1,535,644 research outputs found
"Juan J. Herrera y Piña Arzobispo de Monterrey"
No full textI.O. Juan J. Herrera y Piña Arzobispo de Monterre
Plaza de Toros de Salamanca [Material gráfico] ]: ... tres grandes corridas de toros en los días 11, 12 y 13 de septiembre de 1906.
No full textGanadería: D. Juan de Muriel, D. Felipe de Pablo Romero, Excmo. Sr. Duque de Veragua.Espadas: Antonio Montes, Ricardo Torres (Bombita), Manuel Megia (Bienvenida)Cartel impreso por ambas caras.En anverso ornamentación: litografía orlada con escarapelas y cabeza de toro firmada por Imp. y Lit. de J. Ortega- Valª.En reverso, impreso en rojo: orla, tres viñetas taurinas, el programa y lista de precios.Hoja infomativa [1]: Antonio Montes tomará parte en la corrida junto a Bombita y Bienvenida, el día 11 de septiembre de 1906. Imp. y Lib. de Núñez, Salamanca.Hoja infomativa [2]: Manuel Megía (Biemvenida) tomará parte en la corrida junto a Bombita y Antonio Montes, el día 12 de septiembre de 1906. Imp. y Lib. de Núñez, Salamanca
Plaza de toros de Salamanca [Material gráfico] ]: ferias y fiestas de 1917 : cuatro grandes corridas de toros en los días 11, 12, 13 y 21 de Septiembre.
No full textGanadería: Veragua, Miura, Coquilla, Hijos de Angoso, Sánchez Rico, Alipio Pérez, Hermanos Hidalgo.Espadas: Gaona, Flores, Gallito, Saleri, Fortuna, Angelete.Decorado con litografía representando el retrato del torero Fortuna y plaza de toros en tinta marrón y firmada por Imp. y Lit J. Ortega
Plaza de toros de Salamanca [Material gráfico] ]: ferias y fiestas de 1917 : cuatro grandes corridas de toros en los días 11, 12, 13 y 21 de Septiembre.
No full textGanadería: Veragua, Miura, Coquilla, Hijos de Angoso, Sánchez Rico, Alipio Pérez, Hermanos Hidalgo.Espadas: Gaona, Flores, Gallito, Saleri, Fortuna, Angelete.Decorado con litografía retrato del torero Gallito y de plaza de toros en tinta marrón y firmada por Imp. y Lit J. Ortega
Burgos [Material gráfico]: la plaza mayor / [J. Laurent]
No full textN. 1560Copia digital. Valladolid : Junta de Castilla y León. Consejería de Cultura y Turismo, 2009-201
Measurement of J/Ψ production in pp collisions at √s=7 TeV
No full textThe production of J/psi mesons in proton-proton collisions at root s = 7 TeV is studied with the LHCb detector at the LHC. The differential cross-section for prompt J/psi production is measured as a function of the J/psi transverse momentum p(T) and rapidity y in the fiducial region p(T) is an element of [0; 14] GeV/c and y is an element of [2.0; 4.5]. The differential cross-section and fraction of J/psi from b-hadron decays are also measured in the same p(T) and y ranges. The analysis is based on a data sample corresponding to an integrated luminosity of 5.2 pb(-1). The measured cross-sections integrated over the fiducial region are 10.52 +/- 0.04 +/- 1.40(-2.20)(+1.64) mu b for prompt J/psi production and 1.14 +/- 0.01 +/- 0.16 mu b for J/psi from b-hadron decays, where the first uncertainty is statistical and the second systematic. The prompt J/psi production cross-section is obtained assuming no J/psi polarisation and the third error indicates the acceptance uncertainty due to this assumption
Plaza de Toros [de] Salamanca ... [Material gráfico] ]: se celebrarán tres brillantes corridas de toros en los días 11, 12 y 13 de septiembre de 1896.
No full textGanadería: día 11 : Don Juan Sánchez ; día 12 : D. Teodoro Valle ; día 13 : Excmo. Sr. Duque de Veragua.Espadas: Rafael Guerra (Guerrita), Antonio Reverte.Decoración con litografía en la parte superior de escena taurina en colores firmada por Imp. y Lit. J. Ortega
Suppression of non-prompt J/ψ, prompt J/ψ, and Y(1S) in PbPb collisions at √s NN = 2.76 TeV
No full textThis is the Pre-print verison of the Article. The official published version can be accessed from the link below - Copyright @ 2012 Springer VerlagYields of prompt and non-prompt J/ψ, as well as U (1S) mesons, are measured by the CMS experiment via their μ + μ − decays in PbPb and pp collisions at Ö{s\textNN} = 2.76 sNN=276 TeV for quarkonium rapidity |y| < 2.4. Differential cross sections and nuclear modification factors are reported as functions of y and transverse momentum p T, as well as collision centrality. For prompt J/ψ with relatively high p T (6.5 < p T < 30 GeV/c), a strong, centrality-dependent suppression is observed in PbPb collisions, compared to the yield in pp collisions scaled by the number of inelastic nucleon-nucleon collisions. In the same kinematic range, a suppression of non-prompt J/ψ, which is sensitive to the in-medium b-quark energy loss, is measured for the first time. Also the low-p T U (1S) mesons are suppressed in PbPb collisions.This work was supported by the Austrian Federal Ministry of Science and Research; the Belgium Fonds de la Recherche Scientifique, and Fonds voor Wetenschappelijk
Onderzoek; the Brazilian Funding Agencies (CNPq, CAPES, FAPERJ, and FAPESP); the Bulgarian Ministry of Education and Science; CERN; the Chinese Academy of Sciences, Ministry of Science and Technology, and National Natural Science Foundation of China; the Colombian Funding Agency (COLCIENCIAS); the Croatian Ministry of Science, Education and Sport; the Research Promotion Foundation, Cyprus; the Estonian Academy of Sciences and NICPB; the Academy of Finland, Finnish Ministry of Education and Culture, and Helsinki Institute of
Physics; the Institut National de Physique Nucl´eaire et de Physique des Particules / CNRS, and Commissariat a l’Energie Atomique et aux Energies Alternatives / CEA, France; the Bundesministerium fur Bildung und Forschung, Deutsche Forschungsgemeinschaft, and Helmholtz-Gemeinschaft Deutscher Forschungszentren, Germany; the General Secretariat for Research and Technology, Greece; the National Scientific Research Foundation, and National Office for
Research and Technology, Hungary; the Department of Atomic Energy and the Department of Science and Technology, India; the Institute for Studies in Theoretical Physics and Mathematics, Iran; the Science Foundation, Ireland; the Istituto Nazionale di Fisica Nucleare, Italy; the Korean
Ministry of Education, Science and Technology and the World Class University program of NRF, Korea; the Lithuanian Academy of Sciences; the Mexican Funding Agencies (CINVESTAV, CONACYT, SEP, and UASLP-FAI); the Ministry of Science and Innovation, New Zealand; the Pakistan Atomic Energy Commission; the Ministry of Science and Higher Education and the National Science Centre, Poland; the Fundac¸ ao para a Ciencia e a Tecnologia, Portugal; JINR (Armenia, Belarus, Georgia, Ukraine, Uzbekistan); the Ministry of Education and Science of the Russian Federation, the Federal Agency of Atomic Energy of the Russian Federation, Russian Academy of Sciences, and the Russian Foundation for Basic Research; the Ministry of Science and Technological Development of Serbia; the Ministerio de Ciencia e Innovacion, and Programa Consolider-Ingenio 2010, Spain; the Swiss Funding Agencies (ETH Board, ETH Zurich, PSI, SNF, UniZH, Canton Zurich, and SER); the National Science Council, Taipei; the Scientific and Technical Research Council of Turkey, and Turkish Atomic Energy Authority; the Science and Technology Facilities Council, UK; the US Department of Energy, and the US National Science Foundation
El concepto de crítica en J. Habermas y A. Honneth.
No full textEl presente artículo efectúa una discusión con la concepción de J. Habermas y A. Honneth sobre los parámetros normativos de la crítica social. Pone de manifiesto que estos autores aplican un enfoque formal y cuasitrascendental sobre la problemática de las bases de la crítica. Pretenden explicitar a partir de las relaciones sociales de comunicación y reconocimiento moral los parámetros normativos que sustentan una crítica con pretensión de validez universal. El problema de tal concepción es que pierde de vista la historicidad y perspectivismo inherentes a la actividad crítica y desemboca significativamente en un concepto de crítica débil, incapaz de cuestionar las injusticias características de la formación social capitalista. Con ello el presente artículo muestra la necesidad de avanzar más allá de la teorización sobre la crítica de estos autores, en una dirección en la que se logre compatibilizar la pretensión de validez de la crítica con su carácter histórico y perspectivista.ABSTRAC:
This article makes a discussion with the conception of J. Habermas and A. Honneth on normative parameters of social criticism. It shows that these authors apply a formal, quasi-transcendental approach to the problem of the basis of critique. Intended from explicit social relations and moral recognition communication policy parameters that underpin critical claim universal validity. The problem with this conception is that it loses sight of the historicity and perspectivism inherent critical activity and flows significantly on a concept of weak, unable to challenge the injustices critical features of the capitalist social formation. This article shows this the need to move beyond theorizing about the criticism of these authors, in a direction they are compatible the validity claim of review with historical and perspectival character
Evidence for the decay B0→J/ψω and measurement of the relative branching fractions of meson decays to J/ψη and J/ψη′
No full textFirst evidence of the B 0 → J / ψ ω decay is found and the B s 0 → J / ψ η and B s 0 → J / ψ η ′ decays are studied using a dataset corresponding to an integrated luminosity of 1.0 fb -1 collected by the LHCb experiment in proton-proton collisions at a centre-of-mass energy of sqrt(s) = 7 TeV. The branching fractions of these decays are measured relative to that of the B 0 → J / ψ ρ 0 decay:frac(B (B 0 → J / ψ ω), B (B 0 → J / ψ ρ 0)) = 0.89 ± 0.19 (stat) - 0.13 + 0.07 (syst),frac(B (B s 0 → J / ψ η), B (B 0 → J / ψ ρ 0)) = 14.0 ± 1.2 (stat) - 1.5 + 1.1 (syst) - 1.0 + 1.1 (frac(f d, f s)),frac(B (B s 0 → J / ψ η ′), B (B 0 → J / ψ ρ 0)) = 12.7 ± 1.1 (stat) - 1.3 + 0.5 (syst) - 0.9 + 1.0 (frac(f d, f s)), where the last uncertainty is due to the knowledge of f d / f s, the ratio of b-quark hadronization factors that accounts for the different production rate of B 0 and B s 0 mesons. The ratio of the branching fractions of B s 0 → J / ψ η ′ and B s 0 → J / ψ η decays is measured to befrac(B (B s 0 → J / ψ η ′), B (B s 0 → J / ψ η)) = 0.90 ± 0.09 (stat) - 0.02 + 0.06 (syst)
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