Obtención de vitroplantas de Escobedia grandiflora (Fam: Orobanchaceae) a partir de semilla

Escobedia grandiflora (L.f) Kuntze is an hemiparasite plant, whose propagation is difficult. The aims of this study were: (1) to determine the protocol for E. grandiflora seed disinfection; (2) to evaluate seed germination with 3-Indole Acetic Acid (AIA) and Gibberellic Acid (AG3) application; and (3 to evaluate the in vitro seedling development in two types of gelling with different AIA concentrations. Optimal disinfection was achieved using sodium hypochlorite since 0% of the seedling were contaminated and 100% germinated. Additionally, a better germination was obtained without the use of hormones, also Phytagel gelling favored the seedling growth. Regarding the AIA concentration, the seedlings reached a better length with 10mg/l of AIA, however a greater root length was found without the application of AIA. We conclude that it is possible to obtain E. grandiflora vitroplants from the seed without AIA and AG3 hormones addition. However, it is important to evaluate other hormones and concentrations in order to reduce seedling time in in vitro conditions.Escobedia grandiflora (L.f) Kuntze es una planta hemiparásita, cuya propagación es difícil. Este trabajo se planteó: (1) Determinar el protocolo de desinfección de las semillas, (2) evaluar su germinación con la aplicación de Ácido 3-indol Acético (AIA), y Ácido Giberélico (AG3), y (3) evaluar el desarrollo de plántulas in vitro en dos tipos de gelificante y a diferentes concentraciones de AIA. Mediante esta investigación se encontró que la desinfección de semilla fue mejor en hipoclorito de sodio durante 90 segundos, ya que presentó 0% de contaminación y 100% de germinación. Adicionalmente se obtuvo una mejor germinación sin el uso de hormonas. Por otro lado, el gelificante Phytagel favoreció el mayor crecimiento de plántulas. En cuanto la concentración de AIA, se obtuvo una mayor longitud de la raíz sin la aplicación del AIA, sin embargo, la longitud total de la plántula fue mejor con 1,0 mg/l de AIA. Se concluye que es posible la obtención de vitroplantas de E. grandiflora a partir de semilla, sin adición de las hormonas AIA y AG3 en las concentraciones evaluadas, sin embargo, es importante evaluar otras concentraciones y otras hormonas para acortar el tiempo de las plántulas en condiciones in vitro.Escobedia grandiflora (L.f) Kuntze es una planta hemiparásita, cuya propagación presenta dificultades. Este trabajo se planteó: (1) Determinar el protocolo de desinfección de las semillas, (2) evaluar su germinación con la aplicación de Ácido 3-indol Acético (AIA), y Ácido Giberélico (AG3), y (3) evaluar el desarrollo de plántulas in vitro en dos tipos de gelificante y a diferentes concentraciones de AIA. Mediante esta investigación se encontró que la desinfección de semilla fue mejor en hipoclorito de sodio durante 90 segundos, ya que presentó 0% de contaminación y 100% de germinación. Adicionalmente se obtuvo una mejor germinación sin el uso de hormonas. Por otro lado, el gelificante Phytagel favoreció el mayor crecimiento de plántulas. En cuanto la concentración de AIA, se obtuvo una mayor longitud de la raíz sin la aplicación del AIA, sin embargo, la longitud total de la plántula fue mejor con 1,0 mg/l de AIA. Se concluye que es posible la obtención de vitroplantas de E. grandiflora a partir de semilla, sin adición de las hormonas AIA y AG3 en las concentraciones evaluadas, sin embargo, es importante evaluar otras concentraciones y otras hormonas para acortar el tiempo de las plántulas en condiciones in vitro.Escobedia grandiflora (L.f) Kuntze is an hemiparasite plant, whose propagation is difficult. The aims of this study were: (1) to determine the protocol for E. grandiflora seed disinfection; (2) to evaluate seed germination with 3-Indole Acetic Acid (AIA) and Gibberellic Acid (AG3) application; and (3 to evaluate the in vitro seedling development in two types of gelling with different AIA concentrations. Optimal disinfection was achieved using sodium hypochlorite since 0% of the seedling were contaminated and 100% germinated. Additionally, a better germination was obtained without the use of hormones, also Phytagel gelling favored the seedling growth. Regarding the AIA concentration, the seedlings reached a better length with 10mg/l of AIA, however a greater root length was found without the application of AIA. We conclude that it is possible to obtain E. grandiflora vitroplants from the seed without AIA and AG3 hormones addition. However, it is important to evaluate other hormones and concentrations in order to reduce seedling time in in vitro conditions

Visiones de la educación financiera: Análisis y perspectivas

"Visiones de la educación financiera: análisis y perspectivas es una obra que enmarca la importancia de la educación financiera en la sociedad en el contexto actual. Las decisiones que en este tema realiza un individuo pueden impactar positiva o negativamente su estabilidad económica por un periodo indeterminado, es aquí cuando la educación financiera actúa como una herramienta trascendental en su bienestar personal. Además de tener la función de armadura ante las batallas que se libran en los mercados —como la crisis financiera de 2008— funge como dinamizador de las economías al potenciar los proyectos de inversión con el aumento del emprendedurismo, impactando así en las variables macroeconómicas. Esta área del conocimiento ha adquirido importancia y popularidad a nivel internacional a raíz de las crisis económicas de los últimos años, sin embargo, aún existen, entre otras, brechas sociodemográficas, culturales, económicas, que no permiten el acceso a estas enseñanzas, excluyendo parte de la población del proceso del bienestar económico. Para ejemplificar esta desigualdad, en los capítulos se plasma un panorama internacional de la educación financiera, considerando las implicaciones y retos que han tenido las estrategias nacionales de educación financiera a nivel mundial"

Measurement of the double-differential inclusive jet cross section in proton-proton collisions at s\sqrt{s} = 5.02 TeV

International audienceThe inclusive jet cross section is measured as a function of jet transverse momentum $p_\mathrm{T}$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s}$ = 5.02 TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_\mathrm{T}$ algorithm using a distance parameter of $R$ = 0.4, within the rapidity interval $\lvert y\rvert$$\lt$ 2, and across the kinematic range 0.06 $\lt$$p_\mathrm{T}$$\lt$ 1 TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_\mathrm{S}$

Measurement of the double-differential inclusive jet cross section in proton-proton collisions at s= \sqrt{s} = 5.02 TeV

The inclusive jet cross section is measured as a function of jet transverse momentum $p_{\mathrm{T}}$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s} =$ 5.02 TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4$\,\text{pb}^{-1}$. The jets are reconstructed with the anti-$k_{\mathrm{T}}$ algorithm using a distance parameter of $R=$ 0.4, within the rapidity interval $|y| <$ 2, and across the kinematic range 0.06 $< p_{\mathrm{T}} <$ 1 TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_\mathrm{S}$.The inclusive jet cross section is measured as a function of jet transverse momentum $p_\mathrm{T}$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s}$ = 5.02 TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_\mathrm{T}$ algorithm using a distance parameter of $R$ = 0.4, within the rapidity interval $\lvert y\rvert$$\lt$ 2, and across the kinematic range 0.06 $\lt$$p_\mathrm{T}$$\lt$ 1 TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_\mathrm{S}$

Measurement of the double-differential inclusive jet cross section in proton-proton collisions at s\sqrt{s} = 5.02 TeV

International audienceThe inclusive jet cross section is measured as a function of jet transverse momentum $p_\mathrm{T}$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s}$ = 5.02 TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_\mathrm{T}$ algorithm using a distance parameter of $R$ = 0.4, within the rapidity interval $\lvert y\rvert$$\lt$ 2, and across the kinematic range 0.06 $\lt$$p_\mathrm{T}$$\lt$ 1 TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_\mathrm{S}$

Measurement of the double-differential inclusive jet cross section in proton-proton collisions at s\sqrt{s} = 5.02 TeV

International audienceThe inclusive jet cross section is measured as a function of jet transverse momentum $p_\mathrm{T}$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s}$ = 5.02 TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_\mathrm{T}$ algorithm using a distance parameter of $R$ = 0.4, within the rapidity interval $\lvert y\rvert$$\lt$ 2, and across the kinematic range 0.06 $\lt$$p_\mathrm{T}$$\lt$ 1 TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_\mathrm{S}$

Measurement of the double-differential inclusive jet cross section in proton-proton collisions at s\sqrt{s} = 5.02 TeV

International audienceThe inclusive jet cross section is measured as a function of jet transverse momentum $p_\mathrm{T}$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s}$ = 5.02 TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_\mathrm{T}$ algorithm using a distance parameter of $R$ = 0.4, within the rapidity interval $\lvert y\rvert$$\lt$ 2, and across the kinematic range 0.06 $\lt$$p_\mathrm{T}$$\lt$ 1 TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_\mathrm{S}$

Inclusive nonresonant multilepton probes of new phenomena at s\sqrt{s} = 13 TeV

An inclusive search for nonresonant signatures of beyond the standard model (SM) phenomena in events with three or more charged leptons, including hadronically decaying $\tau$ leptons, is presented. The analysis is based on a data sample corresponding to an integrated luminosity of 138 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}$ = 13 TeV, collected by the CMS experiment at the LHC in 2016-2018. Events are categorized based on the lepton and b-tagged jet multiplicities and various kinematic variables. Three scenarios of physics beyond the SM are probed, and signal-specific boosted decision trees are used for enhancing sensitivity. No significant deviations from the background expectations are observed. Lower limits are set at 95% confidence level on the mass of type-III seesaw heavy fermions in the range 845-1065 GeV for various decay branching fraction combinations to SM leptons. Doublet and singlet vector-like $\tau$ lepton extensions of the SM are excluded for masses below 1045 GeV and in the mass range 125-150 GeV, respectively. Scalar leptoquarks decaying exclusively to a top quark and a lepton are excluded below 1.12-1.42 TeV, depending on the lepton flavor. For the type-III seesaw as well as the vector-like doublet model, these constraints are the most stringent to date. For the vector-like singlet model, these are the first constraints from the LHC experiments. Detailed results are also presented to facilitate alternative theoretical interpretations

Inclusive nonresonant multilepton probes of new phenomena at s\sqrt{s} = 13 TeV

An inclusive search for nonresonant signatures of beyond the standard model (SM) phenomena in events with three or more charged leptons, including hadronically decaying $\tau$ leptons, is presented. The analysis is based on a data sample corresponding to an integrated luminosity of 138 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}$ = 13 TeV, collected by the CMS experiment at the LHC in 2016-2018. Events are categorized based on the lepton and b-tagged jet multiplicities and various kinematic variables. Three scenarios of physics beyond the SM are probed, and signal-specific boosted decision trees are used for enhancing sensitivity. No significant deviations from the background expectations are observed. Lower limits are set at 95% confidence level on the mass of type-III seesaw heavy fermions in the range 845-1065 GeV for various decay branching fraction combinations to SM leptons. Doublet and singlet vector-like $\tau$ lepton extensions of the SM are excluded for masses below 1045 GeV and in the mass range 125-150 GeV, respectively. Scalar leptoquarks decaying exclusively to a top quark and a lepton are excluded below 1.12-1.42 TeV, depending on the lepton flavor. For the type-III seesaw as well as the vector-like doublet model, these constraints are the most stringent to date. For the vector-like singlet model, these are the first constraints from the LHC experiments. Detailed results are also presented to facilitate alternative theoretical interpretations

First evidence for off-shell production of the Higgs boson and measurement of its width

The first evidence for off-shell Higgs production is reported in the final state with two Z bosons decaying into either four charged leptons (muons or electrons), or two charged leptons and two neutrinos, and a measurement of the Higgs boson width is performed. Results are based on data from the CMS experiment at the LHC at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of up to 140 fb$^{-1}$. The total rate of off-shell Higgs boson production beyond the Z boson pair production threshold, relative to its standard model expectation, is constrained to the interval [0.0061, 2.0] at 95% confidence level. The scenario with no off-shell production is excluded at 99.97% confidence level (3.6 standard deviations). The width of the Higgs boson is extracted as $\Gamma_{\mathrm{H}}$ = 3.2$_{-1.7}^{+2.4}$ MeV, in agreement with the standard model expectation of 4.1 MeV. The data are also used to set new constraints on anomalous Higgs boson couplings to W and Z boson pairs