To bind or not to bind: The H-dibaryon in light of chiral effective field theory
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[1] S. Beane,et al. High statistics analysis using anisotropic clover lattices: IV. Volume dependence of light hadron masses , 2011 .
[2] R. Young,et al. Mass of the H dibaryon. , 2011, Physical review letters.
[3] T. Hatsuda,et al. Bound H dibaryon in flavor SU(3) limit of lattice QCD. , 2010, Physical review letters.
[4] S. Beane,et al. Evidence for a bound H dibaryon from lattice QCD. , 2010, Physical review letters.
[5] U. Meißner,et al. DN interaction from meson exchange , 2010, 1008.3794.
[6] J. Haidenbauer. Baryon-baryon interactions from Effective Field Theory , 2010 .
[7] J. Haidenbauer,et al. Predictions for the strangeness S = -3 and -4 baryon-baryon interactions in chiral effective field theory , 2009, 0907.1395.
[8] U. Meißner,et al. Strangeness S=−2 Baryon-Baryon Interaction in Chiral Effective Field Theory , 2007, 0705.3753.
[9] I. G. Park,et al. Search for the H-dibaryon resonance in 12 C (K - ,K + ΛΛX) , 2007 .
[10] Y. Suzuki,et al. Baryon–baryon interactions in the SU6 quark model and their applications to light nuclear systems , 2006, nucl-th/0607013.
[11] H. Polinder,et al. Hyperon–nucleon interactions—a chiral effective field theory approach , 2006, nucl-th/0605050.
[12] Y. Yamamoto,et al. Extended-soft-core Baryon-Baryon Model II. Hyperon-Nucleon Interaction , 2006, nucl-th/0603042.
[13] U. Meißner,et al. Jülich hyperon-nucleon model revisited , 2005, nucl-th/0506019.
[14] E. Epelbaum,et al. The Two-nucleon system at next-to-next-to-next-to-leading order , 2004, nucl-th/0405048.
[15] S. Beane,et al. Exploring Hyperons and Hypernuclei with Lattice QCD , 2003, nucl-th/0311027.
[16] I. Filikhin,et al. Faddeev calculations for the A = 5,6 Lambda Lambda hypernuclei , 2003, nucl-th/0303028.
[17] S. Beane,et al. The Quark-Mass Dependence of Two-Nucleon Systems , 2002, nucl-th/0208021.
[18] U. Meißner,et al. Nuclear forces in the chiral limit , 2002, nucl-th/0207089.
[19] S. Beane,et al. Variation of fundamental couplings and nuclear forces , 2002, hep-ph/0206113.
[20] Chung,et al. Observation of a (Lambda Lambda)He-6 double hypernucleus , 2001 .
[21] R. Timmermans,et al. Hyperon-nucleon scattering and hyperon masses in the nuclear medium , 2001, nucl-th/0109072.
[22] E. Epelbaoum,et al. Nuclear forces from chiral Lagrangians using the method of unitary transformation I : Formalism , 1998, nucl-th/9801064.
[23] C. Nakamoto,et al. Central Force of Baryon-Baryon Interactions with S=−2 in the SU6 Quark Model , 1997 .
[24] P. Ratcliffe. SU(3) breaking effects in hyperon semi-leptonic decays and the extraction of F and D , 1995, hep-ph/9509237.
[25] Savage,et al. Hyperon masses in nuclear matter. , 1995, Physical review. D, Particles and fields.
[26] Pearce Bc,et al. Observable effects of poles and shadow poles in coupled-channel systems. , 1989 .
[27] M. Oka,et al. The di-hyperon state in the quark cluster model , 1983 .
[28] C. J. Sparks,et al. Search with Synchrotron Radiation for Superheavy Elements in Giant-Halo Inclusions. , 1977 .
[29] Robert L. Jaffe,et al. Perhaps a Stable Dihyperon , 1977 .
[30] J. J. de Swart,et al. The octet model and its Clebsch-Gordan coefficients , 1963 .
[31] H. Bethe. Theory of the effective range in nuclear scattering , 1949 .