The Conference on Quantum Mechanics, Elementary Particles, Quantum Cosmology and Complexity was held in honour of Professor Murray Gell-Mann's 80th birthday in Singapore on 24a26 February 2010. The conference paid tribute to Professor Gell-Mann's great achievements in the elementary particle physics. This notable birthday volume contains the presentations made at the conference by many eminent scientists, including Nobel laureates C N Yang, G 't Hooft and K Wilson. Other invited speakers include G Zweig, N Samios, M Karliner, G Karl, M Shifman, J Ellis, S Adler and A Zichichi. About Murray Gell-Mann Murray Gell-Mann, born September 15, 1929, won the 1969 Nobel Prize in physics for his work on the theory of elementary particles. His contributions span the entire history of particle physics, from the early days of the particle zoo to the modern day QCD. Along the way, even as he proposed new quantum numbers to bring order into the zoo, he had fun in naming them. And thus was born Strangeness, Flavor, Hadrons, Baryons, Leptons, the Eightfold Way, Color, Quarks, Gluons and, with Harald Fritzsch, the standard field theory of strong interactions, Quantum Chromodynamics (QCD). He also proposed with Richard Feynman the V-A theory of beta decay. Gell-Mann discovered the Current Algebra, proposed (with Levy) the sigma model of pions and the see-saw mechanism for the neutrino masses. Contents:Murray Gell-Mann a A Scientific Biography (H Fritzsch)Memories of Murray and the Quark Model (G Zweig)Some Problems in Cold Atom Research (C N Yang)Murray and the Omega Minus(N P Samios)From Ic- to Icb (M Karliner)Early History of QCD and Quarks (G Karl)Understanding Confinement in QCD: Elements of a Big Picture (M Shifman)QCD a Mass and Gauge in a Field Theory. QCD Glue Mesons (P Minkowski)The QCD Coupling and Parton Distributions at High Precision (J BlA¼mlein)What We Know and Don't Know about the Origin of the Spin of the Proton (A W Thomas et al.)Determination of Light Quark Masses in QCD (C A Dominguez)The Elusive Higgs Boson(s) (J F Gunion)Prospects for New Physics at the LHC (J Ellis)Murray Gell-Mann and the Last Frontier of LHC Physics: The QGCW Project (A Zichichi)Some Lessons from Sixty Years of Theorizing (M Gell-Mann)New Gauge Symmetry in Gravity and the Evanescent Role of Torsion (H Kleinert)Neutrino Masses and Grand Unification of Flavor (R N Mohapatra)LHC and the Seesaw Mechanism (G SenjanoviA)Neutrino Mixing, Leptonic CP Violation, the See-Saw Mechanism and Beyond (S T Petcov)Some Recent Progress in AdS/CFT (J H Schwarz)Aspects of String Phenomenology (I Antoniadis)String Corrections to QCD (D LA¼st)Maximal Supersymmetry and Exceptional Groups (L Brink)Gauge/Gravity Duality and Some Applications (S R Wadia)Quantum Mechanics and Field Theory with Momentum Defined on an Anti-de-Sitter Space(M Bander)Gauge Symmetry in Phase Space Consequences for Physics and Space-time (I Bars)Composite Higgs Particle (K Yamawaki)Black Holes and Attractors in Supergravity (A Ceresole a S Ferrara)Gauge Theory of Gravity with de Sitter Symmetry as a Solution to the Cosmological Constant Problem and the Dark Energy Puzzle (P Chen)Relaxing the Cosmological Constant on Large Distance Scales (A Zee)Inflation: Theory and Observations (V Mukhanov)Holographic Space-Time and Its Phenomenological Implications (T Banks)Modeling the Flyby Anomalies with Dark Matter Scattering (S L Adler)Physics of Micro Black Holes (G Dvali)Possible Solution of Dark Matter, the Solution of Dark Energy and Gell-Mann as Great Theoretician (P H Frampton)Reasoning by Analogy: Attempts to Solve the Cosmological Constant Paradox (R A Porto a A Zee)Manifestations of Space-Time Variation of Coupling Constants and Fundamental Masses (V V Flambaum a J C Berengut)Classical Cellular Automata and Quantum Field Theory (G at Hooft)Could Testing of the Laws of Physics Ever be Complete? (K G Wilson)and other papers Readership: Researchers and graduate students in high energy physics and theoretical physics. Keywords:Gell-Mann;History of Quark Model;Eightfold Way;Hadron;Baryon;Meson... be written for the second derivative. In this case one has to use the following identity6, 7 ar C(|s0 |) dsg(s)In(s) = ds[F(s) a F(s0)]In(s), (9) ar C(|s0 ... s = s0eix with the angle x defined in the interval x a (aI, I). The RGE then becomes das(x )dxanbsp;...

Title | : | Proceedings of the Conference in Honour of Murray Gell-Mann's 80th Birthday |

Author | : | H Fritzsch, K K Phua |

Publisher | : | World Scientific - 2010-11-04 |

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