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      Evidence of an odd-parity hidden order in a spin–orbit coupled correlated iridate

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          From quantum matter to high-temperature superconductivity in copper oxides.

          The discovery of high-temperature superconductivity in the copper oxides in 1986 triggered a huge amount of innovative scientific inquiry. In the almost three decades since, much has been learned about the novel forms of quantum matter that are exhibited in these strongly correlated electron systems. A qualitative understanding of the nature of the superconducting state itself has been achieved. However, unresolved issues include the astonishing complexity of the phase diagram, the unprecedented prominence of various forms of collective fluctuations, and the simplicity and insensitivity to material details of the 'normal' state at elevated temperatures.
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            Phase-sensitive observation of a spin-orbital Mott state in Sr2IrO4.

            Measurement of the quantum-mechanical phase in quantum matter provides the most direct manifestation of the underlying abstract physics. We used resonant x-ray scattering to probe the relative phases of constituent atomic orbitals in an electronic wave function, which uncovers the unconventional Mott insulating state induced by relativistic spin-orbit coupling in the layered 5d transition metal oxide Sr2IrO4. A selection rule based on intra-atomic interference effects establishes a complex spin-orbital state represented by an effective total angular momentum = 1/2 quantum number, the phase of which can lead to a quantum topological state of matter.
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              NovelJeff=1/2Mott State Induced by Relativistic Spin-Orbit Coupling inSr2IrO4

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                Author and article information

                Journal
                Nature Physics
                Nature Phys
                Springer Science and Business Media LLC
                1745-2473
                1745-2481
                January 2016
                October 26 2015
                January 2016
                : 12
                : 1
                : 32-36
                Article
                10.1038/nphys3517
                5de0017f-51e1-4412-af0d-7df96f64efe3
                © 2016

                http://www.springer.com/tdm

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