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      Polarizing an antiferromagnet by optical engineering of the crystal field

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          Antiferromagnetic spintronics

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            Divergent Nematic Susceptibility in an Iron Arsenide Superconductor

            Within the Landau paradigm of continuous phase transitions, ordered states of matter are characterized by a broken symmetry. Although the broken symmetry is usually evident, determining the driving force behind the phase transition can be complicated by coupling between distinct order parameters. We show how measurement of the divergent nematic susceptibility of the iron pnictide superconductor Ba(Fe(1-x)Co(x))(2)As(2) distinguishes an electronic nematic phase transition from a simple ferroelastic distortion. These measurements also indicate an electronic nematic quantum phase transition near the composition with optimal superconducting transition temperature.
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              Strong increase of T(c) of Sr₂RuO₄ under both tensile and compressive strain.

              A sensitive probe of unconventional order is its response to a symmetry-breaking field. To probe the proposed p(x) ± ip(y) topological superconducting state of Sr2RuO4, we have constructed an apparatus capable of applying both compressive and tensile strains of up to 0.23%. Strains applied along ⟨100⟩ crystallographic directions yield a strong, strain-symmetric increase in the superconducting transition temperature T(c). ⟨110⟩ strains give a much weaker, mostly antisymmetric response. As well as advancing the understanding of the superconductivity of Sr2RuO4, our technique has potential applicability to a wide range of problems in solid-state physics.
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                Author and article information

                Journal
                Nature Physics
                Nat. Phys.
                Springer Science and Business Media LLC
                1745-2473
                1745-2481
                June 22 2020
                Article
                10.1038/s41567-020-0936-3
                7b72ad1e-c9dc-456b-afa3-3b28efff077b
                © 2020

                http://www.springer.com/tdm

                http://www.springer.com/tdm

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