PaperPanorama

Nuclear Theory·nucl-th

Tuesday·October 20, 2015

16 papers10 primary·6 cross-listed

  1. 11

    X-ray Burst Oscillations: From Flame Spreading to the Cooling Wake

    Simin Mahmoodifar (NASA/GSFC) · Tod Strohmayer (NASA/GSFC)

    Type I X-ray bursts are thermonuclear flashes observed from the surfaces of accreting neutron stars (NSs) in Low Mass X-ray Binaries. Oscillations have been observed during the rise and/or decay of some of these X-ray bursts. Those seen during the rise can be well explained by a spreading hot spot model, but large amplitude oscillations in the decay phase remain mysterious because of the absence of a clear-cut source of asymmetry. To date there have not been any quantitative studies that consistently track the oscillation amplitude both during the rise and decay (cooling tail) of bursts. Here we compute the light curves and amplitudes of oscillations in X-ray burst models that realistically account for both flame spreading and subsequent cooling. We present results for several such "cooling wake" models, a "canonical" cooling model where each patch on the NS surface heats and cools identically, or with a latitude-dependent cooling timescale set by the local effective gravity, and an "asymmetric" model where parts of the star cool at significantly different rates. We show that while the canonical cooling models can generate oscillations in the tails of bursts, they cannot easily produce the highest observed modulation amplitudes. Alternatively, a simple phenomenological model with asymmetric cooling can achieve higher amplitudes consistent with the observations.

    astro-ph.HEastro-ph.SRnucl-thApJ(2016)·28 citations
  2. 12

    Schwinger mechanism revisited

    Francois Gelis🇫🇷 · Naoto Tanji🇩🇪

    In this article, we review recent theoretical works on the Schwingermechanism of particle production in external electrical fields. Although the non-perturbative Schwinger mechanism is at the center of this discussion, many of the approaches that we discuss can cope with general time and space dependent fields, and therefore also capture the perturbative contributions to particle production.

    hep-phhep-thnucl-thPPNP(2016)·194 citations
  3. 13

    The calorimetric spectrum of the electron-capture decay of Ho. A preliminary analysis of the preliminary data

    A. De Rújula🇪🇸 · M. Lusignoli🇮🇹

    It is in principle possible to measure directly the electron neutrino mass (or masses and mixing angles) in weak electron-capture decays. The optimal nuclide in this respect is Ho. The favoured experimental technique, currently pursued in various experiments (ECHo, HOLMES and NuMECS) is "calorimetric". The calorimetric energy spectrum is a sum over the unstable vacant orbitals, or "holes", left by the electrons weakly captured by the nucleus. We discuss the current progress in this field and analize the preliminary data. Our conclusion is that, as pointed out by Robertson, the contribution of two-hole states is not negligible. But --in strong contradistinction with the tacit conclusion of previous comparisons of theory and observations-- we find a quite satisfactory agreement. A crucial point is that, in the creation of secondary holes, electron shakeoff and not only electron shakeup must be taken into account.

    hep-phnucl-thphysics.atom-ph14 citations
  4. 14

    The pion-cloud contribution to the electromagnetic nucleon structure

    D. Kupelwieser🇦🇹 · W. Schweiger🇦🇹

    The present contribution continues and extends foregoing work on the calculation of electroweak form factors of hadrons using the point-form of relativistic quantum mechanics. Here we are particularly interested in studying pionic effects on the electromagnetic structure of the nucleon. To this aim we employ a hybrid constituent-quark model that comprises, in addition to the valence component, also a + non-valence component. With a simple wave function for the component we get reasonable results for the nucleon form factors. In accordance with other authors we find that the pionic effect is significant only below ~GeV.

    hep-phnucl-thBled Workshops Phys.(2015)·0 citations
  5. 15

    Two, three, many body systems involving mesons. Multimeson condensates

    E. Oset🇪🇸 · M. Bayar🇹🇷 · A. Dote🇯🇵 · T. Hyodo🇯🇵 · P. K. Khemchandani🇧🇷 · W. H. Liang🇨🇳 · A. Martinez Torres🇧🇷 · M. Oka🇯🇵 · L.Roca🇪🇸 · T. Uchino🇪🇸 · C.W. Xiao🇩🇪

    In this talk we review results from studies with unconventional many hadron systems containing mesons: systems with two mesons and one baryon, three mesons, some novel systems with two baryons and one meson, and finally systems with many vector mesons, up to six, with their spins aligned forming states of increasing spin. We show that in many cases one has experimental counterparts for the states found, while in some other cases they remain as predictions, which we suggest to be searched in BESIII, Belle, LHCb, FAIR and other facilities.

    hep-phnucl-thActa Phys.Polon.B(2016)·3 citations
  6. 16

    Quark deconfinement and the duration of short Gamma Ray Bursts

    Alessandro Drago (1) · Andrea Lavagno (2) · Brian Metzger (3) · Giuseppe Pagliara (1) ((1) Ferrara U. & INFN, Ferrara, (2) Turin Polytechnic & INFN, Turin, (3) Columbia U., Astron. Astrophys.)

    We propose a model for short duration gamma-ray bursts (sGRBs) based on the formation of a quark star after the merger of two neutron stars. We assume that the sGRB central engine is a proto-magnetar, which has been previously invoked to explain the plateau-like X-ray emission observed following both long and short GRBs. Here, we show that: i) a few milliseconds after the merger it is possible to form a stable and massive star made in part of quarks; ii) during the early cooling phase of the incompletely formed quark star, the flux of baryons ablated from the surface by neutrinos is large and it does not allow the outflow to achieve a bulk Lorentz factor high enough to produce a GRB; iii) after the quark burning front reaches the stellar surface, baryon ablation ceases and the jet becomes too baryon poor to produce a GRB; iv) however, between these two phases a GRB can be produced over the finite timescale required for the baryon pollution to cease; a characteristic timescale of the order of s naturally results from the time the conversion front needs to cover the distance between the rotational pole and the latitude of the last closed magnetic field line; v) we predict a correlation between the luminosity of the sGRB and its duration, consistent with the data; vi) our model also predicts a delay of the order of ten seconds between the time of the merger event and the sGRB, allowing for the possibility of precursor emission and implying that the jet will encounter the dense cocoon formed immediately after the merger.

    astro-ph.HEhep-phnucl-thPRD(2016)·34 citations

Affiliations

first authorsco-authorsvia INSPIRE