Nonequilibrium multiple transitions in the core-shell Ising nanoparticles driven by randomly varying magnetic fields
•A cubic core-shell magnetic nanoparticle is considered.•This system is driven by random magnetic field.•A nonequilibrium multiple transitions is observed.•The phase boundary is drawn. The nonequilibrium behaviour of a core-shell nanoparticle has been studied by Monte-Carlo simulation. The core cons...
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Veröffentlicht in: | Journal of magnetism and magnetic materials 2021-06, Vol.527, p.167721, Article 167721 |
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container_title | Journal of magnetism and magnetic materials |
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creator | Vatansever, Erol Acharyya, Muktish |
description | •A cubic core-shell magnetic nanoparticle is considered.•This system is driven by random magnetic field.•A nonequilibrium multiple transitions is observed.•The phase boundary is drawn.
The nonequilibrium behaviour of a core-shell nanoparticle has been studied by Monte-Carlo simulation. The core consists of Ising spins of σ=1/2 and the shell contains Ising spins of S=1. The interactions within the core and in the shell are considered ferromagnetic but the interfacial interaction between core and shell is antiferromagnetic. The nanoparticle system is kept in open boundary conditions and is driven by randomly varying (in time but uniform over the space) magnetic field. Depending on the width of the randomly varying field and the temperature of the system, the core, shell and total magnetization varies in such a manner that the time averages vanish for higher magnitude of the width of random field, exhibiting a dynamical symmetry breaking transitions. The susceptibilities get peaked at two different temperatures indicating nonequilibrium multiple transitions. The phase boundaries of the nonequilibrium multiple transitions are drawn in the plane formed by the axes of temperature and the width of the randomly varying field. Furthermore, the effects of the core and shell thicknesses on the multiple transitions have been discussed. |
doi_str_mv | 10.1016/j.jmmm.2020.167721 |
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The nonequilibrium behaviour of a core-shell nanoparticle has been studied by Monte-Carlo simulation. The core consists of Ising spins of σ=1/2 and the shell contains Ising spins of S=1. The interactions within the core and in the shell are considered ferromagnetic but the interfacial interaction between core and shell is antiferromagnetic. The nanoparticle system is kept in open boundary conditions and is driven by randomly varying (in time but uniform over the space) magnetic field. Depending on the width of the randomly varying field and the temperature of the system, the core, shell and total magnetization varies in such a manner that the time averages vanish for higher magnitude of the width of random field, exhibiting a dynamical symmetry breaking transitions. The susceptibilities get peaked at two different temperatures indicating nonequilibrium multiple transitions. The phase boundaries of the nonequilibrium multiple transitions are drawn in the plane formed by the axes of temperature and the width of the randomly varying field. Furthermore, the effects of the core and shell thicknesses on the multiple transitions have been discussed.</description><identifier>ISSN: 0304-8853</identifier><identifier>EISSN: 1873-4766</identifier><identifier>DOI: 10.1016/j.jmmm.2020.167721</identifier><language>eng</language><publisher>Amsterdam: Elsevier B.V</publisher><subject>Antiferromagnetism ; Boundary conditions ; Broken symmetry ; Core-shell particles ; Core/shell nanoparticles ; Dynamic phase transitions ; Ferromagnetism ; Fields (mathematics) ; Ising model ; Magnetic fields ; Magnetic hyperthermia ; Monte Carlo simulation ; Nanoparticles ; Phase transitions</subject><ispartof>Journal of magnetism and magnetic materials, 2021-06, Vol.527, p.167721, Article 167721</ispartof><rights>2021 Elsevier B.V.</rights><rights>Copyright Elsevier BV Jun 1, 2021</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c328t-72e0368201bbb1e152cf9d037b66d0f808d208ffb2391937b72ad7da79e2a9743</citedby><cites>FETCH-LOGICAL-c328t-72e0368201bbb1e152cf9d037b66d0f808d208ffb2391937b72ad7da79e2a9743</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://dx.doi.org/10.1016/j.jmmm.2020.167721$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,780,784,3548,27923,27924,45994</link.rule.ids></links><search><creatorcontrib>Vatansever, Erol</creatorcontrib><creatorcontrib>Acharyya, Muktish</creatorcontrib><title>Nonequilibrium multiple transitions in the core-shell Ising nanoparticles driven by randomly varying magnetic fields</title><title>Journal of magnetism and magnetic materials</title><description>•A cubic core-shell magnetic nanoparticle is considered.•This system is driven by random magnetic field.•A nonequilibrium multiple transitions is observed.•The phase boundary is drawn.
The nonequilibrium behaviour of a core-shell nanoparticle has been studied by Monte-Carlo simulation. The core consists of Ising spins of σ=1/2 and the shell contains Ising spins of S=1. The interactions within the core and in the shell are considered ferromagnetic but the interfacial interaction between core and shell is antiferromagnetic. The nanoparticle system is kept in open boundary conditions and is driven by randomly varying (in time but uniform over the space) magnetic field. Depending on the width of the randomly varying field and the temperature of the system, the core, shell and total magnetization varies in such a manner that the time averages vanish for higher magnitude of the width of random field, exhibiting a dynamical symmetry breaking transitions. The susceptibilities get peaked at two different temperatures indicating nonequilibrium multiple transitions. The phase boundaries of the nonequilibrium multiple transitions are drawn in the plane formed by the axes of temperature and the width of the randomly varying field. Furthermore, the effects of the core and shell thicknesses on the multiple transitions have been discussed.</description><subject>Antiferromagnetism</subject><subject>Boundary conditions</subject><subject>Broken symmetry</subject><subject>Core-shell particles</subject><subject>Core/shell nanoparticles</subject><subject>Dynamic phase transitions</subject><subject>Ferromagnetism</subject><subject>Fields (mathematics)</subject><subject>Ising model</subject><subject>Magnetic fields</subject><subject>Magnetic hyperthermia</subject><subject>Monte Carlo simulation</subject><subject>Nanoparticles</subject><subject>Phase transitions</subject><issn>0304-8853</issn><issn>1873-4766</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><recordid>eNp9kE1LxDAQhoMouH78AU8Bz10n6W6TghcRv0D0oueQNlM3JU12k3Rh_70t69nTwMvzzAwvITcMlgxYddcv-2EYlhz4FFRCcHZCFkyKsliJqjolCyhhVUi5Ls_JRUo9ALCVrBYkfwSPu9E620Q7DnQYXbZbhzRH7ZPNNvhErad5g7QNEYu0QefoW7L-h3rtw1bHbFuHiZpo9-hpc6CTasLgDnSv42EGB_3jccJoZ9GZdEXOOu0SXv_NS_L9_PT1-Fq8f768PT68F23JZS4ERygryYE1TcOQrXnb1QZK0VSVgU6CNBxk1zW8rFk9xYJrI4wWNXJdi1V5SW6Pe7cx7EZMWfVhjH46qfga5FoKqGeKH6k2hpQidmob7TB9rhiouV3Vq7ldNberju1O0v1Rwun_vcWoUmvRt2hsxDYrE-x_-i_s84Vi</recordid><startdate>20210601</startdate><enddate>20210601</enddate><creator>Vatansever, Erol</creator><creator>Acharyya, Muktish</creator><general>Elsevier B.V</general><general>Elsevier BV</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20210601</creationdate><title>Nonequilibrium multiple transitions in the core-shell Ising nanoparticles driven by randomly varying magnetic fields</title><author>Vatansever, Erol ; Acharyya, Muktish</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c328t-72e0368201bbb1e152cf9d037b66d0f808d208ffb2391937b72ad7da79e2a9743</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2021</creationdate><topic>Antiferromagnetism</topic><topic>Boundary conditions</topic><topic>Broken symmetry</topic><topic>Core-shell particles</topic><topic>Core/shell nanoparticles</topic><topic>Dynamic phase transitions</topic><topic>Ferromagnetism</topic><topic>Fields (mathematics)</topic><topic>Ising model</topic><topic>Magnetic fields</topic><topic>Magnetic hyperthermia</topic><topic>Monte Carlo simulation</topic><topic>Nanoparticles</topic><topic>Phase transitions</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Vatansever, Erol</creatorcontrib><creatorcontrib>Acharyya, Muktish</creatorcontrib><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of magnetism and magnetic materials</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Vatansever, Erol</au><au>Acharyya, Muktish</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Nonequilibrium multiple transitions in the core-shell Ising nanoparticles driven by randomly varying magnetic fields</atitle><jtitle>Journal of magnetism and magnetic materials</jtitle><date>2021-06-01</date><risdate>2021</risdate><volume>527</volume><spage>167721</spage><pages>167721-</pages><artnum>167721</artnum><issn>0304-8853</issn><eissn>1873-4766</eissn><abstract>•A cubic core-shell magnetic nanoparticle is considered.•This system is driven by random magnetic field.•A nonequilibrium multiple transitions is observed.•The phase boundary is drawn.
The nonequilibrium behaviour of a core-shell nanoparticle has been studied by Monte-Carlo simulation. The core consists of Ising spins of σ=1/2 and the shell contains Ising spins of S=1. The interactions within the core and in the shell are considered ferromagnetic but the interfacial interaction between core and shell is antiferromagnetic. The nanoparticle system is kept in open boundary conditions and is driven by randomly varying (in time but uniform over the space) magnetic field. Depending on the width of the randomly varying field and the temperature of the system, the core, shell and total magnetization varies in such a manner that the time averages vanish for higher magnitude of the width of random field, exhibiting a dynamical symmetry breaking transitions. The susceptibilities get peaked at two different temperatures indicating nonequilibrium multiple transitions. The phase boundaries of the nonequilibrium multiple transitions are drawn in the plane formed by the axes of temperature and the width of the randomly varying field. Furthermore, the effects of the core and shell thicknesses on the multiple transitions have been discussed.</abstract><cop>Amsterdam</cop><pub>Elsevier B.V</pub><doi>10.1016/j.jmmm.2020.167721</doi></addata></record> |
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source | ScienceDirect Journals (5 years ago - present) |
subjects | Antiferromagnetism Boundary conditions Broken symmetry Core-shell particles Core/shell nanoparticles Dynamic phase transitions Ferromagnetism Fields (mathematics) Ising model Magnetic fields Magnetic hyperthermia Monte Carlo simulation Nanoparticles Phase transitions |
title | Nonequilibrium multiple transitions in the core-shell Ising nanoparticles driven by randomly varying magnetic fields |
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