{"id":20783,"date":"2026-07-10T13:25:07","date_gmt":"2026-07-10T11:25:07","guid":{"rendered":"https:\/\/scm.iec.cat\/?post_type=sessions&#038;p=20783"},"modified":"2026-09-18T17:17:38","modified_gmt":"2026-09-18T15:17:38","slug":"bmd-2026-especial-sessio-posters","status":"publish","type":"sessions","link":"https:\/\/scm.iec.cat\/eng\/sessions\/bmd-2026-especial-sessio-posters\/","title":{"rendered":"BMD 2026-Special-4-Poster session"},"content":{"rendered":"<p>Hem convidat la comunitat investigadora a mostrar resultats de recerca no inclosos en les pon\u00e8ncies i sessions programades, en format p\u00f2ster. Donem aix\u00ed un valor afegit a les pauses, afavorint\u00a0 l\u2019intercanvi d\u2019idees i les discussions matem\u00e0tiques. En especial, pels joves, \u00e9s una oportunitat per mostrar la seva recerca.<\/p>\n<h3 id=\"tw-target-text\" class=\"tw-data-text tw-text-large tw-ta\" dir=\"ltr\" data-placeholder=\"Traducci\u00f3\" data-ved=\"2ahUKEwiFw5XZ0d2BAxWKVKQEHWHnCywQ3ewLegQICBAQ\">Llistat de p\u00f2sters acceptats<\/h3>\n<ul>\n<li><strong>L\u00b2-boundedness of the n-th Calder\u00f3n commutator on Lipschitz graphs<\/strong><br \/>\nJoan Hern\u00e1ndez Garc\u00eda (Universitat Aut\u00f2noma de Barcelona)<\/li>\n<li><strong>A conic optimization framework for shape-constrained functional regression analysis<\/strong><br \/>\nCristina Molero-R\u00edo (Universidad de Sevilla)<\/li>\n<li class=\"tw-data-text tw-text-large tw-ta\" dir=\"ltr\" data-placeholder=\"Traducci\u00f3\" data-ved=\"2ahUKEwiFw5XZ0d2BAxWKVKQEHWHnCywQ3ewLegQICBAQ\"><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Symmetric Cartan calculus&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><strong>Balanced subtournaments of a random tournament<\/strong><br \/>\nXavier Povill (Universitat Polit\u00e8cnica de Catalunya)<\/span><\/li>\n<li class=\"tw-data-text tw-text-large tw-ta\" dir=\"ltr\" data-placeholder=\"Traducci\u00f3\" data-ved=\"2ahUKEwiFw5XZ0d2BAxWKVKQEHWHnCywQ3ewLegQICBAQ\"><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Zeros of {-1, 0, 1} Power Series, Connectedness Loci and Peephole Sets&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><strong>Decorated groupoids on marked bordered surface<\/strong><br \/>\nBenedetta Facciotti (Universitat Polit\u00e8cnica de Catalunya)<\/span><\/li>\n<li class=\"tw-data-text tw-text-large tw-ta\" dir=\"ltr\" data-placeholder=\"Traducci\u00f3\" data-ved=\"2ahUKEwiFw5XZ0d2BAxWKVKQEHWHnCywQ3ewLegQICBAQ\"><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Castelnuovo-Mumford regularity of projective monomial curves via sumsets&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><strong>Dynamics in the center manifold around a fixed point of a map<\/strong><br \/>\nLeonor Domingo (Universitat de Barcelona)<\/span><\/li>\n<li class=\"tw-data-text tw-text-large tw-ta\" dir=\"ltr\" data-placeholder=\"Traducci\u00f3\" data-ved=\"2ahUKEwiFw5XZ0d2BAxWKVKQEHWHnCywQ3ewLegQICBAQ\"><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Atlas of wandering domains for a Newton family&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><strong>Eccentricity sequences of quasitrees and unicycle graphs<br \/>\n<\/strong>Nacho (Ignacio) L\u00f3pez Lorenzo (Universitat de Lleida)<\/span><\/li>\n<li class=\"tw-data-text tw-text-large tw-ta\" dir=\"ltr\" data-placeholder=\"Traducci\u00f3\" data-ved=\"2ahUKEwiFw5XZ0d2BAxWKVKQEHWHnCywQ3ewLegQICBAQ\"><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Atlas of wandering domains for a Newton family&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><strong>Gender inequality in care work using direct responses and NSUM estimates<\/strong><br \/>\n<\/span>Bel\u00e9n Pulido (Universidad Nacional de Educaci\u00f3n a Distancia)<\/li>\n<li class=\"tw-data-text tw-text-large tw-ta\" dir=\"ltr\" data-placeholder=\"Traducci\u00f3\" data-ved=\"2ahUKEwiFw5XZ0d2BAxWKVKQEHWHnCywQ3ewLegQICBAQ\"><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Atlas of wandering domains for a Newton family&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><strong>Maximum likelihood threshold bounds for colored Gaussian models<\/strong><br \/>\nDanai Deligeorgaki (Universitat de Barcelona)<\/span><\/li>\n<li dir=\"ltr\" data-placeholder=\"Traducci\u00f3\" data-ved=\"2ahUKEwiFw5XZ0d2BAxWKVKQEHWHnCywQ3ewLegQICBAQ\"><strong>Morphisms of Theta Lifts and families of Relative Trace Formulae<\/strong><br \/>\nRon Erez (Tel Aviv University)<\/li>\n<li dir=\"ltr\" data-placeholder=\"Traducci\u00f3\" data-ved=\"2ahUKEwiFw5XZ0d2BAxWKVKQEHWHnCywQ3ewLegQICBAQ\"><strong>Nonlocal Inverse Problems and Long-Range Propagation on Cellular Graphs<br \/>\n<\/strong>Salvish Goomanee and Gr\u00e9goire Malandain (Universit\u00e9 de la C\u00f4te d&#8217;Azur, INRIA)<\/li>\n<li dir=\"ltr\" data-placeholder=\"Traducci\u00f3\" data-ved=\"2ahUKEwiFw5XZ0d2BAxWKVKQEHWHnCywQ3ewLegQICBAQ\"><strong>Simplification of Non-Orientable Maps<\/strong><br \/>\nLingxuan Wu (Universitat Polit\u00e8cnica de Catalunya, Central South University)<\/li>\n<li dir=\"ltr\" data-placeholder=\"Traducci\u00f3\" data-ved=\"2ahUKEwiFw5XZ0d2BAxWKVKQEHWHnCywQ3ewLegQICBAQ\"><strong>Square-Free Parts of Tate&#8211;Shafarevich Groups<br \/>\n<\/strong>Alexandros Konstantinou<strong>\u00a0<\/strong>(Max Planck Institute for Mathematics)<\/li>\n<li dir=\"ltr\" data-placeholder=\"Traducci\u00f3\" data-ved=\"2ahUKEwiFw5XZ0d2BAxWKVKQEHWHnCywQ3ewLegQICBAQ\"><strong>Tracing the Emergence of Nonsmooth Bifurcations in Piecewise-Linear Quasiperiodically Forced Continuous Models<br \/>\n<\/strong>Rafael Martinez Vergara (Universitat de Barcelona)<\/li>\n<li dir=\"ltr\" data-placeholder=\"Traducci\u00f3\" data-ved=\"2ahUKEwiFw5XZ0d2BAxWKVKQEHWHnCywQ3ewLegQICBAQ\"><strong>Unified theory for regularity persistence of vortex patch boundaries<\/strong><br \/>\nMarc Maga\u00f1a Centelles (Universitat Aut\u00f2noma de Barcelona)<\/li>\n<li dir=\"ltr\" data-placeholder=\"Traducci\u00f3\" data-ved=\"2ahUKEwiFw5XZ0d2BAxWKVKQEHWHnCywQ3ewLegQICBAQ\"><strong>Where Fractals Just Touch: A Four-Dimensional Connectedness Atlas for Planar Binary Self-Similar Sets<\/strong><br \/>\nBernat Espigul\u00e9 (Universitat de Girona)<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n<hr \/>\n<h3 dir=\"ltr\" data-placeholder=\"Traducci\u00f3\" data-ved=\"2ahUKEwiFw5XZ0d2BAxWKVKQEHWHnCywQ3ewLegQICBAQ\">Llistat de resums<\/h3>\n<hr \/>\n<h5><strong><em>L\u00b2-boundedness of the n-th Calder\u00f3n commutator on Lipschitz graphs<\/em><\/strong><\/h5>\n<h5><strong><br \/>\nJoan Hern\u00e1ndez Garc\u00eda (Universitat Aut\u00f2noma de Barcelona)<\/strong><\/h5>\n<p><strong>Abstract:<\/strong><\/p>\n<p>Our work investigates the asymptotic behavior of the norm, as a bounded operator in L\u00b2(R), of the n-th Calder\u00f3n commutator T_{A,n} on the graph of a Lipschitz function A. We prove the estimate |T_{A,n}|_{L\u00b2&#8211;&gt; L\u00b2} \\leq Cn |A&#8217;|_\\infty^n, thus formalizing a claim by Mateu and Verdera via a symmetrization strategy and the T1 theorem. We also show that additional regularity on A yields sublinear growth in n. Specifically, for A supported in [0,1], the bound improves to a behavior of the form n^(1\/2)|A&#8217;|_\\infty^n under a Dini condition on A&#8217;, or if A&#8217; belongs to the logarithmic Besov space B^{1,0}_{1,1}(R). This space contains all compactly supported functions in the Sobolev spaces H^s(R) for 0&lt;s&lt;1, as well as functions of bounded variation. These refined estimates are established through an alternative framework based on H\u00f6rmander-type conditions and interpolation, bypassing the standard T1 approach. Counterexamples are provided to demonstrate that the Dini and Sobolev fractional regularity conditions are incomparable.<\/p>\n<p>&nbsp;<\/p>\n<hr \/>\n<h5><em><strong>A conic optimization framework for shape-constrained functional regression analysis<\/strong><\/em><\/h5>\n<h5><strong>Cristina Molero-R\u00edo (Universidad de Sevilla)<\/strong><\/h5>\n<p><strong>Abstract:<\/strong><\/p>\n<p>Functional regression refers to regression models involving functional covariates and\/or a functional response. Often, prior knowledge about the relationship between the covariates and the response &#8212; arising from biological, medical, or engineering processes &#8212; requires that the estimated functional coefficients meet specific shape constraints, such as non-negativity, monotonicity, or convexity\/concavity. However, these requirements are not straightforwardly satisfied when using an unconstrained estimation approach. In this work, we investigate whether the combination of conic optimization and penalized splines (P-splines) developed by Navarro-Garc\\&#8217;ia, Guerrero and Durb\\&#8217;an (2023) can outperform recent approaches in the literature for estimating shape-constrained functional regression coefficients. The comparison will be carried out using both simulated and real datasets.<\/p>\n<hr \/>\n<h5><strong><em>Balanced subtournaments of a random tournament<\/em><\/strong><\/h5>\n<h5><strong><br \/>\n<\/strong><strong><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Symmetric Cartan calculus&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">Xavier Povill (Universitat Polit\u00e8cnica de Catalunya)<\/span><\/strong><\/h5>\n<p><strong><br \/>\nAbstract: <\/strong><\/p>\n<p>We study the size of the largest balanced subtournament in a random tournament on n vertices. A tournament is balanced if all vertices have equal indegree and outdegree. We show that, with high probability, the largest balanced subtournament has size O(n^{2\/3}). Moreover, for every k = o(n^{2\/3}), with high probability the random tournament on n vertices contains a balanced subtournament of size k. Our proof combines enumeration results for tournaments with prescribed degree sequences, due to McKay and Wang, with probabilistic arguments of Krivelevich, Sudakov and Wormald.<\/p>\n<hr \/>\n<h5><strong><em><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Zeros of {-1, 0, 1} Power Series, Connectedness Loci and Peephole Sets&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">Decorated groupoids on marked bordered surface<\/span><\/em><\/strong><\/h5>\n<h5><strong><br \/>\n<\/strong><strong><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Symmetric Cartan calculus&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">Benedetta Facciotti (Universitat Polit\u00e8cnica de Catalunya)<\/span><\/strong><\/h5>\n<p><strong>Abstract: <\/strong><\/p>\n<p>Building on the classical equivalence of groupoids among linear local systems on compact orientable surfaces, linear representations of the fundamental groupoid, linear representations of the action groupoid for the conjugation action of G on the space of G-representations for G=GLn(C), we extend this result to the case of surfaces with marked points on the boundaries, which carry additional data on such special points.<\/p>\n<hr \/>\n<h5><strong><em><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Zeros of {-1, 0, 1} Power Series, Connectedness Loci and Peephole Sets&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">Dynamics in the center manifold around a fixed point of a map<\/span><\/em><\/strong><\/h5>\n<h5><strong><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Symmetric Cartan calculus&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">Leonor Domingo (Universitat de Barcelona)<\/span><\/strong><\/h5>\n<p><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Castelnuovo-Mumford regularity of projective monomial curves via sumsets&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Castelnuovo-Mumford regularity of projective monomial curves via sumsets&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Castelnuovo-Mumford regularity of projective monomial curves via sumsets&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Castelnuovo-Mumford regularity of projective monomial curves via sumsets&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><br \/>\n<strong>Abstract: <\/strong><\/span><\/span><\/span><\/span><\/p>\n<p><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Castelnuovo-Mumford regularity of projective monomial curves via sumsets&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Castelnuovo-Mumford regularity of projective monomial curves via sumsets&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Castelnuovo-Mumford regularity of projective monomial curves via sumsets&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Castelnuovo-Mumford regularity of projective monomial curves via sumsets&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">In this work, we study the asymptotic behavior in the neighborhood of a fixed point of a map. To describe the dynamics near this point, we consider the reduction to the center manifold for a map. Our approach relies on the use of the graph transform method where the invariant center manifold of a fixed point is locally represented as a graph. We numerically compute the parametrization of the center-stable and center-unstable manifolds by using power series expansions around the fixed point. We propose to consider the jet transport technique to obtain an accurate approximation in the expansion of the center manifold through automatic differentiation on the map. The method is considered for an application to celestial mechanics. We are interested in the dynamics near the vicinity of the L3\u00a0point of the Earth-Moon system. The model for studying the dynamics of the problem is the Sun-Earth-Moon Bicircular Problem (BCP). To remove the dependence on time in the BCP model, in particular we consider a stroboscopic map defined at time of the perturbation. In this BCP model, the linear dynamics of the periodic orbit that replaces the L3-equilibrium point of the Restricted Three-Body Problem is described by a hyperbolic direction and two elliptical directions. To describe the different types of orbits in the neighborhood of L3, we uncouple the instability behavior caused by the hyperbolic direction from the other elliptical directions. This can be accomplished by performing the reduction to the center manifold around the dynamical substitute of L3. We numerically compute the high order approximation of the center-stable and center-unstable manifolds around this fixed point. As a result, we can then analyze the bounded motion described by the center manifold near the fixed point and visualize the phase space behavior in the original coordinate system.<br \/>\n<\/span><\/span><\/span><\/span><\/p>\n<hr \/>\n<h5><strong><em><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Zeros of {-1, 0, 1} Power Series, Connectedness Loci and Peephole Sets&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">Eccentricity sequences of quasitrees and unicycle graphs<\/span><\/em><\/strong><\/h5>\n<h5><strong><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Symmetric Cartan calculus&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">Nacho (Ignacio) L\u00f3pez Lorenzo (Universitat de Lleida)<\/span><\/strong><\/h5>\n<p><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Atlas of wandering domains for a Newton family&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Atlas of wandering domains for a Newton family&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Atlas of wandering domains for a Newton family&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Atlas of wandering domains for a Newton family&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><br \/>\n<strong>Abstract: <\/strong><\/span><\/span><\/span><\/span><\/p>\n<p><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Atlas of wandering domains for a Newton family&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Atlas of wandering domains for a Newton family&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Atlas of wandering domains for a Newton family&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Atlas of wandering domains for a Newton family&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">The eccentricity of a vertex in a connected graph is the maximum distance from this vertex. The eccentricity sequence of a graph is the list of eccentricities of its vertices given in nondecreasing order. A sequence of positive integers is a graphical eccentric sequence if it is the eccentricity sequence of some graph. The study of graphical eccentric sequences takes back to the 70&#8217;s of the past century where some results focus on the characterization of these sequences, specially for the family of trees. However, the general problem remains open. In this work we present some necessary and sufficient conditions for a sequence to be a graphical eccentric sequence of some families of graphs related to quasitrees and unicyclic graphs.<\/span><\/span><\/span><\/span><\/p>\n<hr \/>\n<h5><strong><em><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Zeros of {-1, 0, 1} Power Series, Connectedness Loci and Peephole Sets&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">Gender inequality in care work using direct responses and NSUM estimates<\/span><\/em><\/strong><\/h5>\n<h5><strong><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Symmetric Cartan calculus&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">Bel\u00e9n Pulido (Universidad Nacional de Educaci\u00f3n a Distancia)<\/span><\/strong><\/h5>\n<p><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Atlas of wandering domains for a Newton family&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><br \/>\n<strong>Abstract: <\/strong><\/span><\/p>\n<p><strong>Abstract: <\/strong>This study draws on data from CuidaNSUM, an interdisciplinary project examining perceptions of the distribution of care work and time use within Spanish households. The survey targets different gender, cohabiting couples with at least one child under 16 and combines sociodemographic information with direct and indirect questions on household tasks, childcare, employment adjustments, support networks, gender attitudes, and wellbeing.<\/p>\n<p>&nbsp;<\/p>\n<hr \/>\n<h5><strong><em><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Zeros of {-1, 0, 1} Power Series, Connectedness Loci and Peephole Sets&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">Maximum likelihood threshold bounds for colored Gaussian models<\/span><\/em><\/strong><\/h5>\n<h5><strong><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Symmetric Cartan calculus&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">Danai Deligeorgaki (Universitat de Barcelona)<\/span><\/strong><\/h5>\n<p><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Atlas of wandering domains for a Newton family&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Atlas of wandering domains for a Newton family&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Atlas of wandering domains for a Newton family&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Atlas of wandering domains for a Newton family&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Atlas of wandering domains for a Newton family&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><br \/>\n<strong>Abstract: <\/strong><\/span><\/span><\/span><\/span><\/span><\/p>\n<p><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Atlas of wandering domains for a Newton family&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Atlas of wandering domains for a Newton family&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Atlas of wandering domains for a Newton family&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Atlas of wandering domains for a Newton family&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\"><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Atlas of wandering domains for a Newton family&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">Colored Gaussian graphical models are a widely-used class of models which address the issue of statistical inference with limited samples by imposing linear conditions on the concentration matrix of the model. In this article, we apply and extend known methods for bounding maximum likelihood thresholds (MLTs) for uncolored Gaussian graphical models to the colored case.<\/span><\/span><\/span><\/span><\/span><\/p>\n<hr \/>\n<h5><strong><em><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Zeros of {-1, 0, 1} Power Series, Connectedness Loci and Peephole Sets&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">Morphisms of Theta Lifts and families of Relative Trace Formulae<\/span><\/em><\/strong><\/h5>\n<h5><strong><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Symmetric Cartan calculus&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">Ron Erez (Tel Aviv University)<\/span><\/strong><\/h5>\n<p><strong>Abstract:<\/strong><\/p>\n<p>The theta correspondence relates automorphic representations of orthogonal and metaplectic groups and is a fundamental ingredient of the Siegel&#8211;Weil formula and Kudla&#8217;s program. We study when theta lifts of two nontrivial automorphic characters of orthogonal groups are isomorphic. We determine necessary local matching conditions for such morphisms in terms of central characters and Jacquet modules of the associated local representations. We further propose that these morphisms should induce relative trace identities. This philosophy is motivated by a striking resemblance between our local conditions and those arising in the work of Mao and Rallis on families of relative trace formulae, where analogous conditions are formulated using coinvariants of induced representations. Our goal is to better understand the relationship between morphisms of theta lifts and families of relative trace formulae.<\/p>\n<hr \/>\n<h5><strong><em><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Zeros of {-1, 0, 1} Power Series, Connectedness Loci and Peephole Sets&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">Nonlocal Inverse Problems and Long-Range Propagation on Cellular Graphs<\/span><\/em><\/strong><\/h5>\n<h5><strong><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Symmetric Cartan calculus&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">Salvish Goomanee and Gr\u00e9goire Malandain (Universit\u00e9 de la C\u00f4te d&#8217;Azur, INRIA)<\/span><\/strong><\/h5>\n<p><strong>Abstract: <\/strong><\/p>\n<p>We develop a mathematical framework for studying long-range interactions in cellular tissues from partial observations. Cells are represented as nodes of a weighted graph, with nonlocal interactions encoded by a kernel defining a graph operator. The central inverse problem is to determine whether the hidden interaction structure can be recovered from the response of only a subset of observed cells to controlled perturbations. Under a connectedness assumption on the interaction graph, we establish a unique-continuation property for eigenmodes and show that the source-to-solution response contains sufficient spectral information to identify the hidden interaction kernel. We further obtain stability results in the simple-eigenvalue regime, with spectral projectors providing the natural formulation when eigenvalues are repeated. Numerical experiments on synthetic cellular graphs support these theoretical predictions, demonstrating recovery from partial observations across different graph geometries. Finally, we investigate how the spectral gap links tissue connectivity and nonlocal interactions to the characteristic timescale of perturbation propagation. Together, these results provide a spectral perspective on tissue-scale dynamics: long-range cellular interactions leave a recoverable spectral fingerprint that connects hidden interaction structure to the propagation of mechanical signals.<\/p>\n<hr \/>\n<h5><strong><em><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Zeros of {-1, 0, 1} Power Series, Connectedness Loci and Peephole Sets&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">Simplification of Non-Orientable Maps<\/span><\/em><\/strong><\/h5>\n<h5><strong><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Symmetric Cartan calculus&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">Lingxuan Wu (Universitat Polit\u00e8cnica de Catalunya, Central South University)<\/span><\/strong><\/h5>\n<p><strong>Abstract: <\/strong><\/p>\n<p>This poster discusses an ongoing attempt to extend the ordinary\/fully simple correspondence from orientable maps to non-orientable maps. In the orientable setting, ordinary maps allow boundary faces to meet each other or to self-touch at vertices, while fully simple maps forbid these boundary contacts. This correspondence is related to moment-free cumulant relations in free probability and to the x-y duality in topological recursion. Our starting point is the orthogonally invariant real symmetric matrix model. Using orthogonal Weingarten calculus, we derive transformation formulae between ordinary correlators and their fully simple analogues. The aim is to explain these formulae combinatorially in terms of maps on locally orientable surfaces, where twisted and untwisted edge gluings are both allowed, and to interpret the transformation as a non-orientable boundary simplification procedure. This may also give some hints towards real free probability and refined topological recursion.<\/p>\n<hr \/>\n<h5><strong><em><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Zeros of {-1, 0, 1} Power Series, Connectedness Loci and Peephole Sets&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">Square-Free Parts of Tate&#8211;Shafarevich Groups<\/span><\/em><\/strong><\/h5>\n<h5><strong><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Symmetric Cartan calculus&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">Alexandros Konstantinou\u00a0(Max Planck Institute for Mathematics)<\/span><\/strong><\/h5>\n<p><strong>Abstract: <\/strong><\/p>\n<p>The Tate&#8211;Shafarevich group is a central yet mysterious object in the study of rational points on abelian varieties. It measures the obstruction to determining generators for the Mordell&#8211;Weil group and plays a crucial role in the Birch and Swinnerton-Dyer conjecture. Yet it is notoriously difficult to compute or even prove finite. For elliptic curves, it is known to have square order when finite. In higher dimensions, this can fail, a fact long overlooked and often misstated in the literature. We show that every square-free integer arises as the square-free part of the order of the Tate&#8211;Shafarevich group of some abelian variety over the rationals.<strong><br \/>\n<\/strong><\/p>\n<hr \/>\n<h5><strong><em><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Zeros of {-1, 0, 1} Power Series, Connectedness Loci and Peephole Sets&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">Tracing the Emergence of Nonsmooth Bifurcations in Piecewise-Linear Quasiperiodically Forced Continuous Models<\/span><\/em><\/strong><\/h5>\n<h5><strong><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Symmetric Cartan calculus&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">Rafael Martinez Vergara (Universitat de Barcelona)<\/span><\/strong><\/h5>\n<p><strong>Abstract: <\/strong><\/p>\n<p>We introduce a two-parameter family of quasiperiodically forced piecewise-linear maps. We identify a curve b*(a) where a nonsmooth period-doubling bifurcation occurs. The study analyzes fractalization through the growth of the Lipschitz constant of the attractor. This research builds upon and extends previous investigations into quasiperiodically forced systems.<\/p>\n<hr \/>\n<h5><strong><em><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Zeros of {-1, 0, 1} Power Series, Connectedness Loci and Peephole Sets&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">Unified theory for regularity persistence of vortex patch boundaries<\/span><\/em><\/strong><\/h5>\n<h5><strong><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Symmetric Cartan calculus&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">Marc Maga\u00f1a Centelles (Universitat Aut\u00f2noma de Barcelona)<\/span><\/strong><\/h5>\n<p><strong>Abstract: <\/strong><\/p>\n<p>We establish a unified local theory for the persistence of Sobolev regularity of vortex patch boundaries in a family of two-dimensional active scalar equations with radial convolution kernels K(|x-y|). The class includes the 2D Euler equation, the generalized SQG equation in the locally integrable range 0&lt;\\beta&lt;1, and the quasi-geostrophic shallow water equation. Under natural assumptions on K (smoothness, integrability near the origin, monotonicity, and polynomial growth), we prove that if the initial boundary belongs to H^3(\\mathbb T) and satisfies the arc-chord condition, then the contour dynamics equation admits a unique local solution in C([0,T];H^3(\\mathbb T)). Under a stronger integrability condition on the kernel, we also obtain local existence of H^2 solutions. The proof combines Sobolev energy estimates for the contour equation with quantitative control of the arc-chord quantity.<strong><br \/>\n<\/strong><\/p>\n<hr \/>\n<h5><strong><em><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Zeros of {-1, 0, 1} Power Series, Connectedness Loci and Peephole Sets&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">Where Fractals Just Touch: A Four-Dimensional Connectedness Atlas for Planar Binary Self-Similar Sets<\/span><\/em><\/strong><\/h5>\n<h5><strong><span data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Symmetric Cartan calculus&quot;}\" data-sheets-userformat=\"{&quot;2&quot;:513,&quot;3&quot;:{&quot;1&quot;:0},&quot;12&quot;:0}\">Bernat Espigul\u00e9 (Universitat de Girona)<\/span><\/strong><\/h5>\n<p><strong>Abstract:<\/strong><\/p>\n<p>Start with two shrunken copies of the complex plane, place them at -1 and +1, and iterate forever. Some parameter choices produce a connected planar self-similar set; others break apart into dust. This poster studies the frontier where the two symbolic halves just touch. After normalization, relabelling, and conformal or anti-conformal affine conjugacy, every non-degenerate planar binary similarity system belongs to one of three orientation-parity normal forms: direct\u2013direct, direct\u2013opposite, or opposite\u2013opposite. These are controlled by four real parameters: branch angle \u03b1, relative phase \u03b3, magnitude \u03c1, and scale weight w. The resulting parameter space forms a four-dimensional connectedness atlas. Its boundary can be explored as a geometric shell, coloured by finite symbolic address data and organized by watershed cracks where the local address structure changes. The accompanying interactive explorer makes this object visible and navigable. Classical examples such as the twindragon, L\u00e9vy dragon, Heighway dragon, tent-tiles, triangle tile, and H-tree tile appear as landmarks in the same atlas, while the near-H-tree regime reveals exact dyadic branch phenomena.<\/p>\n<p>&nbsp;<\/p>\n<p dir=\"ltr\" data-placeholder=\"Traducci\u00f3\" data-ved=\"2ahUKEwiFw5XZ0d2BAxWKVKQEHWHnCywQ3ewLegQICBAQ\">\n","protected":false},"parent":0,"template":"","categoria_sessions_conferences":[238],"class_list":["post-20783","sessions","type-sessions","status-publish","hentry","categoria_sessions_conferences-bmd-2026"],"acf":[],"_links":{"self":[{"href":"https:\/\/scm.iec.cat\/eng\/wp-json\/wp\/v2\/sessions\/20783","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/scm.iec.cat\/eng\/wp-json\/wp\/v2\/sessions"}],"about":[{"href":"https:\/\/scm.iec.cat\/eng\/wp-json\/wp\/v2\/types\/sessions"}],"wp:attachment":[{"href":"https:\/\/scm.iec.cat\/eng\/wp-json\/wp\/v2\/media?parent=20783"}],"wp:term":[{"taxonomy":"categoria_sessions_conferences","embeddable":true,"href":"https:\/\/scm.iec.cat\/eng\/wp-json\/wp\/v2\/categoria_sessions_conferences?post=20783"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}