S. Pordes
Fermilab
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Featured researches published by S. Pordes.
Journal of Instrumentation | 2012
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.
Physics Letters B | 1978
Aris L S Angelis; R. J. Hollebeek; T.O. White; D. A. Levinthal; T. J. Chapin; James Linnemann; A. M. Smith; Leon M. Lederman; R. A. Vidal; J. M. Yelton; C. Del Papa; S. Pordes; N. Phinney; L. Camilleri; A. Rothenberg; Z. Dimcovski; B. G. Pope; L. Di Lella; R. L. Cool; L. Lyons; J.S. Wallace-Hadrill; Barry Blumenfeld; Michael J. Tannenbaum; A. M. Segar; J. Singh-Sidhu
Abstract The inclusive cross section for larger p T π 0 production near 90° in p-p collisions at the CERN ISR is presented for centre-of-mass energies 30.7, 53.1 and 62.4 GeV. The data are inconsistent with scaling of the form p T − n F ( x T ), with constant n or with n allowed to depend on x T = 2p T / s . For s = 53.1 and 62.4 GeV , the value of n found for 3.5 p T c is n = 8.0 ± 0.5, in agreement with previous experiments. However, for 7.5 p T c the value becomes n = 5.1 ± 0.4.
Physics Letters B | 1993
T. A. Armstrong; D. Bettoni; V. Bharadwaj; Cristina Biino; G. Borreani; D. Broemmelsiek; A. Buzzo; R. Calabrese; A. Ceccucci; M. Church; P. Dalpiaz; Pietro Dalpiaz; R. Dibenedetto; D. Dimitroyannis; M. Fabbri; J. Fast; A. Gianoli; C. M. Ginsburg; K. Gollwitzer; A. Hahn; M. Hasan; S. Hsueh; R. Lewis; E. Luppi; M. A. Macri; A. M. Majewska; M. Mandelkern; F. Marchetto; M. Marinelli; J. Marques
Abstract We present the first high-statistics study of the ηη system over the mass range 1000–3000 MeV/c2. The experiment was performed at the Fermilab Antiproton Accumulator, and the data sample consists of six-photon final states produced in antiproton-proton annihilations at s in the range 2950–3620 MeV. We find evidence for three states with masses 1488 ± 10 MeV/c2, 1748 ± 10 MeV/c2 and 2104 ± 20 MeV/c2 respectively.
Nuclear Physics | 1992
T. A. Armstrong; D. Bettoni; V. Bharadwaj; Cristina Biino; G. Borreani; D. Broemmelsiek; A. Buzzo; R. Calabrese; A. Ceccucci; R. Cester; M. Church; P. Dalpiaz; M. Dameri; D. Dimitroyannis; M. Fabbri; J. Fast; S. Ferroni; M. Gee; C. M. Ginsburg; K. Gollwitzer; A. Hahn; M. Hasan; S. Hsueh; R. Lewis; E. Luppi; M. A. Macri; A. M. Majewska; M. Mandelkern; F. Marchetto; M. Marinelli
We report on a study of the χ1(3P1) and χ2(3P2) states of charmonium formed in antiproton-proton annihilations. An energy scan through the resonances, performed with a very narrow momentum-band beam of antiprotons intersecting a hydrogen jet target, enables us to perform very precise measurements of the mass and the total width of the two resonances. From a sample of 513 χ1 and 585 χ2 events we find Mχ1 = (3510.53±0.13) MeV/c2, Mχ2 = (3556.15±0.14) MeV/c2, Γχ1 = (0.88±0.14) MeV and Γχ2 = (1.98±0.18) MeV. From our measurement of the quantity Γ(R → pp) × BR(R → Jψ → e+ e−), using known branching ratios, we obtain Λ(χ1 → pp) = (69±13) eV and Λ(χ2 → pp) = (180±31) eV.
Journal of Instrumentation | 2014
Mark Adamowski; B. Carls; E. Dvorak; A. Hahn; W. Jaskierny; C. Johnson; H. Jöstlein; C. Kendziora; S. Lockwitz; B. Pahlka; R. Plunkett; S. Pordes; B. Rebel; R. Schmitt; M. Stancari; Terry Tope; E. Voirin; T. Yang
The Liquid Argon Purity Demonstrator was an R&D test stand designed to determine if electron drift lifetimes adequate for large neutrino detectors could be achieved without first evacuating the cryostat. We describe here the cryogenic system, its operations, and the apparatus used to determine the contaminant levels in the argon and to measure the electron drift lifetime. The liquid purity obtained by this system was facilitated by a gaseous argon purge. Additionally, gaseous impurities from the ullage were prevented from entering the liquid at the gas-liquid interface by condensing the gas and filtering the resulting liquid before returning to the cryostat. The measured electron drift lifetime in this test was greater than 6 ms, sustained over several periods of many weeks. Measurements of the temperature profile in the argon, to assess convective flow and boiling, were also made and are compared to simulation.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1991
L. Bartoszek; Vinod K. Bharadwaj; M. Church; A. Hahn; J. Peoples; S. Pordes; P. A. Rapidis; S.J. Werkema; D. Agahi; D.R. Broemmelsiek; J.E. Fast; M. Gee; K.E. Gollwitzer; M. Mandelkern; J.L. Marques; J. Schultz; M.F. Weber; C.M. Ginsburg; M. Masuzawa; R. Ray; J. Rosen; S. Trokenheim; Jing Zhao; T. A. Armstrong; G.E. Hufford; R. Lewis; A.M. Majewska; J. Reid; G. A. Smith; M.A. Hasan
The central calorimeter in Fermilab experiment E760++ has been designed to measure the topology and energies of electrons and photons in the decay of charmonium formed in pp annihilation. The calorimeter is composed of 1280 lead-glass Cherenkov counters read out with photomultiplier tubes. This paper discusses design criteria for the calorimeter and describes how these criteria were met. Data from tests in low energy (10–84 MeV) and medium energy (1–4 GeV) beams are presented showing a spatial resolution of 9 mm, an energy resolution of (3.0 ± 0.3)%√E[GeV] + (1.5 ± 0.5)%, and an effective energy threshold below 10 MeV.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2009
A. Curioni; B. T. Fleming; W. Jaskierny; C. Kendziora; J. Krider; S. Pordes; M. Soderberg; J. Spitz; T. Tope; T. Wongjirad
A filter system for removing electronegative impurities from liquid argon is described. The active components of the filter are adsorbing molecular sieve and activated-copper-coated alumina granules. The system is capable of purifying liquid argon to an oxygen-equivalent impurity concentration of better than 30 parts per trillion, corresponding to an electron drift lifetime of at least 10 ms. Reduction reactions that occur at �250 ◦ C allow the filter material to be regenerated in-situ through a simple procedure. In the following work we describe the filter design, performance, and regeneration process.
Physics Letters B | 1996
T. A. Armstrong; D. Bettoni; V. Bharadwaj; Cristina Biino; G. Blanford; G. Borreani; D. Broemmelsiek; A. Buzzo; R. Calabrese; A. Ceccucci; R. Cester; M. Church; P. Dalpiaz; Pietro Dalpiaz; R. Dibenedetto; D. Dimitroyannis; M. Fabbri; J. Fast; A. Gianoli; C. M. Ginsburg; K. Gollwitzer; G. Govi; A. Hahn; M. Hasan; S. Hsueh; R. Lewis; E. Luppi; M. A. Macri; A. M. Majewska; M. Mandelkern
Abstract Differential cross sections for p p elastic scattering have been measured for very small momentum transfers at six different incident antiproton momenta in the range 3.7 to 6.2 GeV/c by the detection of recoil protons at scattering angles close to 90°. Forward scattering parameters σ T , b , and ϱ have been determined. For the ϱ-parameter, up to an order of magnitude higher level of precision has been achieved compared to that in earlier experiments. It is found that existing dispersion theory predictions are in disagreement with our results for the ϱ-parameter.
Journal of Instrumentation | 2014
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
A workshop was held at Fermilab on March 20-21, 2013 to discuss the development of liquid argon time projection chambers (LArTPCs) in the United States. The workshop was organized under the auspices of the Coordinating Panel for Advanced Detectors, a body that was initiated by the American Physical Society Division of Particles and Fields. All presentations at the workshop were made in seven topical plenary sessions: i) Argon Purity, ii) Cryogenics, iii) TPC and High Voltage, iv) Electronics, Data Acquisition and Triggering, v) Scintillation Light Detection, vi) Calibration and Test Beams, and vii) Software. This document summarizes the current efforts in each of these areas. It also highlights areas in LArTPC research and development that are common between neutrino experiments and dark matter experiments.
Journal of Physics: Conference Series | 2011
B. Rebel; Mark Adamowski; W. Jaskierny; H. Jöstlein; C. Kendziora; R. Plunkett; S. Pordes; R. Schmitt; Terry Tope; T. Yang
The Fermilab Materials Test Stand was developed to test the suitability of materials for use in large liquid argon time projection chambers (TPCs). In addition to determining which materials are viable for use in TPCs, the test stand has also shown that water is especially detrimental to maintaining long electron lifetimes. The Liquid Argon Purity Demonstrator is currently under construction at Fermilab. Its goal is to show that long electron lifetimes can be achieved without evacuation of the cryostat, which is of particular interest in designing large liquid argon TPCs.