [[nuclear reactor]], and as a research tool in neutron scattering experiments and other applications of neutron science (see below). The remainder of this article concentrates on the scattering of thermal neutrons.

== Neutron-matter interaction ==
Because neutrons are electrically neutral, they penetrate more deeply into matter than electrically charged particles of comparable kinetic energy, and thus are valuable as probes of bulk properties.

Neutrons interact with atomic nuclei and with magnetic fields from unpaired electrons, causing pronounced [[Interference (wave propagation)|interference]] and [[energy transfer]] effects in neutron scattering experiments. Unlike an [[x-ray]] [[photon]] with a similar wavelength, which interacts with the [[electron cloud]] surrounding the [[atomic nucleus|nucleus]], neutrons interact primarily with the nucleus itself, as described by [[Fermi's pseudopotential]]. Neutron scattering and absorption [[Neutron cross-section|cross section]]s vary widely from [[isotope]] to isotope.

Neutron scattering can be incoherent or coherent, also depending on isotope. Among all isotopes, hydrogen has the highest scattering cross section. Important elements like carbon and oxygen are quite visible in neutron scattering—this is in marked contrast to [[X-ray scattering]] where cross sections systematically increase with atomic number. Thus neutrons can be used to analyze materials with low atomic numbers, including proteins and surfactants. This can be done at synchrotron sources but very high intensities are needed, which may cause the structures to change. The nucleus provides a very short range, as isotropic potential varies randomly from isotope to isotope, which makes it possible to tune the (scattering) contrast to suit the experiment.

Scattering almost always presents both elastic and inelastic components. The fraction of elastic scattering is determined by the [[Debye-Waller factor]] or the [[Mössbauer-Lamb factor]]. Depending on the research question, most measurements concentrate on either elastic or inelastic scattering.

Achieving a precise velocity, i.e. a precise energy and [[de Broglie wavelength]], of a neutron beam is important. Such single-energy beams are termed 'monochromatic', and monochromaticity is achieved either with a crystal monochromator or with a [[time of flight|time of flight (TOF)]] [[spectrometer]]. In the time-of-flight technique, neutrons are sent through a sequence of two rotating slits such that only neutrons of a particular velocity are selected. Spallation sources have been developed that can create a rapid pulse of neutrons. The pulse contains neutrons of many different velocities or de Broglie wavelengths, but separate velocities of the scattered neutrons can be determined ''afterwards'' by measuring the time of flight of the neutrons between the sample and neutron detector.

=== Magnetic scattering ===

The neutron has a net electric charge of zero, but has a significant [[Nucleon magnetic moment|magnetic moment]], although only about 0.1% of that of the [[electron]]. Nevertheless, it is large enough to scatter from local magnetic fields inside condensed matter, providing a weakly interacting and hence penetrating probe of ordered magnetic structures and electron spin fluctuations.<ref name="Zaliznyak">{{Citation|last1=Zaliznyak|first1=Igor A.|title=Magnetic Neutron Scattering|date=2004|url=https://inis.iaea.org/search/search.aspx?orig_q=RN:36002750|last2=Lee|first2=Seung-Hun}}</ref>

==Inelastic neutron scattering==
[[Image:inelastic-neutron-scattering-basics.png|thumb|300px|Generic layout of an inelastic neutron scattering experiment]]
[[File:Inelastic Neutron Scattering.webm|thumb|Inelastic Neutron Scattering]]
'''Inelastic neutron scattering''' is an experimental technique commonly used in [[condensed matter physics|condensed matter research]] to study atomic and molecular motion as well as magnetic and crystal field excitations.<ref>G L Squires ''Introduction to the Theory of Thermal Neutron Scattering'' Dover 1997 (reprint?)</ref><ref name=PhD-474621>{{cite thesis|degree=DPhil|publisher=University of Oxford|url=http://solo.bodleian.ox.ac.uk/permalink/f/89vilt/oxfaleph019872832|authorlink=Andrew D. Taylor|title=Inelastic Neutron Scattering by Chemical Rate Processes|first= Andrew Dawson|last=Taylor|date=1976|id={{EThOS|uk.bl.ethos.474621}}|website=ox.ac.uk|oclc=500576530}}</ref> It distinguishes itself from other neutron scattering techniques by resolving the change in kinetic energy that occurs when the collision between neutrons and the sample is an inelastic one. Results are generally communicated as the [[dynamic structure factor]] (also called inelastic scattering law) <math>S(\mathbf{Q},\omega)</math>, sometimes also as the dynamic susceptibility <math> \chi^{\prime \prime}(\mathbf{Q},\omega)</math> where the scattering vector <math>\mathbf{Q}</math> is the difference between incoming and outgoing [[wave vector]], and ''<math>\hbar \omega</math>'' is the energy change experienced by the sample (negative that of the scattered neutron). When results are plotted as function of <math>\omega</math>, they can often be interpreted in the same way as spectra obtained by conventional [[spectroscopy|spectroscopic]] techniques; insofar as inelastic neutron scattering can be seen as a special spectroscopy.

Inelastic scattering experiments normally require a [[monochromatization]] of the incident or outgoing beam and an energy analysis of the scattered neutrons. This can be done either through time-of-flight techniques ([[neutron time-of-flight scattering]]) or through [[Bragg reflection]] from single crystals ([[neutron triple-axis spectroscopy]], [[neutron backscattering]]). Monochromatization is not needed in echo techniques ([[neutron spin echo]], [[neutron resonance spin echo]]), which use the quantum mechanical [[phase (waves)|phase]] of the neutrons in addition to their amplitudes.{{cn|date=February 2019}}

== History ==
The first neutron diffraction experiments were performed in the 1930s.<ref name = "ibach"/> However it was not until around 1945, with the advent of nuclear reactors, that high [[neutron flux]]es became possible, leading to the possibility of in-depth structure investigations. The first neutron-scattering instruments were installed in beam tubes at multi-purpose research reactors. In the 1960s, high-flux reactors were built that were optimized for beam-tube experiments. The development culminated in the high-flux reactor of the [[Institut Laue-Langevin]] (in operation since 1972) that achieved the highest neutron flux to this date. Besides a few high-flux sources, there were some twenty medium-flux reactor sources at  universities and other research institutes. Starting in the 1980s, many of these medium-flux sources were shut down, and research concentrated at a few world-leading high-flux sources.

== Facilities ==
{{Main|Neutron facilities}}

Today, most neutron scattering experiments are performed by research scientists who apply for beamtime at neutron sources through a formal proposal procedure. Because of the low count rates involved in neutron scattering experiments, relatively long periods of beam time (on the order of days) are usually required for usable data sets. Proposals are assessed for feasibility and scientific interest.<ref>{{cite web |title=How To Submit a Proposal |url=https://neutrons.ornl.gov/users/how-submit-proposal |website=Neutron Sciences at ORNL |publisher=Oak Ridge National Laboratory |access-date=12 May 2022}}</ref>

== Techniques ==
*[[Neutron diffraction]]
**[[Small angle neutron scattering]]
**[[Spin Echo Small angle neutron scattering]]
**[[Neutron reflectometry]]
*'''[[Neutron diffraction|Inelastic neutron scattering]]'''
**[[Neutron triple-axis spectrometry]]
**[[Neutron time-of-flight scattering]]
**[[Neutron backscattering]]
**[[Neutron spin echo]]

==See also==
*[[Neutron transport]]
*[[LARMOR neutron microscope]]
*[[Born approximation]]

== References ==
{{reflist}}

==External links==
* {{usurped|1=[https://web.archive.org/web/20160310202102/https://www.e-neutrons.org/ Free, EU-sponsored e-learning resource for neutron scattering]}}
* [http://www.iop.org/publications/iop/2011/page_47521.html Neutron scattering - a case study]
* [http://knocknick.files.wordpress.com/2008/04/neutrons-a-primer-by-rogen-pynn.pdf Neutron Scattering - A primer] ([http://library.lanl.gov/cgi-bin/getfile?00326651.pdf LANL-hosted black-and-white version]) - An introductory article written by Roger Pynn ([[Los Alamos National Laboratory]])
* [http://omegataupodcast.net/2010/03/28-neutron-science-at-the-ill/ Podcast Interview with two ILL scientists about neutron science/scattering at the ILL]
* [https://www.youtube.com/watch?v=ss-sj_x3ODg YouTube video explaining the activities of the Jülich Centre for Neutron Scattering]
* [http://neutronsources.org Neutronsources.org] 
* [http://sine2020.eu Science and Innovation with Neutrons in Europe in 2020 (SINE2020)]
* [https://nucleus.iaea.org/sites/accelerators/Pages/Interactive-Map-of-NB-Instruments.aspx IAEA neutron beam instrument database]

[[Category:Neutron scattering| ]]
[[Category:Crystallography]]
[[Category:Neutron-related techniques|scattering]]
[[Category:Scattering|Neutron]]
[[Category:Neutron|Scattering]]

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