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Preface | |
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Non-Abelian Symmetries | |
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Global Non-Abelian Symmetries | |
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The Standard Model | |
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The flavour symmetry SU(2)<sub>f</sub> | |
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The nucleon isospin doublet and the group SU(2) | |
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Larger (higher-dimensional) multiplets of SU(2) in nuclear physics | |
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Isospin in particle physics: flavour SU(2)<sub>f</sub> | |
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Flavour SU(3)<sub>f</sub> | |
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Non-Abelian global symmetries in Lagrangian quantum field theory | |
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SU(2)<sub>f</sub> and SU(3)<sub>f</sub> | |
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Chiral symmetry | |
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Problems | |
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Local Non-Abelian (Gauge) Symmetries | |
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Local SU(2) symmetry | |
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The covariant derivative and interactions with matter | |
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The non-Abelian field strength tensor | |
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Local SU(3) Symmetry | |
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Local non-Abelian symmetries in Lagrangian quantum field theory | |
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Local SU(2) and SU(3) Lagrangians | |
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Gauge field self-interactions | |
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Quantizing non-Abelian gauge fields | |
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Problems | |
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QCD and the Renormalization Group | |
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QCD I: Introduction, Tree Graph Predictions, and Jets | |
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The colour degree of freedom | |
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The dynamics of colour | |
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Colour as an SU(3) group | |
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Global SU(3)<sub>c</sub> invariance, and 'scalar gluons' | |
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Local SU(3)<sub>c</sub> invariance: the QCD Lagrangian | |
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The �-term | |
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Hard scattering processes, QCD tree graphs, and jets | |
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Introduction | |
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Two-jet events in pp collisions | |
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Three-jet events in pp collisions | |
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3-jet events in e<sup>+</sup>e<sup>-</sup> annihilation | |
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Calculation of the parton-level cross section | |
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Soft and collinear divergences | |
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Definition of the two-jet cross section in e<sup>+</sup>e<sup>-</sup> annihilation | |
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Further developments | |
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Test of non-Abelian nature of QCD in e<sup>+</sup>e<sup>-</sup> → 4 jets | |
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Jet algorithms | |
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Problems | |
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QCD II: Asymptotic Freedom, the Renormalization Group, and Scaling Violations | |
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Higher-order QCD corrections to �(e<sup>+</sup>e<sup>-</sup> → hadrons): large logarithms | |
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The renormalization group and related ideas in QED | |
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Where do the large logs come from? | |
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Changing the renormalization scale | |
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The RGE and large -q<sup>2</sup> behaviour in QED | |
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Back to QCD: asymptotic freedom | |
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One loop calculation | |
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Higher-order calculations, and experimental comparison | |
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�(e<sup>+</sup>e<sup>-</sup> → hadrons) revisited | |
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A more general form of the RGE: anomalous dimensions and running masses | |
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QCD corrections to the parton model predictions for deep inelastic scattering: scaling violations | |
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Uncancelled mass singularities at order �<sub>s</sub> | |
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Factorization, and the order �<sub>s</sub> DGLAP equation | |
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Comparison with experiment | |
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Problems | |
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Lattice Field Theory, and the Renormalization Group Revisited | |
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Introduction | |
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Discretization | |
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Scalar fields | |
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Dirac fields | |
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Gauge fields | |
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Representation of quantum amplitudes | |
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Quantum mechanics | |
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Quantum field theory | |
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Connection with statistical mechanics | |
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Renormalization, and the renormalization group, on the lattice | |
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Introduction | |
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Two one-dimensional examples | |
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Connections with particle physics | |
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Lattice QCD | |
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Introduction, and the continuum limit | |
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The static qq potential | |
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Calculation of �(M<sub>Z</sub><sup>2</sup>) | |
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Hadron masses | |
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Problems | |
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Spontaneously Broken Symmetry | |
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Spontaneously Broken Global Symmetry | |
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Introduction | |
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The Fabri-Picasso theorem | |
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Spontaneously broken symmetry in condensed matter physics | |
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The ferromagnet | |
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The Bogoliubov superfluid | |
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Goldstone's theorem | |
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Spontaneously broken global U(1) symmetry: the Goldstone model | |
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Spontaneously broken global non-Abelian symmetry | |
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The BCS superconducting ground state | |
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Problems | |
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Chiral Symmetry Breaking | |
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The Nambu analogy | |
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Two flavour QCD and SU(2)<sub>f L</sub> � SU(2)<sub>f R</sub> | |
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Pion decay and the Goldberger-Treiman relation | |
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Effective Lagrangians | |
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The linear and non-linear �-models | |
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Inclusion of explicit symmetry breaking: masses for pions and quarks | |
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Extension to SU(3)<sub>f L</sub> � SU(3)<sub>f R</sub> | |
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Chiral anomalies | |
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Problems | |
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Spontaneously Broken Local Symmetry | |
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Massive and massless vector particles | |
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The generation of 'photon mass' in a superconductor: Ginzburg-Landau theory and the Meissner effect | |
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Spontaneously broken local U(1) symmetry: the Abelian Higgs model | |
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Flux quantization in a superconductor | |
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't Hooft's gauges | |
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Spontaneously broken local SU(2) � U(1) symmetry | |
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Problems | |
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Weak Interactions and the Electroweak Theory | |
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Introduction to the Phenomenology of Weak Interactions | |
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Fermi's 'current-current' theory of nuclear �-decay, and its generalizations | |
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Parity violation in weak interactions, and V-A theory | |
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Parity violation | |
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V-A theory: chirality and helicity | |
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Lepton number and lepton flavours | |
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The universal current � current theory for weak interactions of leptons | |
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Calculation of the cross section for �<sub>�</sub> + e<sup>-</sup> → �<sup>-</sup> + �<sub>e</sub> | |
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Leptonic weak neutral currents | |
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Quark weak currents | |
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Two generations | |
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Deep inelastic neutrino scattering | |
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Three generations | |
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Non-leptonic weak interactions | |
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Problems | |
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CP Violation and Oscillation Phenomena | |
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Direct CP violation in B decays' | |
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CP violation in B meson oscillations | |
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Time-dependent mixing formalism | |
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Determination of the angles �(�<sub>2</sub>) and �( �<sub>1</sub>) of the unitarity triangle | |
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CP violation in neutral K-meson decays | |
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Neutrino mixing and oscillations | |
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Neutrino mass and mixing | |
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Neutrino oscillations: formulae | |
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Neutrino oscillations: experimental results | |
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Matter effects in neutrino oscillations | |
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Further developments | |
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Problems | |
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The Glashow-Salam-Weinberg Gauge Theory of Electroweak Interactions | |
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Difficulties with the current-current and 'naive' IVB models | |
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Violations of unitarity | |
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The problem of non-renormalizability in weak interactions | |
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The SU(2) � U(1) electroweak gauge theory | |
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Quantum number assignments; Higgs, W and Z masses | |
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The leptonic currents (massless neutrinos): relation to current-current model | |
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The quark currents | |
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Simple (tree-level) predictions | |
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The discovery of the W<sup>�</sup> and Z<sup>0</sup> at the CERN pp collider | |
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Production cross sections for W and Z in pp colliders | |
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Charge asymmetry in W<sup>�</sup> decay | |
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Discovery of the W<sup>�</sup> and Z<sup>0</sup> at the pp collider, and their properties | |
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Fermion masses | |
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One generation | |
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Three-generation mixing | |
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Higher-order corrections | |
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The top quark | |
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The Higgs sector | |
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Introduction | |
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Theoretical considerations concerning m<sub>H</sub> | |
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Higgs boson searches and the 2012 discovery | |
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Problems | |
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Group Theory | |
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Definition and simple examples | |
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Lie groups | |
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Generators of Lie groups | |
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Examples | |
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SO (3) and three-dimensional rotations | |
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SU(2) | |
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SO(4): The special orthogonal group in four dimensions | |
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The Lorentz group | |
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SU(3) | |
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Matrix representations of generators, and of Lie groups | |
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The Lorentz group | |
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The relation between SU(2) and SO(3) | |
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Geometrical Aspects of Gauge Fields | |
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Covariant derivatives and coordinate transformations | |
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Geometrical curvature and the gauge field strength tensor | |
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Dimensional Regularization | |
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Grassmann Variables | |
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Feynman Rules for Tree Graphs in QCD and the Electroweak Theory | |
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QCD | |
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External particles | |
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Propagators | |
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Vertices | |
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The electroweak theory | |
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External particles | |
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Propagators | |
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Vertices | |
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References | |
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Index | |