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Effective Field Theory of the PionNucleonInteraction
Effective Field Theory of the Pion-Nucleon-Interaction∗
H. Leutwyler
Institute for Theoretical Physics, University of Bern, Sidlerstr. 5, CH-3012 Bern,
Switzerland
Abstract
In the first part of the talk, I discussed the nature of the effective theory that
describes the properties of the pion-nucleon-interaction at low energies, using the
static model as a starting point. In the second part, I then pointed out that the
infrared singularities occurring in the πN scattering amplitude are stronger and of a
0 more complex structure than those encountered in ππ scattering. A formulation of the
0 effective theory that properly accounts for these was described and the results obtained
0
2 thereby were illustrated with a few examples. In the following, I restrict myself to a
discussion of some qualitative aspects of this work.
g
u
A INTRODUCTION
2 The static model represents a forerunner of the effective theories of the pion-nucleon
1 interaction used today. In this model, the kinetic energy of the nucleon is neglected: The
nucleon is described as a fixed source that only carries spin and isospin degrees of freedom.
1 For an excellent review of the model and its application to several processes of interest, I
v refer to the book of Henley and Thirring[1].
3
2 The systematic formulation of the effective theory relies on an expansion of the effective
1 Lagrangian in powers of derivatives and quark
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