Abstract New neutrino–nucleus interaction cross-section measurements are required to improve nuclear models sufficiently for future long baseline neutrino experiments to meet their sensitivity goals. ...A time projection chamber (TPC) filled with a high-pressure gas is a promising detector to characterise the neutrino sources used for such experiments. A gas-filled TPC is ideal for measuring low-energy particles, which travel further in gas than in solid or liquid detectors and using high-pressure increases the target density, resulting in more neutrino interactions. We examine the suitability of multiwire proportional chambers (MWPCs) from the ALICE TPC for use as the readout chambers of a high-pressure gas TPC. These chambers were previously operated at atmospheric pressure. We report the successful operation of an ALICE TPC outer readout chamber (OROC) at pressures up to 4.2 bar absolute (barA) with $$\text {Ar-CH}_4$$ Ar-CH 4 mixtures with a $$\text {CH}_{4}$$ CH 4 content between 2.8 and 5.0%, and so far up to 4 bar absolute with $${\text {Ar-CO}}_2$$ Ar-CO 2 (90-10). The charge gain of the OROC was measured with signals induced by an $$^{55}\text {Fe}$$ 55 Fe source. The largest gain achieved at 4.2 bar was $$(29\pm 1)\cdot 10^{3}$$ ( 29 ± 1 ) · 10 3 in $$\text {Ar-CH}_4$$ Ar-CH 4 with 4.0% $$\text {CH}_{4}$$ CH 4 with an anode voltage of $${2975}\,\hbox {V}$$ 2975 V . In $${\text {Ar-CO}}_2$$ Ar-CO 2 with 10% $$\text {CO}_{2}$$ CO 2 at 4 barA, a gain of $$(4.2\pm 0.1)\cdot 10^{3}$$ ( 4.2 ± 0.1 ) · 10 3 was observed with anode voltage $${2975}\,\hbox {V}$$ 2975 V . We extrapolate that at 10 barA, an interesting pressure for future neutrino experiments, a gain of 5000 in $${\text {Ar-CO}}_2$$ Ar-CO 2 with 10% $$\text {CO}_{2}$$ CO 2 (10,000 in $$\text {Ar-CH}_4$$ Ar-CH 4 with $$\sim \!{4}{\%}$$ ∼ 4 % $$\text {CH}_{4}$$ CH 4 ) may be achieved with anode voltage of $${4.6}\,\hbox {kV}$$ 4.6 kV ( $$\sim \!{3.6}\,\hbox {kV}$$ ∼ 3.6 kV ).
With the advance of particle accelerator and detector technologies, the neutrino physics landscape is rapidly expanding. As neutrino oscillation experiments enter the intensity and precision ...frontiers, neutrino–nucleus interaction measurements are providing crucial input. MINERvA is an experiment at Fermilab dedicated to the study of neutrino–nucleus interactions in the regime of incident neutrino energies from one to few GeV. The experiment recorded neutrino and antineutrino scattering data with the NuMI beamline from 2009 to 2019 using the Low-Energy and Medium-Energy beams that peak at 3GeV and 6GeV, respectively. This article reviews the broad spectrum of interesting nuclear and particle physics that MINERvA investigations have illuminated. The newfound, detailed knowledge of neutrino interactions with nuclear targets thereby obtained is proving essential to continued progress in the neutrino physics sector.
This Letter presents the first simultaneous measurement of the quasielasticlike neutrino-nucleus cross sections on C, water, Fe, Pb, and scintillator (hydrocarbon or CH) as a function of longitudinal ...and transverse muon momentum. The ratio of cross sections per nucleon between Pb and CH is always above unity and has a characteristic shape as a function of transverse muon momentum that evolves slowly as a function of longitudinal muon momentum. The ratio is constant versus longitudinal momentum within uncertainties above a longitudinal momentum of 4.5 GeV/c. The cross section ratios to CH for C, water, and Fe remain roughly constant with increasing longitudinal momentum, and the ratios between water or C to CH do not have any significant deviation from unity. Both the overall cross section level and the shape for Pb and Fe as a function of transverse muon momentum are not reproduced by current neutrino event generators. These measurements provide a direct test of nuclear effects in quasielasticlike interactions, which are major contributors to long-baseline neutrino oscillation data samples.
Neutrino-induced charged-current single π^{+} production in the Δ(1232) resonance region is of considerable interest to accelerator-based neutrino oscillation experiments. In this Letter, high ...statistic differential cross sections are reported for the semiexclusive reaction ν_{μ}A→μ^{-}π^{+}+ nucleon(s) on scintillator, carbon, water, iron, and lead targets recorded by MINERvA using a wideband ν_{μ} beam with ⟨E_{ν}⟩≈6 GeV. Suppression of the cross section at low Q^{2} and enhancement of low T_{π} are observed in both light and heavy nuclear targets compared with phenomenological models used in current neutrino interaction generators. The cross sections per nucleon for iron and lead compared with CH across the kinematic variables probed are 0.8 and 0.5 respectively, a scaling which is also not predicted by current generators.
New neutrino-nucleus interaction cross-section measurements are required to improve nuclear models sufficiently for future long-baseline neutrino experiments to meet their sensitivity goals. A time ...projection chamber (TPC) filled with a high-pressure gas is a promising detector to characterise the neutrino sources planned for such experiments. A gas-filled TPC is ideal for measuring low-energy particles as they travel much further in gas than solid or liquid neutrino detectors. Using a high-pressure gas increases the target density, resulting in more neutrino interactions. This paper will examine the suitability of multiwire proportional chambers (MWPCs) taken from the ALICE TPC to be used as the readout chambers of a high-pressure gas TPC. These chambers were previously operated at atmospheric pressure. We tested one such MWPC at up to almost 5 bar absolute (barA) with the UK high-pressure test stand at Royal Holloway, University of London. This paper reports the successful operation of an ALICE TPC outer readout chamber (OROC) at pressures up to 4.8 bar absolute with Ar-CH\(_{4}\) mixtures with a CH\(_{4}\) content between 2.8% and 5.0%, and so far up to 4 bar absolute with Ar-CO\(_{2}\) (90-10). We measured the charge gain of this OROC using signals induced by an \(^{55}\)Fe source. The largest gain achieved at 4.8 bar was \(64\pm2)\cdot10^{3}\) at stable conditions with an anode wire voltage of 2990 V in Ar-CH\(_{4}\) (95.9-4.1). In Ar-CO\(_{2}\) a gain of \((4.2\pm0.1)\cdot10^{3}\) was observed at an anode voltage of 2975 V at 4 barA gas pressure. Based on all our gain measurements, we extrapolate that, at the 10 barA pressure necessary to fit 1 tonne of gas into the ALICE TPC volume, a gain of 5000 in Ar-CO\(_{2}\) (90-10) (10000 in Ar-CH\(_{4}\) with \(\sim\!\) 4% CH\(_{4}\) content) may be achieved with an OROC anode voltage of 4.2 V (\(\sim\!\) 3.1 kV).
Neutron production in antineutrino interactions can lead to bias in energy
reconstruction in neutrino oscillation experiments, but these interactions have
rarely been studied. MINERvA previously ...studied neutron production at an
average antineutrino energy of ~3 GeV in 2016 and found deficiencies in leading
models. In this paper, the MINERvA 6 GeV average antineutrino energy data set
is shown to have similar disagreements. A measurement of the cross section for
an antineutrino to produce two or more neutrons and have low visible energy is
presented as an experiment-independent way to explore neutron production
modeling. This cross section disagrees with several leading models'
predictions. Neutron modeling techniques from nuclear physics are used to
quantify neutron detection uncertainties on this result.
Accelerator based neutrino oscillation experiments seek to measure the relative number of electron and muon neutrinos and antineutrinos at different \(L/E\) values. However high statistics studies of ...neutrino interactions are almost exclusively measured using muon neutrinos and antineutrinos since the dominant flavor of neutrinos produced by accelerator based beams are of the muon type. This work reports new measurements of electron neutrino and antineutrino interactions in hydrocarbon, obtained by strongly suppressing backgrounds initiated by muon flavor neutrinos and antineutrinos. Double differential cross sections as a function of visible energy transfer, \(E_\text{avail}\), and transverse momentum transfer, \(p_T\), or three momentum transfer, \(q_3\) are presented.
