47,687 research outputs found

    Identifying structures in the continuum: Application to 16^{16}Be

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    The population and decay of two-nucleon resonances offer exciting new opportunities to explore dripline phenomena. The understanding of these systems requires a solid description of the three-body (core+N+N) continuum. The identification of a state with resonant character from the background of non-resonant continuum states in the same energy range poses a theoretical challenge. It is the purpose of this work to establish a robust theoretical framework to identify and characterize three-body resonances in a discrete basis. A resonance operator is proposed, which describes the sensitivity to changes in the potential. Resonances are then identified from the lowest eigenstates of the resonance operator. The operator is diagonalized in a basis of Hamiltonian pseudostates, built within the hyperspherical harmonics formalism using the analytical THO basis. The energy and width of the resonance are determined from its time dependence. The method is applied to 16Be in a 14Be+n+n model. An effective core+n potential, fitted to the available information on the subsystem 15Be, is employed. The 0+ ground state resonance of 16Be presents a strong dineutron configuration, which favors the picture of a correlated two-neutron emission. Fitting the three body interaction to the experimental two-neutron separation energy |S2n|=1.35(10) MeV, the computed width is Gamma(0+)=0.16 MeV. From the same Hamiltonian, a 2+ resonance is also predicted with E_r(2+)=2.42 MeV and Gamma(2+)=0.40 MeV. The dineutron configuration and the computed 0+ width are consistent with previous R-matrix calculations for the true three-body continuum. The extracted values of the resonance energy and width converge with the size of the pseudostate basis and are robust under changes in the basis parameters. This supports the reliability of the method in describing the properties of unbound core+N+N systems in a discrete basis.Comment: 11 pages, 14 figures. Accepted as PR

    The Morse-Sard theorem revisited

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    Let n,m,kn, m, k be positive integers with k=nm+1k=n-m+1. We establish an abstract Morse-Sard-type theorem which allows us to deduce, on the one hand, a previous result of De Pascale's for Sobolev Wlock,p(Rn,Rm)W^{k,p}_{\textrm{loc}}(\mathbb{R}^n, \mathbb{R}^m) functions with p>np>n and, on the other hand, also the following new result: if fCk1(Rn,Rm)f\in C^{k-1}(\mathbb{R}^n, \mathbb{R}^m) satisfies lim suph0Dk1f(x+h)Dk1f(x)h<\limsup_{h\to 0}\frac{|D^{k-1}f(x+h)-D^{k-1}f(x)|}{|h|}<\infty for every xRnx\in\mathbb{R}^n (that is, Dk1fD^{k-1}f is a Stepanov function), then the set of critical values of ff is Lebesgue-null in Rm\mathbb{R}^m. In the case that m=1m=1 we also show that this limiting condition holding for every xRnNx\in\mathbb{R}^n\setminus\mathcal{N}, where N\mathcal{N} is a set of zero (n2+α)(n-2+\alpha)-dimensional Hausdorff measure for some 0<α<10<\alpha<1, is sufficient to guarantee the same conclusion.Comment: We corrected some misprints and made some changes in the introductio

    B Mixing and Lifetimes at the Tevatron

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    The Tevatron collider at Fermilab provides a very rich environment for the study of b-hadrons. Both the D0 and CDF experiments have collected a sample of about 1 fb^{-1}. We report results on three topics: b-hadron lifetimes, polarization amplitudes and the decay width difference in Bs to Jpsi Phi, and Bs mixing.Comment: Flavor Physics & CP Violation Conference, Vancouver, 200
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