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Prog. Theor. Phys. Vol. 45 No. 6 (1971) pp. 1849-1878

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Hadron Reactions and Urbaryon Rearrangement. I

— Effective Resonance Structure —

Masahiro Imachi, Takashige Oroguchi, Shoichiro Otsuki and Fumihiko Toyoda*

Department of Physics, Kyushu University, Fukuoka
*The Second Department, Kinki University, Iizuka

(Received November 27, 1970)

Abstract:

By incorporating dynamical aspects of hadron reactions, which closely correspond to the pattern of the urbaryon rearrangement diagram (URD), P8-B8 reaction amplitude is constructed in the impact parameter representation. The main dynamical aspects are that the impact parameter to form observed resonances in P8-B8 reaction takes an almost universal value and that angular distributions have almost energy-independent dips (with the positions t0:t1:t2 and/or u0':u1':u2'≃1:4:9) in such processes that contain the H(s-t dual) and/or Z(s-u dual) type URD amplitudes. Then the interaction densities of these amplitudes are peaked at a constant value b0 of the impact parameter, which we call resonant interaction density. The constant b0 implies a bending effective resonance trajectory αeff\undersets≫1∼√s, and αeff coincides with leading trajectories when s is not large. On the contrary, the interaction density of the X(t-u dual) type URD amplitude has a simple Gaussian form. The s dependence of the interaction densities is described by s-rnR with γ∼0.5, where nR denotes the number of rearranged urbaryons. Quantitative fit of our amplitude to elastic π-N scattering in the forward hemi-sphere and qualitative fit to other P8-B8 reactions in the forward and the backward regions are given. The effective resonances in the URD amplitude and the s-rnR behaviour imply systematic correlations of resonances in the hadron level and may afford clues to the nature of the urbaryon. The interaction densities are related to hadron electromagnetic form factors.


URL : http://ptp.ipap.jp/link?PTP/45/1849/
DOI : 10.1143/PTP.45.1849

[ Full Text PDF : FREE ACCESS (1854K) ] Citation:


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