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Measurement of Bottom-Quark Hadron Masses in ExclusiveJ/ψDecays with the CDF Detector
Acosta, D.,Adelman, J.,Affolder, T.,Akimoto, T.,Albrow, M. G.,Ambrose, D.,Amerio, S.,Amidei, D.,Anastassov, A.,Anikeev, K.,Annovi, A.,Antos, J.,Aoki, M.,Apollinari, G.,Arisawa, T.,Arguin, J-F.,Artikov American Physical Society 2006 Physical review letters Vol.96 No.20
Numerical boundaries for some classical Banach spaces
Acosta, M.D.,Kim, S.G. Academic Press 2009 Journal of mathematical analysis and applications Vol.350 No.2
Globevnik gave the definition of boundary for a subspace A@?C<SUB>b</SUB>(Ω). This is a subset of Ω that is a norming set for A. We introduce the concept of numerical boundary. For a Banach space X, a subset B@?Π(X) is a numerical boundary for a subspace A@?C<SUB>b</SUB>(B<SUB>X</SUB>,X) if the numerical radius of f is the supremum of the modulus of all the evaluations of f at B, for every f in A. We give examples of numerical boundaries for the complex spaces X=c<SUB>0</SUB>, C(K) and d<SUB>*</SUB>(w,1), the predual of the Lorentz sequence space d(w,1). In all these cases (if K is infinite) we show that there are closed and disjoint numerical boundaries for the space of the functions from B<SUB>X</SUB> to X which are uniformly continuous and holomorphic on the open unit ball and there is no minimal closed numerical boundary. In the case of c<SUB>0</SUB>, we characterize the numerical boundaries for that space of holomorphic functions.
Bishop-Phelps-Bollobas property for certain spaces of operators
Acosta, M.D.,Becerra Guerrero, J.,Garcia, D.,Kim, S.K.,Maestre, M. Academic Press 2014 Journal of mathematical analysis and applications Vol.414 No.2
We characterize the Banach spaces Y for which certain subspaces of operators from L<SUB>1</SUB>(μ) into Y have the Bishop-Phelps-Bollobas property in terms of a geometric property of Y, namely AHSP. This characterization applies to the spaces of compact and weakly compact operators. New examples of Banach spaces Y with AHSP are provided. We also obtain that certain ideals of Asplund operators satisfy the Bishop-Phelps-Bollobas property.
Direct photon cross section with conversions at CDF
Acosta, D.,Affolder, T.,Albrow, M. G.,Ambrose, D.,Amidei, D.,Anikeev, K.,Antos, J.,Apollinari, G.,Arisawa, T.,Artikov, A.,Ashmanskas, W.,Azfar, F.,Azzi-Bacchetta, P.,Bacchetta, N.,Bachacou, H.,Badgett American Physical Society 2004 PHYSICAL REVIEW D - Vol.70 No.7
Heavy flavor properties of jets produced inpp¯interactions ats=1.8TeV
Acosta, D.,Ambrose, D.,Anikeev, K.,Antos, J.,Apollinari, G.,Arisawa, T.,Artikov, A.,Azfar, F.,Azzi-Bacchetta, P.,Bacchetta, N.,Barnes, V. E.,Barnett, B. A.,Barone, M.,Bauer, G.,Bedeschi, F.,Behari, S. American Physical Society 2004 PHYSICAL REVIEW D - Vol.69 No.7
The Bishop-Phelps-Bollobas property for operators from c<sub>0</sub> into some Banach spaces
Acosta, M.D.,Garcia, D.,Kim, S.K.,Maestre, M. Academic Press 2017 Journal of mathematical analysis and applications Vol.445 No.2
<P>We exhibit a new class of Banach spaces Y such that the pair (c(0), Y) has the Bishop-Phelps-Bollobas property for operators. This class contains uniformly convex Banach spaces and spaces with the property beta of Lindenstrauss. We also provide new examples of spaces in this class. (C) 2016 Elsevier Inc. All rights reserved.</P>
Acosta, M.,Novak, N.,Jo, W.,Rodel, J. Elsevier Science 2014 Acta materialia Vol.80 No.-
The Ba(Zr<SUB>0.2</SUB>Ti<SUB>0.8</SUB>)O<SUB>3</SUB>-x(Ba<SUB>0.7</SUB>Ca<SUB>0.3</SUB>)TiO<SUB>3</SUB> system was synthesized in a wide compositional range in order to study the relationship between its phase diagram and electromechanical properties. Phase transitions were marked using peaks in temperature-dependent permittivity, providing up to three transitions from the rhombohedral phase to an orthorhombic, tetragonal and finally cubic phase, which meet in a region that is termed the phase convergence region in this work. In situ small and large signal electromechanical properties were studied as a function of temperature with specific emphasis on these transitions. A small signal piezoelectric coefficient, d<SUB>33</SUB>, presents maximized values at the transition from the orthorhombic to the tetragonal phase, while a large signal piezoelectric coefficient, d<SUB>33</SUB><SUP>*</SUP>, does so at both rhombohedral to orthorhombic and to tetragonal phase transitions. Maximum polarization P<SUB>max</SUB> was the only quantity determined that had a clear maximum at the phase convergence region.