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Quarks, partones y QCD.

Quarks, partones y QCD. Rodolfo Sassot Departamento de Fisica, FCEyN, UBA. Porqu é QCD ?. Motivaci ón estadística: antisimetrización f.o. SU(3) f. SU(3) c. Motivaci ón fenomenológica: (e + e - → hadrones) / (e + e - → μ + μ - ).

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Quarks, partones y QCD.

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  1. Quarks, partones y QCD. Rodolfo Sassot Departamento de Fisica, FCEyN, UBA.

  2. Porqué QCD? Motivación estadística: antisimetrización f.o. SU(3)f SU(3)c Motivación fenomenológica: (e+e-→ hadrones) / (e+e- → μ+μ- ) “La Motivación” : dinámica interacciones fuertes dinámica de SU(3)c

  3. Modelo de partones: 2 cuadri-impulsos salientes: 8 conservación E-P: -4 mass shell x2: -2 simetría CM: -1 1 variable independiente 1967: Bjorken “scaling” 1969: SLAC 1969: Feynman “partones libres” modelo de partones 1969: Callan-Gross “spin 1/2”

  4. Modelo de partones: “puntual” “densidad de probabillidad” “define” lo que es “los partones no son los quarks SU(3)”

  5. Modelo de partones: 2 variables:

  6. Modelo de partones: 2 variables:

  7. Modelo de partones: SLAC 1970 HERA 2000

  8. Stanford Linear Accelerator Center (SLAC)

  9. Large Hadron Collider(LHC) p p @ 14 TeV 0.999999 c

  10. ATLAS: 1800 físicos, 34 países

  11. DGLAP mantra: LO, NLO, … ‘naïve’ ‘LO’

  12. DGLAP mantra: LO, NLO, …

  13. DGLAP mantra: LO, NLO, … ‘naïve’ ‘LO’ ‘NLO’ ‘add a gluon’

  14. high-x low-x charged/neutral

  15. TEVATRON @ FNAL jets in p-pbar

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