Hadron Nuclear Physics 2015

from Wednesday, 8 July 2015 (08:00) to Friday, 1 January 2016 (18:00)
Dusit Thani Krabi Beach Resort

        : Sessions
    /     : Talks
        : Breaks
8 Jul 2015
9 Jul 2015
10 Jul 2015
11 Jul 2015
AM
10:00
Session I (until 12:00) (Andaman Grande)
10:00 The transversity of the pion and the nucleon   ()
10:30 Structure of peaks in the initial single chiral particle emission mechanism   ()
11:00 The problems in nucleon structure study   ()
11:30 Charmed baryons and their interactions   ()
08:30 Net-baryon and net-proton kurtosis from chiral fluid dynamics   ()
08:30
Session V (until 10:00) (Andaman Grande)
09:00 Theoretical study of the nuclear structure by the parity-violating electron scattering   ()
09:30 Xi-Nucleus interaction from the first evidence of Xi$^{-14}$ N system   ()
10:00 --- Coffee break ---
10:20 Nucleons and Nucleonic Systems   ()
10:20
Session VI (until 11:50) (Andaman Grande)
10:50 Systematic study of 𝛼 decay properties for long-lived nuclei   ()
11:20 Azimuthal Emission of K$^+$ in NI + NI Collisions at Energy 1.91 A GeV   ()
11:50 --- Lunch ---
08:00 --- Social Trip ---
08:30 Four-quark states and QCD sum rules   ()
08:30
Session IX (until 10:00) (Andaman Grande)
09:00 Ξ(1690) as a molecular state $𝐾\bar Sigma$   ()
09:30 Baryonic spectroscopy at BESIII   ()
10:00 --- Coffee break ---
10:20
Session X (until 11:50) (Andaman Grande)
10:20 The High Altitude Water Cherenkov (HAWC) Gamma Ray Observatory at Mexico   ()
10:50 Heavy exotic baryon resonance Λ$_𝐶$ (2940)$^+$ in a molecule scenario   ()
11:20 Comparison of sea-quark contributions to electromagnetic and axial form factors   ()
11:50 --- Lunch ---
PM
12:00 --- Lunch ---
13:20 Overview of Physics Results from the CMS Experiment   ()
13:20
Session II (until 15:20) (Andaman Grande)
13:50 Recent results from BESIII   ()
14:20 Large $N_c$ QCD and the chiral extrapolation of baryon masses   ()
14:50 Theoretical Interpretation of J-PARC E27 Data with a $\Lambda_c$ (1405) $−𝑝$ Model   ()
15:20 --- Coffee Break ---
15:40 Hadron Structure in the Covariant Confined Quark Model   ()
15:40
Session III (until 17:10) (Andaman Grande)
16:10 What can we learn about Hadron Spectroscopy with Antiproton Annihilation?   ()
16:40 Further study of the NΩ dibaryon within constituent quark models   ()
17:10 --- Break ---
17:30 Production of Charged Particles and $K^- p$ ($K^+ p$) Bound States in $pp$ Collisions at Energy 900 GeV   ()
17:30
Session IV (until 18:30) ()
17:45 Predictions of Kaon and Proton Productions in $pp$ Collisions at 7 TeV   ()
18:00 Study of Elliptic Flow in Heavy Ion Collisions   ()
18:15 Simulation of hypertriton productions in Pb-Pb collisions at high energy using PACIAE model   ()
13:10
Session VII (until 15:10) (Andaman Grande)
13:10 The quark model study of the dibaryon d$^∗$   ()
13:40 Strangeness configurations of 𝜙 meson production in $𝑝\bar 𝑝$ annihilation   ()
14:10 Analysis of heavy hyperhydrogen $_Λ ^6 H$   ()
14:40 Two topics on Charmonium-like states   ()
15:10 --- Coffee break ---
15:30 Parity violation of nucleon-nucleon potential in the 1/$N_c$ expansion   ()
15:30
Session VIII (until 17:30) (Andaman Grande)
16:00 NNLO QCD corrections to quarkonium production and decays: Does NRQCD work well for charmonium?   ()
16:30 Weak 𝐾→𝜋 generalized from factors and transverse quark-spin density from the instanton vacuum   ()
17:00 Dynamical Formation Of Center Domains in Quark-Gluon Plasma   ()
15:30 --- Visit Krabi night market ---
13:10
Session XI (until 14:40) (Andaman Grande)
13:10 The Cosmological Evolution at the Deconfinement Transition   ()
13:40 Automated scanning systems to search for double strangeness nuclei in nuclear emulsion   ()
14:10 The properties of sea quark in baryons   ()
14:40 --- Coffee break ---
15:00 Estimation of the Mass of ground state pentaquarks   ()
15:00
Session XII (until 16:30) (Andaman Grande)
15:30 The specific charged hadron multiplicity in $e^− p + p$ and $e^− + D$ semi-inclusive deep-inelastic scattering in the PYTHIA and PACIAE models   ()
16:00 Some insights into the charmonium-like $XYZ$ states   ()