152 research outputs found

    The HADES Tracking System

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    The tracking system of the dielectron spectrometer HADES at GSI Darmstadt is formed out of 24 low-mass, trapezoidal multi-layer drift chambers providing in total about 30 square meter of active area. Low multiple scattering in the in total four planes of drift chambers before and after the magnetic field is ensured by using helium-based gas mixtures and aluminum cathode and field wires. First in-beam performance results are contrasted with expectations from simulations. Emphasis is placed on the energy loss information, exploring its relevance regarding track recognition.Comment: 6 pages, 4 figures, presented at the 10th Vienna Conference on Instrumentation, Vienna, February 2004, to be published in NIM A (special issue

    A versatile method for simulating pp -> ppe+e- and dp -> pne+e-p_spec reactions

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    We have developed a versatile software package for the simulation of di-electron production in pppp and dpdp collisions at SIS energies. Particular attention has been paid to incorporate different descriptions of the Dalitz decay ΔNe+e\Delta \to N e^+e^- via a common interface. In addition, suitable parameterizations for the virtual bremsstrahlung process NNNNe+eNN \to NN e^+e^- based on one-boson exchange models have been implemented. Such simulation tools with high flexibility of the framework are important for the interpretation of the di-electron data taken with the HADES spectrometer and the design of forthcoming experiments

    Production of Sigma{\pm}pi?pK+ in p+p reactions at 3.5 GeV beam energy

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    We study the production of Sigma^+-pi^+-pK^+ particle quartets in p+p reactions at 3.5 GeV kinetic beam energy. The data were taken with the HADES experiment at GSI. This report evaluates the contribution of resonances like Lambda(1405$, Sigma(1385)^0, Lambda(1520), Delta(1232), N^* and K^*0 to the Sigma^+- pi^-+ p K+ final state. The resulting simulation model is compared to the experimental data in several angular distributions and it shows itself as suitable to evaluate the acceptance corrections properly.Comment: 15 pages, 5 figure

    An upper limit on hypertriton production in collisions of Ar(1.76 AGeV)+KCl

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    A high-statistic data sample of Ar(1.76 AGeV)+KCl events recorded with HADES is used to search for a hypertriton signal. An upper production limit per centrality-triggered event of 1.041.04 x 10310^{-3} on the 3σ3\sigma level is derived. Comparing this value with the number of successfully reconstructed Λ\Lambda hyperons allows to determine an upper limit on the ratio NΛ3H/NΛN_{_{\Lambda}^3H}/N_{\Lambda}, which is confronted with statistical and coalescence-type model calculations

    In-Medium Effects on K0 Mesons in Relativistic Heavy-Ion Collisions

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    We present the transverse momentum spectra and rapidity distributions of π\pi^{-} and KS0^0_S in Ar+KCl reactions at a beam kinetic energy of 1.756 A GeV measured with the spectrometer HADES. The reconstructed KS0^0_S sample is characterized by good event statistics for a wide range in momentum and rapidity. We compare the experimental π\pi^{-} and KS0^0_S distributions to predictions by the IQMD model. The model calculations show that KS0^0_S at low tranverse momenta constitute a particularly well suited tool to investigate the kaon in-medium potential. Our KS0^0_S data suggest a strong repulsive in-medium K0^0 potential of about 40 MeV strength.Comment: 10 pages, 10 figures, accepted by Phys. Rev.

    The Λp\bf{\Lambda p} interaction studied via femtoscopy in p + Nb reactions at sNN=3.18 GeV\mathbf{\sqrt{s_{NN}}=3.18} ~\mathrm{\bf{GeV}}

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    We report on the first measurement of pΛp\Lambda and pppp correlations via the femtoscopy method in p+Nb reactions at sNN=3.18 GeV\mathrm{\sqrt{s_{NN}}=3.18} ~\mathrm{GeV}, studied with the High Acceptance Di-Electron Spectrometer (HADES). By comparing the experimental correlation function to model calculations, a source size for pppp pairs of r0,pp=2.02±0.01(stat)0.12+0.11(sys) fmr_{0,pp}=2.02 \pm 0.01(\mathrm{stat})^{+0.11}_{-0.12} (\mathrm{sys}) ~\mathrm{fm} and a slightly smaller value for pΛp\Lambda of r0,Λp=1.62±0.02(stat)0.08+0.19(sys) fmr_{0,\Lambda p}=1.62 \pm 0.02(\mathrm{stat})^{+0.19}_{-0.08}(\mathrm{sys}) ~\mathrm{fm} is extracted. Using the geometrical extent of the particle emitting region, determined experimentally with pppp correlations as reference together with a source function from a transport model, it is possible to study different sets of scattering parameters. The pΛp\Lambda correlation is proven sensitive to predicted scattering length values from chiral effective field theory. We demonstrate that the femtoscopy technique can be used as valid alternative to the analysis of scattering data to study the hyperon-nucleon interaction.Comment: 12 pages, 11 figure

    Partial Wave Analysis of the Reaction p(3.5GeV)+ppK+Λp(3.5 GeV)+p \to pK^+\Lambda to Search for the "ppKppK^-" Bound State

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    Employing the Bonn-Gatchina partial wave analysis framework (PWA), we have analyzed HADES data of the reaction p(3.5GeV)+ppK+Λp(3.5GeV)+p\to pK^{+}\Lambda. This reaction might contain information about the kaonic cluster "ppKppK^-" via its decay into pΛp\Lambda. Due to interference effects in our coherent description of the data, a hypothetical KNN\overline{K}NN (or, specifically "ppKppK^-") cluster signal must not necessarily show up as a pronounced feature (e.g. a peak) in an invariant mass spectra like pΛp\Lambda. Our PWA analysis includes a variety of resonant and non-resonant intermediate states and delivers a good description of our data (various angular distributions and two-hadron invariant mass spectra) without a contribution of a KNN\overline{K}NN cluster. At a confidence level of CLs_{s}=95\% such a cluster can not contribute more than 2-12\% to the total cross section with a pK+ΛpK^{+}\Lambda final state, which translates into a production cross-section between 0.7 μb\mu b and 4.2 μb\mu b, respectively. The range of the upper limit depends on the assumed cluster mass, width and production process.Comment: 7 Pages, 5 Figure
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