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We present all second order classical integrable systems of the cylindrical type in a three dimensional Euclidean space $\mathbb{E}_3$ with a nontrivial magnetic field. The Hamiltonian and integrals of motion have the form $H =\frac{1}{2}\left(\vec{p
Externí odkaz:
http://arxiv.org/abs/1909.05307
Autor:
Alfaro Fournier, Félix
Publikováno v:
Memoria Digital Vasca = Euskal Memoria Digitala
Fundacion Sancho el Sabio Fundazioa (FSS)
Fundacion Sancho el Sabio Fundazioa (FSS)
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=RECOLECTA___::3b28ba9cf3da35a51a226072a9591a5c
http://hdl.handle.net/10357/52478
http://hdl.handle.net/10357/52478