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    The spin resonance and high frequency optical properties of the cuprates

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    We argue that recently observed superconductivity-induced blue shift of the plasma frequency δωpl\delta \omega_{pl} in Bi2Sr2CaCu2O8+δBi_2Sr_2CaCu_2O_{8+\delta} is related to the change in the integrated dynamical structure factor associated with the development of the spin resonance below TcT_c. We show that the magnitude of δωpl\delta \omega_{pl} is consistent with the small integrated spectral weight of the resonance, and its temperature dependences closely follow that of the spin resonance peak.Comment: 5 pages, 3 figure

    DHCR7 mutations linked to higher vitamin D status allowed early human migration to Northern latitudes

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    PMCID: PMC3708787This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited

    Dispersion Anomalies in Cuprate Superconductors

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    We argue that the shape of the dispersion along the nodal and antinodal directions in the cuprates can be understood as a consequence of the interaction of the electrons with collective spin excitations. In the normal state, the dispersion displays a crossover at an energy where the decay into spin fluctuations becomes relevant. In the superconducting state, the antinodal dispersion is strongly affected by the spin resonance and displays an S-shape whose magnitude scales with the resonance intensity. For nodal fermions, relevant spin excitations do not have resonance behavior, rather they are better characterized as a gapped continuum. As a consequence, the S-shape becomes a kink, and superconductivity does not affect the dispersion as strongly. Finally, we note that optical phonons typically lead to a temperature independent S-shape, in disagreement with the observed dispersion.Comment: 12 pages, 7 eps figure
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