2,485 research outputs found

    The Effects of Negative Legacies on the Adjustment of Parentally Bereaved Children and Adolescents

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    This is a report of a qualitative analysis of a sample of bereaved families in which one parent died and in which children scored in the clinical range on the Child Behavior Check List. The purpose of this analysis was to learn more about the lives of these children. They were considered to be at risk of developing emotional and behavioral problems associated with the death. We discovered that many of these “high risk” children had a continuing bond with the deceased that was primarily negative and troubling for them in contrast to a comparison group of children not at risk from the same study. Five types of legacies, not mutually exclusive, were identified: health related, role related, personal qualities, legacy of blame, and an emotional legacy. Coping behavior on the part of the surviving parent seemed to make a difference in whether or not a legacy was experienced as negative

    CP-violating asymmetries in B^0 decays to K^+K^-K_{S(L)}^0 and K_S^0K_S^0K_{S(L)}^0

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    Decay rates and time-dependent and direct CP asymmetries in the decays B0→K+K−KS(L)B^0\to K^+K^-K_{S(L)} and KSKSKS(L)K_S K_S K_{S(L)} are studied. Resonant and nonresonant contributions to the three-body decays are carefully investigated. Nonresonant effects on 2-body and 3-body matrix elements are constrained by QCD counting rules. The predicted branching ratios are consistent with the data within the theoretical and experimental errors, though the theoretical central values are somewhat smaller than the experimental ones. Owing to the presence of color-allowed tree amplitudes in B0→K+K−KS(L)B^0\to K^+K^-K_{S(L)}, this penguin-dominated mode is subject to a significant tree pollution and the deviation of the mixing-induced \CP asymmetry from that measured in B→J/ψKSB\to J/\psi K_S, namely, Δsin⁥2ÎČK+K−KS(L)≡sin⁥2ÎČK+K−KS(L)−sin⁥2ÎČJ/ψKS\Delta \sin 2\beta_{K^+K^-K_{S(L)}}\equiv \sin 2\beta_{K^+K^-K_{S(L)}}-\sin 2 \beta_{J/\psi K_S}, can be as large as O(0.10). In contrast, the KSKSKS(L)K_SK_SK_{S(L)} modes appear theoretically very clean in our picture with negligible Δsin⁥2ÎČKSKSKS(L)\Delta\sin 2\beta_{K_SK_SK_{S(L)}}. Direct CP asymmetries in K+K−KS(L)K^+K^-K_{S(L)} and KSKSKS(L)K_S K_S K_{S(L)} modes are found to be very small.Comment: 17 pages and 2 figures, the tree contribution is modified due to the new data from BaBar, to appear in Phys. Rev.

    Chirality Correlation within Dirac Eigenvectors from Domain Wall Fermions

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    In the dilute instanton gas model of the QCD vacuum, one expects a strong spatial correlation between chirality and the maxima of the Dirac eigenvectors with small eigenvalues. Following Horvath, {\it et al.} we examine this question using lattice gauge theory within the quenched approximation. We extend the work of those authors by using weaker coupling, ÎČ=6.0\beta=6.0, larger lattices, 16416^4, and an improved fermion formulation, domain wall fermions. In contrast with this earlier work, we find a striking correlation between the magnitude of the chirality density, âˆŁÏˆâ€ (x)Îł5ψ(x)∣|\psi^\dagger(x)\gamma^5\psi(x)|, and the normal density, ψ†(x)ψ(x)\psi^\dagger(x)\psi(x), for the low-lying Dirac eigenvectors.Comment: latex, 25 pages including 12 eps figure

    Combinations of idelalisib with rituximab and/or bendamustine in patients with recurrent indolent non-Hodgkin lymphoma

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    Key Points Combining phosphatidylinositol-3-kinase ÎŽ inhibition with rituximab, bendamustine, or both is feasible and active in relapsed iNHL. The safety of novel combinations should be proven in phase 3 trials before adoption in clinical practice.</jats:p

    Vortex State of Tl2_2Ba2_2CuO6+ÎŽ_{6+\delta} via 205^{205}Tl NMR at 2 Tesla

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    We report a 205^{205}Tl NMR study of vortex state for an aligned polycrystalline sample of an overdoped high-TcT_c superconductor Tl2_2Ba2_2CuO6+ÎŽ_{6+\delta} (Tc∌T_{c}\sim85 K) with magnetic field 2 T along the c axis. We observed an imperfect vortex lattice, so-called Bragg glass at TT=5 K, coexistence of vortex solid with liquid between 10 and 60 K, and vortex melting between 65 and 85 K. No evidence for local antiferromagnetic ordering at vortex cores was found for our sample.Comment: 4 pages with 5 figure

    Analysis of a three-component model phase diagram by Catastrophe Theory

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    We analyze the thermodynamical potential of a lattice gas model with three components and five parameters using the methods of Catastrophe Theory. We find the highest singularity, which has codimension five, and establish its transversality. Hence the corresponding seven-degree Landau potential, the canonical form Wigwam or A6A_6, constitutes the adequate starting point to study the overall phase diagram of this model.Comment: 16 pages, Latex file, submitted to Phys. Rev.

    Nucleon axial charge from quenched lattice QCD with domain wall fermions

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    We present a quenched lattice calculation of the nucleon isovector vector and axial-vector charges gV and gA. The chiral symmetry of domain wall fermions makes the calculation of the nucleon axial charge particularly easy since the Ward-Takahashi identity requires the vector and axial-vector currents to have the same renormalization, up to lattice spacing errors of order O(a^2). The DBW2 gauge action provides enhancement of the good chiral symmetry properties of domain wall fermions at larger lattice spacing than the conventional Wilson gauge action. Taking advantage of these methods and performing a high statistics simulation, we find a significant finite volume effect between the nucleon axial charges calculated on lattices with (1.2 fm)^3 and (2.4 fm)^3 volumes (with lattice spacing, a, of about 0.15 fm). On the large volume we find gA = 1.212 +/- 0.027(statistical error) +/- 0.024(normalization error). The quoted systematic error is the dominant (known) one, corresponding to current renormalization. We discuss other possible remaining sources of error. This theoretical first principles calculation, which does not yet include isospin breaking effects, yields a value of gA only a little bit below the experimental one, 1.2670 +/- 0.0030.Comment: 38 pages, 12 figures, 9 tables, Revtex. Version accepted for publication in Physical Review

    Epitaxial growth of Cu on Cu(001): experiments and simulations

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    A quantitative comparison between experimental and Monte Carlo simulation results for the epitaxial growth of Cu/Cu(001) in the submonolayer regime is presented. The simulations take into account a complete set of hopping processes whose activation energies are derived from semi-empirical calculations using the embedded-atom method. The island separation is measured as a function of the incoming flux and the temperature. A good quantitative agreement between the experiment and simulation is found for the island separation, the activation energies for the dominant processes, and the exponents that characterize the growth. The simulation results are then analyzed at lower coverages, which are not accessible experimentally, providing good agreement with theoretical predictions as well.Comment: Latex document. 7 pages. 3 embedded figures in separate PS files. One bbl fil
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