Universal Dynamics of Magnetic Monopoles in Two-Dimensional Kagomé Ice
A magnetic monopole in spin ice is a novel quasiparticle excitation in condensed matter physics. We found that the ac frequency dependent magnetic susceptibility χ(ω) in the two-dimensional (2D) spin ice (so-called kagomé ice) of Dy2Ti2O7 shows a single scaling form. This behavior can be understood...
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Veröffentlicht in: | Journal of the Physical Society of Japan 2021-12, Vol.90 (12), p.1 |
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creator | Takatsu, Hiroshi Goto, Kazuki Sato, Taku J. Lynn, Jeffrey W. Matsubayashi, Kazuyuki Uwatoko, Yoshiya Higashinaka, Ryuji Matsuhira, Kazuyuki Hiroi, Zenji Kadowaki, Hiroaki |
description | A magnetic monopole in spin ice is a novel quasiparticle excitation in condensed matter physics. We found that the ac frequency dependent magnetic susceptibility χ(ω) in the two-dimensional (2D) spin ice (so-called kagomé ice) of Dy2Ti2O7 shows a single scaling form. This behavior can be understood in terms of the dynamical scaling law for 2D Coulomb gas (CG) systems [Phys. Rev. B 90, 144428 (2014)], characterized by the charge correlation length ξ (∝1/√ω1), where ω1 is a characteristic frequency proportional to the peak position of the imaginary part of χ(ω). It is a generic behavior among a wide variety of models such as the vortex dynamics of 2D superconductors, 2D superfluids, classical XY magnets, and dynamics of melting of Wigner crystals. |
doi_str_mv | 10.7566/JPSJ.90.123705 |
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We found that the ac frequency dependent magnetic susceptibility χ(ω) in the two-dimensional (2D) spin ice (so-called kagomé ice) of Dy2Ti2O7 shows a single scaling form. This behavior can be understood in terms of the dynamical scaling law for 2D Coulomb gas (CG) systems [Phys. Rev. B 90, 144428 (2014)], characterized by the charge correlation length ξ (∝1/√ω1), where ω1 is a characteristic frequency proportional to the peak position of the imaginary part of χ(ω). 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We found that the ac frequency dependent magnetic susceptibility χ(ω) in the two-dimensional (2D) spin ice (so-called kagomé ice) of Dy2Ti2O7 shows a single scaling form. This behavior can be understood in terms of the dynamical scaling law for 2D Coulomb gas (CG) systems [Phys. Rev. B 90, 144428 (2014)], characterized by the charge correlation length ξ (∝1/√ω1), where ω1 is a characteristic frequency proportional to the peak position of the imaginary part of χ(ω). It is a generic behavior among a wide variety of models such as the vortex dynamics of 2D superconductors, 2D superfluids, classical XY magnets, and dynamics of melting of Wigner crystals.</description><subject>Condensed matter physics</subject><subject>Elementary excitations</subject><subject>Magnetic monopoles</subject><subject>Magnetic permeability</subject><subject>Magnets</subject><subject>Scaling laws</subject><subject>Spin ice</subject><subject>Superconductors</subject><subject>Two dimensional models</subject><issn>0031-9015</issn><issn>1347-4073</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><recordid>eNotkMFOAjEURRujiYhuXTdxPeNr30yHLg0oghBNhHXTKS0pYVqcgoRP8jv8MSG4uptzb24OIfcM8qoU4nH88TnOJeSMYwXlBekwLKqsgAovSQcAWSaBldfkJqUVAC8ZLzpkOA_-27ZJr-ngEHTjTaLR0aleBrv1hk5jiJu4ton6QGf7mA18Y0PyMRwbb3oZm98fOjL2llw5vU727j-7ZP7yPOu_ZpP34aj_NMkMCthm2vZ4zWqohUB0UlpTG8bBCYbAhANcuMIa7iwrLHKxMJJzRC65cz3RQ4Nd8nDe3bTxa2fTVq3irj2eSYoLKBGqissjlZ8p08aUWuvUpvWNbg-KgTrJUidZSoI6y8I_ompcVw</recordid><startdate>20211215</startdate><enddate>20211215</enddate><creator>Takatsu, Hiroshi</creator><creator>Goto, Kazuki</creator><creator>Sato, Taku J.</creator><creator>Lynn, Jeffrey W.</creator><creator>Matsubayashi, Kazuyuki</creator><creator>Uwatoko, Yoshiya</creator><creator>Higashinaka, Ryuji</creator><creator>Matsuhira, Kazuyuki</creator><creator>Hiroi, Zenji</creator><creator>Kadowaki, Hiroaki</creator><general>The Physical Society of Japan</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7U5</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0003-2511-4998</orcidid><orcidid>https://orcid.org/0000-0001-5792-0113</orcidid><orcidid>https://orcid.org/0000-0003-3626-4932</orcidid><orcidid>https://orcid.org/0000-0003-1190-2344</orcidid><orcidid>https://orcid.org/0000-0001-7165-3939</orcidid></search><sort><creationdate>20211215</creationdate><title>Universal Dynamics of Magnetic Monopoles in Two-Dimensional Kagomé Ice</title><author>Takatsu, Hiroshi ; Goto, Kazuki ; Sato, Taku J. ; Lynn, Jeffrey W. ; Matsubayashi, Kazuyuki ; Uwatoko, Yoshiya ; Higashinaka, Ryuji ; Matsuhira, Kazuyuki ; Hiroi, Zenji ; Kadowaki, Hiroaki</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c360t-ae82b1b0b6633f99ecbc120f613016f03df4ec2fe14e326dc92233292ff8683c3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2021</creationdate><topic>Condensed matter physics</topic><topic>Elementary excitations</topic><topic>Magnetic monopoles</topic><topic>Magnetic permeability</topic><topic>Magnets</topic><topic>Scaling laws</topic><topic>Spin ice</topic><topic>Superconductors</topic><topic>Two dimensional models</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Takatsu, Hiroshi</creatorcontrib><creatorcontrib>Goto, Kazuki</creatorcontrib><creatorcontrib>Sato, Taku J.</creatorcontrib><creatorcontrib>Lynn, Jeffrey W.</creatorcontrib><creatorcontrib>Matsubayashi, Kazuyuki</creatorcontrib><creatorcontrib>Uwatoko, Yoshiya</creatorcontrib><creatorcontrib>Higashinaka, Ryuji</creatorcontrib><creatorcontrib>Matsuhira, Kazuyuki</creatorcontrib><creatorcontrib>Hiroi, Zenji</creatorcontrib><creatorcontrib>Kadowaki, Hiroaki</creatorcontrib><collection>CrossRef</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of the Physical Society of Japan</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Takatsu, Hiroshi</au><au>Goto, Kazuki</au><au>Sato, Taku J.</au><au>Lynn, Jeffrey W.</au><au>Matsubayashi, Kazuyuki</au><au>Uwatoko, Yoshiya</au><au>Higashinaka, Ryuji</au><au>Matsuhira, Kazuyuki</au><au>Hiroi, Zenji</au><au>Kadowaki, Hiroaki</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Universal Dynamics of Magnetic Monopoles in Two-Dimensional Kagomé Ice</atitle><jtitle>Journal of the Physical Society of Japan</jtitle><date>2021-12-15</date><risdate>2021</risdate><volume>90</volume><issue>12</issue><spage>1</spage><pages>1-</pages><issn>0031-9015</issn><eissn>1347-4073</eissn><abstract>A magnetic monopole in spin ice is a novel quasiparticle excitation in condensed matter physics. We found that the ac frequency dependent magnetic susceptibility χ(ω) in the two-dimensional (2D) spin ice (so-called kagomé ice) of Dy2Ti2O7 shows a single scaling form. This behavior can be understood in terms of the dynamical scaling law for 2D Coulomb gas (CG) systems [Phys. Rev. B 90, 144428 (2014)], characterized by the charge correlation length ξ (∝1/√ω1), where ω1 is a characteristic frequency proportional to the peak position of the imaginary part of χ(ω). 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subjects | Condensed matter physics Elementary excitations Magnetic monopoles Magnetic permeability Magnets Scaling laws Spin ice Superconductors Two dimensional models |
title | Universal Dynamics of Magnetic Monopoles in Two-Dimensional Kagomé Ice |
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