Magnetoelectric effects in the spin-1/2 XXZ model with Dzyaloshinskii-Moriya interaction
We study the 1D spin-1/2 XXZ chain in the presence of the Dzyaloshinskii-Moriya (D-M) interaction and with longitudinal and transverse magnetic fields. We assume the spin-current mechanism of Katsura-Nagaosa-Balatsky at play and interpret the D-M interaction as a coupling between the local electric...
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description | We study the 1D spin-1/2 XXZ chain in the presence of the Dzyaloshinskii-Moriya (D-M) interaction and with longitudinal and transverse magnetic fields. We assume the spin-current mechanism of Katsura-Nagaosa-Balatsky at play and interpret the D-M interaction as a coupling between the local electric polarization and an external electric field. We study the interplay of electric and magnetic order in the ground state using the numerical density matrix renormalization group(DMRG) method. Specifically, we investigate the dependences of the magnetization and electric polarization on the external electric and magnetic fields. We find that for transverse magnetic fields, there are two different regimes of polarization while for longitudinal magnetic fields, there are three different regimes of polarization. The different regimes can be tuned by the external magnetic fields. |
doi_str_mv | 10.1063/1.4918199 |
format | Conference Proceeding |
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We assume the spin-current mechanism of Katsura-Nagaosa-Balatsky at play and interpret the D-M interaction as a coupling between the local electric polarization and an external electric field. We study the interplay of electric and magnetic order in the ground state using the numerical density matrix renormalization group(DMRG) method. Specifically, we investigate the dependences of the magnetization and electric polarization on the external electric and magnetic fields. We find that for transverse magnetic fields, there are two different regimes of polarization while for longitudinal magnetic fields, there are three different regimes of polarization. The different regimes can be tuned by the external magnetic fields.</description><identifier>ISSN: 0094-243X</identifier><identifier>EISSN: 1551-7616</identifier><identifier>DOI: 10.1063/1.4918199</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY ; COUPLING ; DENSITY MATRIX ; ELECTRIC FIELDS ; Electric polarization ; ELECTRICAL PROPERTIES ; GROUND STATES ; MAGNETIC FIELDS ; MAGNETIC PROPERTIES ; Magnetism ; MAGNETIZATION ; Mathematical models ; POLARIZATION ; RENORMALIZATION ; SPIN</subject><ispartof>AIP conference proceedings, 2015, Vol.1665 (1)</ispartof><rights>2015 AIP Publishing LLC.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,309,310,314,776,780,785,786,881,23910,23911,25119,27903,27904</link.rule.ids><backlink>$$Uhttps://www.osti.gov/biblio/22490585$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Thakur Pradeep</creatorcontrib><creatorcontrib>Durganandini, P</creatorcontrib><title>Magnetoelectric effects in the spin-1/2 XXZ model with Dzyaloshinskii-Moriya interaction</title><title>AIP conference proceedings</title><description>We study the 1D spin-1/2 XXZ chain in the presence of the Dzyaloshinskii-Moriya (D-M) interaction and with longitudinal and transverse magnetic fields. We assume the spin-current mechanism of Katsura-Nagaosa-Balatsky at play and interpret the D-M interaction as a coupling between the local electric polarization and an external electric field. We study the interplay of electric and magnetic order in the ground state using the numerical density matrix renormalization group(DMRG) method. Specifically, we investigate the dependences of the magnetization and electric polarization on the external electric and magnetic fields. We find that for transverse magnetic fields, there are two different regimes of polarization while for longitudinal magnetic fields, there are three different regimes of polarization. The different regimes can be tuned by the external magnetic fields.</description><subject>CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY</subject><subject>COUPLING</subject><subject>DENSITY MATRIX</subject><subject>ELECTRIC FIELDS</subject><subject>Electric polarization</subject><subject>ELECTRICAL PROPERTIES</subject><subject>GROUND STATES</subject><subject>MAGNETIC FIELDS</subject><subject>MAGNETIC PROPERTIES</subject><subject>Magnetism</subject><subject>MAGNETIZATION</subject><subject>Mathematical models</subject><subject>POLARIZATION</subject><subject>RENORMALIZATION</subject><subject>SPIN</subject><issn>0094-243X</issn><issn>1551-7616</issn><fulltext>true</fulltext><rsrctype>conference_proceeding</rsrctype><creationdate>2015</creationdate><recordtype>conference_proceeding</recordtype><recordid>eNpFT0tLxDAYDKLgunrwHwQ8ZzfPpjnK-oRdvCgULyVNv9qsNVmbLLL-egsKnmZgHswgdMnogtFCLNlCGlYyY47QjCnFiC5YcYxmlBpJuBTVKTpLaUspN1qXM1Rt7FuAHGEAl0fvMHTdxBL2AececNr5QNiS46p6xR-xhQF_-dzjm--DHWLqfUjv3pNNHP3BTqEMo3XZx3COTjo7JLj4wzl6ubt9Xj2Q9dP94-p6TSJnLJPWdY1VTrtWqc5R1TFZik6DMU05GSbR0bYADRKEAisLrVTbMM0NNSXQRszR1W9vTNnXyfkMrncxhOlFzbk0VJXq37Ub4-ceUq63cT-GaVjNGZdaKG1K8QNpq18i</recordid><startdate>20150624</startdate><enddate>20150624</enddate><creator>Thakur Pradeep</creator><creator>Durganandini, P</creator><general>American Institute of Physics</general><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>OTOTI</scope></search><sort><creationdate>20150624</creationdate><title>Magnetoelectric effects in the spin-1/2 XXZ model with Dzyaloshinskii-Moriya interaction</title><author>Thakur Pradeep ; Durganandini, P</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-o211t-dcfba5c7cd55fc05f1483f7e99b8211fbac0d6e7e4e35ea46755db1729098e0b3</frbrgroupid><rsrctype>conference_proceedings</rsrctype><prefilter>conference_proceedings</prefilter><language>eng</language><creationdate>2015</creationdate><topic>CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY</topic><topic>COUPLING</topic><topic>DENSITY MATRIX</topic><topic>ELECTRIC FIELDS</topic><topic>Electric polarization</topic><topic>ELECTRICAL PROPERTIES</topic><topic>GROUND STATES</topic><topic>MAGNETIC FIELDS</topic><topic>MAGNETIC PROPERTIES</topic><topic>Magnetism</topic><topic>MAGNETIZATION</topic><topic>Mathematical models</topic><topic>POLARIZATION</topic><topic>RENORMALIZATION</topic><topic>SPIN</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Thakur Pradeep</creatorcontrib><creatorcontrib>Durganandini, P</creatorcontrib><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>OSTI.GOV</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Thakur Pradeep</au><au>Durganandini, P</au><format>book</format><genre>proceeding</genre><ristype>CONF</ristype><atitle>Magnetoelectric effects in the spin-1/2 XXZ model with Dzyaloshinskii-Moriya interaction</atitle><btitle>AIP conference proceedings</btitle><date>2015-06-24</date><risdate>2015</risdate><volume>1665</volume><issue>1</issue><issn>0094-243X</issn><eissn>1551-7616</eissn><abstract>We study the 1D spin-1/2 XXZ chain in the presence of the Dzyaloshinskii-Moriya (D-M) interaction and with longitudinal and transverse magnetic fields. We assume the spin-current mechanism of Katsura-Nagaosa-Balatsky at play and interpret the D-M interaction as a coupling between the local electric polarization and an external electric field. We study the interplay of electric and magnetic order in the ground state using the numerical density matrix renormalization group(DMRG) method. Specifically, we investigate the dependences of the magnetization and electric polarization on the external electric and magnetic fields. We find that for transverse magnetic fields, there are two different regimes of polarization while for longitudinal magnetic fields, there are three different regimes of polarization. The different regimes can be tuned by the external magnetic fields.</abstract><cop>Melville</cop><pub>American Institute of Physics</pub><doi>10.1063/1.4918199</doi></addata></record> |
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source | AIP Journals Complete |
subjects | CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY COUPLING DENSITY MATRIX ELECTRIC FIELDS Electric polarization ELECTRICAL PROPERTIES GROUND STATES MAGNETIC FIELDS MAGNETIC PROPERTIES Magnetism MAGNETIZATION Mathematical models POLARIZATION RENORMALIZATION SPIN |
title | Magnetoelectric effects in the spin-1/2 XXZ model with Dzyaloshinskii-Moriya interaction |
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