Chiral Nuclear Dynamics II : From Quarks to Nuclei to Compact Stars
Mannque. Rho
Bok Engelsk 2008 · Electronic books.
| Annen tittel | |
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| Medvirkende | Nowak, Maciej A (Contributor)
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| Utgitt | Singapore : : World Scientific Publishing Company, , 2008.
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| Omfang | 1 online resource (372 p.)
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| Utgave | 2nd ed.
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| Opplysninger | Description based upon print version of record.. - Preface; Contents; 1. Introduction; 2. Multi-Facets Of QCD In Matter; 3. Cheshire Cat Phenomenon; 3.1 Motivation; 3.2 Chiral Bag Picture; 3.2.1 Cheshire Cat as a gauge artifact; 3.2.2 Baryon charge and the exact Cheshire Cat phenomenon; 3.3 Cheshire Cat Principle in Nature; 3.3.1 Flavor singlet axial charge; 3.3.2 "Charge-spin separation" for Cheshire Cat phenomena; 3.4 CCP andMulti-Facets of CBM; 3.4.1 Chiral quark-solitonmodel; 3.4.2 Cloudy bagmodel; 3.4.3 Skyrmion model; 3.4.4 Heavy baryon chiral perturbation approach; 4. Effective Field Theory For Nuclei. - 4.1 Role of Effective Field Theory in Nuclear Physics4.2 Standard Nuclear Physics Approach and EFT; 4.2.1 The power of SNPA; 4.2.2 The power of EFT; 4.3 Chiral Lagrangians; 4.3.1 Relevant scales and degrees of freedom; 4.3.2 Vector mesons and baryons; 4.3.3 Baryon fields; 4.4 Pionless EFT (π/EFT); 4.5 More Effective EFT; 4.5.1 Weinberg's counting rule; 4.5.2 Strategy of MEEFT; 4.5.3 The chiral filter; 4.5.4 Working of MEEFT; 4.5.4.1 What does the chiral filter say?; 4.5.4.2 Sketch of the calculational procedure; 4.5.4.3 How the cutoff enters; 4.5.4.4 Physicalmeaning of Λ. - 4.5.5 Predictions of MEEFT4.5.5.1 Thermal np capture; 4.5.5.2 Polarization observables in np capture; 4.5.5.3 Deuteron form factors; 4.5.5.4 Predicting the solar neutrino processes; 4.5.5.5 Magnetic moments of the trinucleons; 4.5.5.6 Further implications of the ˆ dR term; 4.6 EFT "Completion" of SNPA; 4.7 EFT for Heavy Nuclei and Nuclear Matter; 5. Hidden Local Symmetry For Hadrons; 5.1 Emergence of Local Flavor Symmetry; 5.2 Tower of Hidden Gauge Fields; 5.2.1 Simplest open moose diagram; 5.2.2 General open moose; 5.2.3 Spectrum of the open moose; 5.2.4 Dimensional deconstruction. - 5.3 AdS/QCD and hQCD5.3.1 Objectives; 5.3.2 Bottom-up approach; 5.3.3 Top-down approach; 5.3.4 Vector dominance; 5.3.5 Instanton baryons; 5.4 HLSK=1 fromHolographicDual QCD; 5.4.1 Going from 5D to 4D; 5.4.2 Doing quantum corrections; 5.5 Hidden Local Symmetry and the "Vector Manifestation"; 5.5.1 HLSK=1: Hidden local symmetry `a la Bando et al.; 5.5.2 HLSK=1 with loop corrections; 5.5.2.1 Wilsonian matching; 5.5.2.2 Vector manifestation (VM); 5.5.2.3 "Dropping mass" and local gauge symmetry; 5.5.2.4 Scaling near the VM fixed point; 5.6 Phenomenology with HLSK=. - 5.6.1 Doing chiral perturbation theory5.6.1.1 Chiral counting for the vector mesons in χPT; 5.6.1.2 Loop calculations; 5.6.1.3 Comparison with experiments; 5.6.2 Weinberg sum rules; 5.6.3 Pionmass difference; 5.6.4 Perturbing from the VMpoint; 5.6.4.1 Heavy quark symmetry; 5.6.4.2 Constructing effective Lagrangians; 5.6.4.3 The fixed point Lagrangian; 5.6.4.4 Effects of spontaneous chiral symmetry breaking; 5.6.4.5 Lagrangian in parity eigenfields; 5.6.4.6 Calculation at the matching point; 5.6.4.7 Quantum correction; 5.6.4.8 Mass splitting; 5.7 HLS with ρ and a1: HLSK=. - 5.7.1 HLSK=2 Lagrangian. - This is the sequel to the first volume to treat in one effective field theory framework the physics of strongly interacting matter under extreme conditions. This is vital for understanding the high temperature phenomena taking place in relativistic heavy ion collisions and in the early Universe, as well as the high-density matter predicted to be present in compact stars. The underlying thesis is that what governs hadronic properties in a heat bath and/or a dense medium is hidden local symmetry which emerges from chiral dynamics of light quark systems and from the duality between QCD in 4D and
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| Emner | |
| Sjanger | |
| Dewey | |
| ISBN | 9789812705884. - 9812705880
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