HAL Mines Nantes
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    7271 research outputs found

    Chiral Separation Effect from Holographic QCD

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    International audienceWe analyze the chiral separation effect (CSE) in QCD by using the gauge/gravity duality. In QCD, this effect arises from a combination of chiral anomalies and the axial U(1)U(1) anomaly. Due to the axial gluon anomaly, the value of the CSE conductivity is not determined by the anomalies of QCD but receives radiative corrections, which leads to nontrivial dependence on temperature and density. To analyze this dependence, we use different variants of V-QCD, a complex holographic model, carefully fitted to QCD data. We find our results for the anomalous CSE conductivity at small chemical potential and nonzero temperature to be in good qualitative agreement with recent results from lattice QCD simulations. We furthermore give predictions for the behavior of the conductivity at finite (vectorial and axial) chemical potentials

    Measurement of Λ3H{}_{\Lambda}^{3}\mathrm{H} production in Pb-Pb collisions at sNN\sqrt{s_{\mathrm{NN}}} = 5.02 TeV

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    International audienceThe first measurement of Λ3H_{\Lambda}^{3}\mathrm{H} and Λ3H^3_ {\overline{\Lambda}}\overline{\mathrm{H}} differential production with respect to transverse momentum and centrality in Pb-Pb collisions at sNN=5.02\sqrt{s_{\mathrm{NN}}}=5.02~TeV is presented. The Λ3H_{\Lambda}^{3}\mathrm{H} has been reconstructed via its two-charged-body decay channel, i.e., Λ3H3He+π_{\Lambda}^{3}\mathrm{H} \rightarrow {}^{3}\mathrm{He} + \pi^{-}. A Blast-Wave model fit of the pTp_{\rm T}-differential spectra of all nuclear species measured by the ALICE collaboration suggests that the Λ3H_{\Lambda}^{3}\mathrm{H} kinetic freeze-out surface is consistent with that of other nuclei. The ratio between the integrated yields of Λ3H_{\Lambda}^{3}\mathrm{H} and 3He^3\mathrm{He} is compared to predictions from the statistical hadronisation model and the coalescence model, with the latter being favoured by the presented measurements

    The XLZD Design Book: Towards the Next-Generation Liquid Xenon Observatory for Dark Matter and Neutrino Physics

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    International audienceThis report describes the experimental strategy and technologies for a next-generation xenon observatory sensitive to dark matter and neutrino physics. The detector will have an active liquid xenon target mass of 60-80 tonnes and is proposed by the XENON-LUX-ZEPLIN-DARWIN (XLZD) collaboration. The design is based on the mature liquid xenon time projection chamber technology of the current-generation experiments, LZ and XENONnT. A baseline design and opportunities for further optimization of the individual detector components are discussed. The experiment envisaged here has the capability to explore parameter space for Weakly Interacting Massive Particle (WIMP) dark matter down to the neutrino fog, with a 3σ\sigma evidence potential for the spin-independent WIMP-nucleon cross sections as low as 3×1049cm23\times10^{-49}\rm cm^2 (at 40 GeV/c2^2 WIMP mass). The observatory is also projected to have a 3σ\sigma observation potential of neutrinoless double-beta decay of 136^{136}Xe at a half-life of up to 5.7×10275.7\times 10^{27} years. Additionally, it is sensitive to astrophysical neutrinos from the atmosphere, sun, and galactic supernovae

    First measurement of A = 4 (anti)hypernuclei at the LHC

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    International audienceIn this Letter, the first evidence of the Λˉ4He{}^4_{\bar{\Lambda}}\overline{\mathrm{He}} antihypernucleus is presented, along with the first measurement at the LHC of the production of (anti)hypernuclei with mass number A=4A=4, specifically (anti)Λ4H{}^4_{\Lambda}\mathrm{H} and (anti)Λ4He{}^4_{\Lambda}\mathrm{He}. In addition, the antiparticle-to-particle ratios for both hypernuclei (Λˉ4H{}^4_{\bar{\Lambda}}\overline{\mathrm{H}} / Λ4H{}^4_{\Lambda}\mathrm{H}~and Λˉ4He{}^4_{\bar{\Lambda}}\overline{\mathrm{He}} / Λ4He{}^4_{\Lambda}\mathrm{He}) are shown, which are sensitive to the baryochemical potential of the strongly-interacting matter created in heavy-ion collisions. The results are obtained from a data sample of central Pb--Pb collisions, collected during the 2018 LHC data-taking at a center-of-mass energy per nucleon pair of sNN=\sqrt{s_{\mathrm{NN}}} = 5.02 TeV. The yields measured for the average of the charge-conjugated states are found to be [0.78  ±  0.19  (stat.)  ±  0.17  (syst.)]×106[0.78 \; \pm \; 0.19 \; \mathrm{(stat.)} \; \pm \; 0.17 \; \mathrm{(syst.)}] \times 10^{-6} for the (anti)Λ4H{}^4_{\Lambda}\mathrm{H} and [1.08  ±  0.34  (stat.)  ±  0.20  (syst.)]×106[1.08 \; \pm \; 0.34 \; \mathrm{(stat.)} \; \pm \; 0.20 \; \mathrm{(syst.)}] \times 10^{-6} for the (anti)Λ4He{}^4_{\Lambda}\mathrm{He}, and the measured antiparticle-to-particle ratios are in agreement with unity. The presence of (anti)Λ4H{}^4_{\Lambda}\mathrm{H} and (anti)Λ4He{}^4_{\Lambda}\mathrm{He} excited states is expected to strongly enhance the production yield of these hypernuclei. The yield values exhibit a combined deviation of 3.3σ\sigma from the theoretical ground-state-only expectation, while the inclusion of the excited states in the calculations leads to an agreement within 0.6σ\sigma with the present measurements. Additionally, the measured (anti)Λ4H{}^4_{\Lambda}\mathrm{H} and (anti)Λ4He{}^4_{\Lambda}\mathrm{He} masses are compatible with the world-average values within the uncertainties

    An introduction to Spent Nuclear Fuel decay heat for Light Water Reactors: a review from the NEA WPNCS

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    International audienceThis paper summarized the efforts performed to understand decay heat estimation from existing spent nuclear fuel (SNF), under the auspices of the Working Party on Nuclear Criticality Safety (WPNCS) of the OECD Nuclear Energy Agency. Needs for precise estimations are related to safety, cost, and optimization of SNF handling, storage, and repository. The physical origins of decay heat (a more correct denomination would be decay power) are then introduced, to identify its main contributors (fission products and actinides) and time-dependent evolution. Due to limited absolute prediction capabilities, experimental information is crucial; measurement facilities and methods are then presented, highlighting both their relevance and our need for maintaining the unique current full-scale facility and developing new ones. The third part of this report is dedicated to the computational aspect of the decay heat estimation: calculation methods, codes, and validation. Different approaches and implementations currently exist for these three aspects, directly impacting our capabilities to predict decay heat and to inform decision-makers. Finally, recommendations from the expert community are proposed, potentially guiding future experimental and computational developments. One of the most important outcomes of this work is the consensus among participants on the need to reduce biases and uncertainties for the estimated SNF decay heat. If it is agreed that uncertainties (being one standard deviation) are on average small (less than a few percent), they still substantially impact various applications when one needs to consider up to three standard deviations, thus covering more than 95% of cases. The second main finding is the need of new decay heat measurements and validation for cases corresponding to more modern fuel characteristics: higher initial enrichment, higher average burnup, as well as shorter and longer cooling time. Similar needs exist for fuel types without public experimental data, such as MOX, VVER, or CANDU fuels. A third outcome is related to SNF assemblies for which no direct validation can be performed, representing the vast majority of cases (due to the large number of SNF assemblies currently stored, or too short or too long cooling periods of interest). A few solutions are possible, depending on the application. For the final repository, systematic measurements of quantities related to decay heat can be performed, such as neutron or gamma emission. This would provide indications of the SNF decay heat at the time of encapsulation. For other applications (short- or long-term cooling), the community would benefit from applying consistent and accepted recommendations on calculation methods, for both decay heat and uncertainties. This would improve the understanding of the results and make comparisons easier

    Search for Eccentric Black Hole Coalescences during the Third Observing Run of LIGO and Virgo

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    International audienceDespite the growing number of confident binary black hole coalescences observed through gravitational waves so far, the astrophysical origin of these binaries remains uncertain. Orbital eccentricity is one of the clearest tracers of binary formation channels. Identifying binary eccentricity, however, remains challenging due to the limited availability of gravitational waveforms that include effects of eccentricity. Here, we present observational results for a waveform-independent search sensitive to eccentric black hole coalescences, covering the third observing run (O3) of the LIGO and Virgo detectors. We identified no new high-significance candidates beyond those that were already identified with searches focusing on quasi-circular binaries. We determine the sensitivity of our search to high-mass (total mass M>70MM_\odot) binaries covering eccentricities up to 0.3 at 15 Hz orbital frequency, and use this to compare model predictions to search results. Assuming all detections are indeed quasi-circular, for our fiducial population model, we place an upper limit for the merger rate density of high-mass binaries with eccentricities 0 < e \leq 0.3 at 0.330.33 Gpc3^{-3} yr1^{-1} at 90% confidence level

    Studying strangeness and baryon production mechanisms through angular correlations between charged Ξ\Xi baryons and identified hadrons in pp collisions at s\sqrt{s} = 13 TeV

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    International audienceThe angular correlations between charged Ξ\Xi baryons and associated identified hadrons (pions, kaons, protons, Λ\Lambda baryons, and Ξ\Xi baryons) are measured in pp collisions at s=13\sqrt{s} = 13 TeV with the ALICE detector to give insight into the particle production mechanisms and balancing of quantum numbers on the microscopic level. In particular, the distribution of strangeness is investigated in the correlations between the doubly-strange Ξ\Xi baryon and mesons and baryons that contain a single strange quark, K and Λ\Lambda. As a reference, the results are compared to Ξπ\Xi\pi and Ξp\Xi\mathrm{p} correlations, where the associated mesons and baryons do not contain a strange valence quark. These measurements are expected to be sensitive to whether strangeness is produced through string breaking or in a thermal production scenario. Furthermore, the multiplicity dependence of the correlation functions is measured to look for the turn-on of additional particle production mechanisms with event activity. The results are compared to predictions from the string-breaking model PYTHIA 8, including tunes with baryon junctions and rope hadronisation enabled, the cluster hadronisation model HERWIG 7, and the core-corona model EPOS-LHC. While some aspects of the experimental data are described quantitatively or qualitatively by the Monte Carlo models, no one model can match all features of the data. These results provide stringent constraints on the strangeness and baryon number production mechanisms in pp collisions

    Coherent gluon radiation: beyond leading-log accuracy

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    International audienceResults are presented for the medium-induced, soft coherent radiation spectrum for all 222\to 2 partonic channels in QCD, at leading-order in αs\alpha_s but beyond leading logarithmic accuracy. The general formula is valid in the full kinematic range of the underlying process, and reduces to previous results in special cases. The soft gluon radiation spectrum is expressed in terms of the color density matrix specific to each channel, quantifying the entanglement between the color components of the 222 \to 2 production amplitude. Beyond the leading logarithm, the spectrum depends explicitly on the off-diagonal elements of this matrix, owing to the soft gluon's ability to probe the internal color structure of the parton pair

    On the study of new proxies for second order cumulants of conserved charges in heavy-ion collisions with EPOS4

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    International audienceProxies for cumulants of baryon number BB, electric charge QQ and strangeness SS are usually measured in heavy-ion collisions via moments of net-number distribution of given hadronic species. Since these cumulants of conserved charges are expected to be sensitive to the existence of a critical point in the phase diagram of nuclear matter, it is crucial to ensure that the proxies used as substitutes are as close to them as possible. Hence, we use the EPOS4 framework to generate Au+Au collisions at several collision energies of the RHIC Beam Energy Scan. We compute 2nd2^\text{nd} order net-cumulants of π\pi, KK and pp, for which experimental data has been published, as well as the corresponding conserved charge cumulants. We then compare them with proxies, defined in previous lattice QCD and Hadron Resonance Gas model studies, which are shown to reproduce more accurately their associated conserved charge cumulants. We investigate the impact of hadronic re-scatterings occurring in the late evolution of the system on these quantities, as well as the amount of signal actually originating from the bulk medium which endures a phase transition

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