2,501 research outputs found

    Phase separation and valence instabilities in cuprate superconductors. Effective one-band model approach

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    We study the Cu-O valence instability (VI) and the related phase separation (PS) driven by Cu-O nearest-neighbor repulsion UpdU_{pd}, using an effective extended one-band Hubbard model (HeffH_{eff}) obtained from the extended three-bandHubbard model, through an appropriate low-energy reduction. HeffH_{eff} is solved by exact diagonalization of a square cluster with 10 unit cells and also within a slave-boson mean-field theory. Its parameters depend on doping for Upd0U_{pd}\neq 0 or on-site O repulsion Up0U_p\neq 0. The results using both techniques coincide in that there is neither VI nor PS for doping levels x<0.5x<0.5 if Upd2U_{pd}\lesssim 2 eV. The PS region begins for Upd2U_{pd}\gtrsim 2 eV at large doping x>0.6x>0.6 and increases with increasing UpdU_{pd}. The PS also increases with increasing on-site Cu repulsion UdU_d.Comment: 16 pages and 10 figures in postscript format, compressed with uufile

    Constraints on the χ_(c1) versus χ_(c2) polarizations in proton-proton collisions at √s = 8 TeV

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    The polarizations of promptly produced χ_(c1) and χ_(c2) mesons are studied using data collected by the CMS experiment at the LHC, in proton-proton collisions at √s=8  TeV. The χ_c states are reconstructed via their radiative decays χ_c → J/ψγ, with the photons being measured through conversions to e⁺e⁻, which allows the two states to be well resolved. The polarizations are measured in the helicity frame, through the analysis of the χ_(c2) to χ_(c1) yield ratio as a function of the polar or azimuthal angle of the positive muon emitted in the J/ψ → μ⁺μ⁻ decay, in three bins of J/ψ transverse momentum. While no differences are seen between the two states in terms of azimuthal decay angle distributions, they are observed to have significantly different polar anisotropies. The measurement favors a scenario where at least one of the two states is strongly polarized along the helicity quantization axis, in agreement with nonrelativistic quantum chromodynamics predictions. This is the first measurement of significantly polarized quarkonia produced at high transverse momentum
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