The three-body Helmholtz operator at positive energy induces Fredholm maps on anisotropic spaces after constructing a conormal three-cone algebra modified by second microlocalization and blow-ups.
Propagation of singularities in many-body scattering
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Second microlocalization and Fredholm theory for the three-body problem
The three-body Helmholtz operator at positive energy induces Fredholm maps on anisotropic spaces after constructing a conormal three-cone algebra modified by second microlocalization and blow-ups.