107 research outputs found

    SYNERGY AMONG RESPONDING LYMPHOID CELLS IN THE ONE-WAY MIXED LYMPHOCYTE REACTION : INTERACTION BETWEEN TWO TYPES OF THYMUS-DEPENDENT CELLS

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    The present studies have shown that two subpopulations of thymus-dependent lymphocytes may act synergistically in the mixed lymphocyte reaction (MLR) in the mouse. One subpopulation was well represented in the young adult thymus and the other in lymph nodes. For optimum synergy, both populations must be allogeneic to the stimulator cells. Pretreatment of either population with mitomycin-C abolished synergy. Anti-θ serum abolished both MLR responding and synergizing activities of lymphoid cells. The two thymus-dependent subpopulations were both present in the spleen, and displayed different migratory patterns when injected into irradiated mice: one population went to spleens of the irradiated mice, the other to lymph nodes. The effects of anti-thymocyte serum on the MLR and upon synergy were assessed. While minor differences exist and are herein described, our overall results strongly suggest that in our experiments with synergy in MLR, we may be dealing with the same T1- and T2-cell subpopulations described by Cantor and Asofsky and coworkers (1, 2, 4, 5, 14) as displaying synergy in the graft-vs.-host reaction

    Precision measurements of g1g_1 of the proton and the deuteron with 6 GeV electrons

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    The inclusive polarized structure functions of the proton and deuteron, g1p and g1d, were measured with high statistical precision using polarized 6 GeV electrons incident on a polarized ammonia target in Hall B at Jefferson Laboratory. Electrons scattered at lab angles between 18 and 45 degrees were detected using the CEBAF Large Acceptance Spectrometer (CLAS). For the usual DIS kinematics, Q^2>1 GeV^2 and the final-state invariant mass W>2 GeV, the ratio of polarized to unpolarized structure functions g1/F1 is found to be nearly independent of Q^2 at fixed x. Significant resonant structure is apparent at values of W up to 2.3 GeV. In the framework of perturbative QCD, the high-W results can be used to better constrain the polarization of quarks and gluons in the nucleon, as well as high-twist contributions

    Feasibility studies of time-like proton electromagnetic form factors at PANDA at FAIR

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    Simulation results for future measurements of electromagnetic proton form factors at \PANDA (FAIR) within the PandaRoot software framework are reported. The statistical precision with which the proton form factors can be determined is estimated. The signal channel pˉpe+e\bar p p \to e^+ e^- is studied on the basis of two different but consistent procedures. The suppression of the main background channel, i.e.\textit{i.e.} pˉpπ+π\bar p p \to \pi^+ \pi^-, is studied. Furthermore, the background versus signal efficiency, statistical and systematical uncertainties on the extracted proton form factors are evaluated using two different procedures. The results are consistent with those of a previous simulation study using an older, simplified framework. However, a slightly better precision is achieved in the PandaRoot study in a large range of momentum transfer, assuming the nominal beam conditions and detector performance

    First measurements of the double-polarization observables F, P, and H in ω photoproduction off transversely polarized protons in the N* resonance region

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    First measurements of double-polarization observables in ω photoproduction off the proton are presented using transverse target polarization and data from the CEBAF Large Acceptance Spectrometer (CLAS) FROST experiment at Jefferson Lab. The beam-target asymmetry F has been measured using circularly polarized, tagged photons in the energy range 1200–2700 MeV, and the beam-target asymmetries H and P have been measured using linearly polarized, tagged photons in the energy range 1200–2000 MeV. These measurements significantly increase the database on polarization observables. The results are included in two partial-wave analyses and reveal significant contributions from several nucleon (N∗) resonances. In particular, contributions from new N∗ resonances listed in the Review of Particle Properties are observed, which aid in reaching the goal of mapping out the nucleon resonance spectrum

    Momentum sharing in imbalanced Fermi systems

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    The atomic nucleus is composed of two different kinds of fermions, protons and neutrons. If the protons and neutrons did not interact, the Pauli exclusion principle would force the majority fermions (usually neutrons) to have a higher average momentum. Our high-energy electron scattering measurements using 12C, 27Al, 56Fe and 208Pb targets show that, even in heavy neutron-rich nuclei, short-range interactions between the fermions form correlated high-momentum neutron-proton pairs. Thus, in neutron-rich nuclei, protons have a greater probability than neutrons to have momentum greater than the Fermi momentum. This finding has implications ranging from nuclear few body systems to neutron stars and may also be observable experimentally in two-spin state, ultra-cold atomic gas systems.Comment: Published in Science. 10 pages, 3 figure

    Cross Sections for the Exclusive Photon Electroproduction on the Proton and Generalized Parton Distributions

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    International audienceUnpolarized and beam-polarized fourfold cross sections ðd4σ=dQ2dxBdtdϕÞ for the ep → e0p0γreaction were measured using the CLAS detector and the 5.75-GeV polarized electron beam of theJefferson Lab accelerator, for 110 (Q2; xB; t) bins over the widest phase space ever explored in the valencequarkregion. Several models of generalized parton distributions (GPDs) describe the data well at most ofour kinematics. This increases our confidence that we understand the GPD H, expected to be the dominantcontributor to these observables. Through a leading-twist extraction of Compton form factors, these resultssupport the model predictions of a larger nucleon size at lower quark-momentum fraction xB

    Prognostic model to predict postoperative acute kidney injury in patients undergoing major gastrointestinal surgery based on a national prospective observational cohort study.

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    Background: Acute illness, existing co-morbidities and surgical stress response can all contribute to postoperative acute kidney injury (AKI) in patients undergoing major gastrointestinal surgery. The aim of this study was prospectively to develop a pragmatic prognostic model to stratify patients according to risk of developing AKI after major gastrointestinal surgery. Methods: This prospective multicentre cohort study included consecutive adults undergoing elective or emergency gastrointestinal resection, liver resection or stoma reversal in 2-week blocks over a continuous 3-month period. The primary outcome was the rate of AKI within 7 days of surgery. Bootstrap stability was used to select clinically plausible risk factors into the model. Internal model validation was carried out by bootstrap validation. Results: A total of 4544 patients were included across 173 centres in the UK and Ireland. The overall rate of AKI was 14·2 per cent (646 of 4544) and the 30-day mortality rate was 1·8 per cent (84 of 4544). Stage 1 AKI was significantly associated with 30-day mortality (unadjusted odds ratio 7·61, 95 per cent c.i. 4·49 to 12·90; P < 0·001), with increasing odds of death with each AKI stage. Six variables were selected for inclusion in the prognostic model: age, sex, ASA grade, preoperative estimated glomerular filtration rate, planned open surgery and preoperative use of either an angiotensin-converting enzyme inhibitor or an angiotensin receptor blocker. Internal validation demonstrated good model discrimination (c-statistic 0·65). Discussion: Following major gastrointestinal surgery, AKI occurred in one in seven patients. This preoperative prognostic model identified patients at high risk of postoperative AKI. Validation in an independent data set is required to ensure generalizability

    Feasibility studies for the measurement of time-like proton electromagnetic form factors from p¯ p→ μ+μ- at P ¯ ANDA at FAIR

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    This paper reports on Monte Carlo simulation results for future measurements of the moduli of time-like proton electromagnetic form factors, | GE| and | GM| , using the p¯ p→ μ+μ- reaction at P ¯ ANDA (FAIR). The electromagnetic form factors are fundamental quantities parameterizing the electric and magnetic structure of hadrons. This work estimates the statistical and total accuracy with which the form factors can be measured at P ¯ ANDA , using an analysis of simulated data within the PandaRoot software framework. The most crucial background channel is p¯ p→ π+π-, due to the very similar behavior of muons and pions in the detector. The suppression factors are evaluated for this and all other relevant background channels at different values of antiproton beam momentum. The signal/background separation is based on a multivariate analysis, using the Boosted Decision Trees method. An expected background subtraction is included in this study, based on realistic angular distributions of the background contribution. Systematic uncertainties are considered and the relative total uncertainties of the form factor measurements are presented

    Study of doubly strange systems using stored antiprotons

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    Bound nuclear systems with two units of strangeness are still poorly known despite their importance for many strong interaction phenomena. Stored antiprotons beams in the GeV range represent an unparalleled factory for various hyperon-antihyperon pairs. Their outstanding large production probability in antiproton collisions will open the floodgates for a series of new studies of systems which contain two or even more units of strangeness at the P‾ANDA experiment at FAIR. For the first time, high resolution γ-spectroscopy of doubly strange ΛΛ-hypernuclei will be performed, thus complementing measurements of ground state decays of ΛΛ-hypernuclei at J-PARC or possible decays of particle unstable hypernuclei in heavy ion reactions. High resolution spectroscopy of multistrange Ξ−-atoms will be feasible and even the production of Ω−-atoms will be within reach. The latter might open the door to the |S|=3 world in strangeness nuclear physics, by the study of the hadronic Ω−-nucleus interaction. For the first time it will be possible to study the behavior of Ξ‾+ in nuclear systems under well controlled conditions

    Spin and parity measurement of the Λ(1405) baryon

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    A determination of the spin and parity of the Λ(1405)\Lambda(1405) is presented using photoproduction data from the CLAS detector at Jefferson Lab. The reaction γ+pK++Λ(1405)\gamma + p \to K^+ + \Lambda(1405) is analyzed in the decay channel Λ(1405)Σ++π\Lambda(1405) \to \Sigma^+ + \pi^-, where the decay distribution to Σ+π\Sigma^+ \pi^- and the variation of the Σ+\Sigma^+ polarization with respect to the Λ(1405)\Lambda(1405) polarization direction determines the parity. The Λ(1405)\Lambda(1405) is produced, in the energy range 2.55<W<2.852.55 < W < 2.85 GeV and for 0.6<cosθK+<0.90.6 < \cos \theta_{K^+} < 0.9, with polarization P=0.45±0.02(stat)±0.07(syst)P = 0.45 \pm 0.02 (\text{stat}) \pm 0.07 (\text{syst}). The analysis shows that the decays are in SS wave, with the Σ+\Sigma^+ polarized such that the Λ(1405)\Lambda(1405) has spin-parity JP=1/2J^P = 1/2^-, as expected by most theories.Comment: 6 pages, 4 figures, accepted by Phys. Rev. Let
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