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dc.contributor.authorMartínez López, Antonio 
dc.contributor.authorMilán López, Francisco 
dc.contributor.authorTenenblat, Keti
dc.date.accessioned2015-09-30T11:18:12Z
dc.date.available2015-09-30T11:18:12Z
dc.date.issued2015
dc.identifier.citationMartínez-López, A.; Milán López, F.; Tenenblat, K. Ribaucour type Transformations for the Hessian One Equation. Nonlinear Analysis: Theory, Methods and Applications, 112: 147–155 (2015). [http://hdl.handle.net/10481/37916]es_ES
dc.identifier.issn0362-546X
dc.identifier.urihttp://hdl.handle.net/10481/37916
dc.description.abstractWe extend the classical theory of Ribaucour transformations to the family of improper affine maps and use it to obtain new solutions of the Hessian one equation. We prove that such transformations produce complete, embedded ends of parabolic type and curves of singularities which generically are cuspidal edges. Moreover, we show that these ends and curves of singularities do no intersect. We apply Ribaucour transformations to some helicoidal improper affine maps providing new 3-parameter families with an interesting geometry and a good behavior at infinity. In particular, we construct improper affine maps, periodic in one variable, with any even number of complete embedded ends.es_ES
dc.description.sponsorshipMinisterio de Educación Grants No: MTM2013-43970-P, No: PHB2010-0109, Junta de Anadalucía Grants No. FQM325, N0. P06-FQM-01642. Ministério de Ciência e Tecnologia, CNPq Proc. No. 303774/2009-6. Ministério de Educação, CAPES/DGU Proc. No. 23038010833/2010-37.es_ES
dc.language.isoenges_ES
dc.publisherElsevieres_ES
dc.rightsCreative Commons Attribution-NonCommercial-NoDerivs 3.0 Licensees_ES
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/3.0/es_ES
dc.subjectRibaucour transformationses_ES
dc.subjectImproper affine sphereses_ES
dc.subjectHessian one equationes_ES
dc.titleRibaucour type Transformations for the Hessian One Equationes_ES
dc.typejournal articlees_ES
dc.rights.accessRightsopen accesses_ES
dc.identifier.doi10.1016/j.na.2014.09.013


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