MicroBooNE collaboration’s research while affiliated with Virginia Tech and other places

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Publications (76)


First study of neutrino angle reconstruction using quasielastic-like interactions in MicroBooNE
  • Preprint
  • File available

April 2025

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10 Reads

MicroBooNE collaboration

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D. Andrade Aldana

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[...]

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C. Zhang

We investigate the expected precision of the reconstructed neutrino direction using a {\nu}{\mu}-argon quasielastic-like event topology with one muon and one proton in the final state and the reconstruction capabilities of the MicroBooNE liquid argon time projection chamber. This direction is of importance in the context of DUNE sub-GeV atmospheric oscillation studies. MicroBooNE allows for a data-driven quantification of this resolution by investigating the deviation of the reconstructed muon-proton system orientation with respect to the well-known direction of neutrinos originating from the Booster Neutrino Beam with an exposure of 1.3 x 1021 protons on target. Using simulation studies, we derive the expected sub-GeV DUNE atmospheric-neutrino reconstructed simulated spectrum by developing a reweighting scheme as a function of the true neutrino energy. We further report flux-integrated single- and double-differential cross section measurements of charged-current {\nu}{\mu} quasielastic-like scattering on argon as a function of the muon-proton system angle using the full MicroBooNE data sets. We also demonstrate the sensitivity of these results to nuclear effects and final state hadronic reinteraction modeling.

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FIG. 1. Event display of a candidate (-)
FIG. 8. Correlation matrix of the unfolded differential cross sections.
FIG. 9. Regularization matrix encoding the regularized truth space of the unfolded differential cross sections.
First measurement of νe\nu_e and νˉe\bar{\nu}_e charged current single charged pion production differential cross sections on argon using the MicroBooNE detector

March 2025

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8 Reads

Understanding electron neutrino interactions is crucial for measurements of neutrino oscillations and searches for new physics in neutrino experiments. We present the first measurement of the flux-averaged νe\nu_e and νˉe\bar{\nu}_e charged current single charged pion production cross section on argon using the MicroBooNE detector and data from the NuMI neutrino beam. The total cross section is measured to be (0.93 ±\pm 0.13 (stat.) ±\pm 0.27 (syst.)) ×1039\times 10^{-39} cm2^2/nucleon at a mean νe\nu_e and νˉe\bar{\nu}_e energy of 730 MeV. Differential cross sections are also reported in electron energy, electron and pion angles, and electron-pion opening angle.


FIG. 1. A νµ +Ar → µ − +K + interaction candidate observed in MicroBooNE data recorded by the collection plane. The color scale represents the intensity of the ionization charge collected on the TPC wires (green: low intensity, red: high intensity). The x and y-axes represent the wire position in the beam direction and the distance in the drift direction, respectively. The gap shown on each track is due to a region in the detector with no active wires.
First Measurement of Charged Current Muon Neutrino-Induced K+K^+ Production on Argon using the MicroBooNE Detector

February 2025

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9 Reads

The MicroBooNE experiment is an 85 tonne active mass liquid argon time projection chamber neutrino detector exposed to the on-axis Booster Neutrino Beam (BNB) at Fermilab. One of MicroBooNE's physics goals is the precise measurement of neutrino interactions on argon in the 1 GeV energy regime. Building on the capabilities of the MicroBooNE detector, this analysis identifies K+K^{+} mesons, a key signature for the study of strange particle production in neutrino interactions. This measurement is furthermore valuable for background estimation for future nucleon decay searches and for improved reconstruction and particle identification capabilities in experiments such as the Deep Underground Neutrino Experiment (DUNE). In this letter, we present the first-ever measurement of a flux-integrated cross section for charged-current muon neutrino induced K+K^{+} production on argon nuclei, determined to be 7.93 ±\pm 3.27 (stat.) ±\pm 2.92 (syst.) × 1042  \times~10^{-42}\; cm2^2/nucleon based on an analysis of 6.88×1020\times10^{20} protons on target.


FIG. 1. An example of the dark sector models being probed. An incoming muon-neutrino from the BNB scatters off an argon target producing a dark neutrino. The subsequent decay of the dark neutrino leads to a visible e + e − pair, mediated via a new dark gauge boson (Z ′ ). A simulated event is also shown behind the e + e − arrows to represent what an e + e − pair would actually look like in our LArTPC detector after forming electromagnetic showers.
First Search for Dark Sector e+ee^+e^- Explanations of the MiniBooNE Anomaly at MicroBooNE

February 2025

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24 Reads

We present MicroBooNE's first search for dark sector e+ee^+e^- explanations of the long-standing MiniBooNE anomaly. The MiniBooNE anomaly has garnered significant attention over the past 20 years including previous MicroBooNE investigations into both anomalous electron and photon excesses, but its origin still remains unclear. In this letter, we provide the first direct test of dark sector models in which dark neutrinos, produced through neutrino-induced scattering, decay into missing energy and visible e+ee^+e^- pairs comprising the MiniBooNE anomaly. Many such models have recently gained traction as a viable solution to the anomaly while evading past bounds. Using an exposure of 6.87×10206.87 \times 10^{20} protons-on-target in the Booster Neutrino Beam, we implement a selection targeting forward-going, coherently produced e+ee^+e^- events. After unblinding, we observe 95 events, which we compare with the constrained background-only prediction of 69.7±17.369.7 \pm 17.3. This analysis sets the world's first direct limits on these dark sector models and, at the 95\% confidence level, excludes the majority of the parameter space viable as a solution to the MiniBooNE anomaly.


Inclusive Search for Anomalous Single-Photon Production in MicroBooNE

February 2025

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4 Reads

We present an inclusive search for anomalous production of single-photon events from neutrino interactions in the MicroBooNE experiment. The search and its signal definition are motivated by the previous observation of a low-energy excess of electromagnetic shower events from the MiniBooNE experiment. We use the Wire-Cell reconstruction framework to select a sample of inclusive single-photon final-state interactions with a final efficiency and purity of 7.0% and 40.2%, respectively. We leverage simultaneous measurements of sidebands of charged current νμ\nu_{\mu} interactions and neutral current interactions producing π0\pi^{0} mesons to constrain signal and background predictions and reduce uncertainties. We perform a blind analysis using a dataset collected from February 2016 to July 2018, corresponding to an exposure of 6.34×10206.34\times10^{20} protons on target from the Booster Neutrino Beam (BNB) at Fermilab. In the full signal region, we observe agreement between the data and the prediction, with a goodness-of-fit p-value of 0.11. We then isolate a sub-sample of these events containing no visible protons, and observe 93±22(stat.)±35(syst.)93\pm22\text{(stat.)}\pm35\text{(syst.)} data events above prediction, corresponding to just above 2σ2\sigma local significance, concentrated at shower energies below 600 MeV.


FIG. 4. Two-dimensional x∆Np and x∆0p scaling exclusion sensitivity with Asimov data, a fake data set that exactly matches the prediction. The hashed region indicates the side of each curve which is being excluded. The Pandora and Wire-Cell Asimov data samples correspond to 6.80 × 10 20 and 6.37 × 10 20 POT, respectively. FIG. 5. Two-dimensional xNp and x0p scaling data exclusions. The hashed region indicates the side of each curve which is being excluded. The Pandora and Wire-Cell data samples correspond to 6.80 × 10 20 and 6.37 × 10 20 POT, respectively.
Enhanced Search for Neutral Current Δ\Delta Radiative Single-Photon Production in MicroBooNE

February 2025

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8 Reads

We report results from an updated search for neutral current (NC) resonant Δ\Delta(1232) baryon production and subsequent Δ\Delta radiative decay (NC ΔNγ\Delta\rightarrow N \gamma). We consider events with and without final state protons; events with a proton can be compared with the kinematics of a Δ(1232)\Delta(1232) baryon decay, while events without a visible proton represent a more generic phase space. In order to maximize sensitivity to each topology, we simultaneously make use of two different reconstruction paradigms, Pandora and Wire-Cell, which have complementary strengths, and select mostly orthogonal sets of events. Considering an overall scaling of the NC ΔNγ\Delta\rightarrow N \gamma rate as an explanation of the MiniBooNE anomaly, our data exclude this hypothesis at 94.4% CL. When we decouple the expected correlations between NC ΔNγ\Delta\rightarrow N \gamma events with and without final state protons, and allow independent scaling of both types of events, our data exclude explanations in which excess events have associated protons, and do not exclude explanations in which excess events have no associated protons.


FIG. 4. The production mechanism of simulated Higgs-portal scalar particles (mS = 150 MeV) for (a) Run 1, in which the NuMI horns are configured to focus positively charged mesons; (b) Run 3, in which the NuMI horns are configured to focus negatively charged mesons.
FIG. 6. The distributions of BDT scores for the four BDTs trained to search for Higgs-portal scalar (HPS) particles with masses of 150 MeV in the Run 3 dataset. The quadrature sum of the uncertainties on the background prediction is shown by the gray band, where red indicates the MC statistical uncertainty, and black indicates systematic uncertainty. The simulated signal is shown at a normalization corresponding to θ = 2.9 × 10 −3 . Overflow events are also included in the right-most bin of each BDT score distribution. (a) The BDT trained to distinguish KDIF topologies in the one-shower sample. (b) The BDT trained to distinguish KDAR topologies in the one-shower sample. (c) The BDT trained to distinguish KDIF topologies in the two-shower sample. (d) The BDT trained to distinguish KDAR topologies in the two-shower sample.
Search for the production of Higgs-portal scalar bosons in the NuMI beam using the MicroBooNE detector

January 2025

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16 Reads

We present the strongest limits to date on the mixing angle, θ\theta, with which a new scalar particle, S, mixes with the Higgs field in the mass range 100 MeV<mS<155MeV<m_S<155 MeV. This result uses the MicroBooNE liquid argon time projection chamber to search for decays of these Higgs-portal scalar particles through the Se+eS\rightarrow e^+e^- channel with the decays of kaons in the NuMI neutrino beam acting as the source of the scalar particles. The analysis uses an exposure of 7.01×10207.01\times 10^{20} protons on target of NuMI beam data including a period when the beam focusing system was configured to focus positively charged hadrons and a separate period when negatively charged hadrons were focused. The analysis searches for scalar particles produced from kaons decaying in flight in the beam's decay volume and at rest in the target and absorber. At mS=125m_S=125 MeV (mS=150m_S=150 MeV) we set a limit of θ<2.65×104\theta<2.65\times 10^{-4} (θ<1.72×104\theta<1.72\times 10^{-4}) at the 95%\% confidence level.


FIG. 1. Distributions of control sample events used in this analysis. The prediction is broken down into CC νe and νµ interactions, NC interactions not producing neutral pions, NC interactions that produce neutral pions, and cosmic rays mistaken for neutrino interactions. Only bins up to 1 GeV from the NC π 0 selection are used in the constraint procedure due to low statistics above this energy.
FIG. 2. Distribution of MC simulation compared with data for reconstructed neutrino energy in the 1eNp0π and 1e0p0π signal channels, along with the LEE Signal Model 1. Statistical tests only take bins between 0.15 GeV and 1.55 GeV into account.
FIG. 4. Distribution of MC simulation compared with data for reconstructed shower cos(θ) in the 1eNp0π and 1e0p0π signal channels, along with the LEE Signal Model 2.
FIG. 5. Confidence intervals obtained from all fits performed in this analysis. Confidence intervals shown are generated with the Feldman-Cousins procedure [36].
Search for an Anomalous Production of Charged-Current νe\nu_e Interactions Without Visible Pions Across Multiple Kinematic Observables

December 2024

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15 Reads

This Letter presents an investigation of low-energy electron-neutrino interactions in the Fermilab Booster Neutrino Beam by the MicroBooNE experiment, motivated by the excess of electron-neutrino-like events observed by the MiniBooNE experiment. This is the first measurement to use data from all five years of operation of the MicroBooNE experiment, corresponding to an exposure of 1.11×10211.11\times 10^{21} protons on target, a 70%70\% increase on past results. Two samples of electron neutrino interactions without visible pions are used, one with visible protons and one without any visible protons. MicroBooNE data is compared to two empirical models that modify the predicted rate of electron-neutrino interactions in different variables in the simulation to match the unfolded MiniBooNE low energy excess. In the first model, this unfolding is performed as a function of electron neutrino energy, while the second model aims to match the observed shower energy and angle distributions of the MiniBooNE excess. This measurement excludes an electron-like interpretation of the MiniBooNE excess based on these models at >99%> 99\% CLs_\mathrm{s} in all kinematic variables.


FIG. 7: Reconstructed muon kinematic and hadronic energy distributions for events passing the ν µ CC selection from [34] before and after the missing energy shift and multivariate event reweighting. The reweighting recovers good agreement in these variables despite the incorrect true-to-reconstructed energy mapping. Note that a proton energy shift has no impact on muon kinematic distributions.
FIG. 8: The (a) MicroBooNE BDT reweighted model and (b) DUNE BDT reweighted model from [45].
FIG. 10: Comparison of the BDT reweighted model prediction and various event generator predictions to MicroBooNE ν µ CC1p data from [48]. The χ 2 /ndf values in the legend are calculated using the reported covariance matrix and each prediction is smeared by the reported A C matrix.
FIG. 11: Model validation tests comparing the NuWro fake data sample to the nominal MC prediction for the reconstructed muon scattering angular distribution for FC&PC events. In (a), the red (blue) lines and bands show the prediction without (with) the constraint from the observed muon energy distribution for FC&PC events. The uncertainties of the prediction only include the cross section and statistical terms and are shown in the bands. The data statistical uncertainties are shown on the data points. In (b), the significance of the tension in each bin after the distribution has been constrained and transformed to the eigenvalue basis of the covariance matrix is shown.
Data-driven model validation for neutrino-nucleus cross section measurements

November 2024

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25 Reads

Neutrino-nucleus cross section measurements are needed to improve interaction modeling to meet the precision needs of neutrino experiments in efforts to measure oscillation parameters and search for physics beyond the Standard Model. We review the difficulties associated with modeling neutrino-nucleus interactions that lead to a dependence on event generators in oscillation analyses and cross section measurements alike. We then describe data-driven model validation techniques intended to address this model dependence. The method relies on utilizing various goodness-of-fit tests and the correlations between different observables and channels to probe the model for defects in the phase space relevant for the desired analysis. These techniques shed light on relevant mis-modeling, allowing it to be detected before it begins to bias the cross section results. We compare more commonly used model validation methods which directly validate the model against alternative ones to these data-driven techniques and show their efficacy with fake data studies. These studies demonstrate that employing data-driven model validation in cross section measurements represents a reliable strategy to produce robust results that will stimulate the desired improvements to interaction modeling.


Demonstration of new MeV-scale capabilities in large neutrino LArTPCs using ambient radiogenic and cosmogenic activity in MicroBooNE

October 2024

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22 Reads

Large neutrino liquid argon time projection chamber (LArTPC) experiments can broaden their physics reach by reconstructing and interpreting MeV-scale energy depositions, or blips, present in their data. We demonstrate new calorimetric and particle discrimination capabilities at the MeV energy scale using reconstructed blips in data from the MicroBooNE LArTPC at Fermilab. We observe a concentration of low energy (<<3 MeV) blips around fiberglass mechanical support struts along the TPC edges with energy spectrum features consistent with the Compton edge of 2.614 MeV 208^{208}Tl decay γ\gamma rays. These features are used to verify proper calibration of electron energy scales in MicroBooNE's data to few percent precision and to measure the specific activity of 208^{208}Tl in the fiberglass composing these struts, (11.7±0.2 (stat)±2.8 (syst))(11.7 \pm 0.2 ~\text{(stat)} \pm 2.8~\text{(syst)}) Bq/kg. Cosmogenically-produced blips above 3 MeV in reconstructed energy are used to showcase the ability of large LArTPCs to distinguish between low-energy proton and electron energy depositions. An enriched sample of low-energy protons selected using this new particle discrimination technique is found to be smaller in data than in dedicated CORSIKA cosmic ray simulations, suggesting either incorrect CORSIKA modeling of incident cosmic fluxes or particle transport modeling issues in Geant4.


Citations (20)


... CHARM. Experiments with lower energy scales, either fixed-target or beam dump type, benefit from high-intensity beam lines [82][83][84][85][86][87]. However, constraints from such experiments rely on detailed knowledge of the beam's interaction with the material, especially various nuclei, making predictions more challenging. ...

Reference:

Phenomenology of electroweak portal dark showers: high energy direct probes and low energy complementarity
Design and Construction of the MicroBooNE Detector

... (i) Another SBL accelerator experiment, MicroBooNE did not observe any ν e -like event excess [41][42][43][44][45][46]. It was claimed [19] that MicroBooNE did not explore the entire sterile parameter space favored by MiniBooNE. ...

First constraints on light sterile neutrino oscillations from combined appearance and disappearance searches with the MicroBooNE detector

... In MicroBooNE, a CNN for assigning probabilities of particle identities for single particles in the MicroBooNE LArTPC has been demonstrated on simulated data in Ref. [1]. A semantic segmentation network for LArTPC data [19] has been used for π 0 event reconstruction [20], vertex finding, and track reconstruction [21]. The DUNE experiment has recently presented an updated long-baseline neutrino oscillation sensitivity study incorporating a CNN for neutrino event selection and background rejection [22]. ...

Deep neural network for pixel-level electromagnetic particle identification in the MicroBooNE liquid argon time projection chamber
  • Citing Article
  • January 2019

... For the smaller scalar mass region (m ϕ ≲ 5 GeV), severe constraints have been taken on the scalar mixing α from searches for rare meson decays into final states with ϕ [48][49][50][51][52][53][54][55][56][57][58][59][60]. See ref. [61] for the review of such constraints. ...

Search for long-lived heavy neutral leptons and Higgs portal scalars decaying in the MicroBooNE detector

... (i) Another SBL accelerator experiment, MicroBooNE did not observe any ν e -like event excess [41][42][43][44][45][46]. It was claimed [19] that MicroBooNE did not explore the entire sterile parameter space favored by MiniBooNE. ...

Search for an Excess of Electron Neutrino Interactions in MicroBooNE Using Multiple Final State Topologies

... (i) Another SBL accelerator experiment, MicroBooNE did not observe any ν e -like event excess [41][42][43][44][45][46]. It was claimed [19] that MicroBooNE did not explore the entire sterile parameter space favored by MiniBooNE. ...

Search for an anomalous excess of charged-current quasi-elastic νe\nu_e interactions with the MicroBooNE experiment using Deep-Learning-based reconstruction

... (i) Another SBL accelerator experiment, MicroBooNE did not observe any ν e -like event excess [41][42][43][44][45][46]. It was claimed [19] that MicroBooNE did not explore the entire sterile parameter space favored by MiniBooNE. ...

Search for an anomalous excess of charged-current νe\nu_e interactions without pions in the final state with the MicroBooNE experiment

... (i) Another SBL accelerator experiment, MicroBooNE did not observe any ν e -like event excess [41][42][43][44][45][46]. It was claimed [19] that MicroBooNE did not explore the entire sterile parameter space favored by MiniBooNE. ...

Search for an anomalous excess of inclusive charged-current νe\nu_e interactions in the MicroBooNE experiment using Wire-Cell reconstruction

... (i) Another SBL accelerator experiment, MicroBooNE did not observe any ν e -like event excess [41][42][43][44][45][46]. It was claimed [19] that MicroBooNE did not explore the entire sterile parameter space favored by MiniBooNE. ...

Search for Neutrino-Induced Neutral Current Δ\Delta Radiative Decay in MicroBooNE and a First Test of the MiniBooNE Low Energy Excess Under a Single-Photon Hypothesis

... For the smaller scalar mass region (m ϕ ≲ 5 GeV), severe constraints have been taken on the scalar mixing α from searches for rare meson decays into final states with ϕ [48][49][50][51][52][53][54][55][56][57][58][59][60]. See ref. [61] for the review of such constraints. ...

Search for a Higgs portal scalar decaying to electron-positron pairs in the MicroBooNE detector