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      Exchange Bias in a Layered Metal–Organic Topological Spin Glass

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          Abstract

          <p class="first" id="d463577e292"> <div class="figure-container so-text-align-c"> <img alt="" class="figure" src="/document_file/108f4d5b-0a2f-4754-9c35-cc002a64c4b3/PubMedCentral/image/oc1c00568_0007"/> </div> </p><p id="d463577e294">The discovery of conductive and magnetic two-dimensional (2D) materials is critical for the development of next generation spintronics devices. Coordination chemistry in particular represents a highly versatile, though underutilized, route toward the synthesis of such materials with designer lattices. Here, we report the synthesis of a conductive, layered 2D metal–organic kagome lattice, Mn <sub>3</sub>(C <sub>6</sub>S <sub>6</sub>), using mild solution-phase chemistry. Strong geometric spin frustration in this system mediates spin freezing at low temperatures, which results in glassy magnetic dynamics consistent with a rare geometrically frustrated (topological) spin glass. Notably, we show that this geometric frustration engenders a large, tunable exchange bias of 1625 Oe in Mn <sub>3</sub>(C <sub>6</sub>S <sub>6</sub>), providing the first example of exchange bias in a coordination solid or a topological spin glass. Exchange bias is a critical component in a number of spintronics applications, but it is difficult to rationally tune, as it typically arises due to structural disorder. This work outlines a new strategy for engineering exchange bias systems using single-phase, crystalline lattices. More generally, these results demonstrate the potential utility of geometric frustration in the design of new nanoscale spintronic materials. </p><p class="first" id="d463577e316">Classic exchange bias relies on a disordered interface between a ferromagnet and antiferromagnet, impeding the design of next generation systems. We show that magnetic disorder due to <i>geometric</i> frustration engenders a large, tunable exchange bias in the metal−organic kagome lattice, Mn <sub>3</sub>(C <sub>6</sub>S <sub>6</sub>). As Mn <sub>3</sub>(C <sub>6</sub>S <sub>6</sub>) is a topological spin glass, the exchange bias may be a tuning handle for exotic nonequilibrium states. This work designates designer metal−organic lattices as a platform for novel emergent physical phenomena. </p>

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          Most cited references46

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          Conduction in non-crystalline materials

          N. F. Mott (1969)
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            Two-dimensional magnetic crystals and emergent heterostructure devices

            Magnetism, originating from the moving charges and spin of elementary particles, has revolutionized important technologies such as data storage and biomedical imaging, and continues to bring forth new phenomena in emergent materials and reduced dimensions. The recently discovered two-dimensional (2D) magnetic van der Waals crystals provide ideal platforms for understanding 2D magnetism, the control of which has been fueling opportunities for atomically thin, flexible magneto-optic and magnetoelectric devices (such as magnetoresistive memories and spin field-effect transistors). The seamless integration of 2D magnets with dissimilar electronic and photonic materials opens up exciting possibilities for unprecedented properties and functionalities. We review the progress in this area and identify the possible directions for device applications, which may lead to advances in spintronics, sensors, and computing.
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              Beating the superparamagnetic limit with exchange bias.

              Interest in magnetic nanoparticles has increased in the past few years by virtue of their potential for applications in fields such as ultrahigh-density recording and medicine. Most applications rely on the magnetic order of the nanoparticles being stable with time. However, with decreasing particle size the magnetic anisotropy energy per particle responsible for holding the magnetic moment along certain directions becomes comparable to the thermal energy. When this happens, the thermal fluctuations induce random flipping of the magnetic moment with time, and the nanoparticles lose their stable magnetic order and become superparamagnetic. Thus, the demand for further miniaturization comes into conflict with the superparamagnetism caused by the reduction of the anisotropy energy per particle: this constitutes the so-called 'superparamagnetic limit' in recording media. Here we show that magnetic exchange coupling induced at the interface between ferromagnetic and antiferromagnetic systems can provide an extra source of anisotropy, leading to magnetization stability. We demonstrate this principle for ferromagnetic cobalt nanoparticles of about 4 nm in diameter that are embedded in either a paramagnetic or an antiferromagnetic matrix. Whereas the cobalt cores lose their magnetic moment at 10 K in the first system, they remain ferromagnetic up to about 290 K in the second. This behaviour is ascribed to the specific way ferromagnetic nanoparticles couple to an antiferromagnetic matrix.
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                Author and article information

                Contributors
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                Journal
                ACS Central Science
                ACS Cent. Sci.
                American Chemical Society (ACS)
                2374-7943
                2374-7951
                August 25 2021
                July 20 2021
                August 25 2021
                : 7
                : 8
                : 1317-1326
                Affiliations
                [1 ]Department of Chemistry, University of California, Berkeley, California 94720, United States
                [2 ]Department of Physics, University of California, Berkeley, California 94720, United States
                [3 ]Liquid Sunlight Alliance, Lawrence Berkeley National Laboratory, Berkeley, California 94720 United States
                [4 ]Molecular Foundry, Lawrence Berkeley National Laboratory, Berkeley, California 94720, United States
                [5 ]Department of Chemical and Biomolecular Engineering, University of California, Berkeley, California 94720, United States
                [6 ]Chemical Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, United States
                [7 ]Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, United States
                [8 ]Kavli Energy NanoSciences Institute at Berkeley, Berkeley, California 94720, United States
                Article
                10.1021/acscentsci.1c00568
                79bd0960-30a1-401b-92d4-d72b64ac275a
                © 2021

                https://creativecommons.org/licenses/by-nc-nd/4.0/

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