R. Zwaska’s research while affiliated with Fermi National Accelerator Laboratory (Fermilab) and other places

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Publications (194)


Figure 3: The LBNF infrastructure at FNAL.
Figure 4: The LBNF Neutrino Target Station.
Figure 5: The pre-assembly of a section of the second cryostat for the DUNE far detector at the factory in Arteixo, Spain. Credit: CERN.
Figure 6: A notional, technically limited schedule for DUNE Phase II FD modules 3 (FD3) and 4 (FD4) assuming they are vertical drift LAr TPCs similar to DUNE Phase I FD2. The installation of the FD3 and FD4 cryostats from CERN is expected in 2029 and 2030 respectively.
European Contributions to Fermilab Accelerator Upgrades and Facilities for the DUNE Experiment
  • Preprint
  • File available

March 2025

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9 Reads

DUNE Collaboration

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R. Acciarri

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[...]

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R. Zwaska

The Proton Improvement Plan (PIP-II) to the FNAL accelerator chain and the Long-Baseline Neutrino Facility (LBNF) will provide the world's most intense neutrino beam to the Deep Underground Neutrino Experiment (DUNE) enabling a wide-ranging physics program. This document outlines the significant contributions made by European national laboratories and institutes towards realizing the first phase of the project with a 1.2 MW neutrino beam. Construction of this first phase is well underway. For DUNE Phase II, this will be closely followed by an upgrade of the beam power to > 2 MW, for which the European groups again have a key role and which will require the continued support of the European community for machine aspects of neutrino physics. Beyond the neutrino beam aspects, LBNF is also responsible for providing unique infrastructure to install and operate the DUNE neutrino detectors at FNAL and at the Sanford Underground Research Facility (SURF). The cryostats for the first two Liquid Argon Time Projection Chamber detector modules at SURF, a contribution of CERN to LBNF, are central to the success of the ongoing execution of DUNE Phase I. Likewise, successful and timely procurement of cryostats for two additional detector modules at SURF will be critical to the success of DUNE Phase II and the overall physics program. The DUNE Collaboration is submitting four main contributions to the 2026 Update of the European Strategy for Particle Physics process. This paper is being submitted to the 'Accelerator technologies' and 'Projects and Large Experiments' streams. Additional inputs related to the DUNE science program, DUNE detector technologies and R&D, and DUNE software and computing, are also being submitted to other streams.

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Figure 1: The fraction of CPU resources utilized in each nation for DUNE production processing campaigns for during 2024. These campaigns include reconstruction and simulation for DUNE Far Detectors and ProtoDUNE. The largest single national contribution came from the US, but the total European contribution was greater than 57% of CPU processing.
Figure 2: The DUNE estimates for disk storage needs through 2030 based upon the projections of data volumes from the ProtoDUNE Horizontal Drift (PDHD), ProtoDUNE Vertical Drift (PDVD), Far Detector Horizontal Drift (FDHD), Far Detector Vertical Drift (FDVD), Near Detector SAND (ND-SAND), and Near Detector Liquid Argon and Muon Spectrometer (NDLAr+TMS).
Figure 4: The DUNE estimates for CPU needs through 2030 based upon the projections of data volumes from the ProtoDUNE Horizontal Drift (PDHD), ProtoDUNE Vertical Drift (PDVD), Far Detector Horizontal Drift (FDHD), Far Detector Vertical Drift (FDVD), Near Detector SAND (ND-SAND), and Near Detector Liquid Argon and Muon Spectrometer (NDLAr+TMS).
DUNE Software and Computing Research and Development

March 2025

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4 Reads

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 ambitious physics program of Phase I and Phase II of DUNE is dependent upon deployment and utilization of significant computing resources, and successful research and development of software (both infrastructure and algorithmic) in order to achieve these scientific goals. This submission discusses the computing resources projections, infrastructure support, and software development needed for DUNE during the coming decades as an input to the European Strategy for Particle Physics Update for 2026. The DUNE collaboration is submitting four main contributions to the 2026 Update of the European Strategy for Particle Physics process. This submission to the 'Computing' stream focuses on DUNE software and computing. Additional inputs related to the DUNE science program, DUNE detector technologies and R&D, and European contributions to Fermilab accelerator upgrades and facilities for the DUNE experiment, are also being submitted to other streams.


The DUNE Science Program

March 2025

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12 Reads

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 for 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 previous European Strategy for Particle Physics. The construction of DUNE Phase I is well underway. DUNE Phase II consists of a third and fourth far detector module, an upgraded near detector complex, and an enhanced > 2 MW beam. The fourth FD module is conceived as a 'Module of Opportunity', aimed at supporting the core DUNE science program while also expanding the physics opportunities with more advanced technologies. The DUNE collaboration is submitting four main contributions to the 2026 Update of the European Strategy for Particle Physics process. This submission to the 'Neutrinos and cosmic messengers', 'BSM physics' and 'Dark matter and dark sector' streams focuses on the physics program of DUNE. Additional inputs related to DUNE detector technologies and R&D, DUNE software and computing, and European contributions to Fermilab accelerator upgrades and facilities for the DUNE experiment, are also being submitted to other streams.


The DUNE Phase II Detectors

March 2025

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15 Reads

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 for 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 previous European Strategy for Particle Physics. The construction of DUNE Phase I is well underway. DUNE Phase II consists of a third and fourth far detector module, an upgraded near detector complex, and an enhanced > 2 MW beam. The fourth FD module is conceived as a 'Module of Opportunity', aimed at supporting the core DUNE science program while also expanding the physics opportunities with more advanced technologies. The DUNE collaboration is submitting four main contributions to the 2026 Update of the European Strategy for Particle Physics process. This submission to the 'Detector instrumentation' stream focuses on technologies and R&D for the DUNE Phase II detectors. Additional inputs related to the DUNE science program, DUNE software and computing, and European contributions to Fermilab accelerator upgrades and facilities for the DUNE experiment, are also being submitted to other streams.



FIG. 1. Flux of ν μ neutrinos at the NOvA Near Detector (solid histogram) shown with the total 1-σ uncertainty (shaded band) [46].
FIG. 14. The estimated 2p2h cross section of Fig. 13 displayed in bins of E avail for six contiguous slices of j⃗ qj.
Measurement of d 2 σ / d | q → | d E avail in charged current ν μ -nucleus interactions at ⟨ E ν ⟩ = 1.86 GeV using the NOvA Near Detector

March 2025

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19 Reads

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1 Citation

Physical Review D

Double- and single-differential cross sections for inclusive charged-current ν μ -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 ν μ energy of 1.86 GeV. The measurements are based on an estimated 995,760 ν μ charged-current (CC) interactions in the scintillator medium of the NOvA Near Detector. The subdomain populated by 2-particle-2-hole (2p2h) reactions is identified by the cross section excess relative to predictions for ν μ -nucleus scattering that are constrained by a data control sample. Models for 2-particle-2-hole processes are rated by χ 2 comparisons of the predicted-versus-measured ν μ 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 València and SuSAv2 2p2h models. Published by the American Physical Society 2025


Dual-Baseline Search for Active-to-Sterile Neutrino Oscillations in NOvA

February 2025

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20 Reads

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2 Citations

Physical Review Letters

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


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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39 Reads

Journal of Instrumentation

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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50 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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29 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.


Citations (59)


... Neutrino interaction models consistently show discrepancies when compared to NOvA data [43][44][45][46], mirroring challenges seen in other experiments. Historically, the experiment has relied on GENIE as the default event generator [47], tuned through targeted modifications informed by theoretical advancements, external data constraints, and ND observations, in order to refine the modeling of the different neutrino-nucleus reaction mechanisms. ...

Reference:

Neutrino Scattering: Connections Across Theory and Experiment
Measurement of d 2 σ / d | q → | d E avail in charged current ν μ -nucleus interactions at ⟨ E ν ⟩ = 1.86 GeV using the NOvA Near Detector

Physical Review D

... 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 . ...

Dual-Baseline Search for Active-to-Sterile Neutrino Oscillations in NOvA

Physical Review Letters

... 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

... The first two modules, currently under construction, will employ single-phase horizontal and vertical drift designs. For Phase 2, one additional vertical drift module is proposed together with a fourth module, which is referred to as a module of opportunity, and may be different [3]. ...

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

... 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

... Finally, 1D unfolding was used directly on the net-charge distribution, applying the same 0-1% centrality selection for both the measured and Monte Carlo data. The effectiveness of this method was verified by comparing 1D and 2D unfolding results on a smaller system (p+p reactions), confirming that the difference between the two approaches was negligible [23]. ...

Measurements of higher-order cumulants of multiplicity and net-electric charge distributions in inelastic proton–proton interactions by NA61/SHINE

The European Physical Journal C

... 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 far detector module 1 (FD1) is a horizontal drift time projection chamber (TPC), as developed and operated in ProtoDUNE at CERN [5]. The far detector module 2 (FD2) is a vertical drift TPC [6]. For the cryogenic infrastructure in support of the two LArTPC modules, Phase I will include two large cryostats (one per FD module), 35 kt of LAr, and three nitrogen refrigeration units. ...

The DUNE Far Detector Vertical Drift Technology. Technical Design Report

Journal of Instrumentation