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KM3NeT Collaboration(Adriani, O. et al), Alves Garre, S., Bariego-Quintana, A., Calvo, D., Cecchini, V., Garcia Soto, A., et al. (2026). Constraining gamma-ray burst parameters with the first ultra-high energy neutrino event KM3-230213A. Astron. Astrophys., 710, A168–11pp.
Abstract: Context. The detection of the highest energy neutrino observed to date by KM3NeT, with an estimated energy of 220 PeV, opens up new possibilities for the study and identification of the astrophysical sources responsible for a di ffuse flux of such ultra-high-energy neutrinos, among which gamma-ray bursts are longstanding candidates. Aims. Based on the event KM3-230213A, we derived constraints on the baryon loading and density of the surrounding environment in models of blast waves in long-duration gamma-ray bursts. Methods. We computed the di ffuse flux from gamma-ray burst blast waves, either expanding in a constant density interstellar medium or developing in a radially decreasing density of a wind-like environment surrounding the gamma-ray burst progenitor star, by taking into account the expected neutrino spectra and luminosity function. We used a Poisson likelihood method to constrain the blast wave model parameters by calculating the expected number of neutrino events within the 90% confidence level energy range of KM3-230213A and by using the joint exposure of KM3NeT/ARCA, IceCube, and Pierre Auger. Results. We constrain the baryon loading to be f(b) <= 51 at 90% confidence, with the best-fit and 68% confidence interval being f(b) = 26.9(-17.2)(+11.4) for a constant interstellar medium particle density of n(0) = 1 cm(-3). In the wind-like environment case, the baryon loading is fb similar to 1095 at 90% confidence, with the corresponding 68% confidence interval being f(b) is an element of [8, 231], which is proportional to the sixth power of a variable density parameter of A(*) = 0.1.
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Collar, J. I., Esteban, I., Gomez-Cadenas, J. J., Gonzalez-Garcia, M. C., Ji, L., Larizgoitia, L., et al. (2026). Coherent elastic neutrino-nucleus scattering at the Japan Proton Accelerator Research Complex. J. High Energy Phys., 05(5), 106–44pp.
Abstract: The Japan Proton Accelerator Research Complex (J-PARC) currently delivers a 1 MW, 3 GeV proton beam to the Materials and Life Science Experimental Facility (MLF). Power is expected to increase to 1.3 MW, driven by the needs of Hyper-Kamiokande. As a result, the MLF presently provides the highest neutron yield of any spallation source, while potentially holding the best current and foreseeable conditions for Coherent Elastic Neutrino-Nucleus Scattering (CE nu NS) experimentation. We explore this potential, using as examples detector technologies presently funded for construction and under development. We quantify their sensitivity to a rich variety of particle physics scenarios, finding that very-high-statistics CE nu NS measurements with significant sensitivity to relevant scenarios are feasible at this facility within the next few years.
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KM3NeT Collaboration(van Haren, H. et al), Alves Garre, S., Bariego-Quintana, A., Calvo, D., Cecchini, V., Garcia Soto, A., et al. (2026). Whipped and Mixed Warm Clouds in the Deep Sea. Geophys. Res. Lett., 53(2), e2025GL119998–13pp.
Abstract: Turbulence is indispensable to redistribute nutrients for all life forms larger than microbial, on land and in the ocean. Yet, the development of deep-sea turbulence was not studied in three dimensions to date. As a disproportionate laboratory, an array of nearly 3,000 high-resolution temperature sensors had been installed for three years on the flat 2,500-m deep bottom of the Mediterranean Sea. The time series from the half-cubic hectometer mooring-array allows for the creation of unique movies of deep-sea water motions. Although temperature differences are typically 0.001 degrees C, variable convection-turbulence is observed as expected from geothermal heating through the flat seafloor. During about 40% of the time, an additional turbulence, 3 times stronger in magnitude, is observed from slantwise advected warmer waters to pass in turbulent clouds. Besides turbulent clouds and seafloor heating, movies also reveal weakly turbulent interfacial-wave breakdown that commonly occurs in the open ocean far away from boundaries.
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DUNE Collaboration(Abbaslu, S. et al), Amar Es-Sghir, H., Amedo, P., Barenboim, G., Benitez Montiel, C., Capo, J., et al. (2026). Measurement of exclusive π+-argon interactions using ProtoDUNE-SP. Phys. Rev. D, 113(11), 112002–21pp.
Abstract: We present the measurement of pi(+)-argon inelastic cross sections using the ProtoDUNE single-phase liquid argon time projection chamber in the incident pi(+) kinetic energy range of 500-800 MeV in multiple exclusive channels (absorption, charge exchange, and the remaining inelastic interactions). The results of this analysis are important inputs to simulations of liquid argon neutrino experiments such as the Deep Underground Neutrino Experiment and the Short Baseline Neutrino program at Fermi National Accelerator Laboratory. They will be employed to improve the modeling of final state interactions within neutrino event generators used by these experiments, as well as the modeling of pi(+)-argon secondary interactions within the liquid argon. This is the first measurement of pi(+)-argon absorption at this kinetic energy range as well as the first ever measurement of pi(+)-argon charge exchange.
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LHCb Collaboration(Aaij, R. et al), Fernandez Casani, A., Jaimes Elles, S. J., Jashal, B. K., Libralon, S., Lucio Martinez, M., et al. (2026). Measurement of the Top-Quark Production Cross Section and Charge Asymmetry at LHCb. Phys. Rev. Lett., 136(22), 221801–15pp.
Abstract: The first measurements of the top- and antitop-quark differential production cross sections and the top-quark charge asymmetry in the forward region are presented, using proton-proton collision data collected by the LHCb experiment at a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 5.4 fb(-1). The total production cross sections of top and antitop quarks are also determined. Measurements are performed using the μ+ b-jet final state within a fiducial region defined by b-jet p(T, jet) > 50 GeV and pseudorapidity 2.2 < eta(jet) < 4.0, with the muon from the W-boson decay required to have p(T, mu) > 25 GeV and 2.0 < eta(mu) < 4.5. The muon and b-jet system must satisfy p(T)(mu + jet) > 20 GeV. The measured integrated production cross sections for the top and antitop quarks are sigma(t) = 0.95 +/- 0.04 +/- 0.08 +/- 0.02 pb, sigma((t) over bar) = 0.81 +/- 0.03 +/- 0.07 +/- 0.02 pb, where the first uncertainty is statistical, the second systematic, and the third accounts for the luminosity uncertainty. The top-quark charge asymmetry is measured to be A(C)(t) = 0.08 +/- 0.03 +/- 0.01, where the first uncertainty is statistical and the second is systematic. These results are consistent with next-to-leading order Standard Model predictions.
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