Zichichi | Strong and Weak Interactions Present Problems | E-Book | sack.de
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E-Book, Englisch, 880 Seiten, Web PDF

Zichichi Strong and Weak Interactions Present Problems

1966 International School of Physics Ettore Majorana, a CERN-MPI-NATO Advanced Study Institute Erice, June 19 - July 4
1. Auflage 2013
ISBN: 978-1-4832-6163-8
Verlag: Elsevier Science & Techn.
Format: PDF
Kopierschutz: 1 - PDF Watermark

1966 International School of Physics Ettore Majorana, a CERN-MPI-NATO Advanced Study Institute Erice, June 19 - July 4

E-Book, Englisch, 880 Seiten, Web PDF

ISBN: 978-1-4832-6163-8
Verlag: Elsevier Science & Techn.
Format: PDF
Kopierschutz: 1 - PDF Watermark



Strong and Weak Interactions: Present Problems focuses on the reactions, transformations, and processes involved in strong and weak interaction, including baryonic, mesonic, and strange and non-strange resonances. The selection first offers information on unitary symmetry and hadron and lepton internal symmetries. Topics include internal symmetry for leptons, algebra of the hadron vector current, leptons and hadrons, and the search for higher symmetries. The text then elaborates on algebras and weak interactions and relativistic quark model as representation of algebra. The book takes a look at Regge poles in high-energy scattering and models of strong interactions. Discussions focus on electromagnetic properties, relations among strong vertices, medium-strong mass splittings, moving poles, high-energy kinematics, and Sommerfeld-Watson transformation. The text also ponders on meson resonances, phenomenology of resonances and particle supermultiplets, and meson photoproduction near threshold and commutation algebra. The selection is highly recommended for readers interested in strong and weak interactions.

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1;Front Cover;1
2;Strong and Weak Interactions: Present Problems;10
3;Coppyright Page;11
4;Table of Contents;14
5;FOREWORD;12
6;OPENING CEREMONY;22
7;Discorso Inaugurale;24
8;Ettore Majorana, Man and Scientist Commemoration Speech;31
9;PART I: LECTURES;31
9.1;CHAPTER 1. AN INTRODUCTION TO UNITARY SYMMETRY;99
9.1.1;I. The search for higher symmetries;99
9.1.2;II. SU(3) and its representations;104
9.1.3;III. Applications;131
9.1.4;IV. Ideas of octet enhancement;138
9.1.5;Bibliography;149
9.2;CHAPTER 2. HADRON AND LEPTON INTERNAL SYMMETRIES;150
9.2.1;I. Introduction;150
9.2.2;II. Internal symmetry for leptons;151
9.2.3;III. Algebra of the hadron vector current;155
9.2.4;IV. Leptons and hadrons;162
9.2.5;References;166
9.3;CHAPTER 3. CURRENT ALGEBRA AND WEAK INTERACTIONS;167
9.3.1;I. Introduction;167
9.3.2;II. Outline of weak interaction theory;168
9.3.3;III. A zero energy theorem;182
9.3.4;IV. Applications to leptonic decays of the K mesons;185
9.3.5;V. Non-Ieptonic decays of the K mesons;188
9.3.6;References;193
9.4;CHAPTER 4. CURRENT ALGEBRA;194
9.4.1;I. Algebra of currents – background;194
9.4.2;II. The frame P = 8;199
9.4.3;III. Experimental tests;203
9.4.4;IV. Going beyond SU(3) (x) SU(3) ;207
9.4.5;V. Trying to represent the local U(3) (x) U(3) algebra;210
9.4.6;References;222
9.5;CHAPTER 5. RELATIVISTIC QUARK MODEL AS REPRESENTATION OF CURRENT ALGEBRA;223
9.5.1;I. Current algebra at infinite momentum;223
9.5.2;II. Relativistic representation of current algebra;226
9.5.3;III. Relation to approximate symmetry;232
9.5.4;IV. Covariant formalism;238
9.5.5;V. A simple case solved exactly;244
9.5.6;VI. Outlook;250
9.5.7;Footnotes;255
9.6;CHAPTER 6. IDEAS ABOUT CP†;256
9.6.1;I. The violation of CP;256
9.6.2;II. The neutral kaon system;272
9.6.3;Footnotes and bibliography;287
9.7;CHAPTER 7. REGGE POLES IN HIGH-ENERGY SCATTERING;289
9.7.1;1. Introduction;289
9.7.2;2. Moving poles;290
9.7.3;3. Sommerfeld-Watson transformation;291
9.7.4;4. Signature;293
9.7.5;5. High-energy kinematics;294
9.7.6;6. t-channel poles;295
9.7.7;7. Illustration: pN scattering;295
9.7.8;8. Characteristic Regge properties;299
9.7.9;9. Properties of some other models;302
9.7.10;10. Non-Regge effects;304
9.7.11;11. One-pole test case: p-P - pon;305
9.7.12;12. Another one-pole case: p - P . non;307
9.7.13;13. Two-pole case: KN and KN charge exchange;308
9.7.14;14. SU(3) for p, n, K and K;309
9.7.15;15. Other reactions with boson Regge poles;310
9.7.16;16. Elastic scattering;313
9.7.17;17. Fermion Regge poles;317
9.7.18;18. The rule for zeros;319
9.7.19;19. Outlook;319
9.7.20;References;322
9.8;CHAPTER 8. MODELS OF STRONG INTERACTIONS;336
9.8.1;I. Introduction;336
9.8.2;II. The wave functions of mesons and baryons;339
9.8.3;III. Electromagnetic properties;342
9.8.4;IV. Relations among strong vertices;347
9.8.5;V. Relations between cross-sections;354
9.8.6;VI. A brief description of the U (6, 6) theory;360
9.8.7;VII. Medium-strong mass splittings;367
9.8.8;Appendix;372
9.8.9;References;375
9.9;CHAPTER 9. REGGE POLES AND THE ALGEBRA OF CURRENTS;380
9.9.1;References;397
9.10;CHAPTER 10. MESON RESONANCES;399
9.10.1;Introduction;399
9.10.2;I. Recent results on the existence and quantum numbers of mesons;400
9.10.3;II. Kinematic effects;421
9.10.4;References;428
9.11;CHAPTER 11. PHENOMENOLOGY OF RESONANCES AND PARTICLES SUPERMULTIPLETS;489
9.11.1;I. Baryon resonances with strangeness =0;489
9.11.2;II. Baryon resonances with strangeness # 0;503
9.11.3;III. Particle supermultiplets;515
9.11.4;References;535
9.12;SEMINARS;586
9.13;CHAPTER 12. COMMUTATORS OF CURRENT COMPONENTS;586
9.13.1;References;598
9.14;CHAPTER 13. SOME TOPICS OF RECENT INTEREST IN p and n PHOTOPRODUCTION;599
9.14.1;I. Introduction;599
9.14.2;II. Reasons for current interest in pseudoscalar photoproduction;599
9.14.3;III. Review of some recent experimental results;605
9.14.4;References;612
9.15;CHAPTER 14. RECENT EXPERIMENTS AT DESY;624
9.15.1;I. Introduction;624
9.15.2;II. The experimental programme;624
9.15.3;III. Photoproduction experiments;626
9.15.4;IV. Experiments for investigating the limits of the validity of present Q.E.D;649
9.15.5;V. Other experiments;649
9.15.6;References;653
9.16;CHAPTER 15. MESON PHOTOPRODUCTION NEAR THRESHOLD AND CURRENT CMMUNICATION ALGEBRA;697
9.16.1;References;704
9.17;CHAPTER 16. A POSSIBLE TEST AND SOME APPLICATIONS OF HEGGE POLES;705
9.17.1;1. Curvature of fermion trajectories as a test of the Regge-pole idea;705
9.17.2;2. Background integral of the Regge representation;706
9.17.3;3· Use of Regge poles in the direct channel at low energies;707
9.17.4;4· Reggeized bootstraps;709
9.17.5;References;711
9.18;CHAPTER 17. WEAK BOSONS, DECAY AND PRODUCTION;712
9.18.1;1. Introduction;712
9.18.2;2. Weak interactions;713
9.18.3;3. W mesons;714
9.18.4;4. W decays;714
9.18.5;5. Weak current;715
9.18.6;6. W .. two pseudoscaler mesons (a + b);717
9.18.7;7. W . pseudoscaler meson (P) + vector meson (V);718
9.18.8;8. W . p+n;719
9.18.9;9. SU3 limit;720
9.18.10;10. Quark model;722
9.18.11;11. Absolute decay rate;724
9.18.12;12. Search for W mesons;724
9.18.13;13. "W hunting";725
9.18.14;References;729
9.19;CHAPTER 18. RECENT DEVELOPMENTS IN THE THEORY OF MAGNETICALLY CHARGED PARTICLES;732
9.19.1;I. Introduction;732
9.19.2;II. The quantization condition;735
9.19.3;III. Rotational invariance;742
9.19.4;IV. A more precise version;746
9.19.5;V. Further results;748
9.19.6;Footnotes and references;750
10;DISCUSSIONS;752
10.1;Discussion 1;752
10.2;Discussion 2;759
10.3;Discussion 3;769
10.4;Discussion 4;775
10.5;Discussion 5;779
10.6;Discussion 6;782
10.7;Discussion 7;792
10.8;Discussion 8;794
10.9;Discussion 9;796
10.10;Discussion 10;798
10.11;Discussion 11;801
10.12;Discussion 12;809
10.13;Discussion 13;812
10.14;Discussion 14;816
10.15;Discussion 15;818
10.16;Discussion 16;822
10.17;Discussion 17;830
10.18;Discussion 18;833
10.19;Discussion 19;844
10.20;Discussion 20;847
10.21;Discussion 21;850
10.22;Discussion 22;852
10.23;Discussion 23;853
10.24;Discussion 24;856
10.25;Discussion 25;861
10.26;Discussion 26;864
11;CLOSING CEREMONY;868
12;LIST OF PARTICIPANTS;869



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