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c, ΛΛ̄, one of these amplitudes vanishes in the pole model. However, one must be aware that in this model only lowest lying intermediate states of a spectrum that lies far way from the physical region were considered. Moreover, the model makes a delicate use of crossing symmetry. The actual amplitudes could differ from this simple minded model. For another quark model treatment, see A. Bousfiha, thesis, Faculté des Sciences de Rabat, 1997 .
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c, ΛΛ̄, one of these amplitudes vanishes in the pole model. However, one must be aware that in this model only lowest lying intermediate states of a spectrum that lies far way from the physical region were considered. Moreover, the model makes a delicate use of crossing symmetry. The actual amplitudes could differ from this simple minded model. For another quark model treatment, see A. Bousfiha, thesis, Faculté des Sciences de Rabat, 1997 .
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c, ΛΛ̄, one of these amplitudes vanishes in the pole model. However, one must be aware that in this model only lowest lying intermediate states of a spectrum that lies far way from the physical region were considered. Moreover, the model makes a delicate use of crossing symmetry. The actual amplitudes could differ from this simple minded model. For another quark model treatment, see A. Bousfiha, thesis, Faculté des Sciences de Rabat, 1997 .
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c, ΛΛ̄, one of these amplitudes vanishes in the pole model. However, one must be aware that in this model only lowest lying intermediate states of a spectrum that lies far way from the physical region were considered. Moreover, the model makes a delicate use of crossing symmetry. The actual amplitudes could differ from this simple minded model. For another quark model treatment, see A. Bousfiha, thesis, Faculté des Sciences de Rabat, 1997 .
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