[en] Abstract only

No abstract available

[en] For n non relativistic fermions and for fairly general one-body and two-body interactions, the Hamiltonian is a selfadjoint extension of a simple Hermitian operator. Several consequences for the discrete eigenvalues are deduced from this property, such as new integral equations and the coupling of the eigenvalues for n-fermions to the eigenvalues for n-1 fermions

[en] Two-body systems of predictive mechanics are compared with single particle systems in a potential. Study of the limit where one of the bodies is fixed

[en] The two-body scattering problem is generalized in L²(R³) for Schroedinger operators with momentum dependent interactions. Wave operators are derived

[en] We propose a new approach to treat the nucleon structure in terms of an effective chiral Lagrangian. The state vector of the nucleon is defined on the light front plane and is decomposed in Fock components. An adequate Fock sector dependent renormalization scheme is applied. We present our first results of the calculation of nucleon properties in a two-body Fock truncation.

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No abstract available

[en] We explore the properties of weakly bound bosonic states in the strongly interacting regime. Combining a correlated-Gaussian basis set expansion with a complex-scaling method, we extract the energies and structural properties of bosonic cluster states with N≤6 for different two-body potentials. The identification of five- and six-body resonances attached to the first-excited-Efimov trimer provides strong support to the premise of Efimov universality in bosonic systems. Our study also reveals a rich structure of bosonic cluster states. Besides the lowest cluster states that behave as bosonic droplets, we identify cluster states weakly bound to one or two atoms forming effective cluster-atom dimers and cluster-atom-atom 'trimers'. The experimental signatures of these cluster states are discussed.

No abstract available