Cargando…

Limited Ferromagnetic Interactions in Monolayers of MPS(3) (M = Mn and Ni)

[Image: see text] We present a systematic study of the electronic and magnetic properties of two-dimensional ordered alloys, consisting of two representative hosts (MnPS(3) and NiPS(3)) of transition metal phosphorus trichalcogenides doped with 3d elements. For both hosts, our DFT + U calculations a...

Descripción completa

Detalles Bibliográficos
Autores principales: Autieri, Carmine, Cuono, Giuseppe, Noce, Canio, Rybak, Milosz, Kotur, Kamila M., Agrapidis, Cliò Efthimia, Wohlfeld, Krzysztof, Birowska, Magdalena
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2022
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9037203/
https://www.ncbi.nlm.nih.gov/pubmed/35493696
http://dx.doi.org/10.1021/acs.jpcc.2c00646
_version_ 1784693684007075840
author Autieri, Carmine
Cuono, Giuseppe
Noce, Canio
Rybak, Milosz
Kotur, Kamila M.
Agrapidis, Cliò Efthimia
Wohlfeld, Krzysztof
Birowska, Magdalena
author_facet Autieri, Carmine
Cuono, Giuseppe
Noce, Canio
Rybak, Milosz
Kotur, Kamila M.
Agrapidis, Cliò Efthimia
Wohlfeld, Krzysztof
Birowska, Magdalena
author_sort Autieri, Carmine
collection PubMed
description [Image: see text] We present a systematic study of the electronic and magnetic properties of two-dimensional ordered alloys, consisting of two representative hosts (MnPS(3) and NiPS(3)) of transition metal phosphorus trichalcogenides doped with 3d elements. For both hosts, our DFT + U calculations are able to qualitatively reproduce the ratios and signs of all experimentally observed magnetic couplings. The relative strength of all antiferromagnetic exchange couplings, both in MnPS(3) and in NiPS(3), can successfully be explained using an effective direct exchange model: it reveals that the third-neighbor exchange dominates in NiPS(3) due to the filling of the t(2g) subshell, whereas for MnPS(3), the first-neighbor exchange prevails, owing to the presence of the t(2g) magnetism. On the other hand, the nearest neighbor ferromagnetic coupling in NiPS(3) can only be explained using a more complex superexchange model and is (also) largely triggered by the absence of the t(2g) magnetism. For the doped systems, the DFT + U calculations revealed that magnetic impurities do not affect the magnetic ordering observed in the pure phases, and thus, in general in these systems, ferromagnetism may not be easily induced by such a kind of elemental doping. However, unlike for the hosts, the first and second (dopant–host) exchange couplings are of similar order of magnitude. This leads to frustration in the case of antiferromagnetic coupling and may be one of the reasons of the observed lower magnetic ordering temperature of the doped systems.
format Online
Article
Text
id pubmed-9037203
institution National Center for Biotechnology Information
language English
publishDate 2022
publisher American Chemical Society
record_format MEDLINE/PubMed
spelling pubmed-90372032022-04-26 Limited Ferromagnetic Interactions in Monolayers of MPS(3) (M = Mn and Ni) Autieri, Carmine Cuono, Giuseppe Noce, Canio Rybak, Milosz Kotur, Kamila M. Agrapidis, Cliò Efthimia Wohlfeld, Krzysztof Birowska, Magdalena J Phys Chem C Nanomater Interfaces [Image: see text] We present a systematic study of the electronic and magnetic properties of two-dimensional ordered alloys, consisting of two representative hosts (MnPS(3) and NiPS(3)) of transition metal phosphorus trichalcogenides doped with 3d elements. For both hosts, our DFT + U calculations are able to qualitatively reproduce the ratios and signs of all experimentally observed magnetic couplings. The relative strength of all antiferromagnetic exchange couplings, both in MnPS(3) and in NiPS(3), can successfully be explained using an effective direct exchange model: it reveals that the third-neighbor exchange dominates in NiPS(3) due to the filling of the t(2g) subshell, whereas for MnPS(3), the first-neighbor exchange prevails, owing to the presence of the t(2g) magnetism. On the other hand, the nearest neighbor ferromagnetic coupling in NiPS(3) can only be explained using a more complex superexchange model and is (also) largely triggered by the absence of the t(2g) magnetism. For the doped systems, the DFT + U calculations revealed that magnetic impurities do not affect the magnetic ordering observed in the pure phases, and thus, in general in these systems, ferromagnetism may not be easily induced by such a kind of elemental doping. However, unlike for the hosts, the first and second (dopant–host) exchange couplings are of similar order of magnitude. This leads to frustration in the case of antiferromagnetic coupling and may be one of the reasons of the observed lower magnetic ordering temperature of the doped systems. American Chemical Society 2022-04-12 2022-04-21 /pmc/articles/PMC9037203/ /pubmed/35493696 http://dx.doi.org/10.1021/acs.jpcc.2c00646 Text en © 2022 The Authors. Published by American Chemical Society https://creativecommons.org/licenses/by/4.0/Permits the broadest form of re-use including for commercial purposes, provided that author attribution and integrity are maintained (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Autieri, Carmine
Cuono, Giuseppe
Noce, Canio
Rybak, Milosz
Kotur, Kamila M.
Agrapidis, Cliò Efthimia
Wohlfeld, Krzysztof
Birowska, Magdalena
Limited Ferromagnetic Interactions in Monolayers of MPS(3) (M = Mn and Ni)
title Limited Ferromagnetic Interactions in Monolayers of MPS(3) (M = Mn and Ni)
title_full Limited Ferromagnetic Interactions in Monolayers of MPS(3) (M = Mn and Ni)
title_fullStr Limited Ferromagnetic Interactions in Monolayers of MPS(3) (M = Mn and Ni)
title_full_unstemmed Limited Ferromagnetic Interactions in Monolayers of MPS(3) (M = Mn and Ni)
title_short Limited Ferromagnetic Interactions in Monolayers of MPS(3) (M = Mn and Ni)
title_sort limited ferromagnetic interactions in monolayers of mps(3) (m = mn and ni)
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9037203/
https://www.ncbi.nlm.nih.gov/pubmed/35493696
http://dx.doi.org/10.1021/acs.jpcc.2c00646
work_keys_str_mv AT autiericarmine limitedferromagneticinteractionsinmonolayersofmps3mmnandni
AT cuonogiuseppe limitedferromagneticinteractionsinmonolayersofmps3mmnandni
AT nocecanio limitedferromagneticinteractionsinmonolayersofmps3mmnandni
AT rybakmilosz limitedferromagneticinteractionsinmonolayersofmps3mmnandni
AT koturkamilam limitedferromagneticinteractionsinmonolayersofmps3mmnandni
AT agrapidisclioefthimia limitedferromagneticinteractionsinmonolayersofmps3mmnandni
AT wohlfeldkrzysztof limitedferromagneticinteractionsinmonolayersofmps3mmnandni
AT birowskamagdalena limitedferromagneticinteractionsinmonolayersofmps3mmnandni