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NEW TRENDS IN HIGH-ENERGY PHYSICS (experiment, phenomenology, theory)

NEW TRENDS IN HIGH-ENERGY PHYSICS (experiment, phenomenology, theory) Alushta , Crimea, Ukraine, September 23-29, 2013. Volodymyr Magas. Effects of the next-to-leading order terms in the chiral SU(3) Lagrangian on the S=-1 s-wave meson-baryon interactions.

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NEW TRENDS IN HIGH-ENERGY PHYSICS (experiment, phenomenology, theory)

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  1. NEW TRENDS IN HIGH-ENERGY PHYSICS(experiment, phenomenology, theory) Alushta, Crimea, Ukraine, September 23-29, 2013 Volodymyr Magas Effects of the next-to-leading order terms in the chiral SU(3) Lagrangianon the S=-1 s-wave meson-baryon interactions In collaboration with A. Ramos, A. Feijoo Aliau University of Barcelona, Spain

  2. Perturbative QCD, with quark and gluond.o.f., works well at high energies and high momentum transfers, but fails to describe dynamics of hadrons at low energies Chiral Perturbation Theory: which is based on effective Lagrangian with hadron d.o.f.,which respects the symmetries of QCD, in particular chiral symmetry

  3. Perturbative QCD, with quark and gluond.o.f., works well at high energies and high momentum transfers, but fails to describe dynamics of hadrons at low energies Chiral Perturbation Theory: which is based on effective Lagrangian with hadron d.o.f.,which respects the symmetries of QCD, in particular chiral symmetry The spontaneous chiral symmetry breaking causes the appearance of the Nambu–Goldstone (NG) bosons as the light pseudoscalar mesons and the dynamical mass generation of hadrons.

  4. Baryon meson interaction at lowest order WT: Weimberg-Tomozawa term

  5. WT baryon meson interaction

  6. WT baryon meson interaction The only model parameter is pion decay constant, f En real calculations it is usually taken in order to partly simulate effects of higher order corrections

  7. Perturbative QCD, with quark and gluond.o.f., works well at high energies and high momentum transfers, but fails to describe dynamics of hadrons at low energies Chiral Perturbation Theory: which is based on effective Lagrangian with hadron d.o.f.,which respects the symmetries of QCD, in particular chiral symmetry Unitary extension of Chiral Perturbation Theory The pioneering work -- Kaiser, Siegel, Weise , NP A594 (1995) 325

  8. Lippmann-Schwinger equation On shell factorization System of the algebraic equations Máster Interuniversitario de Física Nuclear (UB)

  9. Loop function

  10. Λ(1405) as a dynamically generated resonance Jones, Dalitz and Horgan, Nucl. Phys. B129 (1977) 45– Λ(1405) is dynamical generated Boost in unitary extensions of chiral perturbation theory 1995-2003: Kaiser, Oset, Ramos, Oller, Meissner, Jido, Hosaka, Garcia-Recio, Vicente Vacas

  11. Λ(1405) as a dynamically generated resonance Jones, Dalitz and Horgan, Nucl. Phys. B129 (1977) 45– Λ(1405) is dynamical generated Boost in unitary extensions of chiral perturbation theory 1995-2003: Kaiser, Oset, Ramos, Oller, Meissner, Jido, Hosaka, Garcia-Recio, Vicente Vacas Surprisingly there are two poles in the neighborhood of the Λ(1405) both contributing to the final experimental invariant mass distribution Mass ~ 1390 MeV Width ~ 130 MeV Mass ~ 1425 MeVWidth ~ 30 MeV

  12. The observed shapes are in good agreement with corresponding chiral unitarity model calculations:  Magas, Oset, Ramos, Phys. Rev. Lett. 95 (05) 052301  Thomas et al., Nucl. Phys. B56 (1973) 15 This combined study gives the first experimental evidence of the two-pole nature of the Λ(1405)

  13. Crystall Ball Collaboration data from (Width ~ 38 MeV) versus Thomas et al., NP B 56 (1973) 15 (Width ~ 60 MeV) Magas, Oset, Ramos, PRL 95 (2005) 052301;also presented at Crimea’2005

  14. Chiral meson-baryon effective Lagrangian at NLO • Recent Publications: • B. Borasoy, R. Nißler, W. Wiese, Eur. Phys. J. A25 (2005) 79 • - Y. Ikeda, T. Hyodo, W. Wiese, Phys. Lett. B706 (2011) 63;Nucl. Phys. A881 (2012) 98 • A. Feijoo Aliau, MasterThesis, U. of Barcelona (Nov 2012) • Z.-H. Guo, J.A. Oller, Phys. Rev. C87 (2013) 035202

  15. Chiral meson-baryon effective Lagrangian at NLO - is the symmetry breaking term

  16. Chiral meson-baryon effective Lagrangian at NLO - is the symmetry breaking term 7 new parameters to be fixed:

  17. Chiral meson-baryon effective Lagrangian at NLO • WT, lowest order term • Next – to – Leading Order term Máster Interuniversitario de Física Nuclear (UB)

  18. Chiral meson-baryon effective Lagrangian at NLO • WT, lowest order term At low energies • Next – to – Leading Order term Máster Interuniversitario de Física Nuclear (UB)

  19. Experimental data - Cross sections for different channels - Branching ratios Máster Interuniversitario de Física Nuclear (UB)

  20. Fitting parameters • Decay constant f • 7 parameters of the NLO Lagrangian: • - 10 subtracting constants 6 constants: isospin symmetry Máster Interuniversitario de Física Nuclear (UB)

  21. Fitting parameters [1] Borasoy, Nißler, Wiese, Eur. Phys. J. A25 (2005) 79

  22. Results • Branching ratios [1] Borasoy, Nißler, Wiese, Eur. Phys. J. A25 (2005) 79 Máster Interuniversitario de Física Nuclear (UB)

  23. Results

  24. Results

  25. These are particularly interesting for us, because for WT interaction channels are very sensitive to the NLO terms in the Lagrangian Also these channels are not included in the other fits!B. Borasoy, R. Nißler, W. Wiese, Eur. Phys. J. A25 (2005) 79 Y. Ikeda, T. Hyodo, W. Wiese, Phys. Lett. B706 (2011) 63; Nucl. Phys. A881 (2012) 98Z.-H. Guo, J.A. Oller, Phys. Rev. C87 (2013) 035202 But studied in the phenomenological model of D. A. Sharov, V. L. Korotkikh, D. E. Lanskoy, Eur. Phys. J. A47 (2011) 109

  26. - Missing contribution from the heavy high spin resonances

  27. In Ref. [Sharov, Korotkikh, Lanskoy, EPJ A47 (11) 109] , trying different combinations, the author conclude thatΣ(2030) and Σ(2250) give the better fit to the data Máster Interuniversitario de Física Nuclear (UB)

  28. Work in progress The propagators of the spin-5/2 and -7/2 fermion fields K. Nakayama, Youngseok Oh, H. Habertzettl, Phys. Rev. C74, 035205 (2006) K. Shing Man, Youngseok Oh, K. Nakayama,, Phys. Rev. C83, 055201 (2011)

  29. Conclusions Chiral Perturbation Theory with unitarization in coupled channels is a very powerful technique to describe low energy hadron dynamics Next – to – leading order calculations are now possible NLO terms in the Lagrangian do improve agreement with data are very interesting and important for fitting NLO parameters Work in progress…

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