PaperPanorama

Nuclear Experiment·nucl-ex

Mon·Apr 4, 2016

4 papers0 primary·4 cross-listed·reconstructed*

  1. 01*

    Correlations and fluctuations of pions at the LHC

    Viktor V. Begun🇵🇱

    The intriguing possibility of Bose-Einstein condensation of pions at the LHC is examined with the use of higher order moments of the multiplicity distribution. The scaled variance, skewness and kurtosis are calculated for the pion system. The obtained results show that the normalized kurtosis has a significant increase for the case of the pion condensation.

    nucl-thhep-exhep-phnucl-exActa Phys.Polon.Supp.(2016)·1 citation
  2. 02*

    Experimental setup and procedure for the measurement of the 7Be(n,{\alpha}){\alpha} reaction at n_TOF

    L. Cosentino🇮🇹 · A. Musumarra🇮🇹 · M. Barbagallo🇮🇹 · A. Pappalardo🇮🇹 · N. Colonna🇮🇹 · L. Damone🇮🇹 · M. Piscopo🇮🇹 · P. Finocchiaro🇮🇹 · E. Maugeri🇨🇭 · S. Heinitz🇨🇭 · D. Schumann🇨🇭 · R. Dressler🇨🇭 and 120 other authors

    The newly built second experimental area EAR2 of the n_TOF spallation neutron source at CERN allows to perform (n, charged particles) experiments on short-lived highly radioactive targets. This paper describes a detection apparatus and the experimental procedure for the determination of the cross-section of the 7Be(n,{\alpha}) reaction, which represents one of the focal points toward the solution of the cosmological Lithium abundance problem, and whose only measurement, at thermal energy, dates back to 1963. The apparently unsurmountable experimental difficulties stemming from the huge 7Be {\gamma}-activity, along with the lack of a suitable neutron beam facility, had so far prevented further measurements. The detection system is subject to considerable radiation damage, but is capable of disentangling the rare reaction signals from the very high background. This newly developed setup could likely be useful also to study other challenging reactions requiring the detectors to be installed directly in the neutron beam.

    physics.ins-dethep-exnucl-exNucl.Instrum.Meth.A(2016)·23 citations
  3. 03*

    Effect of particle fluctuation on isoscaling and isobaric yield ratio of nuclear multifragmentation

    S. Mallik🇮🇳 · G. Chaudhuri🇮🇳

    Isoscaling and isobaric yield ratio parameters are compared from canonical and grand canonical ensembles when applied to multifragmentation of finite nuclei. Source dependence of isoscaling parameters and source and isospin dependence of isobaric yield ratio parameters are examined in the framework of the canonical and the grand canonical models. It is found that as the nucleus fragments more, results from both the ensembles converge and observables calculated from the canonical ensemble coincide more with those obtained from the formulae derived using the grand canonical ensemble.

    nucl-thnucl-exPLB(2013)·17 citations
  4. 04*

    Local measurement of error field using naturally rotating tearing mode dynamics in EXTRAP T2R

    R.M. Sweeney · L. Frassinetti · P. Brunsell · R. Fridström · F.A. Volpe

    An error field (EF) detection technique using the amplitude modulation of a naturally rotating tearing mode (TM) is developed and validated in the EXTRAP T2R reversed field pinch. The technique was used to identify intrinsic EFs of , where and are the poloidal and toroidal mode numbers. The effect of the EF and of a resonant magnetic perturbation (RMP) on the TM, in particular on amplitude modulation, is modeled with a first-order solution of the Modified Rutherford Equation. In the experiment, the TM amplitude is measured as a function of the toroidal angle as the TM rotates rapidly in the presence of an unknown EF and a known, deliberately applied RMP. The RMP amplitude is fixed while the toroidal phase is varied from one discharge to the other, completing a full toroidal scan. Using three such scans with different RMP amplitudes, the EF amplitude and phase are inferred from the phases at which the TM amplitude maximizes. The estimated EF amplitude is consistent with other estimates (e.g. based on the best EF-cancelling RMP, resulting in the fastest TM rotation). A passive variant of this technique is also presented, where no RMPs are applied, and the EF phase is deduced.

    physics.plasm-phnucl-exPlasma Phys.Control.Fusion(2016)·0 citations

* Reconstructed cohort: no mailing for this day survives in the archive. Papers are grouped by their submission times and arXiv's announcement cut-off, assuming announcement without delay; positions follow identifier order. Validated at ~91% exact-day agreement against the archived era.