398 research outputs found
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Neutron-Proton Effective Range Parameters and Zero-Energy Shape Dependence.
No full textA completely model-independent effective range theory fit to available, unpolarized, np scattering data below 3 MeV determines the zero-energy free proton cross section {sigma}{sub 0} = 20.4287 {+-} 0.0078 b, the singlet apparent effective range r{sub s} = 2.754 {+-} 0.018{sub stat} {+-} 0.056{sub syst} fm, and improves the error slightly on the parahydrogen coherent scattering length, a{sub c} = -3.7406 {+-} 0.0010 fm. The triplet and singlet scattering lengths and the triplet mixed effective range are calculated to be a{sub t} = 5.4114 {+-} 0.0015 fm, a{sub s} = -23.7153 {+-} 0.0043 fm, and {rho}{sub t}(0,-{epsilon}{sub t}) = 1.7468 {+-} 0.0019 fm. The model-independent analysis also determines the zero-energy effective ranges by treating them as separate fit parameters without the constraint from the deuteron binding energy {epsilon}{sub t}. These are determined to be {rho}{sub t}(0,0) = 1.705 {+-} 0.023 fm and {rho}{sub s}(0,0) = 2.665 {+-} 0.056 fm. This determination of {rho}{sub t}(0,0) and {rho}{sub s}(0,0) is most sensitive to the sparse data between about 20 and 600 keV, where the correlation between the determined values of {rho}{sub t}(0,0) and {rho}{sub s}(0,0) is at a minimum. This correlation is responsible for the large systematic error in r{sub s}. More precise data in this range are needed. The present data do not event determine (with confidence) that {rho}{sub t}(0,0) {ne} {rho}{sub t}(0, -{epsilon}{sub t}), referred to here as ''zero-energy shape dependence''. The widely used measurement of {sigma}{sub 0} = 20.491 {+-} 0.014 b from W. Dilg, Phys. Rev. C 11, 103 (1975), is argued to be in error
An Arabic-to-English Translation of the Religious Debate between the Nestorian Patriarch Timothy I and the 'Abbāsid Caliph al-Mahdī
No full textFirst observation of low energy electron neutrinos in a liquid argon time projection chamber
No full textThe capabilities of liquid argon time projection chambers (LArTPCs) to reconstruct the spatial and calorimetric information of neutrino events have made them the detectors of choice in a number of experiments, specifically those looking to observe electron neutrino (νe) appearance. The LArTPC promises excellent background rejection capabilities, especially in this "golden" channel for both short and long baseline neutrino oscillation experiments. We present the first experimental observation of electron neutrinos and antineutrinos in the ArgoNeut LArTPC, in the energy range relevant to DUNE and the Fermilab Short Baseline Neutrino Program. We have selected 37 electron candidate events and 274 gamma candidate events, and measured an 80% purity of electrons based on a topological selection. Additionally, we present a separation of electrons from gammas using calorimetric energy deposition, demonstrating further separation of electrons from background gammas
Demonstration of MeV-scale physics in liquid argon time projection chambers using ArgoNeuT
No full textMeV-scale energy depositions by low-energy photons produced in neutrino-argon interactions have been identified and reconstructed in ArgoNeuT liquid argon time projection chamber (LArTPC) data. ArgoNeuT data collected on the NuMI beam at Fermilab were analyzed to select isolated low-energy depositions in the TPC volume. The total number, reconstructed energies, and positions of these depositions have been compared to those from simulations of neutrino-argon interactions using the fluka Monte Carlo generator. Measured features are consistent with energy depositions from photons produced by deexcitation of the neutrino's target nucleus and by inelastic scattering of primary neutrons produced by neutrino-argon interactions. This study represents a successful reconstruction of physics at the MeV scale in a LArTPC, a capability of crucial importance for detection and reconstruction of supernova and solar neutrino interactions in future large LArTPCs
First measurement of the cross section for νμ and ν μ induced single charged pion production on argon using
No full textWe report on the first cross section measurement of charged-current single charged pion production by neutrinos and antineutrinos on argon. This analysis was performed using the ArgoNeuT detector exposed to the NuMI beam at Fermilab. The measurements are presented as functions of muon momentum, muon angle, pion angle, and angle between muon and pion. The flux-averaged cross sections are measured to be 2.7±0.5(stat)±0.5(syst)×10-37 cm2/Ar for neutrinos at a mean energy of 9.6 GeV and 8.4±0.9(stat)-0.8+1.0(syst)×10-38 cm2/Ar for antineutrinos at a mean energy of 3.6 GeV with the charged pion momentum above 100 MeV/c. The results are compared with several model predictions
Measurement of νμ and ν ̄μ neutral current π0→γγ production in the ArgoNeuT detector
No full textThe ArgoNeuT Collaboration reports the first measurement of neutral current π0 production in νμ-argon and ν-μ-argon scattering. This measurement was performed using the ArgoNeuT liquid argon time projection chamber deployed at Fermilab's NuMI neutrino beam with an exposure corresponding to 1.2×1020 protons-on-target from the Fermilab main injector and a mean energy for νμ of 9.6 GeV and for ν-μ of 3.6 GeV. We compare the measured cross section and kinematic distributions to predictions from the GENIE and NuWro neutrino interaction event generators
Protector and friend: Turning points and discursive constructions of the stepparent role
No full textObjective: To understand turning points (TPs) in the development of positive stepparent–stepchild communication and relationships.
Background: Scholars stress the importance of communication in co-constructing healthy stepparent–stepchild relationships. The researchers focused on positive stepparenting via understanding transformational turning point (TP) events across time. Research questions explored how stepparents with an overall positive relationship with a stepchild characterize TPs and the discursive constructions of the stepparent role.
Method: The team analyzed 877 pages of data from 37 in-depth interviews with stepparents who described self-identified TP events, reflected in visual graphs of 279 TPs.
Results: Data were coded into 11 TP types, focused on structural and role changes for stepparents, co-constructed over time. The top three TP types were changes in household composition, communicating support through offering protection and being present/available, and role change, most frequently by functioning as a parent versus friend. All the TPs highlight discursive work to forge positive stepparenting roles.
Conclusions: The findings extend earlier studies of stepchildren’s experiences and communication practices that ground resilience to manage relational resources through investments of quality time and enactment of social support. Implications: Applications suggest support for stepparents to have quality interactions with stepchildren and training to develop healthy communication practices and facilitate resilience
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Data acquisition for RHIC report of the working group
No full textAs experimental configurations for RHIC become better defined, the requirements for data acquisition for each of the evolving experiments becomes susceptible to detailed analysis. An earlier contribution made it clear that the scale of these experiments makes demands on data acquisition that are at least as severe as some of the large-scale collider experiments being mounted at Fermilab and LEP. In this report, we attempt to answer the following questions: what sort of performance is required by each of the experiments; is there a single architecture flexible enough to accommodate all of the proposed experiments; what are the costs associated with such a implementation; and how far in advance of beam does a data acquisition implementation need to be started. 3 refs., 2 figs., 1 tab
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