Thermodynamic properties of Yb sub(2) Ti sub(2) O sub(7) pyrochlore as a function of temperature and magnetic field: Validation of a Quantum spin ice exchange Hamiltonian
The thermodynamic properties of the pyrochlore Yb sub(2) Ti sub(2) O sub(7) material are calculated using the numerical linked-cluster calculation method for an effective anisotropic-exchange spin-[1/2] Hamiltonian with parameters recently determined by fitting the neutron scattering spin-wave data...
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Veröffentlicht in: | Physical review. B, Condensed matter and materials physics Condensed matter and materials physics, 2013-05, Vol.87 (18) |
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creator | Hayre, N R Ross, K A Applegate, R Lin, T Singh, R R P Gaulin, B D Gingras, M J P |
description | The thermodynamic properties of the pyrochlore Yb sub(2) Ti sub(2) O sub(7) material are calculated using the numerical linked-cluster calculation method for an effective anisotropic-exchange spin-[1/2] Hamiltonian with parameters recently determined by fitting the neutron scattering spin-wave data obtained at high magnetic field. Magnetization M(T, h) as a function of temperature T and for different magnetic fields h applied along the three high-symmetry directions [100], [110], and [111] are compared with experimental measurements on the material for temperature T > 1.8 K. The excellent agreement between experimentally measured and calculated M(T, h) over the entire temperature and magnetic field ranges considered provides strong quantitative validation of the effective Hamiltonian. It also confirms that fitting the high-field neutron spin-wave spectra in the polarized paramagnetic state is an excellent method for determining the microscopic exchange constants of rare-earth insulating magnets that are described by an effective spin-[1/2] Hamiltonian. Finally, we present results which demonstrate that a recent analysis of the polarized neutron scattering intensity of Yb sub(2) Ti sub(2) O sub(7) using a random phase approximation method [Chang et al., Nat. Commun. 3. 992 (2012) (http://dx.doi.org/10.1038/ncomms1989)] does not provide a good description of M(T, h) for T [ |
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Magnetization M(T, h) as a function of temperature T and for different magnetic fields h applied along the three high-symmetry directions [100], [110], and [111] are compared with experimental measurements on the material for temperature T > 1.8 K. The excellent agreement between experimentally measured and calculated M(T, h) over the entire temperature and magnetic field ranges considered provides strong quantitative validation of the effective Hamiltonian. It also confirms that fitting the high-field neutron spin-wave spectra in the polarized paramagnetic state is an excellent method for determining the microscopic exchange constants of rare-earth insulating magnets that are described by an effective spin-[1/2] Hamiltonian. Finally, we present results which demonstrate that a recent analysis of the polarized neutron scattering intensity of Yb sub(2) Ti sub(2) O sub(7) using a random phase approximation method [Chang et al., Nat. Commun. 3. 992 (2012) (http://dx.doi.org/10.1038/ncomms1989)] does not provide a good description of M(T, h) for T [<, ~] 10 K, that is, in the entire temperature regime where magnetic correlations become non-negligible. With the compelling evidence that we now have at hand an accurate microscopic Hamiltonian for Yb sub(2) Ti sub(2) O sub(7), our work exposes a paradox: why does this material fail to develop long-range ferromagnetic order?</description><identifier>ISSN: 1098-0121</identifier><identifier>EISSN: 1550-235X</identifier><language>eng</language><subject>Exchange ; Fittings ; Magnetic fields ; Mathematical analysis ; Mathematical models ; Neutron scattering ; Rare earth metals ; Thermodynamic properties</subject><ispartof>Physical review. 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B, Condensed matter and materials physics</title><description>The thermodynamic properties of the pyrochlore Yb sub(2) Ti sub(2) O sub(7) material are calculated using the numerical linked-cluster calculation method for an effective anisotropic-exchange spin-[1/2] Hamiltonian with parameters recently determined by fitting the neutron scattering spin-wave data obtained at high magnetic field. Magnetization M(T, h) as a function of temperature T and for different magnetic fields h applied along the three high-symmetry directions [100], [110], and [111] are compared with experimental measurements on the material for temperature T > 1.8 K. The excellent agreement between experimentally measured and calculated M(T, h) over the entire temperature and magnetic field ranges considered provides strong quantitative validation of the effective Hamiltonian. It also confirms that fitting the high-field neutron spin-wave spectra in the polarized paramagnetic state is an excellent method for determining the microscopic exchange constants of rare-earth insulating magnets that are described by an effective spin-[1/2] Hamiltonian. Finally, we present results which demonstrate that a recent analysis of the polarized neutron scattering intensity of Yb sub(2) Ti sub(2) O sub(7) using a random phase approximation method [Chang et al., Nat. Commun. 3. 992 (2012) (http://dx.doi.org/10.1038/ncomms1989)] does not provide a good description of M(T, h) for T [<, ~] 10 K, that is, in the entire temperature regime where magnetic correlations become non-negligible. With the compelling evidence that we now have at hand an accurate microscopic Hamiltonian for Yb sub(2) Ti sub(2) O sub(7), our work exposes a paradox: why does this material fail to develop long-range ferromagnetic order?</description><subject>Exchange</subject><subject>Fittings</subject><subject>Magnetic fields</subject><subject>Mathematical analysis</subject><subject>Mathematical models</subject><subject>Neutron scattering</subject><subject>Rare earth metals</subject><subject>Thermodynamic properties</subject><issn>1098-0121</issn><issn>1550-235X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2013</creationdate><recordtype>article</recordtype><recordid>eNqVjstKw0AUhoMoWC_vcJbtIjCTNqRxK0p3IoSiq3I6OWlGZs7EuYB9JZ_SqdgHcPV_8F_4L4qZrGtRVsv67TKzaNelkJW8Lm5C-BBCrtpVNSu-u5G8df2R0WoFk3cT-agpgBvgfQ8h7efVAjp9ppdfaBYwHb1To3GeAAMgDIlV1I5PxUg2z2BMJ5N7sHhginl_0GT6B9ii0T2e0wivCTkmC2HSDFoR0JcakQ8Em3zLRMca-a64GtAEuv_T22L-_NQ9bsp8-jNRiDurgyJjkMmlsJONaJtGrBu5_Ef0B6ivY68</recordid><startdate>20130501</startdate><enddate>20130501</enddate><creator>Hayre, N R</creator><creator>Ross, K A</creator><creator>Applegate, R</creator><creator>Lin, T</creator><creator>Singh, R R P</creator><creator>Gaulin, B D</creator><creator>Gingras, M J P</creator><scope>7U5</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope></search><sort><creationdate>20130501</creationdate><title>Thermodynamic properties of Yb sub(2) Ti sub(2) O sub(7) pyrochlore as a function of temperature and magnetic field: Validation of a Quantum spin ice exchange Hamiltonian</title><author>Hayre, N R ; Ross, K A ; Applegate, R ; Lin, T ; Singh, R R P ; Gaulin, B D ; Gingras, M J P</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-proquest_miscellaneous_17097708713</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2013</creationdate><topic>Exchange</topic><topic>Fittings</topic><topic>Magnetic fields</topic><topic>Mathematical analysis</topic><topic>Mathematical models</topic><topic>Neutron scattering</topic><topic>Rare earth metals</topic><topic>Thermodynamic properties</topic><toplevel>online_resources</toplevel><creatorcontrib>Hayre, N R</creatorcontrib><creatorcontrib>Ross, K A</creatorcontrib><creatorcontrib>Applegate, R</creatorcontrib><creatorcontrib>Lin, T</creatorcontrib><creatorcontrib>Singh, R R P</creatorcontrib><creatorcontrib>Gaulin, B D</creatorcontrib><creatorcontrib>Gingras, M J P</creatorcontrib><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Physical review. B, Condensed matter and materials physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Hayre, N R</au><au>Ross, K A</au><au>Applegate, R</au><au>Lin, T</au><au>Singh, R R P</au><au>Gaulin, B D</au><au>Gingras, M J P</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Thermodynamic properties of Yb sub(2) Ti sub(2) O sub(7) pyrochlore as a function of temperature and magnetic field: Validation of a Quantum spin ice exchange Hamiltonian</atitle><jtitle>Physical review. B, Condensed matter and materials physics</jtitle><date>2013-05-01</date><risdate>2013</risdate><volume>87</volume><issue>18</issue><issn>1098-0121</issn><eissn>1550-235X</eissn><abstract>The thermodynamic properties of the pyrochlore Yb sub(2) Ti sub(2) O sub(7) material are calculated using the numerical linked-cluster calculation method for an effective anisotropic-exchange spin-[1/2] Hamiltonian with parameters recently determined by fitting the neutron scattering spin-wave data obtained at high magnetic field. Magnetization M(T, h) as a function of temperature T and for different magnetic fields h applied along the three high-symmetry directions [100], [110], and [111] are compared with experimental measurements on the material for temperature T > 1.8 K. The excellent agreement between experimentally measured and calculated M(T, h) over the entire temperature and magnetic field ranges considered provides strong quantitative validation of the effective Hamiltonian. It also confirms that fitting the high-field neutron spin-wave spectra in the polarized paramagnetic state is an excellent method for determining the microscopic exchange constants of rare-earth insulating magnets that are described by an effective spin-[1/2] Hamiltonian. Finally, we present results which demonstrate that a recent analysis of the polarized neutron scattering intensity of Yb sub(2) Ti sub(2) O sub(7) using a random phase approximation method [Chang et al., Nat. Commun. 3. 992 (2012) (http://dx.doi.org/10.1038/ncomms1989)] does not provide a good description of M(T, h) for T [<, ~] 10 K, that is, in the entire temperature regime where magnetic correlations become non-negligible. With the compelling evidence that we now have at hand an accurate microscopic Hamiltonian for Yb sub(2) Ti sub(2) O sub(7), our work exposes a paradox: why does this material fail to develop long-range ferromagnetic order?</abstract></addata></record> |
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subjects | Exchange Fittings Magnetic fields Mathematical analysis Mathematical models Neutron scattering Rare earth metals Thermodynamic properties |
title | Thermodynamic properties of Yb sub(2) Ti sub(2) O sub(7) pyrochlore as a function of temperature and magnetic field: Validation of a Quantum spin ice exchange Hamiltonian |
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