1996
DOI: 10.1080/00150199608230266
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Isomorphous ion substitutions and order-disorder phenomena in highly electrocaloric lead-scandium tantalate solid solutions

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Cited by 19 publications
(8 citation statements)
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“…It exhibits a first-order ferroelectric to paraelectric (PE) phase transition near room temperature which makes it attractive for air conditioning. This transition can also be driven with an electric field leading to the EC effect, which is predominant at the material’s transition temperature 13 . The largest EC adiabatic temperature change ∆ T adiab 13 reported so far in bulk PST is 2.3 K at 50 kV cm −1 .…”
Section: Introductionmentioning
confidence: 99%
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“…It exhibits a first-order ferroelectric to paraelectric (PE) phase transition near room temperature which makes it attractive for air conditioning. This transition can also be driven with an electric field leading to the EC effect, which is predominant at the material’s transition temperature 13 . The largest EC adiabatic temperature change ∆ T adiab 13 reported so far in bulk PST is 2.3 K at 50 kV cm −1 .…”
Section: Introductionmentioning
confidence: 99%
“…This transition can also be driven with an electric field leading to the EC effect, which is predominant at the material’s transition temperature 13 . The largest EC adiabatic temperature change ∆ T adiab 13 reported so far in bulk PST is 2.3 K at 50 kV cm −1 . Lately, Nair et al 20 measured a larger ∆ T adiab of 5.5 K in PST Multi-Layer Capacitors (MLCs) when driven supercritically at 290 kV cm −1 .…”
Section: Introductionmentioning
confidence: 99%
“…In this paper, we demonstrate a general solution to the net-transfer problem by constructing cooling cycles in which no net heat is exchanged between a homogeneous working body of the archetypal EC material PST 2,18,[36][37][38][39] and an ideal hypothetical regenerator that it traverses in order to achieve a large temperature span T h -T c >> |T|. The underlying principle is that the two regenerator-transit legs of a given cooling cycle can be made to differ by a constant entropy if the field applied during the finite-field leg is varied according to a detailed E(T,S) map of the highly reversible phase transition at finite fields above Curie temperature T C ~ 295 K, where E denotes electric field, T denotes temperature, and S denotes entropy S after subtracting the zero-field entropy at our base temperature of 285 K. In contrast with the highly restrictive solutions discussed above [33][34][35] , our strategy for true regeneration via field variation can be readily achieved by modifying standard cooling cycles, such as Ericsson cycles.…”
mentioning
confidence: 99%
“…3) Following his study, many ceramic materials were studied such as SrTiO 3 4) and KTaO 3 ,5) the antiferroelectric Pb(Zr,Ti)O 3 , 6) and the ferroelectrics Roshelle salt, 3) KH 2 PO 4 , 7) BaTiO 3 , 8) TGS, 9) Pb(Zr,Ti)O 3 , 6,10) Pb(Sc,Ta)O 3 , [11][12][13][14] and Pb(Mg,Nb)O 3 -PbTiO 3 . [15][16][17] However, these temperature changes were smaller than 2.5 K. 18) In 2006, Mischenko et al suggested that a much larger ΔT appears near the para=ferro critical point.…”
Section: Introductionmentioning
confidence: 99%