ar X iv : h ep - p h / 04 06 27 1 v 2 2 6 N ov 2 00 4 The pole structure of the unitary , crossing symmetric low energy ππ scattering amplitudes
نویسندگان
چکیده
The pole structure of the low energy ππ scattering amplitudes is studied using a proper chiral unitarization method combined with crossing symmetry and the low energy phase shift data. It is found that the σ pole position is at M σ = 470 ± 50M eV , Γ σ = 570 ± 50M eV. The existence of the virtual state pole in the IJ=20 channel is reconfirmed. Various threshold parameters are estimated and are found in general in good agreement with the results obtained from the Roy equation analyses. The σ or the f 0 (600) resonance has attracted much interest in recent years [1] and more and more physicists, if not all, believe that it truly exists as a light and broad resonance. [2] There were two main difficulties to accept the σ resonance, one is that being light and broad makes the σ's contribution to the phase shift hard to be distinguishable from background contributions while the latter are often out of control in various phenomenological studies. However , a careful analysis revealed that the cut contribution to the phase shift is negative in the I,J=0,0 channel ππ scattering [3], and thus the σ resonance has to exist to saturate the experimental data. Another objection is that the ππ phase shift in the I=0, J=0 channel does not pass π/2 at moderately low energies which should have appeared if there exist a light σ as required by the standard Breit–Wigner description of resonances. However it is pointed out that a light and broad resonance rejects a simple Breit-Wigner description. As
منابع مشابه
X iv : h ep - p h / 04 06 27 1 v 1 2 4 Ju n 20 04 The pole structure of the unitary , crossing symmetric low energy ππ scattering amplitudes
The pole structure of the low energy ππ scattering amplitudes is studied using a proper chiral unitarization method combined with crossing symmetry and the low energy phase shift data. It is found that the σ position is at M σ = 456 ± 30M eV , Γ σ = 580 ± 50M eV. The existence of the virtual state pole in the IJ=20 channel is reconfirmed. Various threshold parameters are estimated and are found...
متن کاملar X iv : h ep - p h / 06 11 27 1 v 2 2 2 N ov 2 00 6 Structure of the axial - vector meson D s 1 ( 2460 )
متن کامل
ar X iv : h ep - p h / 06 11 27 1 v 1 2 1 N ov 2 00 6 Structure of the axial - vector meson D s 1 ( 2460 )
متن کامل
ar X iv : h ep - p h / 05 10 21 8 v 1 1 7 O ct 2 00 5 ππ scattering amplitudes constrained
The scalar-isoscalar, scalar-isotensor and vector-isovector ππ amplitudes have been fitted simultaneously to experimental data and to to Roy’s equations. Resulting ππ phase shifts up to 1600 MeV and near threshold observables have been analyzed. Only the amplitudes fitted to the ”down-flat” set of phase shifts in scalarisoscalar wave fulfill crossing symmetry conditions and can be regarded as p...
متن کاملar X iv : h ep - p h / 03 10 08 2 v 1 7 O ct 2 00 3 Roy ’ s equations and the ππ experimental data
Roy’s equations are used to check if the scalar-isoscalar ππ scattering amplitudes fitted to experimental data fulfill crossing symmetry conditions. It is shown that the amplitudes describing the “down-flat” phase shift solution satisfy crossing symmetry below 1 GeV while the amplitudes fitted to the “up-flat” data do not. In this way the long standing ”up-down” ambiguity in the phenomenologica...
متن کامل