
AbstractThese Gamow kets span an irreducible representation space for Poincaré transformations which, similar to the Wigner representations for stable particles, are characterized by spin (angular momentum of the partial wave amplitude) and complex mass (position of the resonance pole). The Poincaré transformations of the Gamow kets, as well as of the Lippmann‐Schwinger plane wave scattering states, form only a semigroup of Poincaré transformations into the forward light cone. Their transformation properties are derived. From these one obtains an unambiguous definition of resonance mass and width for relativistic resonances. The physical interpretation of these transformations for the Born probabilities and the problem of causality in relativistic quantum physics is discussed.
High Energy Physics - Theory, Special relativity, Quantum Physics, pole position, FOS: Physical sciences, General and philosophical questions in quantum theory, Quantum measurement theory, state operations, state preparations, life time \(\tau_R\) of the resonance, Mathematical Physics (math-ph), Poincaré semigroup, High Energy Physics - Theory (hep-th), relativistic resonances, Resonance in context of PDEs, S-matrix, transformation property of the Gamow vectors, Quantum Physics (quant-ph), Mathematical Physics, \(S\)-matrix theory, etc. in quantum theory
High Energy Physics - Theory, Special relativity, Quantum Physics, pole position, FOS: Physical sciences, General and philosophical questions in quantum theory, Quantum measurement theory, state operations, state preparations, life time \(\tau_R\) of the resonance, Mathematical Physics (math-ph), Poincaré semigroup, High Energy Physics - Theory (hep-th), relativistic resonances, Resonance in context of PDEs, S-matrix, transformation property of the Gamow vectors, Quantum Physics (quant-ph), Mathematical Physics, \(S\)-matrix theory, etc. in quantum theory
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