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Concepts of the Standard Model: renormalisation FK8022, Lecture 2 Core text: Quarks and leptons: an introductory course in modern physics, Halzen and Martin Further reading: Basics of QCD perturbation theory, D.E. Soper (hep-ph/9702203)
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Lecture outline Infinities arising from loops – Regularisation – Reparameterisation of charge – Renormalisation finite charge, amplitude Renormalisation scale Running of couplings
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A simple QED process e e p1p1 p2p2 p4p4 p3p3 q
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Adding a higher order process + e e ee ee
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Renormalised charge
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Bare and renormalised charges
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Defining the coupling at a scale
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Renormalisation scale [] -- + higher orders (A)(B)(C)
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Higher orders }
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Scale dependence of amplitude r(Q2)r(Q2) Order of calculation e scattering Single photon exchange
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Running coupling
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Consistency check
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Divergence in amplitude from higher order loop Make finite by redefining coupling/charge and remove infinity For a complete expansion the amplitude is independent of r Renormalisation Finite expression for running of coupling/charge with r Coupling/charge depends on an arbitrary kinematic scale r for a given interaction
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Renormalisation works: electromagnetic coupling running Interaction distance (momentum transfer) 2 /GeV 2 Tiny shift
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Physical interpretation of the running coupling + e-e- e-e- e-e- e-e- e-e- e-e- e-e- e +,e - Distance scale Coupling
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Renormalisation of other quantities Different loop diagrams cause other physical quantities to be renormalised. Eg mass Masses also run:
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What about the strong force ? qq qq qq qq qq qq qq qq q,q + other higher order diagrams
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Asymptotic freedom ss Momentum transfer / GeV Interaction distance
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Renormalisation scale setting
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Scale variation
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Summary and discussion (1)
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Summary and discussion (2)
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Summary and discussion (3)
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