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Featured researches published by B. Baller.


Journal of Instrumentation | 2012

The ArgoNeuT Detector in the NuMI Low-Energy beam line at Fermilab

C. E. Anderson; M. Antonello; B. Baller; T. A. Bolton; C. Bromberg; F. Cavanna; E. Church; D. Edmunds; A. Ereditato; S. Farooq; B. T. Fleming; H. Greenlee; R. Guenette; S. Haug; G. Horton-Smith; C. James; E. Klein; K. Lang; A. Lathrop; P. Laurens; S. K. Linden; D. McKee; R. Mehdiyev; B. Page; O. Palamara; K. Partyka; S. Pordes; G. Rameika; B. Rebel; B. Rossi

The ArgoNeuT liquid argon time projection chamber has collected thousands of neutrino and anti-neutrino events during an extended run period in the NuMI beam-line at Fermilab. This paper focuses on the main aspects of the detector layout and related technical features, including the cryogenic equipment, time projection chamber, read-out electronics, and off-line data treatment. The detector commissioning phase, physics run, and first neutrino event displays are also reported. The characterization of the main working parameters of the detector during data-taking, the ionization electron drift velocity and lifetime in liquid argon, as obtained from through-going muon data complete the present report.


Physical Review Letters | 2012

First measurements of inclusive muon neutrino charged current differential cross sections on argon.

C. E. Anderson; M. Antonello; B. Baller; T. Bolton; C. Bromberg; F. Cavanna; E. Church; D. Edmunds; A. Ereditato; S. Farooq; B. T. Fleming; H. Greenlee; R. Guenette; S. Haug; G. Horton-Smith; C. James; E. Klein; K. Lang; P. Laurens; S. K. Linden; D. McKee; R. Mehdiyev; B. Page; O. Palamara; K. Partyka; A. Patch; G. Rameika; B. Rebel; B. Rossi; M. Soderberg

The ArgoNeuT Collaboration presents the first measurements of inclusive muon neutrino charged current differential cross sections on argon. Obtained in the NuMI neutrino beam line at Fermilab, the flux-integrated results are reported in terms of outgoing muon angle and momentum. The data are consistent with the Monte Carlo expectation across the full range of kinematics sampled, 0°<θ(μ)<36° and 0<P(μ)<25 GeV/c. Along with confirming the viability of liquid argon time projection chamber technology for neutrino detection, the measurements allow tests of low-energy neutrino scattering models important for interpreting results from long baseline neutrino oscillation experiments designed to investigate CP violation and the orientation of the neutrino mass hierarchy.


Physical Review D | 2014

Detection of back-to-back proton pairs in charged-current neutrino interactions with the ArgoNeuT detector in the NuMI low energy beam line

R. Acciarri; C. Adams; J. Asaadi; B. Baller; T. Bolton; C. Bromberg; F. Cavanna; E. Church; D. Edmunds; A. Ereditato; S. Farooq; B. T. Fleming; H. Greenlee; G. Horton-Smith; C. James; E. Klein; K. Lang; P. Laurens; R. Mehdiyev; B. Page; O. Palamara; K. Partyka; G. Rameika; B. Rebel; M. Soderberg; J. Spitz; A.M. Szelc; M. Weber; T. Yang; G. P. Zeller

Short range nucleon-nucleon correlations in nuclei (NN SRC) carry important information on nuclear structure and dynamics. NN SRC have been extensively probed through two-nucleon knock- out reactions in both pion and electron scattering experiments. We report here on the detection of two-nucleon knock-out events from neutrino interactions and discuss their topological features as possibly involving NN SRC content in the target argon nuclei. The ArgoNeuT detector in the Main Injector neutrino beam at Fermilab has recorded a sample of 30 fully reconstructed charged current events where the leading muon is accompanied by a pair of protons at the interaction vertex, 19 of which have both protons above the Fermi momentum of the Ar nucleus. Out of these 19 events, four are found with the two protons in a strictly back-to-back high momenta configuration directly observed in the final state and can be associated to nucleon Resonance pionless mechanisms involving a pre-existing short range correlated np pair in the nucleus. Another fraction (four events) of the remaining 15 events have a reconstructed back-to-back configuration of a np pair in the initial state, a signature compatible with one-body Quasi Elastic interaction on a neutron in a SRC pair. The detection of these two subsamples of the collected (mu- + 2p) events suggests that mechanisms directly involving nucleon-nucleon SRC pairs in the nucleus are active and can be efficiently explored in neutrino-argon interactions with the LAr TPC technology.


Physical Review D | 2014

Measurements of inclusive muon neutrino and antineutrino charged current differential cross sections on argon in the NuMI antineutrino beam

R. Acciarri; C. Adams; J. Asaadi; B. Baller; T. Bolton; C. Bromberg; F. Cavanna; E. Church; D. Edmunds; A. Ereditato; S. Farooq; B. T. Fleming; H. Greenlee; R. Hatcher; G. Horton-Smith; C. James; E. Klein; K. Lang; P. Laurens; R. Mehdiyev; B. Page; O. Palamara; K. Partyka; G. Rameika; B. Rebel; M. Soderberg; J. Spitz; A.M. Szelc; M. Weber; T. Yang

The ArgoNeuT collaboration presents measurements of inclusive muon neutrino and antineutrino charged current differential cross sections on argon in the Fermilab NuMI beam operating in the low energy antineutrino mode. The results are reported in terms of outgoing muon angle and momentum at a mean neutrino energy of 9.6 GeV (neutrinos) and 3.6 GeV (antineutrinos), in the range


Physical Review Letters | 2014

First measurement of neutrino and antineutrino coherent charged pion production on argon

R. Acciarri; C. Adams; J. Asaadi; B. Baller; T. Bolton; C. Bromberg; F. Cavanna; E. Church; D. Edmunds; A. Ereditato; S. Farooq; B. T. Fleming; H. Greenlee; R. Hatcher; G. Horton-Smith; C. James; E. Klein; K. Lang; P. Laurens; R. Mehdiyev; B. Page; O. Palamara; K. Partyka; G. Rameika; B. Rebel; E. Santos; A. Schukraft; M. Soderberg; J. Spitz; A.M. Szelc

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Journal of Instrumentation | 2013

A study of electron recombination using highly ionizing particles in the ArgoNeuT Liquid Argon TPC

R. Acciarri; C. Adams; J. Asaadi; B. Baller; T. A. Bolton; C. Bromberg; F. Cavanna; E. Church; D. Edmunds; A. Ereditato; S. Farooq; B. T. Fleming; H. Greenlee; G. Horton-Smith; C. James; E. Klein; K. Lang; P. Laurens; D. McKee; R. Mehdiyev; B. Page; O. Palamara; K. Partyka; G. Rameika; B. Rebel; M. Soderberg; J. Spitz; A.M. Szelc; M. Weber; Mariusz Wojcik

and


Journal of Instrumentation | 2014

Liquid Argon Time Projection Chamber research and development in the United States

B. Baller; C. Bromberg; N. J. Buchanan; F. Cavanna; H. Chen; E. Church; V.M. Gehman; H. Greenlee; E. Guardincerri; B.J.P. Jones; T. Junk; T. Katori; M. Kirby; K. Lang; B Loer; A. Marchionni; T. Maruyama; C. Mauger; A Menegolli; D. Montanari; S. Mufson; B. Norris; S. Pordes; J.L. Raaf; B. Rebel; R Sanders; M. Soderberg; J. St. John; T. Strauss; A.M. Szelc

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Journal of Instrumentation | 2012

Analysis of a large sample of neutrino-induced muons with the ArgoNeuT detector

C. E. Anderson; M. Antonello; B. Baller; T. A. Bolton; C. Bromberg; F. Cavanna; E. Church; D. Edmunds; A. Ereditato; S. Farooq; B. T. Fleming; H. Greenlee; R. Guenette; S. Haug; G. Horton-Smith; C. James; E. Klein; K. Lang; P. Laurens; S. K. Linden; D. McKee; R. Mehdiyev; B. Page; O. Palamara; K. Partyka; G. Rameika; B. Rebel; B. Rossi; M. Soderberg; J. Spitz

, for both neutrinos and antineutrinos.


Journal of Instrumentation | 2015

Summary of the second workshop on liquid argon time projection chamber research and development in the United States

R. Acciarri; M. Adamowski; D. Artrip; B. Baller; C. Bromberg; F. Cavanna; B. Carls; H. Chen; G. Deptuch; L. Epprecht; R. Dharmapalan; W. Foreman; A. Hahn; M. Johnson; B.J.P. Jones; T. Junk; K. Lang; S. Lockwitz; A. Marchionni; C. Mauger; C. Montanari; S. Mufson; M. Nessi; H. Olling Back; G. Petrillo; S. Pordes; J.L. Raaf; B. Rebel; G. Sinins; M. Soderberg

We report on the first cross section measurements for charged current coherent pion production by neutrinos and antineutrinos on argon. These measurements are performed using the ArgoNeuT detector exposed to the NuMI beam at Fermilab. The cross sections are measured to be 2.6(-1.0)(+1.2)(stat)(-0.4)(+0.3)(syst)×10(-38)u2009u2009cm(2)/Ar for neutrinos at a mean energy of 9.6 GeV and 5.5(-2.1)(+2.6)(stat)(-0.7)(+0.6)(syst)×10(-39)u2009u2009cm(2)/Ar for antineutrinos at a mean energy of 3.6 GeV.

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C. Bromberg

Michigan State University

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K. Lang

University of Texas at Austin

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B. Page

Michigan State University

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