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<dim:field authority="EAE2F8B7-F01D-4DAE-886D-71D1EC5DF7D0" element="contributor" qualifier="author" confidence="ACCEPTED" language="es-ES" mdschema="dc">Gay–Balmaz, François</dim:field>
<dim:field authority="0000-0003-0889-0450" element="contributor" qualifier="author" confidence="ACCEPTED" language="es-ES" mdschema="dc">Rodríguez Abella, Álvaro</dim:field>
<dim:field authority="CE85141D-6492-42DC-BBE1-1F943BB92845" element="contributor" qualifier="author" confidence="ACCEPTED" language="es-ES" mdschema="dc">Yoshimura, Hiroaki</dim:field>
<dim:field element="date" qualifier="accessioned" mdschema="dc">2026-04-24T08:10:48Z</dim:field>
<dim:field element="date" qualifier="available" mdschema="dc">2026-04-24T08:10:48Z</dim:field>
<dim:field element="date" qualifier="issued" language="es_ES" mdschema="dc">2026-08-01</dim:field>
<dim:field element="identifier" qualifier="issn" language="es_ES" mdschema="dc">0393-0440</dim:field>
<dim:field element="identifier" qualifier="uri" language="es_ES" mdschema="dc">https://doi.org/10.1016/j.geomphys.2026.105854</dim:field>
<dim:field element="description" language="es_ES" mdschema="dc">Artículos en revistas</dim:field>
<dim:field element="description" qualifier="abstract" language="es-ES" mdschema="dc">.</dim:field>
<dim:field element="description" qualifier="abstract" language="en-GB" mdschema="dc">Part I of this paper introduced the infinite dimensional Lagrange–Dirac theory for physical&#13;
systems on the space of differential forms over a smooth manifold with boundary. This&#13;
approach is particularly well-suited for systems involving energy exchange through the&#13;
boundary, as it is built upon a restricted dual space -a vector subspace of the topological&#13;
dual of the configuration space - that captures information about both the interior&#13;
dynamics and boundary interactions. Consequently, the resulting dynamical equations&#13;
naturally incorporate boundary energy flow. In this second part, the theory is extended&#13;
to encompass vector bundle-valued differential forms and non-Abelian gauge theories.&#13;
To account for two commonly used forms of energy flux and boundary power densities,&#13;
we introduce two distinct but equivalent formulations of the restricted dual. The results&#13;
are derived from both geometric and variational viewpoints and are illustrated through&#13;
applications to matter and gauge field theories. The interaction between gauge and matter&#13;
fields is also addressed, along with the associated boundary conditions, applied to the case&#13;
of the Yang–Mills--Higgs equations.</dim:field>
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<dim:field element="source" language="es_ES" mdschema="dc">Revista: Journal of Geometry and Physics, Periodo: 1, Volumen: 226, Número:  105854, Página inicial: 1, Página final: 42</dim:field>
<dim:field element="title" language="es_ES" mdschema="dc">Infinite-dimensional Lagrange–Dirac systems with boundary  energy flow II: Field theories with bundle-valued forms</dim:field>
<dim:field element="type" language="es_ES" mdschema="dc">info:eu-repo/semantics/article</dim:field>
<dim:field element="description" qualifier="version" language="es_ES" mdschema="dc">info:eu-repo/semantics/publishedVersion</dim:field>
<dim:field element="rights" qualifier="holder" language="es_ES" mdschema="dc">politica editorial embargo de 24 meses</dim:field>
<dim:field element="rights" qualifier="accessRights" language="es_ES" mdschema="dc">info:eu-repo/semantics/restrictedAccess</dim:field>
<dim:field element="keywords" language="es-ES" mdschema="dc">.</dim:field>
<dim:field element="keywords" language="en-GB" mdschema="dc">Dirac mechanics&#13;
Boundary&#13;
Gauge theories&#13;
Lagrange–d’Alembert--Pontryagin principle&#13;
Yang–Mills--Higgs equations</dim:field>
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