PaperPanorama

Nuclear Theory·nucl-th

Thursday·February 28, 2019

9 papers3 primary·6 cross-listed

  1. 01

    and triton clustering in Cl

    Yasutaka Taniguchi

    Coupling of cluster and deformed structures are important for dynamics of nuclear structure. Threshold energy has been discussed to explain cluster structures coupling to deformed states but relation between threshold energy and excitation energy has open problems. Negative-parity superdeformed (SD) states were observed by a -spectroscopy experiment in Cl but its detailed structure is unclear. By analyzing coupling of cluster structures in deformed states and high-lying cluster states in Cl, cluster structures coupling to deformed states and excitation energy of high-lying cluster states are investigated. The antisymmetrized molecular dynamics (AMD) and the generator coordinate method (GCM) are used. An AMD wave function is a Slater determinant of Gaussian wave packets. By energy variational calculations with constraints on deformation and clustering, wave functions of deformed structures and - and -cluster structures are obtained. Adopting those wave functions as GCM basis, wave functions of ground and excited states are calculated. Various deformed bands are obtained and predicted. A deformed band, which corresponds to the observed SD band, dominates deformed structure and compact - and -cluster structure components. Particle-hole configurations of the dominant components with deformed and cluster structures are similar. In high-lying states, almost pure - and -cluster states are obtained in negative-parity states, and excitation energies of the -cluster states are higher than those of -cluster states. In conclusions, particle-hole configurations of cluster structure with small intercluster distance are important for coupling to low-energy deformed states. Threshold energies reflect to excitation energies of high-lying almost pure cluster states.

    nucl-thnucl-exPRC(2019)·4 citations
  2. 02

    Hadron Formation From Quark-Gluon Plasma Using Lattice QCD At Finite Temperature

    Gouranga C Nayak

    Recently we have reported the correct formulation of the lattice QCD method at the zero temperature to study the hadron formation from the quarks and gluons by incorporating the non-zero boundary surface term in QCD which arises due to the confinement of quarks and gluons inside the finite size hadron. In this paper we extend this to the finite temperature QCD and present the correct formulation of the lattice QCD method at the finite temperature to study the hadron formation from the quark-gluon plasma.

    nucl-thhep-ph7 citations
  3. 03

    Ab initio calculations of 5H resonant states

    R. Lazauskas🇫🇷 · E. Hiyama🇯🇵 · J. Carbonell🇫🇷

    By solving the 5-body Faddeev-Yakubovsky equations in configuration space with realistic nuclear Hamiltonians we have studied the resonant states of H isotope. Two different methods, allowing to bypass the exponentially diverging boundary conditions, have been employed providing consistent results. The existence of H broad J=1/2,3/2,5/2 states as S-matrix poles has been confirmed and compared with the, also calculated, resonant states in H isotope. We have established that the positions of these resonances only mildly depend on the nuclear interaction model.

    nucl-thnucl-exphysics.comp-phPLB(2019)·25 citations

Affiliations

first authorsco-authorsvia INSPIRE