417 research outputs found

    Branching Ratios for the Decay of d(2380)d^*(2380)

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    Based on measurements the branching ratios for the decay of the recently discovered dibaryon resonance d(2380)d^*(2380) into two-pion production channels and into the npnp channel are evaluated. Possibilities for a decay into the isoscalar single-pion channel are discussed. Finally also the electromagnetic decay of d(2380)d^*(2380) is considered

    Examination of the Nature of the ABC Effect

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    Recently it has been shown by exclusive and kinematically complete experiments that the appearance of a narrow resonance structure in double-pionic fusion reactions is strictly correlated with the appearance of the so-called ABC effect, which denotes a pronounced low-mass enhancement in the ππ\pi\pi-invariant mass spectrum. Whereas the resonance structure got its explanation by the d(2380)d^*(2380) dibaryonic resonance, a satisfactory explanation for the ABC effect is still pending. In this paper we discuss possible explanations of the ABC effect and their consequences for the internal structure of the dd^* dibaryon

    Novel Six-Quark Hidden-Color Dibaryon States in QCD

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    The recent observation of a hadronic resonance dd^* in the proton-neutron system with isospin I=0I = 0 and spin-parity JP=3+J^P = 3^+ raises the possibility of producing other novel six-quark dibaryon configurations allowed by QCD. A dramatic example of an exotic six-quark color-singlet system is the charge Q=+4Q=+4, isospin I=3, Iz=+3I^z=+3 uuuuuu>|uuuuuu> state which couples strongly to Δ++\Delta^{++} + Δ++.\Delta^{++} . The width and decay properties of such six-quark resonances could be regarded as manifestations of "hidden-color" six-quark configurations, a first-principle prediction of QCD -- SU(3)-color gauge theory for the deuteron distribution amplitude. Other implications and possible future experiments are discussed

    On Sequential Single-Pion Production in Double-Pionic Fusion

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    Recently a two-step process has been proposed for the double-pionic fusion to deuterium pn(I=0)dπ+πpn (I=0) \to d\pi^+\pi^-, which is solely based on total cross section data for the two sequential single-pion production steps pn(I=0)ppπpn (I=0)\to pp\pi^- followed by ppdπ+pp \to d\pi^+. Though this sequential process was aimed to explain the dibaryon resonance d(2380)d^*(2380) peak in double-pionic fusion, we demonstrate that this is not the case. It rather fits to a possible broad bump at 2.31 GeV in the energy dependence of the pndπ0π0pn \to d\pi^0\pi^0 reaction, which was recently interpreted as a consequence of dibaryonic excitations in isoscalar single-pion production

    A new possibility for light-quark Dark Matter

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    Despite many decades of study the physical origin of "dark matter" in the Universe remains elusive. In this letter we calculate the properties of a completely new dark matter candidate - Bose-Einstein condensates formed from a recently discovered bosonic particle in the light-quark sector, the d(2380)\mathbf{ d^*(2380)} hexaquark. In this first study, we show stable d(2380)\mathbf{ d^*(2380)} Bose-Einstein condensates could form in the primordial early universe, with a production rate sufficiently large that they are a plausible new candidate for dark matter. Some possible astronomical signatures of such dark matter are also presented

    Strange Hadron Spectroscopy with a Secondary KL Beam at GlueX

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    We propose to create a secondary beam of neutral kaons in Hall D at Jefferson Lab to be used with the GlueX experimental setup for strange hadron spectroscopy. A flux on the order of 3 x 10^4 KL/s will allow a broad range of measurements to be made by improving the statistics of previous data obtained on hydrogen targets by three orders of magnitude. Use of a deuteron target will provide first measurements on the neutron which is {\it terra incognita}. The experiment will measure both differential cross sections and self-analyzed polarizations of the produced {\Lambda}, {\Sigma}, {\Xi}, and {\Omega} hyperons using the GlueX detector at the Jefferson Lab Hall D. The measurements will span c.m. cos{\theta} from -0.95 to 0.95 in the c.m. range above W = 1490 MeV and up to 3500 MeV. These new GlueX data will greatly constrain partial-wave analyses and reduce model-dependent uncertainties in the extraction of strange resonance properties (including pole positions), and provide a new benchmark for comparisons with QCD-inspired models and lattice QCD calculations. The proposed facility will also have an impact in the strange meson sector by providing measurements of the final-state K{\pi} system from threshold up to 2 GeV invariant mass to establish and improve on the pole positions and widths of all K*(K{\pi}) P-wave states as well as for the S-wave scalar meson {\kappa}(800).Comment: 97 pages, 63 figures, Proposal for JLab PAC45, PR12-17-001; v3 missed citation in Sec 9 (pg 22

    The d*(2380) in neutron stars - a new degree of freedom?

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    Elucidating the appropriate microscopic degrees of freedom within neutron stars remains an open question which impacts nuclear physics, particle physics and astrophysics. The recent discovery of the first non-trivial dibaryon, the d∗(2380), provides a new candidate for an exotic degree of freedom in the nuclear equation of state at high matter densities. In this paper a first calculation of the role of the d∗(2380) in neutron stars is performed, based on a relativistic mean field description of the nucleonic degrees of freedom supplemented by a free boson gas of d∗(2380). The calculations indicate that the d∗(2380) would appear at densities around three times normal nuclear matter saturation density, influencing the upper mass limit for a stable neutron star and the neutron and proton fractions. New possibilities for neutron star cooling mechanisms arising from the d∗(2380)are also predicted
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