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dc.contributor.authorTian, L.-Y.
dc.contributor.authorLevämäki, H.
dc.contributor.authorKuisma, Mikael
dc.contributor.authorKokko, K.
dc.contributor.authorNagy, Á.
dc.contributor.authorVitos, L.
dc.date.accessioned2019-05-29T06:40:13Z
dc.date.available2019-05-29T06:40:13Z
dc.date.issued2019
dc.identifier.citationTian, L.-Y., Levämäki, H., Kuisma, M., Kokko, K., Nagy, Á., & Vitos, L. (2019). Density functional theory description of random Cu-Au alloys. <i>Physical Review B</i>, <i>99</i>(6), Article 064202. <a href="https://doi.org/10.1103/PhysRevB.99.064202" target="_blank">https://doi.org/10.1103/PhysRevB.99.064202</a>
dc.identifier.otherCONVID_28933264
dc.identifier.otherTUTKAID_80730
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/64274
dc.description.abstractDensity functional alloy theory is used to accurately describe the three core effects controlling the thermodynamics of random Cu-Au alloys. These three core effects are exchange correlation (XC), local lattice relaxations (LLRs), and short-range order (SRO). Within the real-space grid-based projector augmented-wave (GPAW) method based on density functional theory (DFT), we adopt the quasinonuniform XC approximation (QNA), and take into account the LLR and the SRO effects. Our approach allows us to study the importance of all three core effects in a unified way within one DFT code. The results demonstrate the importance of the LLR term and show that going from the classical gradient level approximations to QNA leads to accurate formation energies at various degrees of ordering. The order-disorder transition temperatures for the 25%, 50%, and 75% alloys reach quantitative agreement with the experimental values only when also the SRO effects are considered. © 2019 American Physical Society.en
dc.format.mimetypeapplication/pdf
dc.languageeng
dc.language.isoeng
dc.publisherAmerican Physical Society
dc.relation.ispartofseriesPhysical Review B
dc.rightsIn Copyright
dc.subject.otherelectronic structure
dc.subject.otherfirst-principles calculations
dc.subject.otherBinary alloys
dc.subject.otherCopper alloys
dc.subject.otherGold alloys
dc.subject.otherLunar surface analysis
dc.subject.otherThermodynamics
dc.subject.otherDensity functional theory
dc.titleDensity functional theory description of random Cu-Au alloys
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-201905292861
dc.contributor.laitosKemian laitosfi
dc.contributor.laitosDepartment of Chemistryen
dc.type.urihttp://purl.org/eprint/type/JournalArticle
dc.date.updated2019-05-29T06:15:14Z
dc.type.coarhttp://purl.org/coar/resource_type/c_2df8fbb1
dc.description.reviewstatuspeerReviewed
dc.relation.issn2469-9950
dc.relation.numberinseries6
dc.relation.volume99
dc.type.versionpublishedVersion
dc.rights.copyright© 2019 American Physical Society.
dc.rights.accesslevelopenAccessfi
dc.relation.grantnumber295602
dc.subject.ysotiheysfunktionaaliteoria
dc.subject.ysometalliseokset
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p28852
jyx.subject.urihttp://www.yso.fi/onto/yso/p4519
dc.rights.urlhttp://rightsstatements.org/page/InC/1.0/?language=en
dc.relation.doi10.1103/PhysRevB.99.064202
dc.relation.funderSuomen Akatemiafi
dc.relation.funderResearch Council of Finlanden
jyx.fundingprogramTutkijatohtori, SAfi
jyx.fundingprogramPostdoctoral Researcher, AoFen
jyx.fundinginformationThe authors thank the Swedish Research Council, the Swedish Foundation for Strategic Research, the Swedish Foundation for International Cooperation in Research and Higher Education, the Swedish Energy Agency, the Hungarian Scientific Research Fund (OTKA) Grants No. K128229 and No. K123988, and Academy of Finland (Grant No. 295602) for financial support. The Finnish IT Center for Science (CSC), the Finnish Grid and Cloud Infrastructure (FGCI) project, and the Swedish National Infrastructure for Computing (SNIC) at the High Performance Computing Center North (HPC2N) are acknowledged for the computational resources.
dc.type.okmA1


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