Corrigendum to “A general approach to simulate the atom distribution, lattice distortion, and mechanical properties of multi-principal element alloys based on site preference: Using FCC_CoNiV and CoCrNi to demonstrate and compare” [J. Alloy. Compd. 935(1) (2023) 168016] (Journal of Alloys and Compounds (2023) 935(P1), (S0925838822044073), (10.1016/j.jallcom.2022.168016)) - Details

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Correction　contents:　At　the　time,　the　author　calculated　three　systems.　The　author　deleted　the　FCC_CoCrNi　involved　in　this　paper　by　accident　and　left　the　system　that　needed　to　be　deleted.　As　a　result,　we　want　to　change　Fig.　3　into　the　following　Figure,　which　will　have　no　effect　on　the　previous　conclusion　after　modification.　The　authors　regret　“insert　corrigendum　text”.　[Formula　presented]　Fig.　3.　The　configuration　entropies　change　with　the　heat　treatment　temperature　for　the　FCC_CoNiV　and　CoCrNi　MPEAs,　respectively,　superimposed　the　configurational　entropies　of　ideal　mixing　solid　solution　alloy　FCC　phase　calculated　using　the　Boltzmann　formula　for　comparison.　[Formula　presented]　Fig.　3.　The　configuration　entropies　change　with　the　heat　treatment　temperature　for　the　FCC_CoNiV　and　CoCrNi　MPEAs,　respectively,　superimposed　the　configurational　entropies　of　ideal　mixing　solid　solution　alloy　FCC　phase　calculated　using　the　Boltzmann　formula　for　comparison.　Correction　contents:　The　positions　of　the　two　figures　in　Fig.　5(b)　are　reversed　due　to　the　author＇s　carelessness.　We＇d　like　to　replace　them　with　the　Figures　below,　which　will　have　no　effect　on　the　previous　conclusion.　The　authors　regret　“insert　corrigendum　text”.　[Formula　presented]　Fig.　5.　The　atoms　distribution　with　the　real　relative　size　of　FCC_CoNiV　MPA,　with　the　same　occupying　behavior　at　all　temperature.　(a)　Bulk　distribution　of　each　type　of　atom　of　FCC_CoNiV　MPA　(with　the　same　configuration　at　all　temperature).(b)　Slice　distribution　of　each　type　of　atom　on　close-packed　crystal　face　(111)　FCC_CoNiV　MPA　(the　same　configuration　at　all　temperature).(c)　Construction　of　a　30　×　30　×　30　FCC　supercell　based　on　the　prototype　of　L12_AuCu3　for　FCC_CoNiV　MPA　at　all　temperature.(d)　Slice　distribution　of　atom　on　close-packed　crystal　face　(111)　according　to　each　sublattice　in　FCC_CoNiV　MPA　at　973　K,　notice　that　this　alloy　presents　the　same　occupying　behavior　at　all　temperature.　[Formula　presented]　Fig.　5.　The　atoms　distribution　with　the　real　relative　size　of　FCC_CoNiV　MPA,　with　the　same　occupying　behavior　at　all　temperature.　(a)　Bulk　distribution　of　each　type　of　atom　of　FCC_CoNiV　MPA　(with　the　same　configuration　at　all　temperature).(b)　Slice　distribution　of　each　type　of　atom　on　close-packed　crystal　face　(111)　FCC_CoNiV　MPA　(the　same　configuration　at　all　temperature).(c)　Construction　of　a　30　×　30　×　30　FCC　supercell　based　on　the　prototype　of　L12_AuCu3　for　FCC_CoNiV　MPA　at　all　temperature.(d)　Slice　distribution　of　atom　on　close-packed　crystal　face　(111)　according　to　each　sublattice　in　FCC_CoNiV　MPA　at　973　K,　notice　that　this　alloy　presents　the　same　occupying　behavior　at　all　temperature.Correction　contents:　The　positions　of　some　figures　in　Figs.　13　and　14　have　been　changed　due　to　the　author＇s　carelessness.　We　want　to　change　them　into　the　Figures　below,　which　will　have　no　effect　on　the　previous　calculation　results.　The　authors　regret　“insert　corrigendum　text”.　[Formula　presented]　Fig.　13.　Construction　of　a　3　[Formula　presented]　3　[Formula　presented]　3　FCC　supercell　based　on　the　prototype　of　L12_AuCu3　and　the　SOFs　at　973　K　for　FCC_CoNiV　and　CoCrNi　MPEAs　with　sublattice　nested,　respectively.　(a)　FCC_CoNiV.　(b)　FCC_CoCrNi.　[Formula　presented]　Fig.　14.　Construction　of　a　3　[Formula　presented]　3　[Formula　presented]　3　FCC　supercell　based　on　the　prototype　of　L12_AuCu3　and　atom　random　distributing　on　the　full　crystal　lattice　for　FCC_CoNiV　and　CoCrNi　MPEAs　based　on　SQS　approach,　respectively.　(a)　FCC_CoNiV.　(b)　FCC_CoCrNi.　[Formula　presented]　Fig.　13.　Construction　of　a　3　[Formula　presented]　3　[Formula　presented]　3　FCC　supercell　based　on　the　prototype　of　L12_AuCu3　and　the　SOFs　at　973　K　for　FCC_CoNiV　and　CoCrNi　MPEAs　with　sublattice　nested,　respectively.　(a)　FCC_CoNiV.　(b)　FCC_CoCrNi.　[Formula　presented]　Fig.　14.　Construction　of　a　3　[Formula　presented]　3　[Formula　presented]　3　FCC　supercell　based　on　the　prototype　of　L12_AuCu3　and　atom　random　distributing　on　the　full　crystal　lattice　for　FCC_CoNiV　and　CoCrNi　MPEAs　based　on　SQS　approach,　respectively.　(a)　FCC_CoNiV.　(b)　FCC_CoCrNi.　Correction　contents:　We　would　like　to　change　the　third　example　in　Table　4　to　the　following　image　because　we　forgot　to　delete　it.　Which　will　have　no　effect　on　the　previous　conclusion.　The　authors　regret　“insert　corrigendum　text”.　Table　4　Lattice　constant,　relative　lattice　distortion,　total　energy,　and　total　magmom　of　FCC_CoNiV　and　CoCrNi　MPEAs.　[Table　presented]　Table　4　Lattice　constant,　relative　lattice　distortion,　total　energy,　and　total　magmom　of　FCC_CoNiV　and　CoCrNi　MPEAs.　[Table　presented]　The　authors　would　like　to　apologize　for　any　inconvenience　caused.　©　2023　Elsevier　B.V.

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[ 1 ] [Chen R.]Multiscale Computational Materials Facility, Key Laboratory of Eco-Materials Advanced Technology, College of Materials Science and Engineering, Fuzhou University, Fuzhou, 350100, China
[ 2 ] [Xie T.]Multiscale Computational Materials Facility, Key Laboratory of Eco-Materials Advanced Technology, College of Materials Science and Engineering, Fuzhou University, Fuzhou, 350100, China
[ 3 ] [Wu B.]Multiscale Computational Materials Facility, Key Laboratory of Eco-Materials Advanced Technology, College of Materials Science and Engineering, Fuzhou University, Fuzhou, 350100, China
[ 4 ] [Wu B.]Materials Design and Manufacture Simulation Facility, School of Advance Manufacturing, Fuzhou University, Jinjiang, 362200, China
[ 5 ] [Weng L.]Multiscale Computational Materials Facility, Key Laboratory of Eco-Materials Advanced Technology, College of Materials Science and Engineering, Fuzhou University, Fuzhou, 350100, China
[ 6 ] [Ali H.]Multiscale Computational Materials Facility, Key Laboratory of Eco-Materials Advanced Technology, College of Materials Science and Engineering, Fuzhou University, Fuzhou, 350100, China
[ 7 ] [Yang S.]Materials Design and Manufacture Simulation Facility, School of Advance Manufacturing, Fuzhou University, Jinjiang, 362200, China
[ 8 ] [Zhao Y.]Multiscale Computational Materials Facility, Key Laboratory of Eco-Materials Advanced Technology, College of Materials Science and Engineering, Fuzhou University, Fuzhou, 350100, China
[ 9 ] [Zhao P.]Materials Design and Manufacture Simulation Facility, School of Advance Manufacturing, Fuzhou University, Jinjiang, 362200, China
[ 10 ] [Zhang C.]Materials Design and Manufacture Simulation Facility, School of Advance Manufacturing, Fuzhou University, Jinjiang, 362200, China
[ 11 ] [Cao R.]Multiscale Computational Materials Facility, Key Laboratory of Eco-Materials Advanced Technology, College of Materials Science and Engineering, Fuzhou University, Fuzhou, 350100, China
[ 12 ] [Wen J.]Multiscale Computational Materials Facility, Key Laboratory of Eco-Materials Advanced Technology, College of Materials Science and Engineering, Fuzhou University, Fuzhou, 350100, China
[ 13 ] [Yao Q.]Multiscale Computational Materials Facility, Key Laboratory of Eco-Materials Advanced Technology, College of Materials Science and Engineering, Fuzhou University, Fuzhou, 350100, China
[ 14 ] [Cai Q.]Multiscale Computational Materials Facility, Key Laboratory of Eco-Materials Advanced Technology, College of Materials Science and Engineering, Fuzhou University, Fuzhou, 350100, China
[ 15 ] [Zhang H.]Materials Design and Manufacture Simulation Facility, School of Advance Manufacturing, Fuzhou University, Jinjiang, 362200, China
[ 16 ] [Zhang H.]Central Iron & Steel Research Institute Group, Beijing, 100081, China
[ 17 ] [Sa B.]Multiscale Computational Materials Facility, Key Laboratory of Eco-Materials Advanced Technology, College of Materials Science and Engineering, Fuzhou University, Fuzhou, 350100, China
[ 18 ] [Wen C.]Multiscale Computational Materials Facility, Key Laboratory of Eco-Materials Advanced Technology, College of Materials Science and Engineering, Fuzhou University, Fuzhou, 350100, China
[ 19 ] [Lin M.]Department of Ocean and Mechanical Engineering, Florida Atlantic University, Boca Raton, 33431, United States
[ 20 ] [Sun X.]Central Iron & Steel Research Institute Group, Beijing, 100081, China
[ 21 ] [Su H.]Central Iron & Steel Research Institute Group, Beijing, 100081, China
[ 22 ] [Liu Y.]Central Iron & Steel Research Institute Group, Beijing, 100081, China
[ 23 ] [Wang C.]Central Iron & Steel Research Institute Group, Beijing, 100081, China

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