A reverse Monte Carlo algorithm to simulate two-dimensional small-angle scattering intensities.

magnetic nanoparticles reverse Monte Carlo simulations small-angle X-ray scattering small-angle neutron scattering superparamagnetic iron oxide nanoparticles

Journal

Journal of applied crystallography
ISSN: 0021-8898
Titre abrégé: J Appl Crystallogr
Pays: United States
ID NLM: 9876190

Informations de publication

Date de publication:
01 Dec 2022
Historique:
received: 25 05 2022
accepted: 16 09 2022
entrez: 26 12 2022
pubmed: 27 12 2022
medline: 27 12 2022
Statut: epublish

Résumé

Small-angle scattering (SAS) experiments are a powerful method for studying self-assembly phenomena in nanoscopic materials because of the sensitivity of the technique to structures formed by interactions on the nanoscale. Numerous out-of-the-box options exist for analysing structures measured by SAS but many of these are underpinned by assumptions about the underlying interactions that are not always relevant for a given system. Here, a numerical algorithm based on reverse Monte Carlo simulations is described to model the intensity observed on a SAS detector as a function of the scattering vector. The model simulates a two-dimensional detector image, accounting for magnetic scattering, instrument resolution, particle polydispersity and particle collisions, while making no further assumptions about the underlying particle interactions. By simulating a two-dimensional image that can be potentially anisotropic, the algorithm is particularly useful for studying systems driven by anisotropic interactions. The final output of the algorithm is a relative particle distribution, allowing visualization of particle structures that form over long-range length scales (

Identifiants

pubmed: 36570657
doi: 10.1107/S1600576722009219
pii: S1600576722009219
pmc: PMC9721324
doi:

Types de publication

Journal Article

Langues

eng

Pagination

1592-1602

Informations de copyright

© Lester C. Barnsley et al. 2022.

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Auteurs

Lester C Barnsley (LC)

Australian Synchrotron, ANSTO, Clayton 3168, Australia.
Forschungszentrum Jülich GmbH, Jülich Centre for Neutron Science (JCNS) at Heinz Maier-Leibnitz Zentrum (MLZ), 85748 Garching, Germany.

Nileena Nandakumaran (N)

Forschungszentrum Jülich GmbH, Jülich Centre for Neutron Science (JCNS-2) and Peter Grünberg Institut (PGI), JARA-FIT, 52425 Jülich, Germany.
Lehrstuhl für Experimentalphysik IVc, RWTH Aachen University, 52056 Aachen, Germany.

Artem Feoktystov (A)

Forschungszentrum Jülich GmbH, Jülich Centre for Neutron Science (JCNS) at Heinz Maier-Leibnitz Zentrum (MLZ), 85748 Garching, Germany.

Martin Dulle (M)

Forschungszentrum Jülich GmbH, Jülich Centre for Neutron Science (JCNS-1), 52425 Jülich, Germany.

Lisa Fruhner (L)

Forschungszentrum Jülich GmbH, Jülich Centre for Neutron Science (JCNS-1), 52425 Jülich, Germany.

Mikhail Feygenson (M)

European Spallation Source ERIC, SE-22100 Lund, Sweden.
Forschungszentrum Jülich GmbH, Jülich Centre for Neutron Science (JCNS-1), 52425 Jülich, Germany.

Classifications MeSH