2020
DOI: 10.1039/d0ma00652a
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Near-room-temperature reversible giant barocaloric effects in [(CH3)4N]Mn[N3]3 hybrid perovskite

Abstract: We report giant reversible barocaloric effects in [(CH3)4N]Mn[N3]3 hybrid organic-inorganic perovskite, near its first-order cubic-monoclinic structural phase transition at T0 ~ 305 K. When driving the transition thermally at atmospheric...

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Cited by 35 publications
(25 citation statements)
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“…In particular, typical dT/dp values lie in the range 100-200 K GPa −1 (despite values of up to ~400 K GPa -1 have been reached [51]) that may lead to large ∆T at very low pressure changes, which may result in very good cooling performance. Examples include hybrid organic-inorganic perovskites (HOIPs) [51][52][53][54][55] and spin-crossover (SCO) transitions [56][57][58][59]. In HOIPs, giant transition entropy changes emerge basically due to positional and rotational disorder.…”
Section: Discussionmentioning
confidence: 99%
“…In particular, typical dT/dp values lie in the range 100-200 K GPa −1 (despite values of up to ~400 K GPa -1 have been reached [51]) that may lead to large ∆T at very low pressure changes, which may result in very good cooling performance. Examples include hybrid organic-inorganic perovskites (HOIPs) [51][52][53][54][55] and spin-crossover (SCO) transitions [56][57][58][59]. In HOIPs, giant transition entropy changes emerge basically due to positional and rotational disorder.…”
Section: Discussionmentioning
confidence: 99%
“…(b)Reversible adiabatic temperature changes upon 0 → ~1 kbar pressure increase as a function of temperature. Literature data taken from: PG:[12]; C60:[13];[TPrA][Mn(dca)3]:[44]; [(CH3)4N]Mn[N3]3:[45]; MnCoGeB0.03 (asterisk):[46]; (MiNiSi)0.60(FeCoGe)0.40 (diamond) and (MiNiSi)0.61(FeCoGe)0.39 (triangle):[47]; Ni50Mn31.5Ti18.5 (circle):[48].…”
mentioning
confidence: 99%
“…[6][7][8] For a solid-state compound to be considered a good barocaloric, it should fulfill certain characteristics, specially: near-room-temperature phase transition, associated extremely large entropy changes, and easy-achievable operating pressures to avoid irreversible thermal losses. [9][10][11][12] In a first approximation, the ideal barocaloric material for commercial refrigeration would display colossal thermal changes (barocaloric effects of ΔS > 100 J K -1 kg -1 ) near ambient temperature (from ~315 K down to ~273 K, or even lower in the case of freezing devices), and under the application of pressures well-below 1000 bar. 1 Thus, it is primordial to find materials with colossal and reversible isothermal entropy changes, ΔSrev, (and adiabatic temperature changes, ΔTrev), large barocaloric coefficient (dTt/dp) and strength (ΔSrev/Δp) 13 (sensitivity to pressure) and appropiate operating temperature (Top) 14 , which is the thermal region where the barocaloric effect can be reversibly induced.…”
mentioning
confidence: 99%