a r X i v : h e p - p h / 9 8 0 5 3 4 7 v 2 9 N o v 1 9 9 8 OntheD ∗+ s →D + s π 0 decayintheEffectivequark modelwithchiralU(3)×U(3)symmetry A.N.Ivanov ∗† TheoryDivision,CERN,CH–1211Geneva23,Switzerland Abstract ThepartialwidthofthedecayD ∗+...
Proto-strange quark stars from density-dependent quark mass model Download PDF Adamu Issifu ORCID: orcid.org/0000-0002-2843-835X1, Franciele M. da Silva ORCID: orcid.org/0000-0003-2568-29012 & Débora P. Menezes ORCID: orcid.org/0000-0003-0730-66892 672 Accesses Explore all ...
baryons, resonance/widths of, quark model estimates of low-energy matrix elements of currents for, (tWe have now had a glimpse of the elementary particle "zoo". While it contains only a few (six) leptons e , v e , , v , 蟿, v 蟿 , the zoo includes over 200 strongly interacting...
Analysis of crack propagation in asphalt concrete using a cohesive crack model 热度: a r X i v : 0 8 0 8 . 1 6 0 8 v 1 [ h e p - p h ] 1 2 A u g 2 0 0 8 charmedbaryoninaDiquarkmodel Q.W.Wang ∗ InstituteofModernPhysics, ...
≈ M). In the model, the scale M is identified with the constituent quark mass. This is the only free parameter in our analysis and most matrix elements are a sensitive function of it. What are the allowed values for this parameter?
In addition to this, we have also compared our results for the PDF e(x) with the recent CLAS collaboration results. Transverse momentum dependent parton distributions of proton; T-even sub-leading twist TMDs; light-front quark-diquark model....
Quark-meson coupling model at finite temperature 下载积分: 1993 内容提示: ELSEVIER 28 September 1995 Physics Letters B 358 (1995) 179-183 PHYSICS LETTERS 6 Quark-meson coupling model at finite temperature * H.Q. Song O,c, R-K. Su w&c a CCAST (World Laboratory), P.O. Box 8730, ...
We utilize the Quark-Novae (QN) model for fast radio bursts (FRBs) to evaluate its performance in reproducing the distribution and statistical properties of key observations. These include frequency, duration, fluence, dispersion measure (DM), and other relevant features such as repetition, periodic...
View PDF Cited by (10) Spin-orbit force of hyperon-nucleon interaction in the chiral SU (3) quark model 1998, Nuclear Physics A The spin-orbit (LS) force of the hyperon-nucleon interaction is studied in the chiral(3) quark model. The symmetric LS terms from the one gluon exchange (OGE...
The "Schmidt lines" for nuclear magnetic moments are calculated in a quark shell model. In the pairing scheme proposed by Petry et al., the single-nucleon magnetic moment is simply related to the single quark value. The isoscalar part is essentially the same as that of the conventional Schmi...