{"id":325,"date":"2011-02-22T21:57:06","date_gmt":"2011-02-22T20:57:06","guid":{"rendered":"http:\/\/users.unimi.it\/mazza\/?p=325"},"modified":"2011-02-22T23:37:43","modified_gmt":"2011-02-22T22:37:43","slug":"seminario-242","status":"publish","type":"post","link":"https:\/\/sites.unimi.it\/mazza\/2011\/02\/22\/seminario-242\/","title":{"rendered":"seminario 24\/2"},"content":{"rendered":"<p> Il giorno giovedi&#39; 24 Febbraio<br \/> ore 14:30 Aula 5<\/p>\n<p>Il dott. Alexandre Kirilov<br \/> (Dipartimento di Matematica ed Informatica, Universit\u00e0 di Cagliari)<\/p>\n<p>terr\u00e0 un seminario su<\/p>\n<p>&quot;Global regularity and global solvability for smooth vector fields on S3&quot;<\/p>\n<p>Abstract:<br \/> The main goal of this work is to address \u00a0global properties \u00a0for classes of smooth (non)singular vector fields on <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/sites.unimi.it\/mazza\/wp-content\/ql-cache\/quicklatex.com-d1279459b2aa62f712e41858af648f21_l3.png\" class=\"ql-img-inline-formula quicklatex-auto-format\" alt=\"&#83;&#51;\" title=\"Rendered by QuickLaTeX.com\" height=\"12\" width=\"21\" style=\"vertical-align: 0px;\"\/>. It is known that on <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/sites.unimi.it\/mazza\/wp-content\/ql-cache\/quicklatex.com-d1279459b2aa62f712e41858af648f21_l3.png\" class=\"ql-img-inline-formula quicklatex-auto-format\" alt=\"&#83;&#51;\" title=\"Rendered by QuickLaTeX.com\" height=\"12\" width=\"21\" style=\"vertical-align: 0px;\"\/> no <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/sites.unimi.it\/mazza\/wp-content\/ql-cache\/quicklatex.com-69ff5615fd2538cf0bb1b21766387d11_l3.png\" class=\"ql-img-inline-formula quicklatex-auto-format\" alt=\"&#67;&#94;&#105;&#110;&#102;&#116;&#121;\" title=\"Rendered by QuickLaTeX.com\" height=\"19\" width=\"56\" style=\"vertical-align: -4px;\"\/> globally hypoelliptic (GH) and no <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/sites.unimi.it\/mazza\/wp-content\/ql-cache\/quicklatex.com-69ff5615fd2538cf0bb1b21766387d11_l3.png\" class=\"ql-img-inline-formula quicklatex-auto-format\" alt=\"&#67;&#94;&#105;&#110;&#102;&#116;&#121;\" title=\"Rendered by QuickLaTeX.com\" height=\"19\" width=\"56\" style=\"vertical-align: -4px;\"\/> globally solvable (cohomologically free (CF) in the sense of Katok) vector fields exist.<\/p>\n<p>First we consider classes of vector fields with one or two cycles which are attractors for all other integral curves. We show that the cohomological equation <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/sites.unimi.it\/mazza\/wp-content\/ql-cache\/quicklatex.com-45da52b80ed16af5822e9947ef341c9e_l3.png\" class=\"ql-img-inline-formula quicklatex-auto-format\" alt=\"&#76;&#117;&#61;&#102;\" title=\"Rendered by QuickLaTeX.com\" height=\"16\" width=\"56\" style=\"vertical-align: -4px;\"\/>, <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/sites.unimi.it\/mazza\/wp-content\/ql-cache\/quicklatex.com-f9c491a411821555bda38fef5149283f_l3.png\" class=\"ql-img-inline-formula quicklatex-auto-format\" alt=\"&#102;&#105;&#110;&#32;&#67;&#94;&#105;&#110;&#102;&#116;&#121;&#32;&#40;&#83;&#51;&#41;\" title=\"Rendered by QuickLaTeX.com\" height=\"19\" width=\"118\" style=\"vertical-align: -4px;\"\/> has at least one <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/sites.unimi.it\/mazza\/wp-content\/ql-cache\/quicklatex.com-69ff5615fd2538cf0bb1b21766387d11_l3.png\" class=\"ql-img-inline-formula quicklatex-auto-format\" alt=\"&#67;&#94;&#105;&#110;&#102;&#116;&#121;\" title=\"Rendered by QuickLaTeX.com\" height=\"19\" width=\"56\" style=\"vertical-align: -4px;\"\/> solution defined on <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/sites.unimi.it\/mazza\/wp-content\/ql-cache\/quicklatex.com-d1279459b2aa62f712e41858af648f21_l3.png\" class=\"ql-img-inline-formula quicklatex-auto-format\" alt=\"&#83;&#51;\" title=\"Rendered by QuickLaTeX.com\" height=\"12\" width=\"21\" style=\"vertical-align: 0px;\"\/> except the attractors and we can extend the soluion as a weak <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/sites.unimi.it\/mazza\/wp-content\/ql-cache\/quicklatex.com-09af33671cf2df6397d122753c3b185f_l3.png\" class=\"ql-img-inline-formula quicklatex-auto-format\" alt=\"&#76;&#49;\" title=\"Rendered by QuickLaTeX.com\" height=\"13\" width=\"20\" style=\"vertical-align: -1px;\"\/> function near the attractors. Moreover, we describe completely the propagation of singularities of all solutions <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/sites.unimi.it\/mazza\/wp-content\/ql-cache\/quicklatex.com-aac371ae16ade095d8f23fcba9abb7ff_l3.png\" class=\"ql-img-inline-formula quicklatex-auto-format\" alt=\"&#117;\" title=\"Rendered by QuickLaTeX.com\" height=\"8\" width=\"10\" style=\"vertical-align: 0px;\"\/>. As a particular case, we exhibit explicit vector fields whose integral curves coincied with \u00a0the foliations obtained by transversal intersection of linear holomorphic flows in <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/sites.unimi.it\/mazza\/wp-content\/ql-cache\/quicklatex.com-d27bdf20ae937cce116cbd9aff504913_l3.png\" class=\"ql-img-inline-formula quicklatex-auto-format\" alt=\"&#67;&#50;\" title=\"Rendered by QuickLaTeX.com\" height=\"12\" width=\"22\" style=\"vertical-align: 0px;\"\/> \u00a0with <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/sites.unimi.it\/mazza\/wp-content\/ql-cache\/quicklatex.com-d1279459b2aa62f712e41858af648f21_l3.png\" class=\"ql-img-inline-formula quicklatex-auto-format\" alt=\"&#83;&#51;\" title=\"Rendered by QuickLaTeX.com\" height=\"12\" width=\"21\" style=\"vertical-align: 0px;\"\/> under nondegeneracy conditions.<\/p>\n<p>Secondly, for a class of nonsingular vector fields which are invariant on the fibers (two dimensional tori) in &#8220;generalized solid tori&quot; foliations of <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/sites.unimi.it\/mazza\/wp-content\/ql-cache\/quicklatex.com-d1279459b2aa62f712e41858af648f21_l3.png\" class=\"ql-img-inline-formula quicklatex-auto-format\" alt=\"&#83;&#51;\" title=\"Rendered by QuickLaTeX.com\" height=\"12\" width=\"21\" style=\"vertical-align: 0px;\"\/>, we derive necessary and sufficient conditions for partial <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/sites.unimi.it\/mazza\/wp-content\/ql-cache\/quicklatex.com-69ff5615fd2538cf0bb1b21766387d11_l3.png\" class=\"ql-img-inline-formula quicklatex-auto-format\" alt=\"&#67;&#94;&#105;&#110;&#102;&#116;&#121;\" title=\"Rendered by QuickLaTeX.com\" height=\"19\" width=\"56\" style=\"vertical-align: -4px;\"\/> GH and partial <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/sites.unimi.it\/mazza\/wp-content\/ql-cache\/quicklatex.com-69ff5615fd2538cf0bb1b21766387d11_l3.png\" class=\"ql-img-inline-formula quicklatex-auto-format\" alt=\"&#67;&#94;&#105;&#110;&#102;&#116;&#121;\" title=\"Rendered by QuickLaTeX.com\" height=\"19\" width=\"56\" style=\"vertical-align: -4px;\"\/> GS \u00a0with respect to the fibers. We point out that our construction of solid tori yields novel family of <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/sites.unimi.it\/mazza\/wp-content\/ql-cache\/quicklatex.com-99a440d47e87dc90c8bba1c89a41538e_l3.png\" class=\"ql-img-inline-formula quicklatex-auto-format\" alt=\"&#50;&#68;\" title=\"Rendered by QuickLaTeX.com\" height=\"12\" width=\"24\" style=\"vertical-align: 0px;\"\/> tori shrinking to cycles at the end points, different from the Clifford and Lwoson tori.<\/p>\n<p>Moreover, the integral curves of the vector field correspond to foliations obtained by intersection of linear holomorphic flows with<br \/> degeneracies in the Poincare&#39; domain.<\/p>\n<p>We provide also results on the global solvability for more general classes of smooth vector fields (admitting also singular points) associated in a natural way to intersection of \u00a0linear <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/sites.unimi.it\/mazza\/wp-content\/ql-cache\/quicklatex.com-b889431bd82e09b45c63e6c91d67626e_l3.png\" class=\"ql-img-inline-formula quicklatex-auto-format\" alt=\"&#67;\" title=\"Rendered by QuickLaTeX.com\" height=\"12\" width=\"14\" style=\"vertical-align: 0px;\"\/> holomorphic flows and linear <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/sites.unimi.it\/mazza\/wp-content\/ql-cache\/quicklatex.com-68228a7f47035bfd692a9b9bbb59517f_l3.png\" class=\"ql-img-inline-formula quicklatex-auto-format\" alt=\"&#82;&#50;\" title=\"Rendered by QuickLaTeX.com\" height=\"12\" width=\"22\" style=\"vertical-align: 0px;\"\/> actions on <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/sites.unimi.it\/mazza\/wp-content\/ql-cache\/quicklatex.com-d1279459b2aa62f712e41858af648f21_l3.png\" class=\"ql-img-inline-formula quicklatex-auto-format\" alt=\"&#83;&#51;\" title=\"Rendered by QuickLaTeX.com\" height=\"12\" width=\"21\" style=\"vertical-align: 0px;\"\/>. In particular, we are able to classify completely the global properties of the cohomological equation \u00a0<img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/sites.unimi.it\/mazza\/wp-content\/ql-cache\/quicklatex.com-8451276054d350e860d2ce64d878f51a_l3.png\" class=\"ql-img-inline-formula quicklatex-auto-format\" alt=\"&#76;&#117;&#32;&#61;&#102;\" title=\"Rendered by QuickLaTeX.com\" height=\"16\" width=\"56\" style=\"vertical-align: -4px;\"\/> on <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/sites.unimi.it\/mazza\/wp-content\/ql-cache\/quicklatex.com-d1279459b2aa62f712e41858af648f21_l3.png\" class=\"ql-img-inline-formula quicklatex-auto-format\" alt=\"&#83;&#51;\" title=\"Rendered by QuickLaTeX.com\" height=\"12\" width=\"21\" style=\"vertical-align: 0px;\"\/>, provided <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/sites.unimi.it\/mazza\/wp-content\/ql-cache\/quicklatex.com-e51f01b75e66f8991592097bb7aed75c_l3.png\" class=\"ql-img-inline-formula quicklatex-auto-format\" alt=\"&#76;\" title=\"Rendered by QuickLaTeX.com\" height=\"12\" width=\"12\" style=\"vertical-align: 0px;\"\/> is obtained by foliations of linear holomorphic <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/sites.unimi.it\/mazza\/wp-content\/ql-cache\/quicklatex.com-b889431bd82e09b45c63e6c91d67626e_l3.png\" class=\"ql-img-inline-formula quicklatex-auto-format\" alt=\"&#67;\" title=\"Rendered by QuickLaTeX.com\" height=\"12\" width=\"14\" style=\"vertical-align: 0px;\"\/> or linear <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/sites.unimi.it\/mazza\/wp-content\/ql-cache\/quicklatex.com-68228a7f47035bfd692a9b9bbb59517f_l3.png\" class=\"ql-img-inline-formula quicklatex-auto-format\" alt=\"&#82;&#50;\" title=\"Rendered by QuickLaTeX.com\" height=\"12\" width=\"22\" style=\"vertical-align: 0px;\"\/> actions.<\/p>\n<p>[Joint work with A.Bergamasco and T. Gramchev]<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Il giorno giovedi&#39; 24 Febbraio ore 14:30 Aula 5 Il dott. Alexandre Kirilov (Dipartimento di Matematica ed Informatica, Universit\u00e0 di Cagliari) terr\u00e0 un seminario su &quot;Global regularity and global solvability for smooth vector fields on S3&quot; Abstract: The main goal of this work is to address \u00a0global properties \u00a0for classes of smooth (non)singular vector fields &hellip; <a href=\"https:\/\/sites.unimi.it\/mazza\/2011\/02\/22\/seminario-242\/\" class=\"more-link\">Leggi tutto<span class=\"screen-reader-text\"> &#8220;seminario 24\/2&#8221;<\/span><\/a><\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[14],"tags":[],"class_list":["post-325","post","type-post","status-publish","format-standard","hentry","category-seminari"],"_links":{"self":[{"href":"https:\/\/sites.unimi.it\/mazza\/wp-json\/wp\/v2\/posts\/325","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/sites.unimi.it\/mazza\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/sites.unimi.it\/mazza\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/sites.unimi.it\/mazza\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/sites.unimi.it\/mazza\/wp-json\/wp\/v2\/comments?post=325"}],"version-history":[{"count":1,"href":"https:\/\/sites.unimi.it\/mazza\/wp-json\/wp\/v2\/posts\/325\/revisions"}],"predecessor-version":[{"id":326,"href":"https:\/\/sites.unimi.it\/mazza\/wp-json\/wp\/v2\/posts\/325\/revisions\/326"}],"wp:attachment":[{"href":"https:\/\/sites.unimi.it\/mazza\/wp-json\/wp\/v2\/media?parent=325"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/sites.unimi.it\/mazza\/wp-json\/wp\/v2\/categories?post=325"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/sites.unimi.it\/mazza\/wp-json\/wp\/v2\/tags?post=325"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}