| Sample search results for: a4 flavour symmetry |
| 1 | TUM-HEP-723/09 SI-HEP-2009-nn | ||
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Summary: TUM-HEP-723/09 SI-HEP-2009-nn June 4, 2009 Sequential Flavour Symmetry Breaking Thorsten Feldmann... -46071 Valencia, Spain. Abstract The gauge sector of the Standard Model (SM) exhibits a flavour symmetry... of intermediate effective theories, where the flavour ... |
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Source: Siegen, Universität - Fachbereich Physik, Theoretische Physik 1 (Elementarteilchenphysik) |
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Collection: Physics |
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| 2 | Biochemistry 4000 R. Przybylski Course Title: Biochemistry and Chemistry of Food Flavor Formation | ||
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Summary: Course Description: Advanced course in flavour biochemistry will cover biochemical and chemical patterns... and mechanisms involved in perception of flavour components by human sensors will also be covered. Exercises... with individual chemicals, natural food flavouring material and food flavour system will ... |
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Source: Seldin, Jonathan P. - Department of Mathematics and Computer Science, University of Lethbridge |
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Collection: Mathematics |
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| 3 | arXiv:1002.4798v1[hep-ph]25Feb2010 TUM-HEP-747/10 | ||
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Summary: in Effective Theories with Spontaneously Broken Flavour Symmetry M. E. Albrechta , Th. Feldmanna , Th. Mannelb... 1, Fachbereich Physik, Universit¨at Siegen, D-57068 Siegen, Germany. Abstract The Flavour Symmetry... to scalar spurion fields, one can break the flavour ... |
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Source: Siegen, Universität - Fachbereich Physik, Theoretische Physik 1 (Elementarteilchenphysik) |
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Collection: Physics |
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| 4 | Humboldt-Universitat zu Berlin Mathematisch-Naturwissenschaftliche Fakultat I | ||
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Summary: ¨ur Physik Spontaneous breaking of parity-flavour symmetry in two-flavour lattice QCD with dynamical Wilson... ¨asentiert numerische Untersuchungen einer Phase mit spontaner Brechung von Parit¨at und Flavour Symmetrie in der Gitter... Gitters zu h = 0 extrapoliert. F¨ur die Gitter-QCD ... |
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Source: Humboldt-Universität zu Berlin, Institut für Physik, Theorie der Elementarteilchen/Phänomenologie |
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Collection: Physics |
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| 5 | Vol. 40 (2009) ACTA PHYSICA POLONICA B No 11 WEAK COMPLEMENTARITY | ||
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Summary: ] it has been pointed out that a broken flavour symmetry based on the discrete group A4 appears... on alternative discrete or continuous flavour groups have also been considered [4], but the A4 models have a very... Vol. 40 (2009) ACTA PHYSICA ... |
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Source: Magiera, Andrzej - Instytut Fizyki, Uniwersytet Jagiellonski |
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Collection: Physics |
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| 6 | arXiv:hepph/0006171 IMSc/2000/04/15 | ||
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Summary: , the oscillatory term involving ffi 13 averages out to zero: * cos / ffi 13 L 2E !+ = 0: (A:4) The same holds... of the effects of three and four flavour mixings Gautam Dutta, D. Indumathi, M. V. N. Murthy and G. Rajasekaran... of nonvanishing masses and mixings among neutrino flavours on the detection of ... |
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Source: Indumathi, D. - Institute of Mathematical Sciences, Chennai, India |
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Collection: Physics |
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| 7 | Vol. 41 (2010) ACTA PHYSICA POLONICA B No 12 MINIMAL FLAVOUR VIOLATION AND BEYOND | ||
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Summary: an important role in flavour physics? 2. Are there any new flavour symmetries that could help us to understand... symmetry U(3)5, corre- sponding to the independent unitary rotations in flavour space of the five fermion... value of the Higgs field, = v = 246 GeV, while the global ... |
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Source: Magiera, Andrzej - Instytut Fizyki, Uniwersytet Jagiellonski |
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Collection: Physics |
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| 8 | arXiv:1011.6531v1[hep-ph]30Nov2010 LU TP 10-27 | ||
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Summary: (n)L × SU(n)R chiral symmetry on the light quarks, and spin-flavour symmetry on the heavy quarks. Thus HMCh... , the -matrix indices. The Lagrangian (7) satisfies chiral symmetry and heavy quark spin flavour symmetry. We... Lagrangian that respects the ... |
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Source: Lunds Universitet, - Computational Biology and Biological Physics Group |
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Collection: Physics ; Biology and Medicine |
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| 9 | ESI The Erwin Schrodinger International Boltzmanngasse 9 Institute for Mathematical Physics A-1090 Wien, Austria | ||
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Summary: of an R-symmetry chemical potential for flavour fermions. For massless, "AdS-filling" Dp-brane embed... ). When the flavours are massless, the theories possess a global R-symmetry. The angular velocity... on the fermions 2 . The U(1)R symmetry is anomalous for a fixed number of colours ... |
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Source: Pottmann, Helmut - Institut für Diskrete Mathematik und Geometrie, Technische Universität Wien |
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Collection: Mathematics |
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| 10 | d'ordre 131-2008 presentee devant | ||
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Summary: The flavour problem 13 II.1 SM flavour symmetry . . . . . . . . . . . . . . . . . . . . . . . . . . . . 13 II... . . . . . . . . . . . . . . . . . . . . . . . . . . . 118 A.3.8 Thermally averaged cross sections and velocity expansion . . . . 120 A.4 Results... PROBLEM II.1 SM ... |
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Source: Ecole Polytechnique, Centre de mathématiques |
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Collection: Mathematics |
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| 11 | arXiv:0801.1826v1[hep-ph]11Jan2008 Flavour physics of leptons and dipole moments | ||
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Summary: framework and flavour symmetries . . . . . . . . . . . . . . . . . . . . . . . . 10 2.1 The flavour puzzle... . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 10 2.2 Flavour symmetries... dynamical theory of flavour still missing, the ... |
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Source: Kozlov, Mikhail G - Neutron Research Division , Petersburg Nuclear Physics Institute |
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Collection: Physics |
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| 12 | Effective hadronic Lagrangian under SU(4) Coupling constants, form factors | ||
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Summary: -channel only Without form factors #12;Going beyond SU(4) flavour symmetry Chiral symmetry: respect soft pion... Typical results Beyond the SU(4) symmetry Summary Cross sections between charmonia and comovers Zi-wei Lin... Texas A&M University Quark Matter 2002, July 20 #12;Free Lagrangian under SU(4) ... |
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Source: Lin, Zi-wei - Department of Physics, East Carolina University |
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Collection: Physics |
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| 13 | Theory and Phenomenology of CP Violation Thomas Mannela | ||
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Summary: describe. Flavour Symmetries: Isospin or more genrerally flavour SU(3) may be used to relate matrix... , the intrinsic uncertainties emerging from using flavour symme- tries are hard to estimate. Flavour symmetry... the flavour structure observed ... |
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Source: Siegen, Universität - Fachbereich Physik, Theoretische Physik 1 (Elementarteilchenphysik) |
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Collection: Physics |
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| 14 | HumboldtUniversit at zu Berlin MathematischNaturwissenschaftliche Fakult at I | ||
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Summary: Physik Spontaneous breaking of parityflavour symmetry in twoflavour lattice QCD with dynamical Wilson... asentiert numerische Untersuchungen einer Phase mit spontaner Brechung von Paritat und Flavour Symmetrie in der Gitter... ParitatFlavourSymmetrie ... |
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Source: Humboldt-Universität zu Berlin, Institut für Physik, Theorie der Elementarteilchen/Phänomenologie |
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Collection: Physics |
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| 15 | Wolfram Weise Tokyo University 21 September 2009 | ||
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Summary: ) SYMMETRY (x ) = 1 Nc Tr exp i 1 T 0 d A4(x , ) R. Pisarski (2000) Polyakov loop model A global symmetry... -local fermion interaction Temporal background gauge field Polyakov loop = 3 3 + 8 8 = 1 Nc Tr exp i 1/T 0 d A4... (i n, k ) (i n + m)2 + (k + p )2 + M(i n + ... |
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Source: Weise, Wolfram - Physik Department, Technische Universität München |
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Collection: Physics |
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| 16 | Nuclear Physics B307(1988)274-290 North-Holland, Amsterdam | ||
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Summary: flavour symmetry group SU(nf) should not be confused with breaking of chiral UA(1) through instantons [13... (~ - ~;),72~r 2 a; = 6~LSE 1 35k?k~ 189k?k~k~) 3lkl 5 41kl 9 + 41kin ' a'4= ~LSE 36k21k4 189ktk~k 2 ) 21k111... discuss chiral symmetry. 1. Introduction In this paper we wish to ... |
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Source: van Baal, Pierre - Leiden Institute of Physics, Universiteit Leiden |
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Collection: Physics |
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| 17 | Humboldt-Universitat zu Berlin Mathematisch-Naturwissenschaftliche Fakultat I | ||
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Summary: the existence of a phase of spontaneously broken parity-flavour-symmetry, a so-called Aoki phase, is numerically... spontan gebrochener Parit¨ats-flavour-Symmetrie, einer sogenannten Aoki-Phase, nachgewiesen. F¨ur gr... . . . . . . . . . . . . . . . . . . . . 17 2.4.2 Flavour symmetry . . . . . . . . . . . ... |
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Source: Humboldt-Universität zu Berlin, Institut für Physik, Theorie der Elementarteilchen/Phänomenologie |
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Collection: Physics |
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| 18 | Available at: http://publications.ictp.it IC/2010/021 KIASP10014 | ||
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Summary: at which the flavour symmetry is broken. Let us finally comment that in the limit ML # MR that we... with this kind of fits. All of the other coe#cients are as in Appendix A. 4 Constraints from lepton mixing... at the flavour symmetry breaking scale. Moreover, the ... |
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Source: International Centre for Theoretical Physics (ICTP), Trieste, Italy |
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Collection: Physics |
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| 19 | Available at: http://publications.ictp.it IC/2010/021 KIAS-P10014 | ||
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Summary: ,23,32 cannot be really determined with this kind of fits. All of the other coefficients are as in Appendix A. 4... -diagonal entries already at the flavour symmetry breaking scale. Moreover, the trilinear Af matrices are in general... , as predicted by the SU(3) flavour ... |
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Source: International Centre for Theoretical Physics (ICTP), Trieste, Italy |
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Collection: Physics |
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| 20 | JHEP07(2010)056 Published for SISSA by Springer | ||
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Summary: )B ×SU(Nf ) flavour symmetry group. The U(1)B is identified as the "baryon number" symmetry2 under... 7's, which appears as a flavour symmetry at low en- ergies. The separation in the x8-x9 plane... .p.kumar@swansea.ac.uk, pyjames@swansea.ac.uk Abstract: We investigate N = 4 SYM coupled to ... |
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Source: Aarts, Gert - Department of Physics, University of Wales Swansea |
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Collection: Physics |
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| 21 | Vol. 29 (1998) ACTA PHYSICA POLONICA B No 12 A SEARCH FOR A "NEW PHYSICS" IN LEPTON | ||
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Summary: Vol. 29 (1998) ACTA PHYSICA POLONICA B No 12 A SEARCH FOR A "NEW PHYSICS" IN LEPTON FLAVOUR... (Received November 11, 1997) Precision measurements and searches for rare processes in flavour phys- ics... experimental results are discussed. PACS numbers: 13.35. Bv, 14.60. z Symmetries play a fundamental role |
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Source: Magiera, Andrzej - Instytut Fizyki, Uniwersytet Jagiellonski |
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Collection: Physics |
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| 22 | Vol. 34 (2003) ACTA PHYSICA POLONICA B No 12 FIXED POLES, POLARIZED GLUE | ||
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Summary: 8, 2003. (5893) #12; 5894 S.D. Bass been interpreted to imply a small value for the flavour... planned to map out the proton's spinflavour structure and to measure the amount of spin carried... .1. The proton spin problem First consider the flavoursinglet channel. In QCD the axial anomaly [11] induces |
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Source: Magiera, Andrzej - Instytut Fizyki, Uniwersytet Jagiellonski |
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Collection: Physics |
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| 23 | Wolfram Weise QCD Green's Functions, Confinement and Phenomenology ECT*, Trento, 10 September 2009 | ||
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Summary: gauge field Polyakov loop = 3 3 + 8 8 = 1 Nc Tr exp i 1/T 0 d A4 1 3 Tr exp(i/T) SU(3) Effective... + k 2 + Mi(i n, ± n = n ± A4, 0 = n and M(n, p ) = mq + C(n, p )¯. temperatures above Tc... MATTER, CRITICAL POINT, and all that . . . Role of the AXIAL U(1) ANOMALY SYMMETRY ... |
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Source: Weise, Wolfram - Physik Department, Technische Universität München |
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Collection: Physics |
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| 24 | Universite Joseph Fourier Grenoble I Ecole Doctorale de Physique | ||
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Summary: of Dark Matter Annihilation and Non-Minimal Flavour Violation in the MSSM pr´epar´ee au Laboratoire de... include the possibility of non-minimal flavour violation (NMFV) in the squark sector and define "collider... cross sections at the LHC in GMSB with NMFV. We also discuss the phenomenology of flavour mixing |
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Source: Ecole Polytechnique, Centre de mathématiques |
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Collection: Mathematics |
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| 25 | TIFR Annual Report 2006-07 THEORETICAL PHYSICS | ||
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Summary: ensembles created in QCD with two flavours of staggered quarks. High-scale symmetries of non... . These fermions have exact chiral and flavour symmetry on the lattice unlike those used earlier. As a price though... role. Strengths of flavour-dependent long-range leptonic forces were ... |
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Source: Tata Institute of Fundamental Research, Department of Theoretical Physics |
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Collection: Physics |
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| 26 | QCD Thermodynamics from Lattice Gauge Theory | ||
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Summary: input in the calculation. The disadvantage is that the full flavour symmetry is restored only for very... T as as + as . (10) Using these expressions, one obtains [4] a4 s = -6Nc2 Ks Ds + K D , and (11a) a4 s a4 s ( - ... |
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Source: Tata Institute of Fundamental Research, Department of Theoretical Physics |
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Collection: Physics |
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| 27 | CERN-PH-TH/2010-304 DESY 10-246 | ||
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Summary: valid for high tan and high mA - 4µ A 0. (12) Since this condition is only approximate, and since... a wide set of up-to-date constraints from both high-energy collider and flavour physics, the Higgs boson... The explanation behind electroweak symmetry breaking (EWSB) is still largely unknown. As- suming ... |
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Source: Lunds Universitet, - Computational Biology and Biological Physics Group |
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Collection: Physics ; Biology and Medicine |
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| 28 | Modelling the PHASES of QCD Wolfram Weise | ||
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Summary: 3 + 8 8 = 1 Nc Tr exp i 1/T 0 d A4 1 3 Tr exp(i/T) SU(3) Effective potential : Phases of QCD R... (i n, k ) (i n + m)2 + (k + p )2 + M(i n + m, k + p )2 (i n)2 + k 2 + Mi(i n, ± n = n ± A4, 0 = n and M... August 2009 QCD SYMMETRIES and SYMMETRY BREAKING PATTERNS ... |
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Source: Weise, Wolfram - Physik Department, Technische Universität München |
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Collection: Physics |
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| 29 | SFB-Days on July 9 and 10 at MPI fr Kernphysik, Heidelberg Thursday, July 9, MPIK lecture hall | ||
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Summary: : 14:00 - 14:30: A. Adulpravitchai: Confronting Flavour Symmetries and Extended Scalar Sectors... with Lepton Flavour Violation Phenomenology 14:30 - 15:00: D. Fang: Description of the double beta decay |
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Source: Technische Universität München, Physik Department, Experimental Physics and Astroparticle Physics Group |
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Collection: Physics |
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| 30 | Exploring the chiral phase transition of Nf = 2 flavour QCD with valence overlap fermions | ||
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Summary: Exploring the chiral phase transition of Nf = 2 flavour QCD with valence overlap fermions E... .8.2007 Exploring the chiral phase transition of Nf = 2 flavour QCD #12;Introduction Properties of the lowest... -Michael Ilgenfritz Frascati · 7.8.2007 Exploring the chiral phase transition of Nf = 2 flavour QCD #12;Outline 1 |
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Source: Humboldt-Universität zu Berlin, Institut für Physik, Theorie der Elementarteilchen/Phänomenologie |
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Collection: Physics |
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| 31 | ESI The Erwin Schrodinger International Boltzmanngasse 9 Institute for Mathematical Physics A-1090 Wien, Austria | ||
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Summary: + a1LM + a2L2 M + a3L3 M + a4L4 M + a5L5 M + · · · , (60) where LM is defined in (42... for large numbers of components (e.g., 1/N expansions) 11.30.Qc, Spontaneous and radiative symmetry breaking... normally takes into account all terms that have the correct symmetry at the required order and then one |
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Source: Pottmann, Helmut - Institut für Diskrete Mathematik und Geometrie, Technische Universität Wien |
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Collection: Mathematics |
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| 32 | Vol. 38 (2007) ACTA PHYSICA POLONICA B No 3 THE PHYSICS OF BEAUTY (AND CHARM [AND ]) | ||
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Summary: are briefly addressed in Appendix A. 4.1. Rare B decays (B lXc): the inclusive semi-leptonic width has been... V ^= ± 5.0 % , (A.3) |V (cb)|incl = (41.96 ± 0.67) × 10-3 ^= ± 1.6 % , (A.4) where the last line should... and comprehensive flavour studies are a necessity, not a luxury, ... |
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Source: Magiera, Andrzej - Instytut Fizyki, Uniwersytet Jagiellonski |
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Collection: Physics |
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| 33 | arXiv:1010.0110v1[hep-lat]1Oct2010 Minimally doubled fermions and their | ||
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Summary: .3) and a suitable discretization of it is d4(g0) 1 2a (x)4 U4(x)(x+a4)-(x+a4)4U 4 (x)(x) . (3.4) The counterterm... D4 and 1/a 4 the renormalized propagator can be written in the standard form. Then, at one loop we... ))5Uµ(x)(x+aµ) +(x+aµ)(µ +i4 (1-µ4))5 U ... |
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Source: Creutz, Michael - High Energy Theory Group, Brookhaven National Laboratory |
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Collection: Physics |
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| 34 | Future perspective on particle physics Riccardo Barbieri | ||
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Summary: with the given gauge symmetry and particle content the SM as a low energy approximation of a more complete... ) 3. From the flavour tests !nat (400 GeV) mh 115GeV Lcomplete = LSM +!LY=0 ("EWPT )+!LY=0 ("flav... ? Supersymmetry theoretically most appealing !EWPT !nat OK Why no superpartner, no light Higgs, no flavour signal |
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Source: Abbondandolo, Alberto - Scuola Normale Superiore of Pisa |
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Collection: Mathematics |
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| 35 | Preprint typeset in JHEP style -HYPER VERSION NI08005 Higher representations on the lattice | ||
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Summary: the familiar expression: lat(g0) = -0g3 0 - 1g5 0 + O(g7 0) (2.2) 0 = 1 (4)2 11 3 C2(A) - 4 3 TRnf (2.3) 1 = 1... in QCD: as the quark mass is reduced at fixed lattice spacing, flavour symmetry is broken and two... .2) a (Ta RTa R)AB = C2(R)AB, (A.3) and hence: TR = 1 N2 - 1 C2(R)dR ... |
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Source: Isaac Newton Institute for Mathematical Sciences |
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Collection: Mathematics |
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| 36 | Theory of flavour physics Svjetlana Fajfer | ||
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Summary: 1 Theory of flavour physics 27.03.2008 Svjetlana Fajfer Physics Department, University of Ljubljana... level processes in which the neutral currents change flavour! BR(KL µ+ µ- ) = 6.84 × 10-19 #12;CP... of SM in the loops new physics particles #12;Flavour theory #12;Basic questions of the flavour theory |
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Source: Prosen, Toma - Department of Physics, University of Ljubljana |
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Collection: Physics |
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| 37 | LU TP 97/06 hepph/9704233 | ||
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Summary: ) mass we have a symmetry by interchanging them. For the case of two flavours this is known as isospin... . It is a continuous symmetry, SU(2) V . A generalization to three flavours is the GellMannOkubo eightfold way where... with a separate ``isospin'' for both helicities. In the case of 3 massless ... |
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Source: Lunds Universitet, - Computational Biology and Biological Physics Group |
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Collection: Physics ; Biology and Medicine |
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| 38 | TIFR Annual Report 2005-06 THEORETICAL PHYSICS | ||
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Summary: can be meaningfully compared with experiments. Strangeness production and flavour symmetry... neutrinos as well as nearly flavour- diagonal supersymmetry-breaking A-terms giving rise to the observed bi... Bhattacharyya of SINP, Kolkata and Kumar Rao of PRL, Ahmedabad] Flavour Changing Higgs decays in ... |
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Source: Tata Institute of Fundamental Research, Department of Theoretical Physics |
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Collection: Physics |
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| 39 | Particle Physics: the Standard Model and Beyond | ||
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Summary: as "synthetic" physics The gauge sector (3) The flavour sector (2) The EWSB sector (4) The -mass sector (1) (if... knowledge of oscillations only or, maybe, a clash! #12;The Flavour Sector 1 - We know the SM works... for them) 2 - If there are other degrees of freedom at the Fermi scale carrying flavour (e.g. the s |
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Source: Abbondandolo, Alberto - Scuola Normale Superiore of Pisa |
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Collection: Mathematics |
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| 40 | On the Entanglement of CHIRAL and DECONFINEMENT | ||
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Summary: ) physics ? #12;DECONFINEMENT and spontaneous breaking of Z(3) SYMMETRY (x ) = 1 Nc Tr exp i 1 T 0 d A4(x... exp i 1/T 0 d A4 1 3 Tr exp(i/T) SU(3) Effective potential : Phases of QCD R. Pisarski ( Polyakov... . Fukushima (2004)) Polyakov Loop (Thermal Wilson Line) = 1 Nc Tr exp i 1/T 0 ... |
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Source: Weise, Wolfram - Physik Department, Technische Universität München |
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Collection: Physics |
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| 41 | Vol. 29 (1998) ACTA PHYSICA POLONICA B No 5 SPIN EFFECTS IN HEAVY QUARK PROCESSES | ||
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Summary: . The second symmetry of the heavy mass limit is a heavy flavour symmetry which allows us to replace... the different masses. We shall first give a brief account on the heavy flavour symmetries and then discuss a few... in Heavy Quark Processes 1415 The first symmetry ... |
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Source: Magiera, Andrzej - Instytut Fizyki, Uniwersytet Jagiellonski |
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Collection: Physics |
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| 42 | Professor Judah M. Eisenberg Memorial Lecture Judah Moshe Eisenberg | ||
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Summary: DECONFINEMENT and Spontaneous Breaking of Z(3) SYMMETRY (x ) = 1 Nc Tr exp i 1 T 0 d A4(x , ) R. Pisarski (2000... in the N 8 calculations. ¯ T ¯ T=0 Spontaneously broken Chiral Symmetry Lattice QCD (2+1 flavours) almost... in Quantum Chromodynamics (QCD) Quarks & Gluons Hadrons ... |
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Source: Weise, Wolfram - Physik Department, Technische Universität München |
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Collection: Physics |
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| 43 | EPJ manuscript No. (will be inserted by the editor) | ||
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Summary: the recent data on B 0 0 fit into the picture, see above. 2.4 Flavour Symmetries in Non-Leptonic Decays... established, is to make use of flavour symmetries such as isospin, U-spin or even full flavour-SU(3). After... of work has been done using flavour ... |
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Source: Siegen, Universität - Fachbereich Physik, Theoretische Physik 1 (Elementarteilchenphysik) |
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Collection: Physics |
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| 44 | DRAFT 25/9/09 Appendix A: Facilities | ||
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Summary: of Tevatron operation (depending on LHC performance). A.4 High-energy lepton collider Context: In 1999... realisation can be very long. The Higgs mechanism for electroweak symmetry breaking was proposed in 1964... strengths are the study of black holes, symmetry breaking, supersymmetry and string theory, the ... |
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Source: Crowther, Paul - Department of Physics and Astronomy, University of Sheffield |
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Collection: Physics |
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| 45 | Model-independent analysis of U-spin breaking in non-leptonic B-decays | ||
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Summary: -mail: mannel@hep.physik.uni-siegen.de Flavour symmetries represent a powerful tool in analysing model... in the field of QCD methods. The main problem with flavour symmetries is that they hold only approximately... breaking U-spin is an SU(2) subgroup of the full flavour SU(3) ... |
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Source: Siegen, Universität - Fachbereich Physik, Theoretische Physik 1 (Elementarteilchenphysik) |
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Collection: Physics |
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| 46 | WHAT IS THE SIGNIFICANCE OF THE CONSERVATION OF ELECTRIC CHARGE Q? TSAN UNG CHAN | ||
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Summary: is the leptonic number) and total flavour TF. Conservation of electric charge implies obviously conservation of Q... which conserve Q, A and L and all individual flavours conserve obviously BAL and TF; likely weak... -time symmetries and thus must be valid for all known or yet unknown interactions) or material (the conservation |
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Source: Ecole Polytechnique, Centre de mathématiques |
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Collection: Mathematics |
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| 47 | Review of Charm Physics: A Theory Perspective Thomas Mannel | ||
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Summary: an additional flavour symmetry, which would protect it from any FCNC, even at loop level. This flavour symmetry... these spectroscopic data. From the flavour point of view the charm quark offers several unique possibilities... . The flavour structure of the standard ... |
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Source: Siegen, Universität - Fachbereich Physik, Theoretische Physik 1 (Elementarteilchenphysik) |
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Collection: Physics |
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| 48 | ccsd-00083161,version2-11Sep2006 MIXING ANGLES AND NON-DEGENERATE COUPLED SYSTEMS OF PARTICLES | ||
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Summary: between neutrinos and neutral kaons is outlined, together with the role of the symmetry by exchange... a matter of surprise and questioning [1][2]. Symmetries [3] have been invoked, which should be approximate... on flavour eigenstates [6]. In the while, the CP violating parameters L and S of the physical neutral kaons |
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Source: Ecole Polytechnique, Centre de mathématiques |
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Collection: Mathematics |
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| 49 | Phases of QCD and PNJL model beyond mean field theory | ||
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Summary: the quarks move in a back- ground colour gauge field, A4/T = iA0/T, which is connected to the (traced... ) Polyakov loop via = 1 Nc Tr P exp i 0 dA4 = 1 3 Tr ei (3 3+8 8) = 1 3 Tr ei . The interaction V includes... µ µ - iA4 produces in general formally complex ... |
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Source: Weise, Wolfram - Physik Department, Technische Universität München |
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Collection: Physics |
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| 50 | TIFR Annual Report 2002-03 THEORETICAL PHYSICS | ||
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Summary: ] The Phase Transition in QCD with Broken SU(2) Flavour Symmetry A first investigation of the QCD transition... . For the mass range appropriate to the strange quark, the flavour diagonal susceptibility was significantly... a much lower pion screening mass. The flavour off-diagonal susceptibility was found to ... |
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Source: Tata Institute of Fundamental Research, Department of Theoretical Physics |
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Collection: Physics |
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| 51 | LU TP 9611 bbfragmentation and B correlations | ||
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Summary: ]. There is a flavour ordering present throughout the string so that the flavour quan tum number is preserved. Details... right symmetry'', which means that the fragmentation process should look the same irrespective to which end... could in principle depend on the flavour of the associated quark--anti ... |
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Source: Lunds Universitet, - Computational Biology and Biological Physics Group |
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Collection: Physics ; Biology and Medicine |
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| 52 | label name %cocoa cocoa source Pralus Cuba 75 Despite being called Cuba, the blurb on the back talks | ||
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Summary: -free soya lecithinForasteroclear fruity flavour with a hint of coffee yes naturales y organico cacao, panela... naranjavery strong floral flavours with coffee undertones. Very g cocoa beans, cane sugar, cocoa butter... :soya lecithintrinitarioclear fruity flavour with distinct tropical fruit flavours, well ... |
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Source: Reitsma, Femke E. - School of GeoSciences, University of Edinburgh |
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Collection: Geosciences |
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| 53 | CERN2010002 24 June 2010 | ||
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Summary: chromodynamics, physics beyond the Standard Model, flavour physics, effective field theory, cosmology, as well... . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 101 Introduction to flavour physics Y. Grossman... and the electroweak ... |
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Source: Wu, Sau Lan - CERN & Department of Physics, University of Wisconsin at Madison |
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Collection: Physics |
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| 54 | Journal of Experimental Botany, Page 1 of 12 doi:10.1093/jxb/ern294 | ||
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Summary: from leucine or isoleucine (1D, 4E, 5A, 7A). 4 of 12 Mathieu et al. #12;While the pathway... ) RESEARCH PAPER Flavour compounds in tomato fruits: identification of loci and potential pathways affecting... Abstract The unique flavour of a tomato fruit is the sum of a complex interaction among sugars, acids |
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Source: Klee, Harry J. - Horticultural Sciences Department, University of Florida |
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Collection: Biotechnology ; Biology and Medicine |
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| 55 | Vol. 34 (2003) ACTA PHYSICA POLONICA B No 12 MINIMAL FLAVOUR VIOLATION # | ||
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Summary: to this class. Another formulation, a profound one, that uses flavour symmetries has been presented in [7... flavour symmetry breaking e#ects can be reliably calculated. 2.3. The basic idea By now all... #) , V cb = A# 2 +O(# 8 ) , (2.13) V ts = -A# 2 + 1 2 A# 4 [1 - ... |
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Source: Magiera, Andrzej - Instytut Fizyki, Uniwersytet Jagiellonski |
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Collection: Physics |
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| 56 | University of Southampton Research Repository ePrints Soton | ||
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Summary: the light quark part of the QCD Lagrangian. SU(3) flavour symmetry and isospin The light quark part... number. The SU(3) flavour symmetry classi- fies the spectrum of hadrons made up of u, d and s quarks, all... (+ , - , 0 , , K+ , K- , K0 , ¯K0 ) and 1 2 + baryons (n, p, + , 0 , 0 , + , - , 0 ). SU(3) ... |
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Source: Quartly, Graham - National Oceanography Centre Southampton |
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Collection: Environmental Sciences and Ecology ; Geosciences |
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| 57 | Vol. 38 (2007) ACTA PHYSICA POLONICA B No 9 A GUIDE TO FLAVOUR CHANGING NEUTRAL | ||
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Summary: Vol. 38 (2007) ACTA PHYSICA POLONICA B No 9 A GUIDE TO FLAVOUR CHANGING NEUTRAL CURRENTS... Heisenberg-Institut) 80805 München, Germany (Received June 28, 2007) Flavour changing neutral current processes, being... the electroweak scale. Here, we summarise the re- cent progress in flavour physics studies of the Littlest Higgs |
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Source: Magiera, Andrzej - Instytut Fizyki, Uniwersytet Jagiellonski |
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Collection: Physics |
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| 58 | ESI The Erwin Schrodinger International Institute for Mathematical Physics | ||
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Summary: of the Einstein Equations 15:00 - 15:30 COFFEE BREAK 15:30 - 16:30 V. FILEV Flavoured SYM theory on S3... 11:30 - 12:30 K.-Y. KIM Holographic phase diagram of a chiral symmetry breaking gauge theory All |
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Source: Beiglböck, Mathias - Institut für Diskrete Mathematik und Geometrie, Technische Universität Wien |
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Collection: Mathematics |
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| 59 | Vol. 34 (2003) ACTA PHYSICA POLONICA B No 11 NEUTRINO MIXING AND LEPTON FLAVOUR | ||
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Summary: Vol. 34 (2003) ACTA PHYSICA POLONICA B No 11 NEUTRINO MIXING AND LEPTON FLAVOUR VIOLATION IN SUSY... unsuppressed flavourchanging processes. Even if the mass parameters are chosen to give no flavour violation... to the observed large neutrino mixings and potentially large neutrino Yukawa couplings, sizable lepton ... |
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Source: Magiera, Andrzej - Instytut Fizyki, Uniwersytet Jagiellonski |
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Collection: Physics |
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| 60 | Report of the Particle Physics Advisory Panel P. N. Burrows, C. Da Via, T. Gershon, E. W. N. Glover, C. Shepherd-Themistocleous, | ||
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Summary: ? Are there as-yet undiscovered symmetries of nature such as supersymmetry (SUSY)? Are there extra dimensions... ? Recommendation: The UK must lead in exploring the Energy Frontier. 2.2 The Flavour Sector Why does the Universe... -violation with the property of "flavour" which allows us to assemble the family and generation ... |
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Source: Crowther, Paul - Department of Physics and Astronomy, University of Sheffield |
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Collection: Physics |
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| 61 | arXiv:hepph/9907372 IMSc/99/05/22 | ||
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Summary: of flavour mixing Gautam Dutta, D. Indumathi, M. V. N. Murthy and G. Rajasekaran The Institute... vanishing masses and mixings among neutrino flavours on the detection of neutrinos from stellar collapse by a water... Cerenkov detector. We consider a realistic framework in which there are three neutrino flavours whose mass |
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Source: Indumathi, D. - Institute of Mathematical Sciences, Chennai, India |
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Collection: Physics |
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| 62 | UNIVERSITY OF STRATHCLYDE CATERING DEPARTMENT WINE LIST JANUARY 2011 Wines for every occasion will be found in the following list. | ||
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Summary: BRUT N.V. The vibrant pink colour in the glass hints at the strawberries and cream flavours... -LEROY, FLEUR DE CHAMPAGNE, BRUT, NV A fruity style of Champagne with all the biscuity flavour you'd expect... WHITES WITH CRISP, ELEGANT FLAVOURS SAUVIGNON BLANC, KLEINE ZALZE, STELLENBOSCH South Africa is the World |
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Source: Mottram, Nigel - Department of Mathematics, University of Strathclyde |
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Collection: Mathematics |
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| 63 | Wines for every occasion will be found in the following list. We stock a selection that should satisfy the busiest reception as well as the discerning | ||
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Summary: at the strawberries and cream flavours that quickly burst out. Soft and easy to enjoy this is a striking great fun... the biscuity flavour you'd expect and a real depth of character. Widely regarded as the best value Champagne... and complements the ripe heart of the wine. £10.25 #12;WHITE WINE DRY, INTENSE WHITES WITH CRISP, ELEGANT ... |
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Source: Mottram, Nigel - Department of Mathematics, University of Strathclyde |
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Collection: Mathematics |
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| 64 | UNIVERSITY OF STRATHCLYDE CATERING DEPARTMENT WINE LIST AUGUST 2009 Wines for every occasion will be found in the following list. | ||
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Summary: BRUT N.V. The vibrant pink colour in the glass hints at the strawberries and cream flavours... -LEROY, FLEUR DE CHAMPAGNE, BRUT, NV A fruity style of Champagne with all the biscuity flavour you'd expect... WITH CRISP, ELEGANT FLAVOURS SAUVIGNON BLANC, KLEINE ZALZE, STELLENBOSCH South Africa is the World's most |
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Source: Mottram, Nigel - Department of Mathematics, University of Strathclyde |
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Collection: Mathematics |
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| 65 | Vol. 29 (1998) ACTA PHYSICA POLONICA B No 10 INDIRECT CP VIOLATION IN THE Bd-SYSTEM | ||
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Summary: ]. They make use of flavour-tagging either K0 or ¯K0 at t = 0, and study their time evolution in the decays... -violation to be described by charged current flavour mixing of quarks? We believe that the B0 - ¯B0 system is going to play... -system Flavour Number is not conserved by weak interactions, so in 2nd order B0 and ¯B0 ... |
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Source: Magiera, Andrzej - Instytut Fizyki, Uniwersytet Jagiellonski |
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Collection: Physics |
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| 66 | Vol. 38 (2007) ACTA PHYSICA POLONICA B No 9 PARTIALLY QUENCHED AND THREE FLAVOUR | ||
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Summary: Vol. 38 (2007) ACTA PHYSICA POLONICA B No 9 PARTIALLY QUENCHED AND THREE FLAVOUR ChPT AT TWO LOOPS... and Flavours: from EURODAPHNE to EURIDICE", Kazimierz, Poland, 2427 August, 2006. (2777) #12;2778 J. Bijnens... L + i¯qRD/ qR - mq (¯qRqL + ¯qLqR) (1) is invariant under the chiral symmetry SU(3)L× SU(3)R when |
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Source: Magiera, Andrzej - Instytut Fizyki, Uniwersytet Jagiellonski |
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Collection: Physics |
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| 67 | LU TP 95--20 December 1998 | ||
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Summary: Fragmentation 229 12.1 Flavour Selection . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 229 12... which the longrange confinement forces are allowed to distribute the energies and flavours of a parton... distribution functions, which defines the partonic substructure in terms of flavour composition and energy |
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Source: Budker Institute of Nuclear Physics, Detector KEDR Experiments |
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Collection: Fission and Nuclear Technologies |
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| 68 | LU TP 95--20 August 1995 | ||
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Summary: Fragmentation 226 12.1 Flavour Selection : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : 226 12... which the longrange confinement forces are allowed to distribute the energies and flavours of a parton... distribution functions, which defines the partonic substructure in terms of flavour composition and energy |
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Source: Budker Institute of Nuclear Physics, Detector KEDR Experiments; Lunds Universitet, - Computational Biology and Biological Physics Group |
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Collection: Biology and Medicine ; Fission and Nuclear Technologies ; Physics |
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| 69 | PHASES of QCD Wolfram Weise | ||
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Summary: DECONFINEMENT and Spontaneous Breaking of Z(3) SYMMETRY (x ) = 1 Nc Tr exp i 1 T 0 d A4(x , ) R. Pisarski (2000... ,((#-'= 7"3($*( !""#$%#&'(")* +,-./0'1-234/'5&."#167 A#4'->%&%+ B#4>,"%>73#+ dN d dpt = dN dpt [1 + v1(pt... PHASES of QCD Wolfram Weise Symposium ... |
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Source: Weise, Wolfram - Physik Department, Technische Universität München |
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Collection: Physics |
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| 70 | GLASPPE/200906 8 th October 2009 | ||
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Summary: of revealing New Physics in the heavy flavour sector. This contribution will cover the prospects for B physics... channels. SUSY09 Boston, MA, USA #12; 1 Introduction Flavour physics has celebrated many successes over... # s . The experiments at the LHC will open the door to areas of flavour physics that were thus far ... |
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Source: Glasgow, University of - Department of Physics and Astronomy, Particle Physics Experimental Group |
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Collection: Physics |
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| 71 | GLAS-PPE/2009-06 October 2009 | ||
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Summary: of revealing New Physics in the heavy flavour sector. This contribution will cover the prospects for B physics... channels. SUSY09 Boston, MA, USA #12;1 Introduction Flavour physics has celebrated many successes over... at the LHC will open the door to areas of flavour physics that were thus far unreachable. With the full |
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Source: Glasgow, University of - Department of Physics and Astronomy, Particle Physics Experimental Group |
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Collection: Physics |
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| 72 | Institut de Physique Nuclaire de Lyon Universit Claude Bernard Lyon-1 | ||
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Summary: ]. · Models with a (e.g. flavour) symmetry that breaks below the leptogenesis scale, and involve addi- tional... of leptogenesis: finite temperature effects, spectator processes, and in particular the significance of flavour... . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 48 2 ... |
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Source: Ecole Polytechnique, Centre de mathématiques |
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Collection: Mathematics |
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| 73 | SEARCH FOR OTHER NEW PARTICLES AT HERA talk presented at ICHEP '96, Warsaw | ||
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Summary: , with or without lepton flavour violation. All leptoquarks are excluded for masses up to ß 220 GeV in the case... . Limits are set on many previously unprobed channels for lepton flavour violation, while some existing... , but that the symmetry is only broken by a very large mass of the righthanded neutrinos (N ). A direct ... |
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Source: Imperial College London, Department of Physics, High Energy Physics Group |
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Collection: Physics |
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| 74 | Light hadrons from lattice QCD with light (u, d), strange and charm | ||
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Summary: doublet (u, d) in the so called twisted basis reads [3,4] Sl = a4 x {¯l(x) [D[U] + m0,l + iµl53] l... to the twist direction. We thus choose the construction [33,34] Sh = a4 x {¯h(x) [D[U] + m0,h + iµ51 + µ3] h... dynamical flavours also the effects of the strange and charm sea ... |
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Source: Humboldt-Universität zu Berlin, Institut für Physik, Theorie der Elementarteilchen/Phänomenologie |
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Collection: Physics |
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| 75 | Theoretical Aspects of Heavy Flavour Physics Thomas Mannel | ||
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Summary: Theoretical Aspects of Heavy Flavour Physics Thomas Mannel Theoretische Physik 1, Siegen University... , 57068 Siegen, Germany 1 Introduction Favour physics and in particular heavy flavour physics is currently... the flavour sector of the standard model, which have to be supported by theoretical progress in order |
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Source: Siegen, Universität - Fachbereich Physik, Theoretische Physik 1 (Elementarteilchenphysik) |
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Collection: Physics |
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| 76 | On the Relation of Confinement and Chiral Symmetry | ||
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Summary: flavours of quarks in the adjoint representation Features: adjoint, massive quarks respect center symmetry... On the Relation of Confinement and Chiral Symmetry Breaking in Gauge Theories Tina Katharina Herbst... -Meson Formulation 4 Conclusion Confinement and Chiral Symmetry Breaking in Gauge Theories Tina K. ... |
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Source: Rossak, Wilhelm R. - Fakultät für Mathematik und Informatik, Friedrich-Schiller-Universität Jena |
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Collection: Computer Technologies and Information Sciences |
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| 77 | TH`ESE de DOCTORAT de l'UNIVERSITE PARIS XI | ||
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Summary: . . . . . . . . . . . . . . . . . . . . . . . . . 15 1.2.1 The Mikheyev-Smirnov-Wolfenstein (MSW) effect . . . . . 20 1.2.2 3 flavours in matter... . Let us briefly remind the milestones in the dis- covery of neutrinos of different flavours as well... flavour. In the same time, other crucial properties of neutrinos were being ... |
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Source: Ecole Polytechnique, Centre de mathématiques |
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Collection: Mathematics |
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| 78 | Modeling the QCD-Phase diagram in and beyond mean field theory | ||
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Summary: ) Substitute the Matsubara frequencies n by n + iA4 « Analogy to the QCD gauge coupling MF = NJL|n n+iA4 + U... Due to the minimal substitution n n + iA4 the inverse propagator S-1 is not hermitian « The fermion... symmetry breaking 2 ... |
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Source: Weise, Wolfram - Physik Department, Technische Universität München |
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Collection: Physics |
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| 79 | Vol. 29 (1998) ACTA PHYSICA POLONICA B No 12 NEUTRINOS AND SYMMETRIES STUDIED BY | ||
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Summary: symmetries. Nuclear states in nuclei have approximately good quantum numbers. Parities(), flavours(s, c... . J. Mod. Phys. A4, 1851 (1989). [5] A. Morales, LFNAE-94-004 (1994). [6] M. Moe, P. Vogel, Ann. Rev... Vol. 29 (1998) ACTA PHYSICA POLONICA B No 12 NEUTRINOS AND SYMMETRIES STUDIED ... |
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Source: Magiera, Andrzej - Instytut Fizyki, Uniwersytet Jagiellonski |
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Collection: Physics |
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| 80 | Multiquarks and Steiner trees Jean-Marc Richard | ||
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Summary: to this Conference, where references can be found. Flavour symmetry breaking and chromoelectric binding We adopt here... this favourable symmetry breaking works with flavour-independent potentials. The corresponding four-body problem... calculations, and predict several multiquark states in configurations ... |
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Source: Ecole Polytechnique, Centre de mathématiques |
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Collection: Mathematics |
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| 81 | HOT & DENSE HADRONIC MATTER Wolfram Weise | ||
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Summary: i 1/T 0 d A4 1 3 Tr exp(i/T) = 3 3 + 8 8 SU(3) { Effective potential : A global symmetry emerges... + 8 8 = 1 Nc Tr exp i 1/T 0 d A4 1 3 Tr exp(i/T) SU(3) Effective potential (Z(3) invariant) Phases... hadron phase CSC phase Nature of Transitions ? 1st order vs. 2nd order vs. ... |
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Source: Weise, Wolfram - Physik Department, Technische Universität München |
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Collection: Physics |
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| 82 | University of Southampton Research Repository ePrints Soton | ||
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Summary: is an approximate flavour symmetry. i {1, 2, 3} and {1, 2}. . . . 46 xi #12;5.1 The abbreviated notation... is imposed in order to avoid rapid proton decay. ZH 2 is an approximate flavour symmetry. In the E6ZS 2 SSM... xix Overview 1 1 The Standard Model 3 1.1 Gauge Symmetry and ... |
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Source: Quartly, Graham - National Oceanography Centre Southampton |
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Collection: Environmental Sciences and Ecology ; Geosciences |
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| 83 | arXiv:hep-ph/0609281v127Sep2006 Polyakov loop, diquarks and the | ||
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Summary: A4 = iA0, where A0 = µ0 gAµ a ta with the SU(3)c gauge fields Aµ a and the generators ta = a /2... arXiv:hep-ph/0609281v127Sep2006 Polyakov loop, diquarks and the two-flavour phase diagram S. R... : confinement and sponta- neous chiral symmetry breaking. This paper extends our previous PNJL calculations |
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Source: Weise, Wolfram - Physik Department, Technische Universität München |
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Collection: Physics |
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| 84 | Chiral symmetry restoration of QCD and the Gross-Neveu model Institut fur Theoretische Physik, | ||
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Summary: at sufficently high temperature. For two flavours the symmetry restoring transition is widely accepted... 1 Chiral symmetry restoration of QCD and the Gross-Neveu model T. Reisza a Institut f... ¨ur Theoretische Physik, Universit¨at Heidelberg, Philosophenweg 16, D-69120 Heidelberg, Germany Two flavour |
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Source: Ecole Polytechnique, Centre de mathématiques |
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Collection: Mathematics |
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| 85 | Hot and Dense Hadronic Matter -Selected Topics - | ||
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Summary: ( · + 4 ^m0 - A4) + V(, ) , (4.2) where is the Nf = 2 doublet quark field and ^m0 = diag(mu, md... ) is the quark mass matrix. The quarks move in a background color gauge field A4 T = iA0, where #12;Hot... = n ± A4, 0 = n and (n, p ) = m0 + C(n, p )¯. Above Tc ... |
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Source: Weise, Wolfram - Physik Department, Technische Universität München |
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Collection: Physics |
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| 86 | R. Barbieri PLHC 2011, Perugia, June 5-11 | ||
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Summary: ;Some (approximate) flavour symmetry must be operative U(2) q3 q1,2 with little communication between... R. Barbieri PLHC 2011, Perugia, June 5-11 EWSB: Which physical origin for the Fermi scale? Flavour... tests (EWPT, flavour) indicate no new scale below several TeV's, the Higgs boson mass is apparently |
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Source: Abbondandolo, Alberto - Scuola Normale Superiore of Pisa |
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Collection: Mathematics |
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| 87 | Nuclear PhysicsB225 [FS9] (1983) 475-496 North-Holland PublishingCompany | ||
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Summary: will assume that flavour symmetry is unbroken. Fermions on the lattice are usually described by the Wilson [13... get in this way Rl(t) ~ e-m'~°q=°+ e-M'-lt'=l R2(t) - e -m'-°'=°- e -M'=I'-' . (A.4) If the mass... to compute the flavour singlet sector of the massspectrum, and comment ... |
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Source: Hamber, Herbert W. - Department of Physics, University of California, Irvine |
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Collection: Physics |
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| 88 | Vol. 39 (2008) ACTA PHYSICA POLONICA B No 12 A COMPARISON OF THE CUT-OFF EFFECTS FOR | ||
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Summary: - doubled fermions3. They describe two flavours of quarks and preserve exact chiral symmetry. However... µ °p2 µ + M(p)2 , (6) where F(p) = 1 + a4 2 µ< ^p2 µ ^p2 , M(p) = 1 a 1 + ma 2 - 1 - ma 2 F(p)-1... of either explicitly breaking chiral symmetry (even in the massless limit), ... |
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Source: Magiera, Andrzej - Instytut Fizyki, Uniwersytet Jagiellonski |
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Collection: Physics |
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| 89 | Vol. 38 (2007) ACTA PHYSICA POLONICA B No 9 MERGING FLAVOUR SYMMETRIES | ||
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Summary: Vol. 38 (2007) ACTA PHYSICA POLONICA B No 9 MERGING FLAVOUR SYMMETRIES WITH QCD FACTORISATION FOR B... (Received June 28, 2007) The interplay between flavour symmetries connecting Bs KK decays with the recently... : flavour symmetries and 1/mb-expansion methods (QCD ... |
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Source: Magiera, Andrzej - Instytut Fizyki, Uniwersytet Jagiellonski |
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Collection: Physics |
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| 90 | Glueballs, Hybrids, Multiquarks. Experimental facts versus QCD inspired concepts. | ||
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Summary: breaks SU(3) symmetry and transforms f0(980) into state with a 1 2 (u¯u + d ¯d)s¯s flavour structure... doubt and there is evidence that both f0(1500) and f0(1710) are flavour octet states, possibly... background into which all scalar flavour singlet mesons collapse. There is an abundance of meson ... |
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Source: Bonn, Universität - Physikalisches Institut, Crystal Barrel Experiment an ELSA |
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Collection: Physics |
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| 91 | hepph/9902437 Preprint typeset in JHEP style. HYPER VERSION LU TP 9902 | ||
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Summary: n (OE; j) + hX 2 (OE; j)E 2n\Gamma2 (OE; j)i) : (A.4) The last terms are the EOM terms of chiral... , this also holds for the matrices E 2n (OE; j) in (A.4). In particular, E 2n (OE; j) can be taken... to be traceless in all generality since the trace of E 2n (OE; j) does not contribute in ... |
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Source: Lunds Universitet, - Computational Biology and Biological Physics Group |
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Collection: Physics ; Biology and Medicine |
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| 92 | PHASES of QCD -LatticeThermodynamics vs. PNJL Model - | ||
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Summary: . Polyakov Loop (ThermalWilson Line) L(x) = P exp i = 1 T 0 d A4(x, ) #12;Phases of QCD Comparison... Tr L = 1 3 Tr exp (iA4/T) Dµ = µ - iAµ V([A], ¯[A]; T) Aµ = µ0 A0 treat as classical field thermal... SU(N ) gauge symmetry of QCD c GLOBAL SU(N ) symmetry of ... |
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Source: Weise, Wolfram - Physik Department, Technische Universität München |
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Collection: Physics |
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| 93 | Symmetry Breaking Patterns in QCD: CHIRAL and DECONFINEMENT Transitions | ||
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Summary: interaction Temporal background gauge field Polyakov loop = 3 3 + 8 8 = 1 Nc Tr exp i 1/T 0 d A4 1 3 Tr exp... (i n + m, k + p )2 (i n)2 + k 2 + Mi(i n, ± n = n ± A4, 0 = n and M(n, p ) = mq + C(n, p... Symmetry Breaking Patterns in QCD: CHIRAL and DECONFINEMENT Transitions Wolfram ... |
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Source: Weise, Wolfram - Physik Department, Technische Universität München |
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Collection: Physics |
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| 94 | PHASES of QCD LATTICE THERMODYNAMICS and QUASIPARTICLES | ||
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Summary: background gauge field Polyakov loop = 3 3 + 8 8 = 1 Nc Tr exp i 1/T 0 d A4 1 3 Tr exp(i/T) SU(3... )) 2.2 Polyakov Loop (Thermal Wilson Line) = 1 Nc Tr exp i 1/T 0 d A4 1 3 Tr exp(i/T) = 3 3 + 8 8... introductory guide through the #12;SYMMETRIES and SYMMETRY ... |
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Source: Weise, Wolfram - Physik Department, Technische Universität München |
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Collection: Physics |
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| 95 | Vol. 41 (2010) ACTA PHYSICA POLONICA B No 1 INSIGHTS FROM THE INTERPLAY OF K | ||
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Summary: be written as [5,11,22] Br(K+ + ¯) = + ~r2 A4 R2 t |XK|2 + 2~r ¯Pc(x)A2 Rt|XK| cos K X + ¯Pc(x)2 , (12) Br... (KL 0 ¯) = L~r2 A4 R2 t |XK|2 sin2 K X , (13) with XK = X0(xt) + 1 (K) t RK¯ eiK¯ |XK| eiK X , (14) K... 2 A4 R2 t X0(xt)2 cos2 ( - s) + 2~r ... |
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Source: Magiera, Andrzej - Instytut Fizyki, Uniwersytet Jagiellonski |
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Collection: Physics |
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| 96 | Universite Joseph Fourier -Grenoble 1 Ecole doctorale de Physique | ||
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Summary: symmetry breaking and particle mixing . . . . . 13 2.3 The MSSM with non-minimal flavour violation... Docteur en Sciences de l'Universit´e Joseph Fourier QCD-resummation and non-minimal flavour... effects of flavour violation may occur. In this case, the flavour structure in the squark ... |
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Source: Ecole Polytechnique, Centre de mathématiques |
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Collection: Mathematics |
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| 97 | Knowledge Transfer Centre University of Reading, Whiteknights, Reading, RG6 6AH Tel: +44 (0)118 378 8628 Email: workingwithbusiness@reading.ac.uk www.reading.ac.uk/working-with-business | ||
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Summary: and technology. · The Flavour Centre (FC) at the University of Reading provides clients with an understanding... of the flavour chemistry of their products and provides consultancy and technical expertise during the product... by the Flavour Chemistry Research Group (FCRG) at the University of Reading led to a joint research ... |
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Source: Reading, University of - School of Systems Engineering, Ambient and Pervasive Intelligence Research Group |
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Collection: Engineering ; Computer Technologies and Information Sciences |
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| 98 | GLAS-PPE/2009-26 November 2009 | ||
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Summary: to be carried out, both at LHCb, LHC's dedicated heavy flavour experiment, and at ATLAS and CMS. The aim... of these studies is to over-constrain the CKM matrix in order to search for New Physics in the flavour sector... it would be directly discovered. And even in the era of the Large Hadron Collider (LHC), flavour studies |
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Source: Glasgow, University of - Department of Physics and Astronomy, Particle Physics Experimental Group |
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Collection: Physics |
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| 99 | Modelling the CHIRAL and DECONFINEMENT | ||
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Summary: ;DECONFINEMENT and spontaneous breaking of Z(3) SYMMETRY (x ) = 1 Nc Tr exp i 1 T 0 d A4(x , ) R. Pisarski (2000... i 1/T 0 d A4 1 3 Tr exp(i/T) = 3 3 + 8 8 SU(3) { Effective potential : A global symmetry emerges... Lagrangian: - Polyakov Loop: = 3 3 + 8 8 ... |
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Source: Weise, Wolfram - Physik Department, Technische Universität München |
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Collection: Physics |
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| 100 | Particle Physics Phenomenology 7. Hadronization | ||
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Summary: causally disconnected can proceed in arbitrary order leftright symmetry P(1, 2) = P(1) × P(1 2) = P(2... ¨ostrand PPP 7: Hadronization slide 19/47 #12;Flavour composition Combination of q from one break and q (qq... ". There is one V and one PS for each qq flavour set, but baryons are more complicated, e.g. uuu ++ whereas ... |
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Source: Sjöstrand, Torbjörn - Department of Theoretical Physics, Lunds Universitet |
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Collection: Physics |
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