January 2024
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2 Reads
IFAC-PapersOnLine
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January 2024
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2 Reads
IFAC-PapersOnLine
June 2022
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126 Reads
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14 Citations
Foundations of Computational Mathematics
The classical notion of retraction map used to approximate geodesics is extended and rigorously defined to become a powerful tool to construct geometric integrators and it is called discretization map. Using the geometry of the tangent and cotangent bundles, we are able to tangently and cotangent lift such a map so that these lifts inherit the same properties as the original one and they continue to be discretization maps. In particular, the cotangent lift of a discretization map is a natural symplectomorphism, what plays a key role for constructing geometric integrators and symplectic methods. As a result, a wide range of (higher-order) numerical methods are recovered and canonically constructed by using different discretization maps, as well as some operations with Lagrangian submanifolds.
April 2018
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96 Reads
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8 Citations
We develop a geometric version of the inverse problem of the calculus of variations for discrete mechanics and constrained discrete mechanics. The geometric approach consists of using suitable Lagrangian and isotropic submanifolds. We also provide a transition between the discrete and the continuous problems and propose variationality as an interesting geometric property to take into account in the design and computer simulation of numerical integrators for constrained systems. For instance, nonholonomic mechanics is generally non variational but some special cases admit an alternative variational description. We apply some standard nonholonomic integrators to such an example to study which ones conserve this property.
August 2016
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116 Reads
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8 Citations
Monatshefte für Mathematik
The language of Lagrangian submanifolds is used to extend a geometric characterization of the inverse problem of the calculus of variations on tangent bundles to regular Lie algebroids. Since not all closed sections are locally exact on Lie algebroids, the Helmholtz conditions on Lie algebroids are necessary but not sufficient, so they give a weaker definition of the inverse problem. As an application the Helmholtz conditions on Atiyah algebroids are obtained so that the relationship between the inverse problem and the reduced inverse problem by symmetries can be described. Some examples and comparison with previous approaches in the literature are provided.
December 2015
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4 Reads
January 2015
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9 Reads
Automatica
In this paper, we propose new conditions guaranteeing that the trajectories of a mechanical control system can track any curve on the configuration manifold. We focus on systems that can be represented as forced affine connection control systems and we generalize the sufficient conditions for tracking known in the literature. The new results are proved by a combination of averaging procedures by highly oscillating controls with the notion of kinematic reduction.
January 2015
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131 Reads
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21 Citations
International Journal of Geometric Methods in Modern Physics
We show how to use boundary conditions to drive the evolution on a Quantum Mechanical system. We will see how this problem can be expressed in terms of a time-dependent Schr\"{o}dinger equation. In particular we will need the theory of self-adjoint extensions of differential operators in manifolds with boundary. An introduction of the latter as well as meaningful examples will be given. It is known that different boundary conditions can be used to describe different topologies of the associated quantum systems. We will use the previous results to study how this topology change can be accomplished in a dynamical way.
December 2014
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30 Reads
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6 Citations
The inverse problem of the calculus of variations consists in determining if the solutions of a given system of second order differential equations correspond with the solutions of the Euler-Lagrange equations for some regular Lagrangian. This problem in the general version remains unsolved. Here, we contribute to it with a novel description in terms of Lagrangian submanifolds of a symplectic manifold, also valid under some adaptation for the non-autonomous version. One of the advantages of this new point of view is that we can easily extend our description to the study of the inverse problem of the calculus of variations for second order systems along submanifolds. In this case, instead of Lagrangian submanifolds we will use isotropic submanifolds, covering both the nonholonomic and holonomic constraints for autonomous and non-autonomous systems as particular examples. Moreover, we use symplectic techniques to extend these isotropic submanifolds to Lagrangian ones, allowing us to describe the constrained solutions as solutions of a variational problem now without constraints. Mechanical examples such as the rolling disk are provided to illustrate the main results.
December 2012
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97 Reads
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9 Citations
International Journal of Geometric Methods in Modern Physics
The symmetric product of vector fields on a manifold arises when one studies the controllability of certain classes of mechanical control systems. A geometric description of the symmetric product is provided using parallel transport, along the lines of the flow interpretation of the Lie bracket. This geometric interpretation of the symmetric product is used to provide an intrinsic proof of the fact that the distributions closed under the symmetric product are exactly those distributions invariant under the geodesic flow.
November 2012
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67 Reads
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3 Citations
SIAM Journal on Control and Optimization
We geometrically describe optimal control problems in terms of Morse families in the Hamiltonian framework. These geometric structures allow us to recover the classical first order necessary conditions for optimality and the starting point to run an integrability algorithm. Moreover the integrability algorithm is adapted to optimal control problems in such a way that the trajectories originated by discontinuous controls are also obtained. From the Hamiltonian viewpoint we obtain the equations of motion for optimal control problems in the Lagrangian formalism by means of a proper Lagrangian submanifold. Singular optimal control problems and overdetermined ones are also studied along the paper.
... The first assertion is immediate from point (1) in Definition 4.1. The idea for the second assertion is as follows: it is easy to see by direct computation using the Inverse Function Theorem (or invoking Proposition 2.1 in [BLnMdD22] together with the fact that R is a discretization map as in Definition 2.2 of the same paper) that R is a local diffeomorphism in a neighborhood of Z X . Then, the existence of the open subsets V R and W R follows using Theorem 1 in [CP07] ...
June 2022
Foundations of Computational Mathematics
... where terms of order 4 in ∆t or ∆x have been truncated. This modified equation does preserve some features of the original equation (1). It is variational and multisymplectic. ...
April 2018
... As for the Hamiltonian perspective, the reduced dynamics is determined by the Hamilton-Poincaré equations on the orbit space of components of Tulczyjew's triplet, namely, the symplectomorphisms, are postponed in Sec. 4. More precisely, in Sec. ...
August 2016
Monatshefte für Mathematik
... , H 2 (Ω) being the Sobolev space of order 2 on the Thick Quantum Graph, and A 0 ∈ R. This system represents, assuming natural units, a quantum particle on a spire of radius 1, that encircles a solenoid that generates a magnetic flux of magnitud 2πa(t)A 0 through the spire [PBI15]. The term a ′ (t)xA 0 is the electric potential associated with Faraday's induction law corresponding to the time-varying magnetic flux determined by the magnetic potential a(t)A 0 . ...
January 2015
International Journal of Geometric Methods in Modern Physics
... As a consequence we obtain a new and shorter proof for the relation of being totally geodesic with the so called symmetric product, [5,18,3]. ...
December 2012
International Journal of Geometric Methods in Modern Physics
... This opens the question of trying to characterise when a given nonholonomic system admits a purely Lagrangian or Hamiltonian formulation in the manner of the classical inverse problem in the calculus of variations, see [13,18]. A recent approach consists in trying to view the trajectories of the nonholonomic system as the restriction to the constraint submanifold of the trajectories of a Lagrangian system, that is, the Euler-Lagrange equations of a Lagrangian gives us the nonholonomic equations when we restrict the initial conditions to the constraint submanifold [4,6], other approaches include Chaplygin Hamiltonisation [14]. ...
December 2014
... This formulation combines both the Lagrangian and Hamiltonian formalism and this is why it is sometimes called unified formalism. The Skinner-Rusk formalism has been extended to time-dependent systems [3][4][5], nonholonomic and vakonomic mechanics [6], higher-order mechanical systems [7][8][9][10], control systems [11,12] and field theory [13][14][15][16][17][18]. Recently, the Skinner-Rusk unified formalism was extended to contact [19] and k-contact [20] systems. ...
June 2008
... In this paper, we wish to take an alternative point of view and generalize Dirac systems in such a way that dynamics is defined by means of a Lagrangian submanifold of the phase space. We will use Morse families to generate those Lagrangian submanifolds, an approach that has already been applied in the realm of optimal control problems [BLIPMdD15]. With this notion of generalized Dirac system we are able to recover many examples in the literature in a unified intrinsic formalism, including nonholonomic and vakonomic mechanics, optimal control problems and constrained problems on linear almost Poisson manifolds. ...
Reference:
Morse families and Dirac systems
November 2012
SIAM Journal on Control and Optimization
... 2.2]) can be followed for this toy problem and many other control problems with constraints given by partial differential equations. This would lead to analogs of the PMP (compare, for instance, [11,3]) under strong regularity assumptions, results which can be considered as the first step of differential-geometric type of the approach we are promoting. The direct proof of Theorem 1.1 given in this paper can be then considered as guiding line for extending the results of the "first step" to reach results under low regularity assumptions. ...
October 2012
Calculus of Variations and Partial Differential Equations
... This formulation combines both the Lagrangian and Hamiltonian formalism and this is why it is sometimes called unified formalism. The Skinner-Rusk formalism has been extended to time-dependent systems [3][4][5], nonholonomic and vakonomic mechanics [6], higher-order mechanical systems [7][8][9][10], control systems [11,12] and field theory [13][14][15][16][17][18]. Recently, the Skinner-Rusk unified formalism was extended to contact [19] and k-contact [20] systems. ...
September 2007