12 research outputs found

    Involvement of Plant Hormones and Plant Growth Regulators on in vitro Somatic Embryogenesis

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    In spite of the importance attained by somatic embryogenesis and of the many studies that have been conducted on this developmental process, there are still many aspects that are not fully understood. Among those features, the involvement of plant hormones and plant growth regulators on deTermining the conversion of somatic onto embryogenic tissues, and on allowing progression and maturation of somatic embryos, are far away from being completely comprehended. Part of these difficulties relies on the frequent appearance of contradictory results when studying the effect of a particular stimulus over a specific stage in somatic embryogenesis. Recent progress achieved on understanding the interaction between exogenously added plant growth regulators over the concentration of endogenous hormones, together with the involvement of sensitivity of the tissues to particular hormone groups, might help clarifying the occurrence of divergent patterns in somatic embryogenesis, and in tissue culture in general. The aspects described above, emphasizing on the effect of the concentration of plant hormones and of the addition of plant growth regulators during the different phases of somatic embryogenesis, will be reviewed in this paper. Citations will be limited to review articles as much as possible and to individual articles only in those cases in which very specific or recent information is presented.UCR::VicerrectorĂ­a de InvestigaciĂłn::Unidades de InvestigaciĂłn::Ciencias Agroalimentarias::Centro para Investigaciones en Granos y Semillas (CIGRAS

    Toward CUPID-1T

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    Current experiments to search for broken lepton-number symmetry through the observation of neutrinoless double-beta decay (0νββ0\mathrm{\nu\beta\beta}) provide the most stringent limits on the Majorana nature of neutrinos and the effective Majorana neutrino mass (mββm_{\beta\beta}). The next-generation experiments will focus on the sensitivity to the 0νββ0\mathrm{\nu\beta\beta} half-life of O(1027\mathcal{O}(10^{27}--102810^{28}~years)) and mββ≲15m_{\beta\beta}\lesssim15~meV, which would provide complete coverage of the so-called Inverted Ordering region of the neutrino mass parameter space. By taking advantage of recent technological breakthroughs, new, future calorimetric experiments at the 1-ton scale can increase the sensitivity by at least another order of magnitude, exploring the large fraction of the parameter space that corresponds to the Normal neutrino mass ordering. In case of a discovery, such experiments could provide important insights toward a new understanding of the mechanism of 0νββ0\mathrm{\nu\beta\beta}. We present here a series of projects underway that will provide advancements in background reduction, cryogenic readout, and physics searches beyond 0νββ0\mathrm{\nu\beta\beta}, all moving toward the next-to-next generation CUPID-1T detector

    Optimization of the first CUPID detector module

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    CUPID will be a next generation experiment searching for the neutrinoless double β\beta decay, whose discovery would establish the Majorana nature of the neutrino. Based on the experience achieved with the CUORE experiment, presently taking data at LNGS, CUPID aims to reach a background free environment by means of scintillating Li2_{2} 100^{100}MoO4_4 crystals coupled to light detectors. Indeed, the simultaneous heat and light detection allows us to reject the dominant background of α\alpha particles, as proven by the CUPID-0 and CUPID-Mo demonstrators. In this work we present the results of the first test of the CUPID baseline module. In particular, we propose a new optimized detector structure and light sensors design to enhance the engineering and the light collection, respectively. We characterized the heat detectors, achieving an energy resolution of (5.9 ±\pm 0.2) keV FWHM at the QQ-value of 100^{100}Mo (about 3034 keV). We studied the light collection of the baseline CUPID design with respect to an alternative configuration which features gravity-assisted light detectors' mounting. In both cases we obtained an improvement in the light collection with respect to past measures and we validated the particle identification capability of the detector, which ensures an α\alpha particle rejection higher than 99.9%, fully satisfying the requirements for CUPID

    Toward CUPID-1T

    No full text
    Current experiments to search for broken lepton-number symmetry through the observation of neutrinoless double-beta decay (0νββ0\mathrm{\nu\beta\beta}) provide the most stringent limits on the Majorana nature of neutrinos and the effective Majorana neutrino mass (mββm_{\beta\beta}). The next-generation experiments will focus on the sensitivity to the 0νββ0\mathrm{\nu\beta\beta} half-life of O(1027\mathcal{O}(10^{27}--102810^{28}~years)) and mββ≲15m_{\beta\beta}\lesssim15~meV, which would provide complete coverage of the so-called Inverted Ordering region of the neutrino mass parameter space. By taking advantage of recent technological breakthroughs, new, future calorimetric experiments at the 1-ton scale can increase the sensitivity by at least another order of magnitude, exploring the large fraction of the parameter space that corresponds to the Normal neutrino mass ordering. In case of a discovery, such experiments could provide important insights toward a new understanding of the mechanism of 0νββ0\mathrm{\nu\beta\beta}. We present here a series of projects underway that will provide advancements in background reduction, cryogenic readout, and physics searches beyond 0νββ0\mathrm{\nu\beta\beta}, all moving toward the next-to-next generation CUPID-1T detector

    Toward CUPID-1T

    No full text
    Current experiments to search for broken lepton-number symmetry through the observation of neutrinoless double-beta decay (0νββ0\mathrm{\nu\beta\beta}) provide the most stringent limits on the Majorana nature of neutrinos and the effective Majorana neutrino mass (mββm_{\beta\beta}). The next-generation experiments will focus on the sensitivity to the 0νββ0\mathrm{\nu\beta\beta} half-life of O(1027\mathcal{O}(10^{27}--102810^{28}~years)) and mββ≲15m_{\beta\beta}\lesssim15~meV, which would provide complete coverage of the so-called Inverted Ordering region of the neutrino mass parameter space. By taking advantage of recent technological breakthroughs, new, future calorimetric experiments at the 1-ton scale can increase the sensitivity by at least another order of magnitude, exploring the large fraction of the parameter space that corresponds to the Normal neutrino mass ordering. In case of a discovery, such experiments could provide important insights toward a new understanding of the mechanism of 0νββ0\mathrm{\nu\beta\beta}. We present here a series of projects underway that will provide advancements in background reduction, cryogenic readout, and physics searches beyond 0νββ0\mathrm{\nu\beta\beta}, all moving toward the next-to-next generation CUPID-1T detector

    Determination of the quark coupling strength vertical bar V-ub vertical bar using baryonic decays

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    In the Standard Model of particle physics, the strength of the couplings of the b quark to the u and c quarks, vertical bar V-ub vertical bar and vertical bar V-ub vertical bar, are governed by the coupling of the quarks to the Higgs boson. Using data from the LHCb experiment at the Large Hadron Collider, the probability for the Lambda(0)(b) baryon to decay into the p mu(-)(nu) over bar (mu) final state relative to the Lambda(+)(c)mu(-)(nu) over bar (mu) final state is measured. Combined with theoretical calculations of the strong interaction and a previously measured value of vertical bar V-ub vertical bar, the first vertical bar V-ub vertical bar measurement to use a baryonic decay is performed. This measurement is consistent with previous determinations of vertical bar V-ub vertical bar using B meson decays to specific final states and confirms the existing incompatibility with those using an inclusive sample of final states
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