M. A. Acero’s research while affiliated with University of Atlántico and other places

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Publications (58)


Dual-Baseline Search for Active-to-Sterile Neutrino Oscillations in NOvA
  • Article
  • Full-text available

February 2025

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13 Reads

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1 Citation

Physical Review Letters

M. A. Acero

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B. Acharya

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P. Adamson

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[...]

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R. Zwaska

We report a search for neutrino oscillations to sterile neutrinos under a model with three active and one sterile neutrinos ( 3 + 1 model). This analysis uses the NOvA detectors exposed to the NuMI beam, running in neutrino mode. The data exposure, 13.6 × 10 20 protons on target, doubles that previously analyzed by NOvA, and the analysis is the first to use ν μ charged-current interactions in conjunction with neutral-current interactions. Neutrino samples in the near and far detectors are fitted simultaneously, enabling the search to be carried out over a Δ m 41 2 range extending 2 (3) orders of magnitude above (below) 1 eV 2 . NOvA finds no evidence for active-to-sterile neutrino oscillations under the 3 + 1 model at 90% confidence level. New limits are reported in multiple regions of parameter space, excluding some regions currently allowed by IceCube at 90% confidence level. We additionally set the most stringent limits for anomalous ν τ appearance for Δ m 41 2 ≤ 3 eV 2 . Published by the American Physical Society 2025

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The track-length extension fitting algorithm for energy measurement of interacting particles in liquid argon TPCs and its performance with ProtoDUNE-SP data

February 2025

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26 Reads

Journal of Instrumentation

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R. Acciarri

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[...]

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R. Zwaska

This paper introduces a novel track-length extension fitting algorithm for measuring the kinetic energies of inelastically interacting particles in liquid argon time projection chambers (LArTPCs). The algorithm finds the most probable offset in track length for a track-like object by comparing the measured ionization density as a function of position with a theoretical prediction of the energy loss as a function of the energy, including models of electron recombination and detector response. The algorithm can be used to measure the energies of particles that interact before they stop, such as charged pions that are absorbed by argon nuclei. The algorithm's energy measurement resolutions and fractional biases are presented as functions of particle kinetic energy and number of track hits using samples of stopping secondary charged pions in data collected by the ProtoDUNE-SP detector, and also in a detailed simulation. Additional studies describe the impact of the dE/dx model on energy measurement performance. The method described in this paper to characterize the energy measurement performance can be repeated in any LArTPC experiment using stopping secondary charged pions.


Fig. 9: A 3 GeV ν e CC resonant pion production interaction with an electron, charged pion, neutral pion (decays to two photons) and proton in the final state. Hits from the W view in black, reconstructed vertex in red.
Fig. 15: 2.8 GeV NC interaction with a π 0 → γγ and either (left) a neutron or (right) proton in the final state. The true interaction vertex is indicated by the blue circle, while the reconstructed interaction vertex is indicated by the red circle.
Fig. 18: 24.9 GeV CC interaction with a µ, a π + and either (left) a neutron or (right) proton in the final state. The true interaction vertex is indicated by the blue circle, while the reconstructed interaction vertex is indicated by the red circle.
Neutrino Interaction Vertex Reconstruction in DUNE with Pandora Deep Learning

February 2025

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34 Reads

The Pandora Software Development Kit and algorithm libraries perform reconstruction of neutrino interactions in liquid argon time projection chamber detectors. Pandora is the primary event reconstruction software used at the Deep Underground Neutrino Experiment, which will operate four large-scale liquid argon time projection chambers at the far detector site in South Dakota, producing high-resolution images of charged particles emerging from neutrino interactions. While these high-resolution images provide excellent opportunities for physics, the complex topologies require sophisticated pattern recognition capabilities to interpret signals from the detectors as physically meaningful objects that form the inputs to physics analyses. A critical component is the identification of the neutrino interaction vertex. Subsequent reconstruction algorithms use this location to identify the individual primary particles and ensure they each result in a separate reconstructed particle. A new vertex-finding procedure described in this article integrates a U-ResNet neural network performing hit-level classification into the multi-algorithm approach used by Pandora to identify the neutrino interaction vertex. The machine learning solution is seamlessly integrated into a chain of pattern-recognition algorithms. The technique substantially outperforms the previous BDT-based solution, with a more than 20\% increase in the efficiency of sub-1\,cm vertex reconstruction across all neutrino flavours.


Monte Carlo method for constructing confidence intervals with unconstrained and constrained nuisance parameters in the NOvA experiment

February 2025

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23 Reads

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1 Citation

Journal of Instrumentation

Measuring observables to constrain models using maximum-likelihood estimation is fundamental to many physics experiments. Wilks' theorem provides a simple way to construct confidence intervals on model parameters, but it only applies under certain conditions. These conditions, such as nested hypotheses and unbounded parameters, are often violated in neutrino oscillation measurements and other experimental scenarios. Monte Carlo methods can address these issues, albeit at increased computational cost. In the presence of nuisance parameters, however, the best way to implement a Monte Carlo method is ambiguous. This paper documents the method selected by the NOvA experiment, the profile construction. It presents the toy studies that informed the choice of method, details of its implementation, and tests performed to validate it. It also includes some practical considerations which may be of use to others choosing to use the profile construction.


DUNE Phase II: scientific opportunities, detector concepts, technological solutions

December 2024

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86 Reads

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6 Citations

Journal of Instrumentation

The international collaboration designing and constructing the Deep Underground Neutrino Experiment (DUNE) at the Long-Baseline Neutrino Facility (LBNF) has developed a two-phase strategy toward the implementation of this leading-edge, large-scale science project. The 2023 report of the US Particle Physics Project Prioritization Panel (P5) reaffirmed this vision and strongly endorsed DUNE Phase I and Phase II, as did the European Strategy for Particle Physics. While the construction of the DUNE Phase I is well underway, this White Paper focuses on DUNE Phase II planning. DUNE Phase-II consists of a third and fourth far detector (FD) module, an upgraded near detector complex, and an enhanced 2.1 MW beam. The fourth FD module is conceived as a “Module of Opportunity”, aimed at expanding the physics opportunities, in addition to supporting the core DUNE science program, with more advanced technologies. This document highlights the increased science opportunities offered by the DUNE Phase II near and far detectors, including long-baseline neutrino oscillation physics, neutrino astrophysics, and physics beyond the standard model. It describes the DUNE Phase II near and far detector technologies and detector design concepts that are currently under consideration. A summary of key R&D goals and prototyping phases needed to realize the Phase II detector technical designs is also provided. DUNE's Phase II detectors, along with the increased beam power, will complete the full scope of DUNE, enabling a multi-decadal program of groundbreaking science with neutrinos.


FIG. 1. GEANT4 predicted total inelastic cross section and elastic cross section of positively charged kaons on argon as a function of kinetic energy [15-17]. Predictions made using interfaces in Ref. [18].
FIG. 14. Difference in the endpoint along the detector length (Z) between the truth-level information and the calibrated reconstructed information for the 6 GeV=c simulation sample. The mean offset measured in the 6 GeV=c simulation sample is 0.539 cm with a standard deviation of 1.231 cm using a Gaussian fit.
First measurement of the total inelastic cross section of positively charged kaons on argon at energies between 5.0 and 7.5 GeV

November 2024

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69 Reads

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2 Citations

Physical Review D

ProtoDUNE Single-Phase (ProtoDUNE-SP) is a 770-ton liquid argon time projection chamber that operated in a hadron test beam at the CERN Neutrino Platform in 2018. We present a measurement of the total inelastic cross section of charged kaons on argon as a function of kaon energy using 6 and 7 GeV / c beam momentum settings. The flux-weighted average of the extracted inelastic cross section at each beam momentum setting was measured to be 380 ± 26 mbarns for the 6 GeV / c setting and 379 ± 35 mbarns for the 7 GeV / c setting. Published by the American Physical Society 2024


Search for C P -Violating Neutrino Nonstandard Interactions with the NOvA Experiment

November 2024

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47 Reads

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4 Citations

Physical Review Letters

This Letter reports a search for charge-parity ( C P ) symmetry violating nonstandard interactions (NSI) of neutrinos with matter using the NOvA Experiment, and examines their effects on the determination of the standard oscillation parameters. Data from ν μ ( ν ¯ μ ) → ν μ ( ν ¯ μ ) and ν μ ( ν ¯ μ ) → ν e ( ν ¯ e ) oscillation channels are used to measure the effect of the NSI parameters ϵ e μ and ϵ e τ . With 90% CL the magnitudes of the NSI couplings are constrained to be | ϵ e μ | ≲ 0.3 and | ϵ e τ | ≲ 0.4 . A degeneracy at | ϵ e τ | ≈ 1.8 is reported, and we observe that the presence of NSI limits sensitivity to the standard C P phase δ C P . Published by the American Physical Society 2024


White paper on light sterile neutrino searches and related phenomenology

October 2024

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61 Reads

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34 Citations


Figure 1. Event yield per number of tracks divided by neutrino interaction types in the muon-neutrino CC sample.
Figure 5. Efficiency distributions for each cos θµ slice. The values decrease as the muon kinetic energy increases. Conversely, the efficiency increases as more forward-going muons are selected. This pattern results from the containment requirement.
Measurement of the double-differential cross section of muon-neutrino charged-current interactions with low hadronic energy in the NOvA Near Detector

October 2024

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37 Reads

The NOvA collaboration reports cross-section measurements for νμ\nu_{\mu} charged-current interactions with low hadronic energy (maximum kinetic energy of 250 MeV for protons and 175 MeV for pions) in the NOvA Near Detector. The results are presented as a double-differential cross section as a function of the direct observables of the final-state muon kinematics. Results are also presented as a single-differential cross section as a function of the derived square of the four-momentum transfer, Q2Q^{2}, and as a function of the derived neutrino energy. The data correspond to an accumulated 8.09×1020\times10^{20} protons-on-target (POT) in the neutrino mode of the NuMI beam, with a narrow band of neutrino energies peaked at 1.8 GeV. The analysis provides a sample of neutrino-nucleus interactions with an enhanced fraction of quasi-elastic and two-particle-two-hole (2p2h) interactions. This enhancement allows quantitative comparisons with various nuclear models. We find strong disagreement between data and theory-based models in various regions of the muon kinematic phase space, especially in the forward muon direction.


Measurement of d2sigma/d|q|dEavail in charged current neutrino-nucleus interactions at = 1.86 GeV using the NOvA Near Detector

October 2024

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49 Reads

Double- and single-differential cross sections for inclusive charged-current neutrino-nucleus scattering are reported for the kinematic domain 0 to 2 GeV/c in three-momentum transfer and 0 to 2 GeV in available energy, at a mean muon-neutrino energy of 1.86 GeV. The measurements are based on an estimated 995,760 muon-neutrino CC interactions in the scintillator medium of the NOvA Near Detector. The subdomain populated by 2-particle-2-hole reactions is identified by the cross-section excess relative to predictions for neutrino-nucleus scattering that are constrained by a data control sample. Models for 2-particle-2- hole processes are rated by chi-square comparisons of the predicted-versus-measured muon-neutrino CC inclusive cross section over the full phase space and in the restricted subdomain. Shortfalls are observed in neutrino generator predictions obtained using the theory-based Val`encia and SuSAv2 2p2h models.


Citations (37)


... In the Standard Model, there are in general two types of axial-vector FFs of a hadron in the weak sector: the weak-charged ones via the weak-charged current interactions mediated by the W ± bosons, and the weakneutral ones via the weak-neutral current interactions mediated by the Z 0 bosons. These axial-vector FFs also serve as important quantities for constraining the systematic uncertainties of high-precision measurements in (anti)neutrino oscillation experiments [23][24][25][26][27][28][29][30][31]. On the theory side, tremendous progress has been reported in the last few years from the first-principle lattice QCD side ; theoretical evaluations of the nucleon axial-vector FFs and their contributions to the associated cross sections based on chiral perturbation theory and various models/approaches are still rapidly developing . ...

Reference:

Nucleon relativistic weak-neutral axial-vector four-current distributions
Dual-Baseline Search for Active-to-Sterile Neutrino Oscillations in NOvA

Physical Review Letters

M. A. Acero

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B. Acharya

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P. Adamson

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[...]

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R. Zwaska

... The 2D contours in the (γ 2 , E b ) space are obtained following the profiled Feldman-Cousins approach [22], treating ϕ and γ 1 as nuisance parameters. The 1D intervals on γ 2 and E b are computed with a similar procedure, treating also E b or Each row corresponds to one specific fit. ...

Monte Carlo method for constructing confidence intervals with unconstrained and constrained nuisance parameters in the NOvA experiment
  • Citing Article
  • February 2025

Journal of Instrumentation

... Phase I will be composed of two 17 kton far detectors (FD) liquid argon time projection chambers (LArTPCs), a near detector (ND) with a LArTPC module (ND-LAr), a muon spectrometer (TMS), with the addition of an on-axis solenoid magnet plus electromagnetic calorimeter (SAND), and a beam line capable of providing (anti-)neutrinos with a 1.2 MW power. Phase II aims at expanding DUNE capabilities by limiting systematics with a more capable ND and greatly increasing statistics with the construction of another two FDs in addition to boosting beam power to 2.1 MW [2]. ...

DUNE Phase II: scientific opportunities, detector concepts, technological solutions
  • Citing Article
  • December 2024

Journal of Instrumentation

... To advance this analysis in future LArTPC measurements, it is necessary to increase statistics, reduce large detector systematics (especially those related to the recombination of electrons with argon nuclei), refine reconstruction algorithms for short tracks, and improve the identification of kaon tracks that undergo reinteractions. Furthermore, the uncertainty related to kaon reinteractions on argon nuclei could be refined by using data from LArIAT [46], and the DUNE prototypes at CERN [48]. More statistics will come from analyzing MicroBooNE's full dataset with a total of 1.2 ×10 21 POT. ...

First measurement of the total inelastic cross section of positively charged kaons on argon at energies between 5.0 and 7.5 GeV

Physical Review D

... Figure 14 presents a summary of the reported allowed regions at 90% CL of the NSI couplings, where the off-diagonal elements have been assumed real-valued with δ αβ = 0 or π for comparison. The results of IC-DeepCore 2021 [46], MINOS 2013 [47] and NOvA 2024 [48] were re-scaled to match the NSI down-quark coupling convention used in this study (see eq. (1.3)). ...

Search for C P -Violating Neutrino Nonstandard Interactions with the NOvA Experiment

Physical Review Letters

... Then, we need to implement non-unitarity into the (3 + 1) model. We note that the problem of sterile neutrinos [54] or non-unitarity [53] is widely discussed in the community as possible candidates for physics beyond the νSM. But, in our setting we need the both, "sterile neutrino and non-unitarity". ...

White paper on light sterile neutrino searches and related phenomenology

... The commissioning of individual 2x2 modules took place between 2021 and 2023 at the University of Bern. In total O(100e6) cosmic-ray events were collected, allowing for first characterisation and performance demonstrations of the novel technologies [14]. During these operations, the charge readout observed a stable data rate with a 20:1 signal-to-noise ratio and was continuously active in self-triggering mode with a threshold as low as 200 keV. ...

Performance of a Modular Ton-Scale Pixel-Readout Liquid Argon Time Projection Chamber

Instruments

... Our main motivation in this work is to assess the effectiveness of reactions of the type 2 in Ar/CF 4 admixtures, through a direct measurement of the scintillation yields and time profiles. We target specifically future neutrino experiments performed with pressurized argon TPCs (as presently intended by the DUNE collaboration [31,33], or under consideration for the upgrade of COHERENT [34]), for which we explored a range of CF 4 concentrations from 0.1% up to 10% (per volume), at a pressure around 10 bar. According to simulations performed in [35], an optical response in the range of 1000 ph/MeV with time constants of few 10's of ns would enable time tagging (T 0 ) with ns-level accuracy, in future neutrino detectors such as the high pressure TPC of DUNE's ND-GAr. ...

DUNE Phase II: Scientific Opportunities, Detector Concepts, Technological Solutions

... The scintillation light collecting system will have bar-shaped X-Arapucas placed in between the APAs [3]. The other module will have its anodes composed of perforated PCB layers with conductive strips that will be disposed vertically in the cryostat so that the electron field will be applied vertically, this being called the Vertical Drift (VD) module [4]. Its Photon Detection System (PDS) will have rectangular X-Arapucas positioned along the cryostat walls (outside the active volume) and also on the cathode, in a high voltage environment. ...

The DUNE Far Detector Vertical Drift Technology. Technical Design Report

Journal of Instrumentation

... Outside such region increases as the FC shorter sides are also instrumented with PD units. The fraction of light emitted at 176 nm due to Xe doping was 53% while the remaining LAr scintillation light was assumed to be reduced by an extra factor of 30% [4,11]. Although the total number of photons produced is lower when Xe is present at minimal levels in the volume, the 176 nm light propagation characteristics allows light to reach PD units farther from the light source events resulting in higher expected values and a more uniform map than with pure LAr. ...

Doping liquid argon with xenon in ProtoDUNE Single-Phase: effects on scintillation light

Journal of Instrumentation