1. Signature of strange dibaryon in kaon-induced reaction Shota Ohnishi A in collaboration with; Y. Ikeda B, H. Kamano C, T. Sato A A; Department of Physics, Osaka University B; Department of Physics, Tokyo Institute of Technology C; Department of Physics, Osaka City University

2. Contents Introduction Three-body Scattering Equation Model of 2-body Interaction Results Conclusion

3. Introduction Three-body Scattering Equation Model of 2-body Interaction Results Conclusion

4. J  =1/2 -,  q^3(uds): P-wave excited state  unstable bound state Dalitz, Wong, Tajasekaran, PR 153(1967)1617 strongly attractive interaction in I=0, L=0 deeply bound kaonic nuclei are proposed u d s Yamazaki, Akaishi, PLB535, 70(2002)

5. simplest deeply bound kaonic nuclei many particle dynamics can be examined accurately theoretical analyses: strange dibaryon phenomenologicalChiral SU(3) FaddeevShevchenko, Gal, MaresIkeda, Sato VariationalAkaishi, Yamazaki Wycech, Green Doté, Hyodo, Weise

6. signal of strange dibaryon resonance from reactions Optical potential approach : Koike, Harada, PRC80, 055208(2009) Purpose of this work : within Faddeev approach –study 3-body scattering amplitude –examine signal of strange dibaryon resonances –examine dynamics of in resonance production reaction ・・・ strange dibaryon

7. Introduction Three-body Scattering Equation Model of 2-body Interaction Results Conclusion

8. Coupled channel equation for Faddeev eq. separable 2-body Interaction ； Alt-Grassberger-Sandhas(AGS) eq. : X ij ； quasi two-body amplitude

9. Singularity of particle exchange interaction methods to handle moon shape singularity numerically spline interpolation, point method moon shape singularity Z-diagram

10. Point method L. Schlessinger, PR 167, 1411(1968) evaluate X at finite  i Extrapolate X at  =0 continued fraction Kamada, Koike, Glökle, TP 109 (2003), 869.

11. Introduction Three-body Scattering Equation Model of 2-body Interaction Results Conclusion

12. Interaction meson-baryon interaction based on WT Lagrangian “energy-independent” potentials (static approximation ) “energy-dependent” potentials E; two body scattering energy (chiral unitary)

13. pole positions of two-body amplitude E-indep.; only one poleE-dep.; two poles ~ chiral unitary model Possibility to distinguish two models from strange dibaryon production reaction * two Y* resonances : Jido, Oller, Oset, Ramos, Meissner, NPA 725(2003)263

14. Introduction Three-body Scattering Equation Model of 2-body Interaction Results Conclusion

15. Model of system 2-body meson-baryon interaction ; 3-body particle exchange ( Z) interaction report on our first results on only meson-baryon S=-1 interaction, only kaon exchange Z.

16. |X(W,p’,p)| 2 W1W1 W1W1 W 1’ W1 depend on momentum. correspond to moon shape singularity

17. |X(W,p’,p)| 2 W1W1 W1W1 W 1’ W1 depend on momentum. correspond to moon shape singularity resonance Quasi two-body amplitudes depend on two-body potential models.

18. Introduction Three-body Scattering Equation Model of 2-body Interaction Results Conclusion

19. Signal of dibaryon resonance shows up in the quasi two-body amplitude X. Strange dibaryon production reaction can be used to distinguish dynamical model of  (1405). Future plan Include complete 3-body dynamics (include N and  exchange Z) Study, etc.

20. Thank you!

21. test of approximation method three identical bosons model of Amado scattering of a boson b from a two-boson bound state d We can use this method for coupled-channel AGS eq. Matsuyama, Sato, Lee, PR439, 193(2003) m; boson mass, E; total energy, B; two-body binding energy,  ; cut-off

22. model dependence of X Three-body amplitudes depend on two-body potential models.

23. |X(W,p’,p)| 2 W1W1 W1W1

24. cutoff (model parameters) cutoff which reproduce invariant mass & 2-body cross sections.

25. pole positions of strange dibaryon