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      Room Temperature Electrocaloric Effect in 2D Ferroelectric CuInP\(_2\)S\(_6\) for Nano-refrigerators

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          Abstract

          A material with reversible temperature change capability under an external electric field, known as the electrocaloric effect (ECE), has long been considered as a promising solid-state cooling solution. However, electrocaloric (EC) performance of EC materials generally is not sufficiently high for real cooling applications. As a result, exploring new EC materials with high performance is of great interest and importance. Here, we report on the ECE of a new class of EC material, the 2D ferroelectric materials (CuInP\(_2\)S\(_6\) or CIPS in this work in particular) for the first time. Over 60% polarization charge change is observed within a temperature change of only 10 K at Curie temperature, as the result of a second order phase transition in CIPS. Large adiabatic temperature change (|{\Delta}T|) of 3.5 K, isothermal entropy change (|{\Delta}S|) of 6.1 J kg\(^{-1}\) K\(^{-1}\) at |{\Delta}E|=142.0 kV cm\(^{-1}\) at 315 K (above and near room temperature) are achieved, with a large EC strength (|{\Delta}T|/|{\Delta}E|) of 29.2 mK cm kV\(^{-1}\). The ECE of CIPS is also investigated theoretically by numerical simulation and a further EC performance projection is provided.

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          Giant electrocaloric effect in thin film Pb Zr_0.95 Ti_0.05 O_3

          An applied electric field can reversibly change the temperature of an electrocaloric material under adiabatic conditions, and the effect is strongest near phase transitions. This phenomenon has been largely ignored because only small effects (0.003 K V^-1) have been seen in bulk samples such as Pb0.99Nb0.02(Zr0.75Sn0.20Ti0.05)0.98O3 and there is no consensus on macroscopic models. Here we demonstrate a giant electrocaloric effect (0.48 K V^-1) in 300 nm sol-gel PbZr0.95Ti0.05O3 films near the ferroelectric Curie temperature of 222oC. We also discuss a solid state device concept for electrical refrigeration that has the capacity to outperform Peltier or magnetocaloric coolers. Our results resolve the controversy surrounding macroscopic models of the electrocaloric effect and may inspire ab initio calculations of electrocaloric parameters and thus a targeted search for new materials.
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            Room-temperature ferroelectricity in CuInP2S6 ultrathin flakes

            Two-dimensional (2D) materials have emerged as promising candidates for various optoelectronic applications based on their diverse electronic properties, ranging from insulating to superconducting. However, cooperative phenomena such as ferroelectricity in the 2D limit have not been well explored. Here, we report room-temperature ferroelectricity in 2D CuInP2S6 (CIPS) with a transition temperature of ∼320 K. Switchable polarization is observed in thin CIPS of ∼4 nm. To demonstrate the potential of this 2D ferroelectric material, we prepare a van der Waals (vdW) ferroelectric diode formed by CIPS/Si heterostructure, which shows good memory behaviour with on/off ratio of ∼100. The addition of ferroelectricity to the 2D family opens up possibilities for numerous novel applications, including sensors, actuators, non-volatile memory devices, and various vdW heterostructures based on 2D ferroelectricity.
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              CuInP₂S₆ Room Temperature Layered Ferroelectric.

              We explore ferroelectric properties of cleaved 2-D flakes of copper indium thiophosphate, CuInP2S6 (CITP), and probe size effects along with limits of ferroelectric phase stability, by ambient and ultra high vacuum scanning probe microscopy. CITP belongs to the only material family known to display ferroelectric polarization in a van der Waals, layered crystal at room temperature and above. Our measurements directly reveal stable, ferroelectric polarization as evidenced by domain structures, switchable polarization, and hysteresis loops. We found that at room temperature the domain structure of flakes thicker than 100 nm is similar to the cleaved bulk surfaces, whereas below 50 nm polarization disappears. We ascribe this behavior to a well-known instability of polarization due to depolarization field. Furthermore, polarization switching at high bias is also associated with ionic mobility, as evidenced both by macroscopic measurements and by formation of surface damage under the tip at a bias of 4 V-likely due to copper reduction. Mobile Cu ions may therefore also contribute to internal screening mechanisms. The existence of stable polarization in a van-der-Waals crystal naturally points toward new strategies for ultimate scaling of polar materials, quasi-2D, and single-layer materials with advanced and nonlinear dielectric properties that are presently not found in any members of the growing "graphene family".
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                Author and article information

                Journal
                19 January 2019
                Article
                1901.06616
                feaada04-f25b-4033-9f95-38fb71ffaae0

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

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                Custom metadata
                19 pages, 10 figures
                cond-mat.mtrl-sci cond-mat.mes-hall physics.app-ph

                Condensed matter,Technical & Applied physics,Nanophysics
                Condensed matter, Technical & Applied physics, Nanophysics

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