2022
DOI: 10.1039/d2cp00559j
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Sizable magnetic entropy change in bismuth-substituted La0.75Bi0.1Na0.15MnO3 manganite

Abstract: The sample La0.75Bi0.1Na0.15MnO3 exhibits large ΔSMaxm of 4.4 J kg−1 K−1 near room temperature (RT) at low field of 1.5 T (LF). The coexistence of long and short-range interactions leading to first order like phase transition is responsible for LFRT magnetic entropy change.

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Cited by 3 publications
(4 citation statements)
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“…In the above discussion, the relative cooling power (RCP) was used to evaluate the cooling efficiency, which is inadequate especially for materials with low entropy change. [ 44 ] For low entropy change materials, the temperature averaged entropy change (TEC) is an appropriate parameter compared with that of RCP. Therefore, we further estimated the TEC of FMSP according to the equation TEC(Tlift)=1normalΔTlift0.33em[TmidnormalΔTlift2TmidnormalΔTlift2ΔS(T)ΔH;TdT]${\rm{TEC}}( {{T}_{lift}} ) = \frac{1}{{\Delta {T}_{lift}}}\ [ {\int_{{{T}_{mid} - \frac{{\Delta {T}_{lift}}}{2}}}^{{{T}_{mid} - \frac{{\Delta {T}_{lift}}}{2}}}{{\Delta S{{( T )}}_{\Delta H;T}dT}}} ]$.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…In the above discussion, the relative cooling power (RCP) was used to evaluate the cooling efficiency, which is inadequate especially for materials with low entropy change. [ 44 ] For low entropy change materials, the temperature averaged entropy change (TEC) is an appropriate parameter compared with that of RCP. Therefore, we further estimated the TEC of FMSP according to the equation TEC(Tlift)=1normalΔTlift0.33em[TmidnormalΔTlift2TmidnormalΔTlift2ΔS(T)ΔH;TdT]${\rm{TEC}}( {{T}_{lift}} ) = \frac{1}{{\Delta {T}_{lift}}}\ [ {\int_{{{T}_{mid} - \frac{{\Delta {T}_{lift}}}{2}}}^{{{T}_{mid} - \frac{{\Delta {T}_{lift}}}{2}}}{{\Delta S{{( T )}}_{\Delta H;T}dT}}} ]$.…”
Section: Resultsmentioning
confidence: 99%
“…In the above discussion, the relative cooling power (RCP) was used to evaluate the cooling efficiency, which is inadequate especially for materials with low entropy change. [44] For low entropy change materials, the temperature averaged entropy change (TEC) is an appropriate parameter compared with that of RCP. Therefore, we further estimated the TEC of FMSP according to the equation TEC( [45] The estimated TEC for field changes of 0-0.5 to 0-1.5 T and ΔT lift of 2, 3, 6, and 9 K for both 𝜇 0 H⊥c and 𝜇 0 H//c are displayed in Figure 5.…”
Section: Resultsmentioning
confidence: 99%
“…A few examples for this class of materials with a giant MCE are Gd 5 Si 2 Ge 2 , 5,6 Fe-Rh alloys, 7,8 La(Fe,Si) 13 -based alloys, 9,10 MnAs Heusler alloys [11][12][13] and RE 1Àx A x Mn 1Ày TM y O 3 (RE -rare earth metal, A -divalent/monovalent ion, TM -transition metal) perovskite manganites. [14][15][16][17][18][19] Among perovskite manganites, lanthanum-based mixedvalence manganites with the general formula La 1Àx A x MnO 3 (A is mostly a divalent ion, Ca, Ba or Sr) show a variety of fascinating properties, like colossal magnetoresistance (CMR), [20][21][22] charge ordering (CO), 23,24 phase separation (PS), 25,26 the magnetocaloric effect (MCE), 1,[27][28][29][30] etc. For (La,Ca)MnO 3 , both end members LaMnO 3 and CaMnO 3 are typical antiferromagnets with T N close to 140 K and 130 K, respectively.…”
Section: Introductionmentioning
confidence: 99%
“…Among perovskite manganites, lanthanum-based mixed-valence manganites with the general formula La 1− x A x MnO 3 (A is mostly a divalent ion, Ca, Ba or Sr) show a variety of fascinating properties, like colossal magnetoresistance (CMR), 20–22 charge ordering (CO), 23,24 phase separation (PS), 25,26 the magnetocaloric effect (MCE), 1,27–30 etc. For (La,Ca)MnO 3 , both end members LaMnO 3 and CaMnO 3 are typical antiferromagnets with T N close to 140 K and 130 K, respectively.…”
Section: Introductionmentioning
confidence: 99%