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The concept of scattering refers to physical process in which some matter or wave which has stable, say linear trajectory (or wave distribution) in distant past, comes into the area where it interacts with some localized perturbation (or other such waves), which results in different stable state (or distribution of states) in far future. Examples include light scattering, scattering of matter beams, scatterring of solitons and multisolitons (which preserve their identity after a long while), and scattering in quantum mechanics, including variants like QFT and superstring theory. The condition that the perturbation (interaction) is localized is someties relaxed (for example, in the case of the scattering for Schroedinger operator corresponding to the Coulomb potential, the waves are substantially perturbed even asymptotically at infinity, because the Coulomb potential does not fall sufficiently fast far away from the source).
The basic concepts are time evolution operator, adiabatic switching, interaction picture and the ingoing and outgoing states.
Scattering theory wants to predict the so called scattering data which give the distribution of scattered waves (particles), i.e. of outgoing states in terms of ingoing states and knowledge of the scattering interaction/potential on which the waves are scattered. This is the direct problem of scattering. Conversely, one can try to find out the potential/interaction by observing the results of scattering experiments, what boils to the knowledge of scattering data; hence finding the physics from knowledge of scattering data. Symbolically, fundamental physics experiments in fact seek for the interaction which will correspond to scattering data. However, when we try to do this literally, calculating the interaction potential from the scattering data, we call it the inverse scattering method. While in quantum mechanics, the inverse scattering method applies to a linear problem a variant applies to the study of nonlinear equations like nonlinear Schroedinger equation; some cases lead to the integrability at classical or at quantized level. Thus we have the classical and the quantum inverse scattering method? within the subject of integrable systems.
See the references at S-matrix.
See also
Classification of possible long-range forces, hence of scattering processes of massless fields, by classification of suitably factorizing and decaying Poincaré-invariant S-matrices depending on particle spin, leading to uniqueness statements about Maxwell/photon-, Yang-Mills/gluon-, gravity/graviton- and supergravity/gravitino-interactions:
Steven Weinberg, Feynman Rules for Any Spin. 2. Massless Particles, Phys. Rev. 134 (1964) B882 (doi:10.1103/PhysRev.134.B882)
Steven Weinberg, Photons and Gravitons in $S$-Matrix Theory: Derivation of Charge Conservationand Equality of Gravitational and Inertial Mass, Phys. Rev. 135 (1964) B1049 (doi:10.1103/PhysRev.135.B1049)
Steven Weinberg, Photons and Gravitons in Perturbation Theory: Derivation of Maxwell’s and Einstein’s Equations,” Phys. Rev. 138 (1965) B988 (doi:10.1103/PhysRev.138.B988)
Paolo Benincasa, Freddy Cachazo, Consistency Conditions on the S-Matrix of Massless Particles (arXiv:0705.4305)
David A. McGady, Laurentiu Rodina, Higher-spin massless S-matrices in four-dimensions, Phys. Rev. D 90, 084048 (2014) (arXiv:1311.2938, doi:10.1103/PhysRevD.90.084048)
Review:
Claus Kiefer, section 2.1.3 of: Quantum Gravity, Oxford University Press 2007 (doi:10.1093/acprof:oso/9780199585205.001.0001, cds:1509512)
Daniel Baumann, What long-range forces are allowed?, 2019 (pdf)
Last revised on December 18, 2019 at 06:27:17. See the history of this page for a list of all contributions to it.