Estudio acústico de la sala 8 de los cines Kinépolis de Ciudad de la Imagen

Este proyecto consistira en la realization de un estudio aciistico sobre la sala 8 de los cines Kinepolis de Ciudad de la Imagen, que dispone de 408 butacas. Los cines Kinepolis es uno de los mayores complejos multisala de Europa. Cuenta con mas de 9.200 butacas en total distribuidas en 25 salas a las que se accede mediante dos grandes pasillos conectados por el hall. En 1998, ano de su apertura, el complejo recibio el Record Guinness a la sala cinematografica mas grande del mundo, que dispone de 996 butacas. El objetivo de este proyecto es conseguir caracterizar acusticamente una sala de cine a traves de la medicion de parametros acusticos de la sala y de un modelo virtual de la misma. Para llevar a cabo el proyecto, primero se van a realizar tanto una medicion geometrica como acustica de la sala mediante el sistema de medida DIRAC. Los resultados de estas mediciones nos serviran para construir y validar un modelo virtual de la sala real con el software de simulacion EASE. La medicion acustica se va a realizar con el sistema de medicion DIRAC. Este sistema nos dara information sobre una amplia variedad de parametros acusticos. En este proyecto no se va a trabajar con todos ellos, solo con los mas significativos. Estos se describen a continuacion en la introduccion teorica. La medicion geometrica nos va a servir para construir un modelo virtual que tenga las mismas dimensiones que la sala original. Esta medicion la realizaremos mediante un medidor laser y una cinta metrica. Una vez construido el modelo virtual, se procedera a su validacion. Este proceso se realiza ajustando el tiempo de reverberacion del modelo mediante la introduccion de distintos materiales acusticos en las superficies del mismo, de manera que, variando la absorcion de la sala, el tiempo de reverberacion promedio del modelo se asemeje lo mas posible al medido en la sala real. Este proceso tiene como objetivo comprobar que el modelo virtual tiene un comportamiento acustico similar al de la sala real. Es necesario validar adecuadamente el modelo para que las comparaciones y conclusiones sean fiables. Por ultimo, tras la simulacion acustica del modelo, se compararan los resultados simulados con los medidos en la sala. En este proceso se contrastaran algunos de los parametros que guardan relation con el tiempo de reverberacion. De esta manera se verificara si el tiempo de reverberacion es o no un parametro acustico fiable para la validacion de un modelo virtual de una sala de cine. Anteriormente se han realizado proyectos iguales de otras salas de diferente tamano de Kinepolis. El objetivo de realizar el mismo estudio en distintas salas, es comprobar si el tamano de la sala influye en la validacion de los modelos virtuales mediante el tiempo de reverberacion. ABSTRACT. This Project consists on the development of an acoustic research of the movie theater 8 of the Kinepolis complex in Ciudad de la Imagen, Madrid. This room has 408 spots. Kinepolis is one of the biggest multiplex complexes in Europe. It has 9,200 locations disposed in 25 rooms. There are two large corridors which give access to all of theaters. In the middle of the structure, there is the main hall that connects these corridors. In 1998, at the time when the complex was open, it was awarded with the Record Guinness for the biggest theater in the world, which has 996 locations. The target of this project is to successfully characterize the acoustics of a movie theater through reverberation time and a virtual model. In order to reach this goal, in the first place, we are going to perform both, an acoustic and a geometric measurement of the room using DIRAC measurement system. The results of these measures will allow us to build and validate a virtual model of the room, using the simulation software EASE. We are going to use the DIRAC system in order to accomplish the acoustic measure. This operation gives us a huge variety of acoustic parameters. Not all of these are going to be used for this research, only the most significant ones. These are described in the theoretical introduction. The geometric measure is essential to help us to build the virtual model, because the model has to be exactly equal as the real room. This measurement will be performed with an electronic distance meter and a measuring tape. Once the virtual model is finished, it will be proved. This validation process will be realized by adjusting the reverberation time in the model. We will change the walls materials, therefore, the overall absorption of the room will change. We want the model reverberation time resemble to the real one. This practice is going to ensure that the model acoustic performance is close to the real one. In addition, it has to be successfully validate of we want the future comparisons to be reliable. Finally, after the model virtual simulation, we will compare the simulated results with the measure in the room. In this process, we will compare not only the reverberation time, but others parameters that keep relation with the reverberation time. We will verify this way, if the reverberation time is or is not an appropriate acoustic parameter to validate a virtual model of a movie theater. There have been done others similar acoustic researches in different theaters with different sizes. The aim of performing similar researches in different rooms is to determine if the size of the room infers in the validation process.

Estudio acústico de la sala de control de los estudios de grabación Sadman

En este proyecto se ha realizado el estudio del campo acústico de un estudio de grabación, en concreto el estudio de grabación “Sadman”, situado en Madrid. El estudio viene motivado por una serie de problemas de resonancia en frecuencias graves de la sala de control del estudio, lo cual genera algunas alteraciones desagradables cuando se realiza una escucha por el sistema de altavoces en dicha sala. Además de estudiar este problema, se han estudiado otros parámetros acústicos para poder plantear, si fuese necesario, posibles mejoras que faciliten las labores que se realizan en la sala. Para realizar tanto el estudio del campo acústico de la sala como su modelado se han utilizado herramientas tales como AutoCAD, Ease, Dirac y Spectraplus. Palabras clave: Acústica, modos de vibración, frecuencia, resonancia, Dirac, Ease, AutoCAD, Spectraplus, absorbente, difusor. ABSTRACT. The present project is aimed to study the acoustics of a recording studio. A report on "Sadman Studios" located in Madrid. The investigation was made due to a low frequency vibration problem on the control room that generated undesirable acoustic disturbances when the main monitoring system was running. Apart from the modal frequencies problem, several acoustic parameters have been submitted to investigation in case improvements in the acoustic field needed to be implemented, if required. System tools like AutoCAD, Ease, Dirac and Spectraplus were used to properly understand and reflect the issues we were faced with under the investigation of the within matter.

Propriedades de continuação única para soluções de equações de Schrödinger com ponto de interação

Neste trabalho, estudamos propriedades de continuação única para as soluções da equação tipo Schrödinger com um ponto interação centrado em x=0, \\partial_tu=i(\\Delta_Z+V)u, onde V=V(x,t) é uma função de valor real e -\\Delta_Z é o operador escrito formalmente como \\[-\\Delta_Z=-\\frac\\frac{d^2}{dx^2}+Z\\delta_0,\\] sendo \\delta_0 a delta de Dirac centrada em zero e Z qualquer número real. Logo, usamos estes resultados para ver o possível fenômeno de concentração das soluções, que explodem, da equação de tipo Schrödinger não linear com um ponto de interação em x=0, \\[\\partial_tu=i(\\Delta_Zu+|u|^u),\\] com ho>5. Também, mostramos que para certas condições sobre o potencial dependente do tempo V, a equação linear em cima tem soluções não triviais.

Subband energy in two-band δ-doped semiconductors

We study electron dynamics in a two-band δ-doped semiconductor within the envelope-function approximation. Using a simple parametrization of the confining potential arising from the ionized donors in the δ -doping layer, we are able to find exact solutions of the Dirac-type equation describing the coupling of host bands. As an application we then consider Si δ -doped GaAs. In particular we find that the ground subband energy scales as a power law of the Si concentration per unit area in a wide range of doping levels. In addition, the coupling of host bands leads to a depression of the subband energy due to nonparabolicity effects.

Colossal anisotropy in diluted magnetic topological insulators

We consider dilute magnetic doping in the surface of a three dimensional topological insulator where a two dimensional Dirac electron gas resides. We find that exchange coupling between magnetic atoms and the Dirac electrons has a strong and peculiar effect on both. First, the exchange-induced single ion magnetic anisotropy is very large and favors off-plane orientation. In the case of a ferromagnetically ordered phase, we find a colossal magnetic anisotropy energy, of the order of the critical temperature. Second, a persistent electronic current circulates around the magnetic atom and, in the case of a ferromagnetic phase, around the edges of the surface.

Efficient intrinsic spin relaxation in graphene due to flexural distortions

We propose an intrinsic spin scattering mechanism in graphene originated by the interplay of atomic spin-orbit interaction and the local curvature induced by flexural distortions of the atomic lattice. Starting from a multiorbital tight-binding Hamiltonian with spin-orbit coupling considered non-perturbatively, we derive an effective Hamiltonian for the spin scattering of the Dirac electrons due to flexural distortions. We compute the spin lifetime due to both flexural phonons and ripples and we find values in the 1-10 ns range at room temperature. The proposed mechanism dominates the spin relaxation in high mobility graphene samples and should also apply to other planar aromatic compounds.

Anisotropic intrinsic spin relaxation in graphene due to flexural distortions

We propose an intrinsic spin scattering mechanism in graphene originated by the interplay of atomic spin-orbit interaction and the local curvature induced by flexural distortions of the atomic lattice. Starting from a multiorbital tight-binding Hamiltonian with spin-orbit coupling considered nonperturbatively, we derive an effective Hamiltonian for the spin scattering of the Dirac electrons due to flexural distortions. We compute the spin lifetime due to both flexural phonons and ripples and we find values in the microsecond range at room temperature. Interestingly, this mechanism is anisotropic on two counts. First, the relaxation rate is different for off-plane and in-plane spin quantization axis. Second, the spin relaxation rate depends on the angle formed by the crystal momentum with the carbon-carbon bond. In addition, the spin lifetime is also valley dependent. The proposed mechanism sets an upper limit for spin lifetimes in graphene and will be relevant when samples of high quality can be fabricated free of extrinsic sources of spin relaxation.

Quantum anomalous Hall effect in graphene coupled to skyrmions

Skyrmions are topologically protected spin textures, characterized by a topological winding number N, that occur spontaneously in some magnetic materials. Recent experiments have demonstrated the capability to grow graphene on top Fe/Ir, a system that exhibits a two-dimensional skyrmion lattice. Here we show that a weak exchange coupling between the Dirac electrons in graphene and a two-dimensional skyrmion lattice withN = ±1 drives graphene into a quantum anomalous Hall phase, with a band gap in bulk, a Chern number C = 2N, and chiral edge states with perfect quantization of conductance G = 2N e2 h . Our findings imply that the topological properties of the skyrmion lattice can be imprinted in the Dirac electrons of graphene.

Orbital Magnetization of Quantum Spin Hall Insulator Nanoparticles

Both spin and orbital degrees of freedom contribute to the magnetic moment of isolated atoms. However, when inserted in crystals, atomic orbital moments are quenched because of the lack of rotational symmetry that protects them when isolated. Thus, the dominant contribution to the magnetization of magnetic materials comes from electronic spin. Here we show that nanoislands of quantum spin Hall insulators can host robust orbital edge magnetism whenever their highest occupied Kramers doublet is singly occupied, upgrading the spin edge current into a charge current. The resulting orbital magnetization scales linearly with size, outweighing the spin contribution for islands of a few nm in size. This linear scaling is specific of the Dirac edge states and very different from Schrodinger electrons in quantum rings. By modeling Bi(111) flakes, whose edge states have been recently observed, we show that orbital magnetization is robust with respect to disorder, thermal agitation, shape of the island, and crystallographic direction of the edges, reflecting its topological protection.

Edge states in graphene-like systems

The edges of graphene and graphene like systems can host localized states with evanescent wave function with properties radically different from those of the Dirac electrons in bulk. This happens in a variety of situations, that are reviewed here. First, zigzag edges host a set of localized non-dispersive state at the Dirac energy. At half filling, it is expected that these states are prone to ferromagnetic instability, causing a very interesting type of edge ferromagnetism. Second, graphene under the influence of external perturbations can host a variety of topological insulating phases, including the conventional quantum Hall effect, the quantum anomalous Hall (QAH) and the quantum spin Hall phase, in all of which phases conduction can only take place through topologically protected edge states. Here we provide an unified vision of the properties of all these edge states, examined under the light of the same one orbital tight-binding model. We consider the combined action of interactions, spin–orbit coupling and magnetic field, which produces a wealth of different physical phenomena. We briefly address what has been actually observed experimentally.

Lectures on quantum electrodynamics,

Mode of access: Internet.

Coherent state construction of representations of osp(2|2) and primary fields of osp(2|2) conformal field theory

Representations of the superalgebra osp(2/2)(k)((1)) and current superalgebra. osp(2/2)k in the standard basis are investigated. All finite-dimensional typical and atypical representations of osp(2/2) are constructed by the vector coherent state method. Primary fields of the non-unitary conformal field theory associated with osp(2/2)(k)((1)) in the standard basis are obtained for arbitrary level k. (C) 2004 Elsevier B.V. All rights reserved.

Application of density functional theory to analysis of energetic heterogeneity and pore size distribution of activated carbons

A new approach based on the nonlocal density functional theory to determine pore size distribution (PSD) of activated carbons and energetic heterogeneity of the pore wall is proposed. The energetic heterogeneity is modeled with an energy distribution function (EDF), describing the distribution of solid-fluid potential well depth (this distribution is a Dirac delta function for an energetic homogeneous surface). The approach allows simultaneous determining of the PSD (assuming slit shape) and EDF from nitrogen or argon isotherms at their respective boiling points by using a set of local isotherms calculated for a range of pore widths and solid-fluid potential well depths. It is found that the structure of the pore wall surface significantly differs from that of graphitized carbon black. This could be attributed to defects in the crystalline structure of the surface, active oxide centers, finite size of the pore walls (in either wall thickness or pore length), and so forth. Those factors depend on the precursor and the process of carbonization and activation and hence provide a fingerprint for each adsorbent. The approach allows very accurate correlation of the experimental adsorption isotherm and leads to PSDs that are simpler and more realistic than those obtained with the original nonlocal density functional theory.

Axial Anomaly for Eguchi-Hanson Metrics with Nonzero Total Mass

We compute the Dirac indexes for. the two spin structures kappa(0) and kappa(1) for Eguchi-Hanson metrics with nonzero total mass. It shows that the Dirac indexes do not vanish in general, and axial anomaly exists. When the metric has zero total mass, the Dirac index vanishes for the spin structure no, and no axial anomaly exists in this case.

Dual-symmetric Lagrangians in quantum electrodynamics: I. Conservation laws and multi-polar coupling

By using a complex field with a symmetric combination of electric and magnetic fields, a first-order covariant Lagrangian for Maxwell's equations is obtained, similar to the Lagrangian for the Dirac equation. This leads to a dual-symmetric quantum electrodynamic theory with an infinite set of local conservation laws. The dual symmetry is shown to correspond to a helical phase, conjugate to the conserved helicity. There is also a scaling symmetry, conjugate to the conserved entanglement. The results include a novel form of the photonic wavefunction, with a well-defined helicity number operator conjugate to the chiral phase, related to the fundamental dual symmetry. Interactions with charged particles can also be included. Transformations from minimal coupling to multi-polar or more general forms of coupling are particularly straightforward using this technique. The dual-symmetric version of quantum electrodynamics derived here has potential applications to nonlinear quantum optics and cavity quantum electrodynamics.