S. Biedron’s research while affiliated with University of New Mexico and other places

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Publications (9)


FIG. 2. Parameter space for the two-mediator models, consisting of one long-lived boson produced through charged pion threebody decays into a 20 MeV scalar ϕ coupling to muons and scattering via a vector mediator V as in Eq. (1). The exclusions (CCM120, KARMEN, LSND, and MicroBooNE) and projections for future CCM200 (in nominal background and background-free scenarios) and future MicroBooNE sensitivity are shown at 95% CL, while the MiniBooNE fits are shown at 68% and 95% CL in dark and light blue, respectively.
FIG. 4. Parameter space for the single mediator scenario where a massive vector V couples to the pion doublet via charged pion coupling g π AE and neutral pion coupling g π 0 as in Eq. (4). The production channels via these couplings are therefore neutral pion decay π 0 → γV and IB2 decay π AE → lνV, while the detection takes place via π 0 -mediated VN → γN scattering. The exclusions (CCM120, KARMEN, LSND, and MicroBooNE) and projections (CCM200 and MicroBooNE) are shown at 95% CL, while the MiniBooNE fits are shown at 68% and 95% CL in dark and light blue, respectively.
FIG. 5. Same as Fig. 4 but for m V ¼ 10 MeV (left) and m V ¼ 20 MeV (right).
Addendum to “Testing meson portal dark sector solutions to the MiniBooNE anomaly at CCM”
  • Article
  • Full-text available

February 2025

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10 Reads

Physical Review D

A. A. Aguilar-Arevalo

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S. Biedron

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J. Boissevain

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[...]

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In Aguilar-Arevalo [], we explored various effective field theories that could explain the MiniBooNE excess involving long-lived particles produced from charged meson decays and the sensitivity of the Coherent CAPTAIN Mills experiment to these models. In this addendum, we extend the analysis to project sensitivity of upcoming MicroBooNE data to the long-lived particle models considered in the previous work. We find that a dedicated MicroBooNE analysis of the single photon final state with longer exposure and improved signal efficiency will be sensitive to these new physics explanations of the MiniBooNE excess, and could rule them out with a null observation at the 95% confidence level. Published by the American Physical Society 2025

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FIG. 3. Cross sections for the photoconversion of a massive vector (scalar) mediated by a massive scalar (vector) through the dimension-5 vertex. We fix the mass of the incoming boson to 1 MeV in each case. The cross sections in the case of the photoconversion of a massive pseudoscalar are similar, varying only up to a constant factor.
Testing meson portal dark sector solutions to the MiniBooNE anomaly at the Coherent CAPTAIN Mills experiment

May 2024

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27 Reads

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3 Citations

Physical Review D

A solution to the MiniBooNE excess invoking rare three-body decays of the charged pions and kaons to new states in the MeV mass scale was recently proposed as a dark-sector explanation. This class of solution illuminates the fact that, while the charged pions were focused in the target-mode run, their decay products were isotropically suppressed in the beam-dump-mode run in which no excess was observed. This suggests a new physics solution correlated to the mesonic sector. We investigate an extended set of phenomenological models that can explain the MiniBooNE excess as a dark sector solution, utilizing long-lived particles that might be produced in the three-body decays of the charged mesons and the two-body anomalous decays of the neutral mesons. Over a broad set of interactions with the long-lived particles, we show that these scenarios can be compatible with constraints from LSND, KARMEN, and MicroBooNE, and evaluate the sensitivity of the ongoing and future data taken by the Coherent CAPTAIN Mills experiment to a potential discovery in this parameter space. Published by the American Physical Society 2024


FIG. 6. The CCM120 high energy subtraction spectrum used for the search search. Only events between 22.4 and 200 MeV reconstructed energy were included in this spectrum. Also shown are example spectra from the Dark Sector for the 5 models tested with CCM120, using points on the 68% confidence level.
FIG. 7. Parameter space for the two-mediator models, consisting of one long-lived boson produced through charged pion three-body decays and scattering via a secondary heavy mediator are shown. Left: a 20 MeV scalar ϕ coupling to muons and scattering via a vector mediator V as in Eq. 14. Center: a 0.5 MeV pseudoscalar a coupling to electrons and scattering via a vector mediator V as in Eq. 15. Right: a 20 MeV vector V coupling through the IB3 pion contact interaction and scattering via a massive scalar ϕ as in Eq. 16. The exclusions (CCM120, KARMEN, LSND, and MicroBooNE) and projections for CCM200 are shown at 95% C.L., while the MiniBooNE fits are shown at 68% and 95% C.L. in dark and light blue, respectively.
FIG. 8. Parameter space for the single mediator scenario where a massive vector V couples to the pion doublet via charged pion coupling g π ± and neutral pion coupling g π 0 as in Eq. 17. We vary the vector mass mV from left to right as 5 MeV (top), 10 MeV (lower left), and 20 MeV (lower right).The exclusions (CCM120, KARMEN, LSND, and MicroBooNE) and projections for CCM200 are shown at 95% C.L., while the MiniBooNE fits are shown at 68% and 95% C.L. in dark and light blue, respectively.
FIG. 12. The pre-horn π + flux (black) using the Sanford-Wang parameterized cross section convolved with the BNB proton beamspot, and the post-horn flux (blue) after modeling the transport through the magnetic horn system are both shown as a function of the pion angle with respect to the beam axis. In both cases 5 · 10 5 simulated POT were used.
Testing Meson Portal Dark Sector Solutions to the MiniBooNE Anomaly at CCM

September 2023

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39 Reads

A solution to the MiniBooNE excess invoking rare three-body decays of the charged pions and kaons to new states in the MeV mass scale was recently proposed as a dark-sector explanation. This class of solution illuminates the fact that, while the charged pions were focused in the target-mode run, their decay products were isotropically suppressed in the beam-dump-mode run in which no excess was observed. This suggests a new physics solution correlated to the mesonic sector. We investigate an extended set of phenomenological models that can explain the MiniBooNE excess as a dark sector solution, utilizing long-lived particles that might be produced in the three-body decays of the charged mesons and the two-body anomalous decays of the neutral mesons. Over a broad set of interactions with the long-lived particles, we show that these scenarios can be compatible with constraints from LSND, KARMEN, and MicroBooNE, and evaluate the sensitivity of the ongoing and future data taken by the Coherent CAPTAIN Mills experiment (CCM) to a potential discovery in this parameter space.


FIG. 2. CCM experiment layout. On the left protons from the LANSCE accelerator are compressed in the proton storage ring (PSR) to pulses of 290 ns width at 20 Hz. They impact the tungsten target from above making all experiments on the Lujan floor 90° from the beam axis. The CCM detector (right) is placed 23 m away from the target. There is approximately 5 m of steel, 2 m of concrete, and 10 cm of borated polly shielding between the target and detector to reduce fast and thermal neutrons. The middle figure shows some of the various production and detection processes occurring in the experiment.
FIG. 9. The CCM120 data and background spectra from the prebeam steady state background prediction and the measured data in the beam ROI, for 1.79 × 10 21 POT.
FIG. 12. The expected and actual 90% C.L.s from CCM120 for the ALP-electron coupling g ae at tree level (top) and with an effective photon coupling at loop level (bottom). Also included are projections for CCM200, using the same background specifications as in Fig. 11, for a 3-year run. QCD axion model parameter spaces for the DFSZ(I) and DFSZ(II) benchmark scenarios span the regions indicated by the arrows [85]. The region excluded by missing energy searches at NA64 is shown in gray, and the bound derived this work from the CCM120 engineering run is set at marginally lower couplings than the NA64 region. Even in the conservative assumption that loop-level a → γγ decays are not suppressed (bottom panel), CCM200 is projected to reach beyond the more stringent constraints set from E137 in this scenario.
FIG. 15. The generated smearing matrix for the ALP search across the expected potential ALP energies. The smearing matrix includes the efficiency for each energy, with the total for each column being equal to the total efficiency for that energy ALP.
Prospects for detecting axionlike particles at the Coherent CAPTAIN-Mills experiment

May 2023

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84 Reads

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16 Citations

Physical Review D

We show results from the Coherent CAPTAIN Mills (CCM) 2019 engineering run which begin to constrain regions of parameter space for axionlike particles (ALPs) produced in electromagnetic particle showers in an 800 MeV proton beam dump, and further investigate the sensitivity of ongoing data-taking campaigns for the CCM200 upgraded detector. Based on beam-on background estimates from the engineering run, we make realistic extrapolations for background reduction based on expected shielding improvements, reduced beam width, and analysis-based techniques for background rejection. We obtain reach projections for two classes of signatures; ALPs coupled primarily to photons can be produced in the tungsten target via the Primakoff process, and then produce a gamma-ray signal in the liquid argon CCM detector either via inverse Primakoff scattering or decay to a photon pair. ALPs with significant electron couplings have several additional production mechanisms (Compton scattering, e+e− annihilation, ALP-bremsstrahlung) and detection modes (inverse Compton scattering, external e+e− pair conversion, and decay to e+e−). In some regions, the constraint is marginally better than both astrophysical and terrestrial constraints. With the beginning of a three year run, CCM will be more sensitive to this parameter space by up to an order of magnitude for both ALP-photon and ALP-electron couplings. The CCM experiment will also have sensitivity to well-motivated parameter space of QCD axion models. It is only a recent realization that accelerator-based large volume liquid argon detectors designed for low-energy coherent neutrino and dark matter scattering searches are also ideal for probing ALPs in the unexplored ∼MeV mass scale.


FIG. 1. Leptophobic DM (χ) is produced at the LANSCE through decays of light vector mediators (V B ) coupled to baryon number, which in turn can be produced in rare pion decays. This generates a flux of DM particles that can coherently scatter off
FIG. 2. The top frame shows the reconstructed energy distribution after all cuts are applied. The background prediction based on the beam-out-of-time window is the shaded region, and measured data in the beam signal region of interest are the solid lines. The bottom frame shows the background subtracted distribution along with a blue line that is arbitrarily normalized to show the shape of the expected DM distribution. The thickness of the blue line shows the variation due to 383 different m V , m χ mass combinations.
FIG. 3. Median sensitivity (dotted black curve) and observed 90% C.L. exclusions (solid black curve) set by CCM120 on the baryonic coupling strength of the vector portal mediator α B as a function of the DM mass m χ . The green line denotes the m χ − α B relation that predicts the observed DM thermal relic abundance, under the assumption of a small effective V B − γ kinetic mixing of ϵ B ¼ e ffiffiffiffiffi ffi α B p =ð4πÞ 3=2 . The shaded gray regions have been constrained by previous experiments [3,12,13,17,18]. The shaded blue region highlights the new parameter space covered by CCM120. Sensitivity projections for the upgraded CCM200 three-year run are shown as colored dotted lines under different assumptions. Blue, current shielding and filtered LAr; orange, improved shielding and filtered LAr; pink, improved shielding and underground LAr. See Ref. [11] for details.
First Leptophobic Dark Matter Search from the Coherent-CAPTAIN-Mills Liquid Argon Detector

July 2022

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46 Reads

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24 Citations

Physical Review Letters

We report the first results of a search for leptophobic dark matter (DM) from the Coherent-CAPTAIN-Mills (CCM) liquid argon (LAr) detector. An engineering run with 120 photomultiplier tubes (PMTs) and 17.9×10^{20} protons on target (POT) was performed in fall 2019 to study the characteristics of the CCM detector. The operation of this 10-ton detector was strictly light based with a threshold of 50 keV and used coherent elastic scattering off argon nuclei to detect DM. Despite only 1.5 months of accumulated luminosity, contaminated LAr, and nonoptimized shielding, CCM's first engineering run has already achieved sensitivity to previously unexplored parameter space of light dark matter models with a baryonic vector portal. With an expected background of 115 005 events, we observe 115 005+16.5 events which is compatible with background expectations. For a benchmark mediator-to-DM mass ratio of m_{V_{B}}/m_{χ}=2.1, DM masses within the range 9 MeV≲m_{χ}≲50 MeV are excluded at 90% C. L. in the leptophobic model after applying the Feldman-Cousins test statistic. CCM's upgraded run with 200 PMTs, filtered LAr, improved shielding, and 10 times more POT will be able to exclude the remaining thermal relic density parameter space of this model, as well as probe new parameter space of other leptophobic DM models.


FIG. 9. The process for finding pulses from a PMT waveform. (Top row) The raw waveform coming from the CAEN digitizers. (Second row) Exponential average of the raw waveform. (Third row) Running average or smoothed waveform of the exponential average. (Bottom row) The derivative of the waveform after all smoothing. The start (green) and stop (red) of each pulse, after a 5-ADC integral threshold is applied, are marked to point out where single photoelectrons (SPEs) are observed. Note how the noise is reduced as subsequent smoothing techniques are applied.
FIG. 10. Examples of an accumulated waveform where each PMT is represented by a different color (nine colors for 120 PMTs). The pulses from the PMTs are represented by a triangle with an area equal to the integral of the pulse. The threshold is indicated by a long-dashed line. The start, 90 ns, and end of an event are represented by dashed-dot-dot, dot, and dashed lines respectively. Only events that passed source calibration cuts have start, 90 ns, and end lines.
FIG. 15. Progression of event selection criteria for both (a) DAQ time and (b) reconstructed energy. The region to the left of the short-dashed vertical line is the beam-out-of-time region and the region between the thick long-dashed vertical lines is the beam ROI. The reconstructed energy plot is for the beamout-of-time region only.
FIG. 16. The top frame shows the reconstructed energy distribution after all selection criteria are applied. The background prediction based off the beam-out-of-time window is the shaded region, and measured data in the beam signal region of interest are the solid lines. The bottom frame shows the background subtracted distribution along with a blue line that is arbitrarily normalized to show the shape of the expected DM distribution. The thickness of the blue line shows the variation due to 383 different m V , m χ mass combinations.
FIG. 19. CCM200 expected improvements in efficiency from simulations. The biggest effect is from the improved attenuation length from the clean argon. The pink (DM) and orange ( 39 Ar) lines are for clean/filtered LAr expected with CCM200, while the black (DM) and blue ( 39 Ar) lines are with the contaminated LAr in CCM120. When convoluting this with the expected spectrum, the CCM200 energy integrated DM efficiency is about 25% while only 1% for 39 Ar decay.
First dark matter search results from Coherent CAPTAIN-Mills

July 2022

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138 Reads

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67 Citations

Physical Review D

This paper describes the operation of the Coherent CAPTAIN-Mills (CCM) detector located at the Los Alamos Neutron Science Center at Los Alamos National Laboratory. CCM is a 10-ton liquid argon detector located 20 meters from a high flux neutron/neutrino source and is designed to search for sterile neutrinos (νs’s) and light dark matter (LDM). An engineering run was performed in fall 2019 to study the characteristics of the CCM120 detector by searching for coherent scattering signals consistent with νs’s and LDM resulting from the production and decays of π+ and π0 in the tungsten target. New parameter space in a leptophobic dark matter (DM) model was excluded for DM masses between ∼2.0 and 30 MeV. The lessons learned from this run have guided the development and construction of the new CCM200 detector that will begin operations in 2021 and significantly improve on these searches.


Axion-Like Particles at Coherent CAPTAIN-Mills

December 2021

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98 Reads

We investigate the sensitivity of Coherent CAPTAIN-Mills (CCM), an 800 MeV proton-beam fixed-target experiment, to axion-like particles (ALPs) coupled to photons and electrons. Based on beam-on background estimates from the CCM engineering run performed in 2019, we make realistic extrapolations for background reduction based on expected shielding improvements, reduced beam width, and analysis-based techniques for background rejection. We obtain reach projections for two classes of signatures. ALPs coupled primarily to photons can be produced in the tungsten target via the Primakoff process, and then produce a gamma-ray signal in the Liquid Argon (LAr) CCM detector either via inverse Primakoff scattering or decay to a photon pair. ALPs with significant electron couplings have several additional production mechanisms (Compton scattering, e+ee^+e^- annihilation, ALP-bremmstrahlung) and detection modes (inverse Compton scattering, external e+ee^+e^- pair conversion, and decay to e+ee^+e^-). We show that CCM will be the first laboratory-based experiment to constrain regions of parameter space in the ALP-photon and ALP-electron couplings that, to date, have only been probed by astrophysical observations. CCM will also have sensitivity to well-motivated parameter space of QCD axion models, including the "cosmological triangle."


First Leptophobic Dark Matter Search from Coherent CAPTAIN-Mills

September 2021

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65 Reads

We report the first results of a search for leptophobic dark matter from the Coherent CAPTAIN-Mills (CCM) liquid argon (LAr) detector. An engineering run with 120 photomultiplier tubes (PMTs) and 17.9×102017.9 \times 10^{20} POT was performed in Fall 2019 to study the characteristics of the CCM detector. The operation of this 10-ton detector was strictly light-based with a threshold of 50 keV and used coherent elastic scattering off argon nuclei to detect dark matter. Despite only 1.5 months of accumulated luminosity, contaminated LAr, and non-optimized shielding, CCM's first engineering run already achieved sensitivity to previously unexplored parameter space of light dark matter models with a baryonic vector portal. For a benchmark mediator-to-dark matter mass ratio of mVB/mχ=2.1m_{_{V_B}}/m_{\chi}=2.1, dark matter masses within the range 9MeVmχ50MeV9\,\text{MeV} \lesssim m_\chi \lesssim 50\,\text{MeV} have been excluded at 90% C.L. CCM's upgraded run with 200 PMTs, filtered LAr, improved shielding, and ten times more POT will be able to exclude the remaining thermal relic density parameter space of this model, as well as probe new parameter space of other leptophobic dark matter models.


First Dark Matter Search Results From Coherent CAPTAIN-Mills

May 2021

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95 Reads

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3 Citations

This paper describes the operation of the Coherent CAPTAIN-Mills (CCM) detector located in the Lujan Neutron Science Center at Los Alamos National Laboratory. CCM is a 10-ton liquid argon (LAr) detector located 20 meters from a high flux neutron/neutrino source and is designed to search for sterile neutrinos and light dark matter. An engineering run was performed in Fall 2019 to study the characteristics of the CCM120 detector by searching for signals consistent with sterile neutrinos and light dark matter resulting from pi-plus and pi-zero decays in the tungsten target. The lessons learned from this run have guided the development and construction of the new CCM200 detector that will begin operations in 2021 and significantly improve on these searches.

Citations (5)


... The anomalous observation of excess electronlike events by MiniBooNE [2][3][4] is a focus of existing and ongoing analyses of MicroBooNE data. In Ref. [5], building off of Ref. [6], a set of phenomenological models that could explain the MiniBooNE anomaly were studied, as well as the future sensitivity of the Coherent CAPTAIN Mills (CCM) experiment to these models. These phenomenological models made use of production and detection mechanisms, schematically, where a long-lived particle X can be produced via 3-body decays of the charged mesons that are produced by the BNB target, propagating to the detector with negligible attenuation in flux, and scatter by exchanging a mediator Y (arising from a dimension-5 operator) with nucleons in detector material. ...

Reference:

Addendum to “Testing meson portal dark sector solutions to the MiniBooNE anomaly at CCM”
Testing meson portal dark sector solutions to the MiniBooNE anomaly at the Coherent CAPTAIN Mills experiment

Physical Review D

... For example, the solar axions are being probed using electron and nuclear interactions and detected by atomic and nuclear absorptions, respectively [63][64][65][66]. Beam dump experiments are also able to probe these couplings separately using electron scattering and nuclear absorption [67][68][69]. A positive signal in axion-photon conversion experiments [70][71][72][73][74] will determine f a , in which case measurement of any one of the couplings C ae ; C ap , or C an in beam dump or solar axion searches would test our model. ...

Prospects for detecting axionlike particles at the Coherent CAPTAIN-Mills experiment

Physical Review D

... The detector physical design (see Figure 5) is based on the successful Coherent Captain-Mills (CCM) experiment which is performing accelerator-based sterile neutrino, dark matter, and axion searches at LANSCE Lujan center [24][25][26]. Even though the CCM experiment is liquid argon based, the physical structures, PMT's, electronics, data analysis, and simulations will share many of the physics features of the νFLASH detector. ...

First Leptophobic Dark Matter Search from the Coherent-CAPTAIN-Mills Liquid Argon Detector

Physical Review Letters

... Recently, CEνNS detection has also been reported for reactor and solar neutrinos [6][7][8][9], further expanding the reach of this phenomenon beyond accelerator-based sources. These developments are also relevant for dark matter direct detection, as CEνNS represents an important background in next-generation experiments [7,8,10,11]. ...

First dark matter search results from Coherent CAPTAIN-Mills

Physical Review D

... Such beyond Standard Model (SM) particles are motivated by models of light dark matter [3][4][5][6][7][8][9], the origin of neutrino masses [10][11][12], and the strong-CP problem [13][14][15][16]; for a recent overview of different models and motivations, see, e.g., ref. [2]. A broad, competitive, and comprehensive experimental program has emerged with relevant facilities ranging from neutrino experiments at spallation sources [17][18][19][20][21], KEK [22], and Fermilab [23][24][25], to electron beam dumps at CERN [26], SLAC [27], and J-LAB [28]. In this work we focus on the Search for Hidden Particles (SHiP) experiment at CERN's SPS, which was approved in March 2024 [29][30][31]. ...

First Dark Matter Search Results From Coherent CAPTAIN-Mills