La "imagen" de la caverna y la tentación constante de corregir a Platón: Benjamin Jowett como ejemplo

Las traducciones de los primeros capítulos del libro VII de la República de Platón en los que aparece su famosa imagen de la caverna, eikón, presentan una sorprendente e intrigante variedad interpretativa: "alegoría", "mito", "fábula", "parábola", "símil", "comparación"... Este artículo, tomando como ejemplo la notable fidelidad al texto del traductor victoriano de Platón, B. Jowett, y mediante un análisis riguroso de los términos que acompañan la imagen, mantiene la necesidad de no interpretar ni corregir en este caso al gran filósofo idealista o "ideocéntrico", señalando al mismo tiempo, si es otro el proceder, las contradicciones resultantes y el uso de algún término ajeno al léxico platónico como "alegoría".

Quantum black hole entropy and newton constant renormalization

ty that low-energy effective field theory could be sufficient to understand the microscopic degrees of freedom underlying black hole entropy. We propose a qualitative physical picture in which black hole entropy refers to a space of quasicoherent states of infalling matter, together with its gravitational field. We stress that this scenario might provide a low-energy explanation of both the black hole entropy and the information puzzle.

Canonical formalism for path dependent Lagrangians. Coupling constant expansions

A canonical formalism obtained for path-dependent Lagrangians is applied to Fokker-type Lagrangians. The results are specialized for coupling constant expansions and later on are applied to relativistic systems of particles interacting through symmetric scalar and vector mesodynamics and electrodynamics.

Magnetic properties of amorphous Fe-Si compositionally modulated thin films

The present paper reports on a magnetometric study of Fe‐Si compositionally modulated thin films. The low‐temperature dependence of the magnetization exhibit Bloch's T3/2 dependence with a minor T5/2 correction term. The spin‐wave stiffness constant deduced from the temperature coefficient depends on the characteristic modulation length and its values are much lower that in glassy alloys.