PaperPanorama

Nuclear Theory·nucl-th

Tuesday·December 11, 2018

16 papers11 primary·5 cross-listed

  1. 12

    A holographic description of heavy-flavoured baryonic matter decay involving glueball

    Si-wen Li🇨🇳

    We holographically investigate the decay of heavy-flavoured baryonic hadron involving glueball by using the Witten-Sakai-Sugimoto model. Since baryon in this model is recognized as the D4-brane wrapped on and the glueball field is identified as the bulk gravitational fluctuations, the interaction of the bulk graviton and the baryon brane could be naturally interpreted as glueball-baryon interaction through the holography which is nothing but the close-open string interaction in string theory. In order to take account into the heavy flavour, an extra pair of heavy-flavoured branes separated from the other flavour branes with a heavy-light open string is embedded into the bulk. Due to the finite separation of the flavour branes, the heavy-light string creates massive multiplets which could be identified as the heavy-light meson fields in this model. As the baryon brane on the other hand could be equivalently described by the instanton configuration on the flavour brane, we solve the equations of motion for the heavy-light fields with the Belavin-Polyakov-Schwarz-Tyupkin (BPST) instanton solution for the flavoured gauge fields. Then with the solutions, we evaluate the soliton mass by deriving the flavoured onshell action in strongly coupling limit and heavy quark limit. After the collectivization and quantization, the quantum mechanical system for glueball and heavy-flavoured baryon is obtained in which the effective Hamiltonian is time-dependent. Finally we use the standard technique for the time-dependent quantum mechanical system to analyze the decay of heavy-flavoured baryon involving glueball and we find one of the decay process might correspond to the decay of baryonic B-meson involving the glueball candidate . This work is a holographic approach to study the decay of heavy-flavoured hadron in nuclear physics.

    hep-thnucl-thPRD(2019)·6 citations
  2. 13

    Exotic baryons from meson-baryon scattering

    Gloria Montana🇪🇸 · Angels Ramos🇪🇸 · Albert Feijoo🇨🇿

    A meson-baryon interaction in the charm , strangeness and isospin sector is built from a t-channel vector meson exchange model employing effective Lagrangians. The implementation of coupled-channel unitarization in the s-wave scattering amplitudes gives rise to two structures that have similar masses and widths to those of the and states recently observed by the LHCb collaboration. A meson-baryon molecular interpretation of these resonances would assign their spin-parity to be .

    hep-phnucl-thJ.Phys.Conf.Ser.(2019)·1 citation
  3. 14

    The molecular nature of some states

    Gloria Montana🇪🇸 · Angels Ramos🇪🇸 · Albert Feijoo🇨🇿

    A vector meson exchange model based on effective Lagrangians is used to build the meson--baryon interaction in the charm , strangeness and isospin sector. The s-wave scattering amplitudes resulting from the unitarization in coupled-channels show two resonances with masses and widths that are in very good agreement with those of the experimental and states observed by the LHCb collaboration. The interpretation of these resonances as pseudoscalar meson--baryon molecules would mean the assignment to their spin--parity.

    hep-phnucl-thSpringer Proc.Phys.(2020)·1 citation
  4. 15

    Quasi equilibrium state of expanding quantum fields and two-pion Bose-Einstein correlations in collisions at the LHC

    S.V. Akkelin🇺🇦

    We argue that the two-particle momentum correlation functions of high-multiplicity collisions at the LHC provide a signal for a ground state structure of a quasi equilibrium state of the longitudinally boost-invariant expanding quantum field which lies in the future light cone of a collision. The physical picture is that pions are produced by the expanding quantum emitter with two different scales approximately attributed to the expanding ideal gas in local equilibrium state and ground-state condensate. Specifically, we show that the effect of suppressing the two-particle Bose-Einstein momentum correlation functions increases with increasing transverse momentum of a like-sign pion pair due to different momentum-dependence of the corresponding particle emission regions.

    hep-phhep-exnucl-exnucl-thEPJA(2019)·7 citations
  5. 16

    Computing the gluon Sivers function at small-

    Xiaojun Yao🇺🇸 · Yoshikazu Hagiwara🇯🇵 · Yoshitaka Hatta🇺🇸

    We compute the gluon Sivers function of the transversely polarized nucleon at small- by exploiting the known connection between the dipole gluon Sivers function and the Odderon. We numerically solve the evolution equation for the Odderon both in the linear and nonlinear regimes. While we find that the and dependences of the Sivers function do not factorize as a result of the quantum evolution, factorization breaking is not numerically significant, and is much milder than what one expects in the case of unpolarized TMDs. We also point out the possibility that, due to the presence of a node in the Sivers function, single spin asymmetry for open charm production in semi-inclusive deep inelastic scattering flips signs as the transverse momentum of D-mesons is varied. This can be tested at the future Electron-Ion Collider.

    hep-phhep-exnucl-thPLB(2019)·34 citations

Affiliations

first authorsco-authorsvia INSPIRE