2005 CERN-CLAF School of High-Energy Physics: Malargüe, Argentina, 27 February-12 March 2005 : Proceedings, Issue 15Nick Ellis |
From inside the book
Results 1-3 of 28
Page 6
... observables are represented by self - adjoint operators that in the Heisenberg picture depend on time . Therefore measurements are localized in time but are global in space . The situation is radically different in the relativistic case ...
... observables are represented by self - adjoint operators that in the Heisenberg picture depend on time . Therefore measurements are localized in time but are global in space . The situation is radically different in the relativistic case ...
Page 92
... observables in hadronic collisions : Σ / f ( x1 , Qi ) ƒk ( x2 . Qi ) do dX = j , k where dôjk ( Qi › Qƒ ) F ( X → X ; Qi , Qf ) , ( 47 ) dX X is some hadronic observable ( e.g. , the transverse momentum of a pion ) ; the sum over j ...
... observables in hadronic collisions : Σ / f ( x1 , Qi ) ƒk ( x2 . Qi ) do dX = j , k where dôjk ( Qi › Qƒ ) F ( X → X ; Qi , Qf ) , ( 47 ) dX X is some hadronic observable ( e.g. , the transverse momentum of a pion ) ; the sum over j ...
Page 134
... observables are correlated within the SM . For ex- ample , the SM predicts that the CP asymmetries in B → Ks and in B Ks , which proceed through different quark transitions , are equal to each other ( to a few per cent accuracy ) [ 36 ...
... observables are correlated within the SM . For ex- ample , the SM predicts that the CP asymmetries in B → Ks and in B Ks , which proceed through different quark transitions , are equal to each other ( to a few per cent accuracy ) [ 36 ...
Contents
Introduction to QCD in hadronic collisions | 81 |
CP violation in meson decays | 131 |
Experimental aspects of cosmic rays | 177 |
Copyright | |
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air showers amplitude angle anomaly Auger Observatory bosons calculation calorimeter charged particles Cherenkov collisions colour constraints contribution cosmic rays coupling constant CP violation cross-section dead-time decays defined density depends detector diagram Dirac effect electric field electromagnetic electrons emission energy equation event example experimental fermions flavour fluorescence gauge group gauge invariance gauge transformations given gluon hadronic Hamiltonian high-energy integral interaction ionization Lagrangian lepton Lett Lorentz LVL1 trigger magnetic field mass massless matrix measurements meson momentum muons neutrinos non-Abelian Nucl observables operators pair parameters parton perturbation phase photon Phys physics Pierre Auger Observatory potential processes quantization quantum field theory quark radiation readout renormalization representation result scalar field scale shown in Fig signal spinor Standard Model supersymmetric symmetry T/DAQ Tevatron vacuum vector Xmax