311 research outputs found
Innovar para Educar: PrĂĄcticas universitarias exitosas. Tomo 5
La Universidad del Norte y el Centro para la Excelencia Docente (CEDU), interesados en compartir con la comunidad acadĂ©mica y pĂșblico en general las experiencias pedagĂłgicas exitosas realizadas por docentes de diferentes ĂĄreas disciplinares, trae ahora el tomo 5 de la colecciĂłn âInnovar para Educar: PrĂĄcticas universitarias exitosasâ, en donde encontrarĂĄn 8 capĂtulos que describen las diferentes propuestas de 14 docentes de la instituciĂłn, que en un momento de reflexiĂłn decidieron cambiar el desarrollo habitual de sus clases. Este impulso los condujo por caminos de planificaciĂłn, implementaciĂłn y evaluaciĂłn sistemĂĄtica que hoy se ven reflejados en su buena prĂĄctica de aula y en los resultados de aprendizaje de sus estudiantes
POR UNA CULTURA DE PAZ: UNA MIRADA DESDE LAS CIENCIAS DE LA CONDUCTA
Enâ© virtudâ© deâ© loâ© anterior,â© losâ© estudiososâ© deâ© lasâ© cienciasâ© deâ© laâ© conductaâ© â©deâ© laâ© Universidadâ©AutĂłnoma â©delâ© Estado â©de â©MĂ©xico,â©â©ante â©laâ©persistenciaâ© y â©proliferaciĂłnâ© deâ© estos â©hechosâ© enâ© diversasâ© partesâ© delâ©Mundoâ© yâ© deâ© nuestro â©paĂs â©en â©particular, seâ© convocĂłâ© aâ© losâ© estudiososâ© interesadosâ© yâ© aâ© laâ© sociedadâ© enâ© generalâ© aâ© presentarâ© trabajosâ© paraâ© analizar,â© debatirâ© yâ© proponerâ© estrategiasâ© deâ© acciĂłnâ© yâ© direcciĂłn,â© queâ©
fortalezcanâ© unaâ© convivencia y bienestar con sentido humanista para una cultura de paz.
Elâ© presenteâ© textoâ© esâ© productoâ© de â©esta convocatoria â©queâ© recoge â©losâ©trabajos â©de â©â©losâ© interesados â©en â©laâ© temĂĄtica,â©â© deâ© diferentes â©paĂsesâ©(España,â©Argentina,â©Cuba,â©Brasil,â©Costaâ© Ricaâ© yâ© MĂ©xico)â© retomandoâ© conâ© elloâ© susâ© experienciasâ© relativasâ© alâ© estudio,â© anĂĄlisis,â© comprensiĂłnâ© eâ© instrumentaciĂłnâ© deâ© laâ© culturaâ© deâ© pazâ© enâ© losâ© distintosâ© ĂĄmbitosâ© institucionalesâ© enâ© losâ© queâ© participan:â© educativo,â© salud,â© penitenciario,â©
social,â©laboral,â©familia,â©alimentario,â©psicolĂłgico,â©por â©mencionar â©algunos.â©
Elâ© presenteâ© libro,â© propiciaâ© unâ© espacioâ© deâ© reflexiĂłn,â© diĂĄlogoâ© yâ© posicionamientoâ© deâ© las â©ciencias â©de â©la â©conductaâ© para â©la â©apropiaciĂłn,â©anĂĄlisis,â©debateâ© y â©propuestas â©queâ© fortalezcan â©unaâ© culturaâ© de â©pazâ© aâ©travĂ©sâ© de â©laâ© convivencia â©yâ© el â©bienestarâ© social â©conâ© sentido â©humanista.â©Elâ© sistema â©econĂłmicoâ© neoliberalâ© y â©el â©procesoâ© de â©globalizaciĂłn â©hanâ© contribuidoâ©alâ© logroâ© deâ© avancesâ© significativosâ© enâ© laâ© cienciaâ© yâ© laâ© tecnologĂa,â© peroâ© tambiĂ©nâ© hanâ© propiciadoâ© laâ© polarizaciĂłnâ© deâ© lasâ© sociedadesâ© loâ© queâ© haâ© impactadoâ© deâ© maneraâ© negativaâ© aâ© laâ© sociedadâ© enâ© suâ© conjunto,â© peroâ© enâ© mayorâ© medidaâ© aâ© los gruposâ© vulnerables. Dichaâ© polarizaciĂłnâ© haâ© traĂdoâ© consigoâ© unâ© desarrolloâ© desigualâ© delâ© mundoâ© queâ© seâ© expresaâ© deâ© diferentesâ© manerasâ© tantoâ© enâ© paĂsesâ© desarrolladosâ© comoâ© enâ© losâ© llamadosâ© delâ© tercerâ© mundo,â© enâ© dondeâ© noâ© estĂĄnâ© satisfechasâ© lasâ© necesidadesâ© humanas â©elementalesâ© deâ© todos â©losâ©sectores â©de â©la â©poblaciĂłn,â©siempre â©falta â©algo. â©Si â©aâ© esto â©leâ© sumamos â©losâ©conflictosâ© internacionales porâ© diferentesâ© motivosâ© queâ© enfrentanâ© algunasâ© naciones,â© unaâ© insuficienteâ© coberturaâ© educativaâ© yâ© deâ© salud,â©â© desempleoâ© yâ© pobreza â©extrema,â© entre â©otrasâ© cosasÍŸ â©estamosâ© frenteâ© aâ©retos â©deâ© granâ© envergaduraâ© paraâ© losâ© gobiernos,â© paraâ© losâ© estudiososâ© yâ© paraâ© laâ© sociedadâ© civilâ© enâ© general. Uno â©de â©losâ© intentosâ© paraâ© frenar â©y prevenir â©laâ© agudizaciĂłnâ© de â©estas â©problemĂĄticasâ© esâ© laâ© cultura â©de â©paz,â©cuyoâ© estudioâ©y propuestas â©han â©ido â©avanzando â©en â©diferentesâ© sentidos â©y â©de â©manera â©favorable,â©el â©tema â©estĂĄ â©presente â©en â©diferentes â©Organismosâ© Internacionalesâ© comoâ© laâ© ONU,â© laâ© UNESCO,â© laâ© OCDE,â© Elâ© Bancoâ© Mundial,â© entreâ© otros.â© Peroâ© falta â©mucho â©por â©hacer.Universidad AutĂłnoma del Estado de MĂ©xic
Les droits disciplinaires des fonctions publiques : « unification », « harmonisation » ou « distanciation ». A propos de la loi du 26 avril 2016 relative à la déontologie et aux droits et obligations des fonctionnaires
The production of tt⟠, W+bb⟠and W+cc⟠is studied in the forward region of protonâproton collisions collected at a centre-of-mass energy of 8 TeV by the LHCb experiment, corresponding to an integrated luminosity of 1.98±0.02 fbâ1 . The W bosons are reconstructed in the decays WââÎœ , where â denotes muon or electron, while the b and c quarks are reconstructed as jets. All measured cross-sections are in agreement with next-to-leading-order Standard Model predictions.The production of , and is studied in the forward region of proton-proton collisions collected at a centre-of-mass energy of 8 TeV by the LHCb experiment, corresponding to an integrated luminosity of 1.98 0.02 \mbox{fb}^{-1}. The bosons are reconstructed in the decays , where denotes muon or electron, while the and quarks are reconstructed as jets. All measured cross-sections are in agreement with next-to-leading-order Standard Model predictions
Measurement of forward production in collisions at TeV
A measurement of the cross-section for production in collisions is presented using data corresponding to an integrated luminosity of fb collected by the LHCb experiment at a centre-of-mass energy of TeV. The electrons are required to have more than GeV of transverse momentum and to lie between 2.00 and 4.25 in pseudorapidity. The inclusive production cross-sections, where the decays to , are measured to be \begin{align*} \begin{split} \sigma_{W^{+} \to e^{+}\nu_{e}}&=1124.4\pm 2.1\pm 21.5\pm 11.2\pm 13.0\,\mathrm{pb},\\ \sigma_{W^{-} \to e^{-}\bar{\nu}_{e}}&=\,\,\,809.0\pm 1.9\pm 18.1\pm\,\,\,7.0\pm \phantom{0}9.4\,\mathrm{pb}, \end{split} \end{align*} where the first uncertainties are statistical, the second are systematic, the third are due to the knowledge of the LHC beam energy and the fourth are due to the luminosity determination. Differential cross-sections as a function of the electron pseudorapidity are measured. The cross-section ratio and production charge asymmetry are also reported. Results are compared with theoretical predictions at next-to-next-to-leading order in perturbative quantum chromodynamics. Finally, in a precise test of lepton universality, the ratio of boson branching fractions is determined to be \begin{align*} \begin{split} \mathcal{B}(W \to e\nu)/\mathcal{B}(W \to \mu\nu)=1.020\pm 0.002\pm 0.019, \end{split} \end{align*} where the first uncertainty is statistical and the second is systematic.A measurement of the cross-section for production in collisions is presented using data corresponding to an integrated luminosity of fb collected by the LHCb experiment at a centre-of-mass energy of TeV. The electrons are required to have more than GeV of transverse momentum and to lie between 2.00 and 4.25 in pseudorapidity. The inclusive production cross-sections, where the decays to , are measured to be \begin{equation*} \sigma_{W^{+} \to e^{+}\nu_{e}}=1124.4\pm 2.1\pm 21.5\pm 11.2\pm 13.0\,\mathrm{pb}, \end{equation*} \begin{equation*} \sigma_{W^{-} \to e^{-}\bar{\nu}_{e}}=\,\,\,809.0\pm 1.9\pm 18.1\pm\,\,\,7.0\pm \phantom{0}9.4\,\mathrm{pb}, \end{equation*} where the first uncertainties are statistical, the second are systematic, the third are due to the knowledge of the LHC beam energy and the fourth are due to the luminosity determination. Differential cross-sections as a function of the electron pseudorapidity are measured. The cross-section ratio and production charge asymmetry are also reported. Results are compared with theoretical predictions at next-to-next-to-leading order in perturbative quantum chromodynamics. Finally, in a precise test of lepton universality, the ratio of boson branching fractions is determined to be \begin{equation*} \mathcal{B}(W \to e\nu)/\mathcal{B}(W \to \mu\nu)=1.020\pm 0.002\pm 0.019, \end{equation*} where the first uncertainty is statistical and the second is systematic.A measurement of the cross-section for W â eÎœ production in pp collisions is presented using data corresponding to an integrated luminosity of 2 fb collected by the LHCb experiment at a centre-of-mass energy of TeV. The electrons are required to have more than 20 GeV of transverse momentum and to lie between 2.00 and 4.25 in pseudorapidity. The inclusive W production cross-sections, where the W decays to eÎœ, are measured to be where the first uncertainties are statistical, the second are systematic, the third are due to the knowledge of the LHC beam energy and the fourth are due to the luminosity determination
Measurement of the J/Ï pair production cross-section in pp collisions at TeV
The production cross-section of J/Ï pairs is measured using a data sample of pp collisions collected by the LHCb experiment at a centre-of-mass energy of TeV, corresponding to an integrated luminosity of 279 ±11 pb. The measurement is performed for J/Ï mesons with a transverse momentum of less than 10 GeV/c in the rapidity range 2.0 < y < 4.5. The production cross-section is measured to be 15.2 ± 1.0 ± 0.9 nb. The first uncertainty is statistical, and the second is systematic. The differential cross-sections as functions of several kinematic variables of the J/Ï pair are measured and compared to theoretical predictions.The production cross-section of pairs is measured using a data sample of collisions collected by the LHCb experiment at a centre-of-mass energy of , corresponding to an integrated luminosity of . The measurement is performed for mesons with a transverse momentum of less than in the rapidity range . The production cross-section is measured to be . The first uncertainty is statistical, and the second is systematic. The differential cross-sections as functions of several kinematic variables of the pair are measured and compared to theoretical predictions
Measurement of the B0sâÎŒ+ÎŒâ Branching Fraction and Effective Lifetime and Search for B0âÎŒ+ÎŒâ Decays
A search for the rare decays Bs0âÎŒ+ÎŒ- and B0âÎŒ+ÎŒ- is performed at the LHCb experiment using data collected in pp collisions corresponding to a total integrated luminosity of 4.4ââfb-1. An excess of Bs0âÎŒ+ÎŒ- decays is observed with a significance of 7.8 standard deviations, representing the first observation of this decay in a single experiment. The branching fraction is measured to be B(Bs0âÎŒ+ÎŒ-)=(3.0±0.6-0.2+0.3)Ă10-9, where the first uncertainty is statistical and the second systematic. The first measurement of the Bs0âÎŒ+ÎŒ- effective lifetime, Ï(Bs0âÎŒ+ÎŒ-)=2.04±0.44±0.05ââps, is reported. No significant excess of B0âÎŒ+ÎŒ- decays is found, and a 95% confidence level upper limit, B(B0âÎŒ+ÎŒ-)<3.4Ă10-10, is determined. All results are in agreement with the standard model expectations.A search for the rare decays and is performed at the LHCb experiment using data collected in collisions corresponding to a total integrated luminosity of 4.4 fb. An excess of decays is observed with a significance of 7.8 standard deviations, representing the first observation of this decay in a single experiment. The branching fraction is measured to be , where the first uncertainty is statistical and the second systematic. The first measurement of the effective lifetime, ps, is reported. No significant excess of decays is found and a 95 % confidence level upper limit, , is determined. All results are in agreement with the Standard Model expectations
Measurements of prompt charm production cross-sections in pp collisions at TeV
Production cross-sections of prompt charm mesons are measured using data from collisions at the LHC at a centre-of-mass energy of TeV. The data sample corresponds to an integrated luminosity of pb collected by the LHCb experiment. The production cross-sections of , , , and mesons are measured in bins of charm meson transverse momentum, , and rapidity, . They cover the rapidity range and transverse momentum ranges for and and for and mesons. The inclusive cross-sections for the four mesons, including charge-conjugate states, within the range of are determined to be \begin{equation*} \sigma(pp\rightarrow D^0 X) = 1190 \pm 3 \pm 64\,\mu\text{b} \end{equation*} \begin{equation*} \sigma(pp\rightarrow D^+ X) = 456 \pm 3 \pm 34\,\mu\text{b} \end{equation*} \begin{equation*} \sigma(pp\rightarrow D_s^+ X) = 195 \pm 4 \pm 19\,\mu\text{b} \end{equation*} \begin{equation*} \sigma(pp\rightarrow D^{*+} X)= 467 \pm 6 \pm 40\,\mu\text{b} \end{equation*} where the uncertainties are statistical and systematic, respectively.Production cross-sections of prompt charm mesons are measured using data from pp collisions at the LHC at a centre-of-mass energy of 5 TeV. The data sample corresponds to an integrated luminosity of 8.60 ± 0.33 pb collected by the LHCb experiment. The production cross-sections of D, D, D , and D mesons are measured in bins of charm meson transverse momentum, p, and rapidity, y. They cover the rapidity range 2.0 < y < 4.5 and transverse momentum ranges 0 < p < 10 GeV/c for D and D and 1 < p < 10 GeV/c for D and D mesons. The inclusive cross-sections for the four mesons, including charge-conjugate states, within the range of 1 < p < 8 GeV/c are determined to be where the uncertainties are statistical and systematic, respectively.Production cross-sections of prompt charm mesons are measured using data from collisions at the LHC at a centre-of-mass energy of TeV. The data sample corresponds to an integrated luminosity of pb collected by the LHCb experiment. The production cross-sections of , , , and mesons are measured in bins of charm meson transverse momentum, , and rapidity, . They cover the rapidity range and transverse momentum ranges for and and for and mesons. The inclusive cross-sections for the four mesons, including charge-conjugate states, within the range of are determined to be \sigma(pp\rightarrow D^0 X) = 1004 \pm 3 \pm 54\,\mu\text{b} \sigma(pp\rightarrow D^+ X) = 402 \pm 2 \pm 30\,\mu\text{b} \sigma(pp\rightarrow D_s^+ X) = 170 \pm 4 \pm 16\,\mu\text{b} \sigma(pp\rightarrow D^{*+} X)= 421 \pm 5 \pm 36\,\mu\text{b} where the uncertainties are statistical and systematic, respectively
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