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Magnetic structure and glassiness in Fe 0.5 Ni 0.5 PS 3

Goossens, Darren; Brazier-Hollins, Sam; James, Daniel; Hutchinson, W.D.; Hester, James

Description

This work explores the magnetic properties of Fe0.5Ni 0.5PS3. The system shows pronounced hysteresis in the magnetic phase transition temperature as a function of the direction of the change in temperature. Field cooled/zero field cooled hysteresis is not pronounced. However, the transition temperature between antiferromagnetic and paramagnetic order occurs at approximately 97 K on cooling, but at 138 K on warming, whether the warming is after zero field or field cooling. This is indicative of...[Show more]

dc.contributor.authorGoossens, Darren
dc.contributor.authorBrazier-Hollins, Sam
dc.contributor.authorJames, Daniel
dc.contributor.authorHutchinson, W.D.
dc.contributor.authorHester, James
dc.date.accessioned2015-12-10T23:07:42Z
dc.identifier.issn0304-8853
dc.identifier.urihttp://hdl.handle.net/1885/62983
dc.description.abstractThis work explores the magnetic properties of Fe0.5Ni 0.5PS3. The system shows pronounced hysteresis in the magnetic phase transition temperature as a function of the direction of the change in temperature. Field cooled/zero field cooled hysteresis is not pronounced. However, the transition temperature between antiferromagnetic and paramagnetic order occurs at approximately 97 K on cooling, but at 138 K on warming, whether the warming is after zero field or field cooling. This is indicative of magnetic glassiness, and made all the more unusual because all measurements exhibit a transition to a third magnetic phase existing at temperatures below ∼14K. The intermediate phase relaxes on a laboratory time scale of the order of 48 min, into an antiferromagnetic state whose magnetic structure is, from neutron diffraction, indistinguishable from the low temperature state. This low temperature state shows magnetic ordering consistent with that observed in CoPS3 and NiPS3. Analysis of the neutron measurements shows that the direction of moments cannot be along the b-axis. It is also shown that the moments are unlikely to lie in the c * direction. Therefore, we suggest that the moments lie along the a-axis.
dc.publisherElsevier
dc.sourceJournal of Magnetism and Magnetic Materials
dc.subjectKeywords: A transitions; Antiferromagnetic state; Antiferromagnetics; FePS 3 ; Field cooled; Field cooling; Intermediate phase; Low-temperature state; Magnetic glass; Magnetic phase; Magnetic phase transitions; Neutron measurements; Time-scales; Zero field Antiferromagnetism; FePS3; Layered magnetism; Magnetic glass
dc.titleMagnetic structure and glassiness in Fe 0.5 Ni 0.5 PS 3
dc.typeJournal article
local.description.notesImported from ARIES
local.identifier.citationvolume334
dc.date.issued2013
local.identifier.absfor030606 - Structural Chemistry and Spectroscopy
local.identifier.absfor020404 - Electronic and Magnetic Properties of Condensed Matter; Superconductivity
local.identifier.ariespublicationU4217927xPUB757
local.type.statusPublished Version
local.contributor.affiliationGoossens, Darren, College of Physical and Mathematical Sciences, ANU
local.contributor.affiliationBrazier-Hollins, Sam, College of Engineering and Computer Science, ANU
local.contributor.affiliationJames, Daniel, College of Engineering and Computer Science, ANU
local.contributor.affiliationHutchinson, W.D., University of New South Wales
local.contributor.affiliationHester, James, Australian Nuclear Science and Technology Organisation
local.description.embargo2037-12-31
local.bibliographicCitation.startpage82
local.bibliographicCitation.lastpage86
local.identifier.doi10.1016/j.jmmm.2013.01.023
local.identifier.absseo970103 - Expanding Knowledge in the Chemical Sciences
dc.date.updated2016-02-24T10:45:12Z
local.identifier.scopusID2-s2.0-84874740848
local.identifier.thomsonID000315744100014
CollectionsANU Research Publications

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