Ivan Esteban
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Research Subjects
Ivan Esteban has a total of 55 co-authors. Here are the top co-authors by number of shared publications:
- Maria Concepcion Gonzalez-Garcia
Stony Brook University
26 shared publications - Michele Maltoni
Instituto de Física Teórica (IFT-CFTMAT) CSIC-UAM Calle de Nicolás Cabrera 13-15 Cam- pus de Cantoblanco E-28049 Madrid Spain
16 shared publications - Jordi Salvado
Departament de Fisíca Quántica i Astrofísica and Institut de Ciencies del Cosmos, Universitat de Barcelona, Diagonal 647, E-08028 Barcelona, Spain
12 shared publications - Ivan Martinez-Soler
Durham University
10 shared publications - Pilar Coloma
Universidad Autónoma de Madrid
9 shared publications - Thomas Schwetz
Karlsruher Institut für Technologie (KIT)
7 shared publications
Latest Publications
- Open Access
- 1 October 2026
- Published by IOP Publishing in Journal of Cosmology and Astroparticle Physics
- Vol. 2026 (10)
Exploring neutrino loss with difusse astrophysical neutrino fluxes
We study the sensitivity of the difusse high-energy neutrino flux observed in IceCube to new-physics effects resulting in an exponential flux attenuation along the trajectory, such as invisible neutrino decay or new interactions with the background encountered during propagation. We argue that, even though the sources and production redshifts of these astrophysical neutrinos are unknown, conservative energy-conservation arguments allow to severely constrain neutrino loss in most scenarios beyond the strongest existing bounds. By performing a fit to the High-Energy Starting Events from IceCube, we quantify the bounds and study their variation with the energy dependence of the attenuation, the assumed redshift distribution of the neutrino sources, and whether the attenuation affects neutrinos exclusively or no. We also show that including an energy-dependent attenuation at the level allowed in the fit may impact the determination of the spectral index of the diffuse flux.
- 1 October 2026
- Published by IOP Publishing in Journal of Cosmology and Astroparticle Physics
- Vol. 2026 (10)
Open AccessExploring neutrino loss with difusse astrophysical neutrino fluxes
We study the sensitivity of the difusse high-energy neutrino flux observed in IceCube to new-physics effects resulting in an exponential flux attenuation along the trajectory, such as invisible neutrino decay or new interactions with the background encountered during propagation. We argue that, even though the sources and production redshifts of these astrophysical neutrinos are unknown, conservative energy-conservation arguments allow to severely constrain neutrino loss in most scenarios beyond the strongest existing bounds. By performing a fit to the High-Energy Starting Events from IceCube, we quantify the bounds and study their variation with the energy dependence of the attenuation, the assumed redshift distribution of the neutrino sources, and whether the attenuation affects neutrinos exclusively or no. We also show that including an energy-dependent attenuation at the level allowed in the fit may impact the determination of the spectral index of the diffuse flux.
- Open Access
- 11 May 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (5) , 106
Coherent elastic neutrino-nucleus scattering at the Japan Proton Accelerator Research Complex
A bstract: 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 ν 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 ν NS measurements with significant sensitivity to relevant scenarios are feasible at this facility within the next few years.
- 11 May 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (5) , 106
Open AccessCoherent elastic neutrino-nucleus scattering at the Japan Proton Accelerator Research Complex
A bstract: 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 ν 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 ν NS measurements with significant sensitivity to relevant scenarios are feasible at this facility within the next few years.
- Open Access
- 10 April 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (4)
Lessons from the first JUNO results
A bstract: First results from the JUNO reactor neutrino experiment already determine with world-leading precision the small neutrino squared-mass splitting $$ \Delta {m}_{21}^2 $$ and the mixing angle θ 12 . In this article we perform an exploratory study beyond these, taking advantage of the first JUNO data release to discuss its sensitivity to the large squared-mass splitting, $$ \Delta {m}_{3\ell}^2 $$ . When combined with constraints from global oscillation data, this may already contain some information on the neutrino mass ordering. Indeed, we find that the combination of the complementary $$ \Delta {m}_{3\ell}^2 $$ -determinations gives a slight preference for Normal Ordering, with a p -value for Inverted Ordering of 2%–2.6% (2 . 2 σ –2 . 3 σ ). We study the robustness of this result with respect to potential systematic uncertainties and statistical fluctuations. Taken at face value, a full global analysis of oscillation data including the publicly available JUNO information and data leads to a preference for Normal Ordering with ∆ χ 2 = 4.6 and 9.4 without and with Super-K and IceCube-24 atmospheric neutrino data, respectively.- 10 April 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (4)
Open AccessLessons from the first JUNO results
A bstract: First results from the JUNO reactor neutrino experiment already determine with world-leading precision the small neutrino squared-mass splitting $$ \Delta {m}_{21}^2 $$ and the mixing angle θ 12 . In this article we perform an exploratory study beyond these, taking advantage of the first JUNO data release to discuss its sensitivity to the large squared-mass splitting, $$ \Delta {m}_{3\ell}^2 $$ . When combined with constraints from global oscillation data, this may already contain some information on the neutrino mass ordering. Indeed, we find that the combination of the complementary $$ \Delta {m}_{3\ell}^2 $$ -determinations gives a slight preference for Normal Ordering, with a p -value for Inverted Ordering of 2%–2.6% (2 . 2 σ –2 . 3 σ ). We study the robustness of this result with respect to potential systematic uncertainties and statistical fluctuations. Taken at face value, a full global analysis of oscillation data including the publicly available JUNO information and data leads to a preference for Normal Ordering with ∆ χ 2 = 4.6 and 9.4 without and with Super-K and IceCube-24 atmospheric neutrino data, respectively. - Open Access
- 1 April 2026
- Published by IOP Publishing in Journal of Cosmology and Astroparticle Physics
- Vol. 2026 (04)
Attenuation of the ultra-high-energy neutrino flux by dark matter scatterings
A flux of ultra-high-energy (UHE) neutrinos, produced by astrophysical sources at cosmological distances, is anticipated to exist and reach Earth. In this paper, we investigate the impact on the total flux, energy spectrum, and arrival directions of UHE neutrinos of neutrino-dark matter (DM) scatterings. We study scatterings both in the intergalactic medium and in the Milky Way. We emphasize the complementarity among neutrino detectors at different latitudes, that can probe anisotropies induced by neutrinos scattering with the Milky Way DM halo. We also discuss that, with mild astrophysical assumptions, limits on the DM-ν scattering cross section can be placed even if the neutrino sources are unknown. Finally, we explore all this phenomenology with the recent UHE neutrino event KM3230213A, and place the corresponding limits on the DM-ν scattering cross section.
- 1 April 2026
- Published by IOP Publishing in Journal of Cosmology and Astroparticle Physics
- Vol. 2026 (04)
Open AccessAttenuation of the ultra-high-energy neutrino flux by dark matter scatterings
A flux of ultra-high-energy (UHE) neutrinos, produced by astrophysical sources at cosmological distances, is anticipated to exist and reach Earth. In this paper, we investigate the impact on the total flux, energy spectrum, and arrival directions of UHE neutrinos of neutrino-dark matter (DM) scatterings. We study scatterings both in the intergalactic medium and in the Milky Way. We emphasize the complementarity among neutrino detectors at different latitudes, that can probe anisotropies induced by neutrinos scattering with the Milky Way DM halo. We also discuss that, with mild astrophysical assumptions, limits on the DM-ν scattering cross section can be placed even if the neutrino sources are unknown. Finally, we explore all this phenomenology with the recent UHE neutrino event KM3230213A, and place the corresponding limits on the DM-ν scattering cross section.
- Open Access
- 1 June 2025
- Published by IOP Publishing in Journal of Cosmology and Astroparticle Physics
- Vol. 2025 (06)
Origin of cosmological neutrino mass bounds: background versus perturbations
The cosmological upper bound on the total neutrino mass is the dominant limit on this fundamental parameter. Recent observations — soon to be improved — have strongly tightened it, approaching the lower limit set by oscillation data. Understanding its physical origin, robustness, and model-independence becomes pressing. Here, we explicitly separate for the first time the two distinct cosmological neutrino-mass effects: the impact on background evolution, related to the energy in neutrino masses; and the “kinematic” impact on perturbations, related to neutrino free-streaming. We scrutinize how they affect CMB anisotropies, introducing two effective masses enclosing background (∑ m ν Backg.) and perturbations (∑ m ν Pert.) effects. We analyze CMB data, finding that the neutrino-mass bound is mostly a background measurement, i.e., how the neutrino energy density evolves with time. The bound on the “kinematic” variable ∑ m ν Pert.. is largely relaxed, ∑ m ν Pert. < 0.8 eV. This work thus adds clarity to the physical origin of the cosmological neutrino-mass bound, which is mostly a measurement of the neutrino equation of state, providing also hints to evade such a bound.
- 1 June 2025
- Published by IOP Publishing in Journal of Cosmology and Astroparticle Physics
- Vol. 2025 (06)
Open AccessOrigin of cosmological neutrino mass bounds: background versus perturbations
The cosmological upper bound on the total neutrino mass is the dominant limit on this fundamental parameter. Recent observations — soon to be improved — have strongly tightened it, approaching the lower limit set by oscillation data. Understanding its physical origin, robustness, and model-independence becomes pressing. Here, we explicitly separate for the first time the two distinct cosmological neutrino-mass effects: the impact on background evolution, related to the energy in neutrino masses; and the “kinematic” impact on perturbations, related to neutrino free-streaming. We scrutinize how they affect CMB anisotropies, introducing two effective masses enclosing background (∑ m ν Backg.) and perturbations (∑ m ν Pert.) effects. We analyze CMB data, finding that the neutrino-mass bound is mostly a background measurement, i.e., how the neutrino energy density evolves with time. The bound on the “kinematic” variable ∑ m ν Pert.. is largely relaxed, ∑ m ν Pert. < 0.8 eV. This work thus adds clarity to the physical origin of the cosmological neutrino-mass bound, which is mostly a measurement of the neutrino equation of state, providing also hints to evade such a bound.
- 9 May 2025
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 134 (18) , 181003
Detectable MeV Neutrino Signals from Neutron-Star Common-Envelope Systems
Common envelope evolution-where a star is engulfed by a companion-is a critical but poorly understood step in, e.g., the formation pathways for gravitational-wave sources. However, it has been extremely challenging to identify observable signatures of such systems. We show that for systems involving a neutron star, the hypothesized super-Eddington accretion onto the neutron star produces MeV-range, months-long neutrino signals within reach of present and planned detectors. While there are substantial uncertainties on the rate of such events (0.01-1/century in the Milky Way) and the neutrino luminosity (which may be less than the accretion power), this signal can only be found if dedicated new analyses are developed. If detected, the neutrino signal would probe super-Eddington accretion, leading to significant new insights into the astrophysics of common envelope evolution.
- 9 May 2025
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 134 (18) , 181003
Detectable MeV Neutrino Signals from Neutron-Star Common-Envelope Systems
Common envelope evolution-where a star is engulfed by a companion-is a critical but poorly understood step in, e.g., the formation pathways for gravitational-wave sources. However, it has been extremely challenging to identify observable signatures of such systems. We show that for systems involving a neutron star, the hypothesized super-Eddington accretion onto the neutron star produces MeV-range, months-long neutrino signals within reach of present and planned detectors. While there are substantial uncertainties on the rate of such events (0.01-1/century in the Milky Way) and the neutrino luminosity (which may be less than the accretion power), this signal can only be found if dedicated new analyses are developed. If detected, the neutrino signal would probe super-Eddington accretion, leading to significant new insights into the astrophysics of common envelope evolution.
- Top Cited PapersOpen Access
- 30 December 2024
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2024 (12) , 1-33
NuFit-6.0: updated global analysis of three-flavor neutrino oscillations
We present an updated global analysis of neutrino oscillation data as of September 2024. The parameters θ 12, θ 13, $$ \Delta {m}_{21}^2 $$ , and $$ \mid \Delta {m}_{3\ell}^2\mid $$ (ℓ = 1, 2) are well-determined with relative precision at 3σ of about 13%, 8%, 15%, and 6%, respectively. The third mixing angle θ 23 still suffers from the octant ambiguity, with no clear indication of whether it is larger or smaller than 45 ° . The determination of the leptonic CP phase δ CP depends on the neutrino mass ordering: for normal ordering the global fit is consistent with CP conservation within 1σ, whereas for inverted ordering CP-violating values of δ CP around 270° are favored against CP conservation at more than 3.6σ. While the present data has in principle 2.5–3σ sensitivity to the neutrino mass ordering, there are different tendencies in the global data that reduce the discrimination power: T2K and NOvA appearance data individually favor normal ordering, but they are more consistent with each other for inverted ordering. Conversely, the joint determination of $$ \mid \Delta {m}_{3\ell}^2\mid $$ from global disappearance data prefers normal ordering. Altogether, the global fit including long-baseline, reactor and IceCube atmospheric data results into an almost equally good fit for both orderings. Only when the χ 2 table for atmospheric neutrino data from Super-Kamiokande is added to our χ 2, the global fit prefers normal ordering with ∆χ 2 = 6.1. We provide also updated ranges and correlations for the effective parameters sensitive to the absolute neutrino mass from β-decay, neutrinoless double-beta decay, and cosmology.- 30 December 2024
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2024 (12) , 1-33
Top Cited PapersOpen AccessNuFit-6.0: updated global analysis of three-flavor neutrino oscillations
We present an updated global analysis of neutrino oscillation data as of September 2024. The parameters θ 12, θ 13, $$ \Delta {m}_{21}^2 $$ , and $$ \mid \Delta {m}_{3\ell}^2\mid $$ (ℓ = 1, 2) are well-determined with relative precision at 3σ of about 13%, 8%, 15%, and 6%, respectively. The third mixing angle θ 23 still suffers from the octant ambiguity, with no clear indication of whether it is larger or smaller than 45 ° . The determination of the leptonic CP phase δ CP depends on the neutrino mass ordering: for normal ordering the global fit is consistent with CP conservation within 1σ, whereas for inverted ordering CP-violating values of δ CP around 270° are favored against CP conservation at more than 3.6σ. While the present data has in principle 2.5–3σ sensitivity to the neutrino mass ordering, there are different tendencies in the global data that reduce the discrimination power: T2K and NOvA appearance data individually favor normal ordering, but they are more consistent with each other for inverted ordering. Conversely, the joint determination of $$ \mid \Delta {m}_{3\ell}^2\mid $$ from global disappearance data prefers normal ordering. Altogether, the global fit including long-baseline, reactor and IceCube atmospheric data results into an almost equally good fit for both orderings. Only when the χ 2 table for atmospheric neutrino data from Super-Kamiokande is added to our χ 2, the global fit prefers normal ordering with ∆χ 2 = 6.1. We provide also updated ranges and correlations for the effective parameters sensitive to the absolute neutrino mass from β-decay, neutrinoless double-beta decay, and cosmology. - 5 December 2024
- Published by American Physical Society (APS) in Physical Review D
- Vol. 110 (12)
Milky Way satellite velocities reveal the dark matter power spectrum at small scales
- 5 December 2024
- Published by American Physical Society (APS) in Physical Review D
- Vol. 110 (12)
Milky Way satellite velocities reveal the dark matter power spectrum at small scales
- 2 August 2024
- Published by American Physical Society (APS) in Physical Review D
- Vol. 110 (4) , 043004
New limits on neutrino decay from high-energy astrophysical neutrinos
Since neutrinos have mass differences they could decay into one another, but their lifetimes are likely long, even when shortened by new physics, so decay likely impacts neutrinos only during long trips. This makes high-energy astrophysical neutrinos, traveling for up to billions of light years, sensitive probes of decay. However, their sensitivity must be tempered by reality. We derive from them thorough bounds on the neutrino lifetimes accounting for critical astrophysical unknowns and the nuances of neutrino detection. Using the diffuse neutrino flux, we disfavor lifetimes , based on present IceCube data, and forecast factor-of-10 improvements by upcoming detectors. Using, for the first time, neutrinos from the active galaxy NGC 1068, extant unknowns preclude placing lifetime bounds today, but upcoming detectors could disfavor .- 2 August 2024
- Published by American Physical Society (APS) in Physical Review D
- Vol. 110 (4) , 043004
New limits on neutrino decay from high-energy astrophysical neutrinos
Since neutrinos have mass differences they could decay into one another, but their lifetimes are likely long, even when shortened by new physics, so decay likely impacts neutrinos only during long trips. This makes high-energy astrophysical neutrinos, traveling for up to billions of light years, sensitive probes of decay. However, their sensitivity must be tempered by reality. We derive from them thorough bounds on the neutrino lifetimes accounting for critical astrophysical unknowns and the nuances of neutrino detection. Using the diffuse neutrino flux, we disfavor lifetimes , based on present IceCube data, and forecast factor-of-10 improvements by upcoming detectors. Using, for the first time, neutrinos from the active galaxy NGC 1068, extant unknowns preclude placing lifetime bounds today, but upcoming detectors could disfavor .- Open Access
New limits on neutrino decay from high-energy astrophysical neutrinos
Since neutrinos have mass differences, they could decay into one another. But their lifetimes are likely long, even when shortened by new physics, so decay likely impacts neutrinos only during long trips. This makes high-energy astrophysical neutrinos, traveling for up to billions of light-years, sensitive probes of decay. However, their sensitivity must be tempered by reality. We derive from them thorough bounds on the neutrino lifetimes accounting for critical astrophysical unknowns and the nuances of neutrino detection. Using the diffuse neutrino flux, we disfavor lifetimes $τ\lesssim 20$-450 s $(m/{\rm eV})$, based on present IceCube data, and forecast factor-of-10 improvements by upcoming detectors. Using, for the first time, neutrinos from the active galaxy NGC 1068, extant unknowns preclude placing lifetime bounds today, but upcoming detectors could disfavor $τ\sim 100$-5000 s $(m/{\rm eV})$.Open AccessNew limits on neutrino decay from high-energy astrophysical neutrinos
Since neutrinos have mass differences, they could decay into one another. But their lifetimes are likely long, even when shortened by new physics, so decay likely impacts neutrinos only during long trips. This makes high-energy astrophysical neutrinos, traveling for up to billions of light-years, sensitive probes of decay. However, their sensitivity must be tempered by reality. We derive from them thorough bounds on the neutrino lifetimes accounting for critical astrophysical unknowns and the nuances of neutrino detection. Using the diffuse neutrino flux, we disfavor lifetimes $τ\lesssim 20$-450 s $(m/{\rm eV})$, based on present IceCube data, and forecast factor-of-10 improvements by upcoming detectors. Using, for the first time, neutrinos from the active galaxy NGC 1068, extant unknowns preclude placing lifetime bounds today, but upcoming detectors could disfavor $τ\sim 100$-5000 s $(m/{\rm eV})$.