Problemas de Electrodinámica Clásica.

Corresponde a un trabajo desarrollado por cuatro profesores del Area de Electromagnetismo de las Universidades de Salamanca y Valladolid. El objetivo fundamental del proyecto es paliar la escasez de bibliografía en aspectos prácticos (esencialmente problemas) de la asignatura de Electrodinámica Clásica (troncal de segundo ciclo en la Licenciatura en Física). Para ello se ha partido de las colecciones de problemas de los autores, que durante muchos años han impartido la citada asignatura se ha efectuado una selección, se ha consultado la bibliografía y se ha planteado un borrador que se ha ido discutiendo en diversas reuniones de los autores del trabajo hasta llegar a la redacción final que se presenta. Consideramos que el trabajo, que próximamente someteremos a publicación, constituirá una valiosa ayuda para los alumnos de la Licenciatura en Física.

La electrodinámica de cables espaciales

Se discuten los fundamentos que subyacen en la concepción y en las aplicaciones de un cable espacial, o tether. Si el cable es metálico y órbita en un planeta con ionosfera y campo magnético propio —la Tierra misma, o uno de los grandes planetas exteriores-, su movimiento genera una fuerza electromotriz por el mismo proceso de inducción magnética de un simple generador eléctrico, y el circuito conductor se "cierra" a través del plasma ionosférico. Se analiza el problema técnico central al que se enfrentan los tethers electrodinámicos de potencia: cómo establecer un buen contacto eléctrico entre el cable y la rarificada ionosfera. Se discute una reciente solución al problema.

Tópicos da teoria da relatividade

Dissertação de Mestrado, Matemática para Professores, 25 de Outubro 2013, Universidade dos Açores.

La dispersió Møller i els inicis de l’electrodinàmica quàntica: treball de recerca per al mestratge en Història de les Ciències

S’hi analitza la deducció teòrica i la contrastació experimental originals de la dispersió electró-electró (dispersió Møller, 1932), amb l’objectiu d’esbrinar quin paper van tenir en el desenvolupament de l’electrodinàmica quàntica. S’hi mostra que Christian Møller (1904-1980) va deduir la fórmula que du el seu nom mitjançant la noció de correspondència, evitant així els problemes que plantejava una incipient teoria quàntica de camps. La fórmula només va assolir el seu estatus actual d’aplicació paradigmàtica de l’electrodinàmica quàntica després de la Segona Guerra Mundial, un cop la teoria va haver superat aquests problemes a través del procés de renormalització. El treball aclareix d’aquesta manera un episodi clau en el desenvolupament d’una de les teories fonamentals de la física del segle XX.

Oscillatory magnetic tweezers based on ferromagnetic beads and simple coaxial coils

We report the design and validation of simple magnetic tweezers for oscillating ferromagnetic beads in the piconewton and nanometer scales. The system is based on a single pair of coaxial coils operating in two sequential modes: permanent magnetization of the beads through a large and brief pulse of magnetic field and generation of magnetic gradients to produce uniaxial oscillatory forces. By using this two step method, the magnetic moment of the beads remains constant during measurements. Therefore, the applied force can be computed and varies linearly with the driving signal. No feedback control is required to produce well defined force oscillations over a wide bandwidth. The design of the coils was optimized to obtain high magnetic fields (280 mT) and gradients (2 T/m) with high homogeneity (5% variation) within the sample. The magnetic tweezers were implemented in an inverted optical microscope with a videomicroscopy-based multiparticle tracking system. The apparatus was validated with 4.5 ¿m magnetite beads obtaining forces up to ~2 pN and subnanometer resolution. The applicability of the device includes microrheology of biopolymer and cell cytoplasm, molecular mechanics, and mechanotransduction in living cells.

Hadronic vacuum polarization and the Lamb shift

Recent improvements in the determination of the running of the fine-structure constant also allow an update of the hadronic vacuum-polarization contribution to the Lamb shift. We find a shift of -3.40(7) kHz to the 1S level of hydrogen. We also comment on the contribution of this effect to the determination by elastic electron scattering of the rms radii of nuclei.

SL(3,C) elementary instanton configurations

Several SL(3,C) self-dual instanton solutions of the Yang-Mills equations are presented which have very striking properties. While one of them is regular and SU(3) inside (outside) a sphere of arbitrarily large (small) radius, another one has all the characteristics of a meron solution (in particular its topological charge is concentrated at one point) although its Pontryagin number equals one. Their continuation to Minkowski space is also studied.

Finite-temperature QED effects in atoms

We argue that low-temperature effects in QED can, if anywhere, only be quantitatively interesting for bound electrons. Unluckily the dominant thermal contribution turns out to be level independent, so that it does not affect the frequency of the transition radiation.

Three-party entanglement from positronium

The decay of orthopositronium into three photons produces a physical realization of a pure state with three-party entanglement. Its quantum correlations are analyzed using recent results on quantum information theory, looking for the final state that has the maximal amount of Greenberger, Horne, and Zeilinger like correlations. This state allows for a statistical dismissal of local realism stronger than the one obtained using any entangled state of two spin one-half particles.

Renormalization-group improvement of the spectrum of hydrogenlike atoms with massless fermions

We obtain the next-to-next-to-leading-logarithmic renormalization-group improvement of the spectrum of hydrogenlike atoms with massless fermions by using potential NRQED. These results can also be applied to the computation of the muonic hydrogen spectrum where we are able to reproduce some known double logarithms at O(m¿s6). We compare with other formalisms dealing with logarithmic resummation available in the literature.

Invariant decomposition of the retarded electromagnetic field.

The integral representation of the electromagnetic two-form, defined on Minkowski space-time, is studied from a new point of view. The aim of the paper is to obtain an invariant criteria in order to define the radiative field. This criteria generalizes the well-known structureless charge case. We begin with the curvature two-form, because its field equations incorporate the motion of the sources. The gauge theory methods (connection one-forms) are not suited because their field equations do not incorporate the motion of the sources. We obtain an integral solution of the Maxwell equations in the case of a flow of charges in irrotational motion. This solution induces us to propose a new method of solving the problem of the nature of the retarded radiative field. This method is based on a projection tensor operator which, being local, is suited to being implemented on general relativity. We propose the field equations for the pair {electromagnetic field, projection tensor J. These field equations are an algebraic differential first-order system of oneforms, which verifies automatically the integrability conditions.

Classical predictive electrodynamics of two charges with radiation: General framework. I.

Outgoing radiation is introduced in the framework of the classical predictive electrodynamics using LorentzDiracs equation as a subsidiary condition. In a perturbative scheme in the charges the first radiative self-terms of the accelerations, momentum and angular momentum of a two charge system without external field are calculated.

Classical predictive electrodynamics of two charges with radiation: Energy and 3. momentum balance and scattering crossections-II

We deal with a classical predictive mechanical system of two spinless charges where radiation is considered and there are no external fields. The terms (2,2)Paa of the expansion in the charges of the HamiltonJacobi momenta are calculated. Using these, together with known previous results, we can obtain the paa up to the fourth order. Then we have calculated the radiated energy and the 3-momentum in a scattering process as functions of the impact parameter and the incident energy for the former and 3-momentum for the latter. Scattering cross-sections are also calculated. Good agreement with well known results, including those of quantum electrodynamics, has been found.

Finite-temperature QED effects in atoms

We argue that low-temperature effects in QED can, if anywhere, only be quantitatively interesting for bound electrons. Unluckily the dominant thermal contribution turns out to be level independent, so that it does not affect the frequency of the transition radiation.