Abstract:The Poincaré-covariant Faddeev equation and its solution in rainbow-ladder truncation, i.e., with a generalized gluon exchange as irreducible two-particle-interaction, is presented. The covariant decomposition of baryon amplitudes, representing relativistic three-quark states, is discussed and explicitly given for the ∆-baryon. The calculated ∆ mass compares favourably with the experimental one.
Light Cone 2010: Relativistic Hadronic and Particle Physics
“…They are expressed as tensor products of flavor, color and spin parts which describe a baryon in terms of its constituent quarks. For spin-3 /2 baryons the spin part is itself a mixed tensor with four Dirac indices and one Lorentz index [26][27][28]. Substituting (10) in (2) or in (3), and keeping only the singular terms, we arrive at the Bethe-Salpeter equation for the three-quark bound state…”
Section: Baryon Bethe-salpeter Equation and Coupling To An Externmentioning
The electromagnetic form factors of the ∆ and Ω baryons are calculated in the framework of Poincaré-covariant bound-state equations. The quark-quark interaction is truncated to a single dressed-gluon exchange where for the dressings we use two different models and compare the results. The calculation predicts an oblate shape for the electric charge distribution and a prolate shape for the magnetic dipole distribution. We also identify the necessity of including pion-cloud corrections at low photon-momentum transfer.
“…They are expressed as tensor products of flavor, color and spin parts which describe a baryon in terms of its constituent quarks. For spin-3 /2 baryons the spin part is itself a mixed tensor with four Dirac indices and one Lorentz index [26][27][28]. Substituting (10) in (2) or in (3), and keeping only the singular terms, we arrive at the Bethe-Salpeter equation for the three-quark bound state…”
Section: Baryon Bethe-salpeter Equation and Coupling To An Externmentioning
The electromagnetic form factors of the ∆ and Ω baryons are calculated in the framework of Poincaré-covariant bound-state equations. The quark-quark interaction is truncated to a single dressed-gluon exchange where for the dressings we use two different models and compare the results. The calculation predicts an oblate shape for the electric charge distribution and a prolate shape for the magnetic dipole distribution. We also identify the necessity of including pion-cloud corrections at low photon-momentum transfer.
“…For the sake of physical interpretation it is convenient to perform a partial-wave decomposition and classify the basis elements with respect to their quark-spin and relative orbital angular momentum content in the baryon's rest frame. The explicit derivation of such a basis is quite involved [28] and presented in Appendix A. The most significant aspects of this construction are:…”
Section: Faddeev Equation and Rainbow-ladder Truncationmentioning
We present the solution of the Poincaré-covariant Faddeev equation for the ∆(1232) and Ω(1672) baryons. The covariant structure of the corresponding baryon amplitudes and their decomposition in terms of internal spin and orbital angular momentum is explicitly derived. The interaction kernel is truncated to a rainbow-ladder dressed-gluon exchange such that chiral symmetry and its dynamical breaking are correctly implemented. The resulting physical masses agree reasonably with experiment and their evolution with the pion mass compares favorably with lattice calculations. Evidence for the non-sphericity of the ∆−resonance is discussed as well.
“…To this end one should note that the ghost-gluon vertex becomes bare in the limit of vanishing ghost momentum due to the transversality of the gluon propagator. This has been noticed already 40 years ago [10] and 2 We thank Jan Pawlowski for discussing with us his work in preparation and Lorenz von Smekal for a compilation of the data (see also his talk under http://www.thphys.uni-heidelberg.de/∼smp/view/Main/Delta10Programme).…”
Section: Infrared Structure Of Landau Gauge Yang-mills Theorymentioning
confidence: 58%
“…However, in order to determine them in cona e-mail: reinhard.alkofer@uni-graz.at b e-mail: mario.mitter@uni-graz.at c e-mail: bernd-jochen.schaefer@uni-graz.at 1 A recent example of such calculations can be found in [1,2] and references therein. tinuum quantum field theory, in principle, an infinite hierarchy of coupled complicated equations has to be solved.…”
Section: Functional Approaches To Qcdmentioning
confidence: 99%
“…[9] where DSE and FRG methods have been combined. 2 How has this success of functional methods been achieved? To this end one should note that the ghost-gluon vertex becomes bare in the limit of vanishing ghost momentum due to the transversality of the gluon propagator.…”
Section: Infrared Structure Of Landau Gauge Yang-mills Theorymentioning
Abstract. After presenting a brief summary of functional approaches to QCD at vanishing temperatures and densities the application of QCD Green's functions at non-vanishing temperature and vanishing density is discussed. It is pointed out in which way the infrared behavior of the gluon propagator reflects the (de-)confinement transition. Numerical results for the quark propagator are given thereby verifying the relation between (de-)-confinement and dynamical chiral symmetry breaking (restoration). Last but not least some results of DysonSchwinger equations for the color-superconducting phase at large densities are shown.
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