J. D. Zornoza’s research while affiliated with Instituto de Física Corpuscular and other places

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Publications (200)


Figure 3. Distribution of λ values from 2000 pseudo-experiments used to carry out the goodness-of-fit test. The vertical line indicates the observed value of λ corresponding to the best fit to the data.
Figure 4. Allowed region at 90% CL obtained from ORCA6 data for the θ 23 − α 3 parameters. The best-fit value is indicated with a dot.
Figure 5. Profiled log-likelihood ratio of the invisible decay parameter, α 3 . The black line represents the observed result. Horizontal dashed lines represent the 68% and 90% CL thresholds assuming Wilks' theorem, while the red and blue lines show respectively the 68% and 90% Feldman-Cousins CL. The uncertainty bands are the standard deviation with respect to the CLs derived by sampling the pseudo-experiments with replacement.
Figure 6. Distribution of the test statistic ∆λ, obtained from a set of 2000 pseudo-experiments generated assuming as true NuFit v5.0 values and α 3 = 0. The vertical line indicates the observed test statistic value.
Probing invisible neutrino decay with the first six detection units of KM3NeT/ORCA
  • Article
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April 2025

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53 Reads

Journal of High Energy Physics

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A. R. Alhebsi

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N. Zywucka

A bstract In the era of precision measurements of neutrino oscillation parameters, it is necessary for experiments to disentangle discrepancies that may indicate physics beyond the Standard Model in the neutrino sector. KM3NeT/ORCA is a water Cherenkov neutrino detector under construction and anchored at the bottom of the Mediterranean Sea. The detector is designed to study the oscillations of atmospheric neutrinos and determine the neutrino mass ordering. This paper focuses on the initial configuration of ORCA, referred to as ORCA6, which comprises six out of the foreseen 115 detection units of photosensors. A high-purity neutrino sample was extracted during 2020 and 2021, corresponding to an exposure of 433 kton-years. This sample is analysed following a binned log-likelihood approach to search for invisible neutrino decay, in a three-flavour neutrino oscillation scenario, where the third neutrino mass state ν 3 decays into an invisible state, e.g. a sterile neutrino. The resulting best fit of the invisible neutrino decay parameter is α3=0.920.57+1.08×104 {\alpha}_3={0.92}_{-0.57}^{+1.08}\times {10}^{-4} α 3 = 0.92 − 0.57 + 1.08 × 10 − 4 eV ² , corresponding to a scenario with θ 23 in the second octant and normal neutrino mass ordering. The results are consistent with the Standard Model, within a 2.1 σ interval.

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The ANTARES detector: two decades of neutrino searches in the Mediterranean Sea

April 2025

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13 Reads

Interest for studying cosmic neutrinos using deep-sea detectors has increase after the discovery of a diffuse flux of cosmic neutrinos by the IceCube collaboration and the possibility of wider multi-messenger studies with the observations of gravitational waves. The ANTARES detector was the first neutrino telescope in seawater, operating successfully in the Mediterranean Sea for more than a decade and a half. All challenges related to the operation in the deep sea were accurately addressed by the collaboration. Deployment and connection operations became smoother over time; data taking and constant re-calibration of the detector due to the variable environmental conditions were fully automated. A wealth of results on the subject of astroparticle physics, particle physics and multi-messenger astronomy have been obtained, despite the relative modest size of the detector, paving the way to a new generation of larger undersea detectors. This review summarizes the efforts by the ANTARES collaboration that made the possibility to operate neutrino telescopes in seawater a reality and the results obtained in this endeavor.


First searches for dark matter with the KM3NeT neutrino telescopes

March 2025

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20 Reads

Indirect dark matter detection methods are used to observe the products of dark matter annihilations or decays originating from astrophysical objects where large amounts of dark matter are thought to accumulate. With neutrino telescopes, an excess of neutrinos is searched for in nearby dark matter reservoirs, such as the Sun and the Galactic Centre, which could potentially produce a sizeable flux of Standard Model particles. The KM3NeT infrastructure, currently under construction, comprises the ARCA and ORCA undersea Čerenkov neutrino detectors located at two different sites in the Mediterranean Sea, offshore of Italy and France, respectively. The two detector configurations are optimised for the detection of neutrinos of different energies, enabling the search for dark matter particles with masses ranging from a few GeV/c ² to hundreds of TeV/c ² . In this work, searches for dark matter annihilations in the Galactic Centre and the Sun with data samples taken with the first configurations of both detectors are presented. No significant excess over the expected background was found in either of the two analyses. Limits on the velocity-averaged self-annihilation cross section of dark matter particles are computed for five different primary annihilation channels in the Galactic Centre. For the Sun, limits on the spin-dependent and spin-independent scattering cross sections of dark matter with nucleons are given for three annihilation channels.


Search for quantum decoherence in neutrino oscillations with six detection units of KM3NeT/ORCA

March 2025

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28 Reads

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2 Citations

Neutrinos described as an open quantum system may interact with the environment which introduces stochastic perturbations to their quantum phase. This mechanism leads to a loss of coherence along the propagation of the neutrino - a phenomenon commonly referred to as decoherence - and ultimately, to a modification of the oscillation probabilities. Fluctuations in space-time, as envisaged by various theories of quantum gravity, are a potential candidate for a decoherence-inducing environment. Consequently, the search for decoherence provides a rare opportunity to investigate quantum gravitational effects which are usually beyond the reach of current experiments. In this work, quantum decoherence effects are searched for in neutrino data collected by the KM3NeT/ORCA detector from January 2020 to November 2021. The analysis focuses on atmospheric neutrinos within the energy range of a few GeV to 100 GeV. Adopting the open quantum system framework, decoherence is described in a phenomenological manner with the strength of the effect given by the parameters Γ21 and Γ31. Following previous studies, a dependence of the type Γ ij ∝ (E/E 0) ⁿ on the neutrino energy is assumed and the cases n = -2,-1 are explored. No significant deviation with respect to the standard oscillation hypothesis is observed. Therefore, 90% CL upper limits are estimated as Γ21 < 4.6· 10²¹GeV and Γ31 < 8.4· 10²¹GeV for n = -2 and Γ21 < 1.9· 10⁻²²GeV and Γ31 < 2.7· 10⁻²²GeV for n = -1, respectively.



Search for non-standard neutrino interactions with the first six detection units of KM3NeT/ORCA

February 2025

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55 Reads

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1 Citation

KM3NeT/ORCA is an underwater neutrino telescope under construction in the Mediterranean Sea. Its primary scientific goal is to measure the atmospheric neutrino oscillation parameters and to determine the neutrino mass ordering. ORCA can constrain the oscillation parameters Δm ² 31 and θ 23 by reconstructing the arrival direction and energy of multi-GeV neutrinos crossing the Earth. Searches for deviations from the Standard Model of particle physics in the forward scattering of neutrinos inside Earth matter, produced by Non-Standard Interactions, can be conducted by investigating distortions of the standard oscillation pattern of neutrinos of all flavours. This work reports on the results of the search for non-standard neutrino interactions using the first six detection units of ORCA and 433 kton-years of exposure. No significant deviation from standard interactions was found in a sample of 5828 events reconstructed in the 1 GeV-1 TeV energy range. The flavour structure of the non-standard coupling was constrained at 90% confidence level to be |εμτ | ≤ 5.4 × 10⁻³, |εeτ | ≤ 7.4 × 10⁻², |εeμ | ≤ 5.6 × 10⁻² and -0.015 ≤ εττ - εμμ ≤ 0.017. The results are comparable to the current most stringent limits placed on the parameters by other experiments.


KM3NeT Constraint on Lorentz-Violating Superluminal Neutrino Velocity

February 2025

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60 Reads

Lorentz invariance is a fundamental symmetry of spacetime and foundational to modern physics. One of its most important consequences is the constancy of the speed of light. This invariance, together with the geometry of spacetime, implies that no particle can move faster than the speed of light. In this article, we present the most stringent neutrino-based test of this prediction, using the highest energy neutrino ever detected to date, KM3-230213A. The arrival of this event, with an energy of 220110+570PeV220^{+570}_{-110}\,\text{PeV}, sets a constraint on δcν21<4×1022\delta \equiv c_\nu^2-1 < 4\times10^{-22}.


On the Potential Galactic Origin of the Ultra-High-Energy Event KM3-230213A

February 2025

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54 Reads

The KM3NeT observatory detected the most energetic neutrino candidate ever observed, with an energy between 72 PeV and 2.6 EeV at the 90% confidence level. The observed neutrino is likely of cosmic origin. In this article, it is investigated if the neutrino could have been produced within the Milky Way. Considering the low fluxes of the Galactic diffuse emission at these energies, the lack of a nearby potential Galactic particle accelerator in the direction of the event and the difficulty to accelerate particles to such high energies in Galactic systems, we conclude that if the event is indeed cosmic, it is most likely of extragalactic origin.


The ultra-high-energy event KM3-230213A within the global neutrino landscape

February 2025

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34 Reads

On February 13th, 2023, the KM3NeT/ARCA telescope detected a neutrino candidate with an estimated energy in the hundreds of PeVs. In this article, the observation of this ultra-high-energy neutrino is discussed in light of null observations above tens of PeV from the IceCube and Pierre Auger observatories. Performing a joint fit of all experiments under the assumption of an isotropic E2E^{-2} flux, the best-fit single-flavour flux normalisation is E2Φν+νˉ1f=7.5×1010 GeVcm2s1sr1E^2 \Phi^{\rm 1f}_{\nu + \bar \nu} = 7.5 \times 10^{-10}~{\rm GeV cm^{-2} s^{-1} sr^{-1}} in the 90% energy range of the KM3NeT event. Furthermore, the ultra-high-energy data are then fit together with the IceCube measurements at lower energies, either with a single power law or with a broken power law, allowing for the presence of a new component in the spectrum. The joint fit including non-observations by other experiments in the ultra-high-energy region shows a slight preference for a break in the PeV regime if the ``High-Energy Starting Events'' sample is included, and no such preference for the other two IceCube samples investigated. A stronger preference for a break appears if only the KM3NeT data is considered in the ultra-high-energy region, though the flux resulting from such a fit would be inconsistent with null observations from IceCube and Pierre Auger. In all cases, the observed tension between KM3NeT and other datasets is of the order of 2.5σ3σ2.5\sigma-3\sigma, and increased statistics are required to resolve this apparent tension and better characterise the neutrino landscape at ultra-high energies.


Fig. 1 | Views of the event. a, Side and top views of the event. The reconstructed trajectory of the muon is shown as a red line, along with an artist's representation of the Cherenkov light cone. The hits of individual PMTs are represented by spheres stacked along the direction of the PMT orientations. Only the first five hits on each PMT are shown. As indicated in the legend, the spheres are coloured according to the detection time relative to the first triggered hit. The size of the spheres is proportional to the number of photons detected by the corresponding PMT. The locations of the secondary cascades, discussed in the Supplementary Material, are indicated by the black spheres along the muon trajectory. The north direction is indicated by a red arrow. A 100-m scale and the Eiffel Tower (330 m height, 125 m base width) are shown for size comparison. b, Zoomed-in view of the optical modules that are close to the first two observed secondary showers in the event. Here light-blue spheres represent hits that arrive within −5 to 25 ns of the expected Cherenkov arrival times.
Fig. 2 | Number of PMTs in the event. The normalized distributions of the number of PMTs participating in the triggering of the event for simulated muon energies of 10, 100 and 1,000 PeV. The vertical dashed line indicates the observed value in KM3-230213A, N = 3,672 trig PMT . The dashed histograms represent the distributions from the nominal simulations, whereas, in the filled histograms, systematic uncertainties are included by weighting the simulations according to a normal distribution, centred at the nominal value of the nuisance parameter and with a ±10% uncertainty. At the highest energy, the distributions seem to be truncated around N = 6,000
Observation of an ultra-high-energy cosmic neutrino with KM3NeT

February 2025

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300 Reads

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59 Citations

Nature

The detection of cosmic neutrinos with energies above a teraelectronvolt (TeV) offers a unique exploration into astrophysical phenomena1–3. Electrically neutral and interacting only by means of the weak interaction, neutrinos are not deflected by magnetic fields and are rarely absorbed by interstellar matter: their direction indicates that their cosmic origin might be from the farthest reaches of the Universe. High-energy neutrinos can be produced when ultra-relativistic cosmic-ray protons or nuclei interact with other matter or photons, and their observation could be a signature of these processes. Here we report an exceptionally high-energy event observed by KM3NeT, the deep-sea neutrino telescope in the Mediterranean Sea⁴, which we associate with a cosmic neutrino detection. We detect a muon with an estimated energy of 12060+11012{0}_{-60}^{+110} petaelectronvolts (PeV). In light of its enormous energy and near-horizontal direction, the muon most probably originated from the interaction of a neutrino of even higher energy in the vicinity of the detector. The cosmic neutrino energy spectrum measured up to now5–7 falls steeply with energy. However, the energy of this event is much larger than that of any neutrino detected so far. This suggests that the neutrino may have originated in a different cosmic accelerator than the lower-energy neutrinos, or this may be the first detection of a cosmogenic neutrino⁸, resulting from the interactions of ultra-high-energy cosmic rays with background photons in the Universe.


Citations (62)


... More recently, IceCube discovered a point-source of neutrinos from the active galaxy NGC1068 [5]. In the UHE range, a 120 PeV neutrino has been detected by KM3NeT; however, it is as of yet not associated with any known sources [6]. The UHE neutrino sky is thus largely unexplored and can provide unique insights into particle astrophysics at the highest energies. ...

Reference:

Sensitivity of BEACON to Ultra-High Energy Diffuse and Transient Neutrinos
Author Correction: Observation of an ultra-high-energy cosmic neutrino with KM3NeT

Nature

... Therefore, precise knowledge of the atmospheric neutrino flux and neutrino-water cross section in this energy range is essential. Recent analyses with an initial six-line configuration have demonstrated ORCA's immense potential not only for studying neutrino oscillations but also for probing BSM physics [51][52][53][54][55]. The event generator used to simulate neutrino interaction in this analyses is GENIE. ...

Search for quantum decoherence in neutrino oscillations with six detection units of KM3NeT/ORCA

... Therefore, precise knowledge of the atmospheric neutrino flux and neutrino-water cross section in this energy range is essential. Recent analyses with an initial six-line configuration have demonstrated ORCA's immense potential not only for studying neutrino oscillations but also for probing BSM physics [51][52][53][54][55]. The event generator used to simulate neutrino interaction in this analyses is GENIE. ...

Search for non-standard neutrino interactions with the first six detection units of KM3NeT/ORCA

... In [4] the experiment KM3Net [5] reports the detection of an extremely high energy muon with energy E μ = 120 +110 −60 PeV by the ARCA detector in the Mediterranean sea. The muon traverses the full detector for a length of approximately l μ ∼ 500 m implying that at about 90 % confidence level the decay length is larger than (l μ /2.3) ∼ 220 m, 2 the most likely value for the muon Lorentz factor is γ = 120PeV/(m μ c 2 ) ∼ 1.15 × 10 9 and the value 1-σ lower is γ σ = 60PeV/(m μ c 2 ) ∼ 0.57 × 10 9 . ...

Observation of an ultra-high-energy cosmic neutrino with KM3NeT

Nature

... Modern accelerator-based neutrino experiments are capable of expansive physics programs that address a variety of important topics. These include charge-parity violation in the neutrino sector [1,2], the neutrino mass ordering [3], measurements of rare standard model processes [4][5][6][7], searches for sterile neutrinos [8,9], and other physics beyond the standard model (BSM) [10,11]. Many of these analyses require measuring the rate of interactions that produce single electrons [12][13][14][15][16], single photons [4,6], or boosted and overlapping e þ e − or γγ pairs [17][18][19][20] by selecting events that leave an electromagnetic shower signature in the detector. ...

White paper on light sterile neutrino searches and related phenomenology

... l. (2010, their Figure 12), we find Phaedra located in the region common to spiral galaxies, starburst galaxies, and luminous IR galaxies. Being in the starburst region indicates that Phaedra may be experiencing a starburst, potentially caused by AGN feedback, which provides another potential site of particle acceleration (A. Marinelli et al. 2021;S. Aiello et al. 2024). While we lack direct observational evidence for star-forming galaxies as UHE neutrino sources (K. Bechtol et al. 2017), there are numerous models that predict these areas can produce neutrinos up to PeV energies (A. M. Bykov et al. 2015). ...

Differential Sensitivity of the KM3NeT/ARCA detector to a diffuse neutrino flux and to point-like source emission: Exploring the case of the Starburst Galaxies
  • Citing Article
  • October 2024

Astroparticle Physics

... ARCA's main goal is the detection of high-energy neutrinos from astrophysical sources, with energies ranging from a few TeV to PeV [56]. Due to its geographical location and excellent pointing accuracy, ARCA is particularly well-suited for identifying neutrino sources within the Milky Way at TeV energies. ...

Astronomy potential of KM3NeT/ARCA

The European Physical Journal C

... The energy aligns with the peak of the boosted CνB flux as shown in the upper panel of Fig. 4, and this coincidence allows us to entertain the possibility of explain- KM3NeT. Also shown are limits on the diffuse cosmogenic flux from IceCube (90% CL) [43,46], Pierre Auger (90% CL) [44], and ANTARES (95% CL) [51], alongside the measured astrophysical neutrino spectrum from IceCube analysis of high-energy starting events (HESE) [52], northern sky tracks (NST) [53], and downgoing PeV events (DPeV) [54]. Various cosmogenic neutrino flux models [55][56][57] are also shown as gray curves for comparison. ...

Constraints on the energy spectrum of the diffuse cosmic neutrino flux from the ANTARES neutrino telescope