output
19932022
most citedNeutron star radii and crusts: uncertainties and unified equations of state

335 citations

Showing 2009Show all

6 papers · 1 filter

nucl-th2009★ 8 cited

Color symmetric superconductivity in a phenomenological QCD model

Henrik Bohr, Constança Providência, João da Providência

In this paper, we construct a theory of the NJL-type where superconductivity is present, and yet the super-conducting state remains, in the average, color symmetric. This shows tha…

hep-ph2009★ 26 cited

Comment on "Study of D(sJ) decays to D(*)K in inclusive e(+)e(-) interactions"

Eef van Beveren, George Rupp

We comment on the recent observation of the decay mode D(sJ)(*)(2860)-->D(*)K by the BABAR Collaboration [arXiv:0908.0806], and contest their peremptory conclusion that the data ex…

hep-ph2009★ 16 cited

Production of hadron pairs in electron-positron annihilation near the K(+)K(-), D-Dbar, B-Bbar and Lambda(c)(+)-Lambda(c)(-) thresholds

Eef van Beveren, George Rupp

We study the structures in cross sections and R ratios concerning electron-positron annihilation reactions, for open-strangeness, open-charm and open-beauty hadron-pair production,…

nucl-th2009★ 76 cited

The Y(4260) as a system

A. Martínez Torres, K. P. Khemchandani, D. Gamermann +1

A study of the and systems, treating them as coupled channels, has been made by solving the Faddeev equations, with the purpose of investigating the possibil…

nucl-th2009★ 11 cited

Searching for exotic states in the system

K. P. Khemchandani, A. Martínez Torres, E. Oset

We study the system in order to investigate the possibility of existence of strangeness +1 resonance(s). The formalism consists of solving the Faddeev equations with the $N…

nucl-th2009★ 52 cited

Searching for signatures around 1920 MeV of a state of three hadron nature

A. Martínez Torres, K. P. Khemchandani, Ulf-G. Meißner +1

We provide a series of arguments which support the idea that the peak seen in the reaction around 1920 MeV should correspond to the recently predicted state of $J^P=…