Transformation Electromagnetics and Metamaterials: Fundamental Principles and Applications

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This can allow for the construction of new composite artificial devices , which probably could not exist without metamaterials and coordinate transformation. Computing power that became available in the late s enables prescribed quantitative values for the permittivity and permeability , the constitutive parameters , which produce localized spatial variations.

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The aggregate value of all the constitutive parameters produces an effective value , which yields the intended or desired results. Hence, complex artificial materials, known as metamaterials , are used to produce transformations in optical space. The mathematics underpinning transformation optics is similar to the equations that describe how gravity warps space and time, in general relativity.

However, instead of space and time , these equations show how light can be directed in a chosen manner, analogous to warping space. For example, one potential application is collecting sunlight with novel solar cells by concentrating the light in one area. Hence, a wide array of conventional devices could be markedly enhanced by applying transformation optics. Transformation optics has its beginnings in two research endeavors, and their conclusions.

They were published on May 25, , in the same issue of the peer-reviewed journal Science.

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The two papers describe tenable theories on bending or distorting light to electromagnetically conceal an object. Both papers notably map the initial configuration of the electromagnetic fields on to a Cartesian mesh. Twisting the Cartesian mesh, in essence, transforms the coordinates of the electromagnetic fields, which in turn conceal a given object.

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Hence, with these two papers, transformation optics is born. Transformation optics subscribes to the capability of bending light , or electromagnetic waves and energy , in any preferred or desired fashion, for a desired application. Maxwell's equations do not vary even though coordinates transform. Instead values of chosen parameters of materials "transform", or alter, during a certain time period.

Electrodynamics of transformation-based invisibility cloaking

Transformation optics developed from the capability to choose which parameters for a given material, known as a metamaterial. Hence, since Maxwell's equations retain the same form, it is the successive values of permittivity and permeability that change, over time. Permittivity and permeability are in a sense responses to the electric and magnetic fields of a radiated light source respectively, among other descriptions. The precise degree of electric and magnetic response can be controlled in a metamaterial, point by point. Since so much control can be maintained over the responses of the material, this leads to an enhanced and highly flexible gradient-index material.

Conventionally predetermined refractive index of ordinary materials become independent spatial gradients, that can be controlled at will. Therefore, transformation optics is a new method for creating novel and unique optical devices. Transformation optics can go beyond cloaking mimic celestial mechanics because its control of the trajectory and path of light is highly effective. Transformation optics is a field of optical and material engineering and science embracing nanophotonics , plasmonics , and optical metamaterials.

Developments in this field focus on advances in research of transformation optics.

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Transformation optics is the foundation for exploring a diverse set of theoretical , numerical , and experimental developments, involving the perspectives of the physics and engineering communities. The multi-disciplinary perspectives for inquiry and designing of materials develop understanding of their behaviors, properties, and potential applications for this field. If a coordinate transformation can be derived or described, a ray of light in the optical limit will follow lines of a constant coordinate. There are constraints on the transformations, as listed in the references. In general, however, a particular goal can be accomplished using more than one transformation.

The classic cylindrical cloak first both simulated and demonstrated experimentally can be created with many transformations. The simplest, and most often used, is a linear coordinate mapping in the radial coordinate. There is significant ongoing research into determining advantages and disadvantages of particular types of transformations, and what attributes are desirable for realistic transformations. One example of this is the broadband carpet cloak: the transformation used was quasi-conformal.

Such a transformation can yield a cloak that uses non-extreme values of permittivity and permeability , unlike the classic cylindrical cloak, which required some parameters to vary towards infinity at the inner radius of the cloak. General coordinate transformations can be derived which compress or expand space, bend or twist space, or even change the topology e. Much current interest involves designing invisibility cloaks , event cloaks , field concentrators, or beam-bending waveguides. The interactions of light and matter with spacetime , as predicted by general relativity , can be studied using the new type of artificial optical materials that feature extraordinary abilities to bend light which is actually electromagnetic radiation.


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This research creates a link between the newly emerging field of artificial optical metamaterials to that of celestial mechanics , thus opening a new possibility to investigate astronomical phenomena in a laboratory setting. The recently introduced, new class, of specially designed optical media can mimic the periodic , quasi-periodic and chaotic motions observed in celestial objects that have been subjected to gravitational fields.

CIPTz have applications as optical cavities. As such, CIPTs can control, slow and trap light in a manner similar to celestial phenomena such as black holes , strange attractors , and gravitational lenses. A composite of air and the dielectric Gallium Indium Arsenide Phosphide GaInAsP , operated in the infrared spectral range and featured a high refractive index with low absorptions. This opens an avenue to investigate light phenomena that imitates orbital motion , strange attractors and chaos in a controlled laboratory environment by merging the study of optical metamaterials with classical celestial mechanics.


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If a metamaterial could be produced that did not have high intrinsic loss and a narrow frequency range of operation then it could be employed as a type of media to simulate light motion in a curved spacetime vacuum. Such a proposal is brought forward, and metamaterials become prospective media in this type of study. The classical optical-mechanical analogy renders the possibility for the study of light propagation in homogeneous media as an accurate analogy to the motion of massive bodies, and light, in gravitational potentials. A direct mapping of the celestial phenomena is accomplished by observing photon motion in a controlled laboratory environment.

The materials could facilitate periodic, quasi-periodic and chaotic light motion inherent to celestial objects subjected to complex gravitational fields. Twisting the optical metamaterial effects its "space" into new coordinates. The light that travels in real space will be curved in the twisted space, as applied in transformational optics. This effect is analogous to starlight when it moves through a closer gravitational field and experiences curved spacetime or a gravitational lensing effect.

This analogue between classic electromagnetism and general relativity, shows the potential of optical metamaterials to study relativity phenomena such as the gravitational lens. Observations of such celestial phenomena by astronomers can sometimes take a century of waiting. Chaos in dynamic systems is observed in areas as diverse as molecular motion, population dynamics and optics. In particular, a planet around a star can undergo chaotic motion if a perturbation, such as another large planet, is present.

However, owing to the large spatial distances between the celestial bodies, and the long periods involved in the study of their dynamics, the direct observation of chaotic planetary motion has been a challenge. The use of the optical-mechanical analogy may enable such studies to be accomplished in a bench-top laboratory setting at any prescribed time.

The study also points toward the design of novel optical cavities and photon traps for application in microscopic devices and lasers systems. Matter propagating in a curved spacetime is similar to the electromagnetic wave propagation in a curved space and in an in homogeneous metamaterial, as stated in the previous section. Hence a black hole can possibly be simulated using electromagnetic fields and metamaterials. In July a metamaterial structure forming an effective black hole was theorized, and numerical simulations showed a highly efficient light absorption.

The first experimental demonstration of electromagnetic black hole at microwave frequencies occurred in October The proposed black hole was composed of non-resonant, and resonant, metamaterial structures, which can absorb electromagnetic waves efficiently coming from all directions due to the local control of electromagnetic fields. It was constructed of a thin cylinder at This structure created a gradient index of refraction , necessary for bending light in this way.

However, it was characterized as being artificially inferior substitute for a real black hole. It is singularly a light absorber. The light absorption capability could be beneficial if it could be adapted to technologies such as solar cells. However, the device is limited to the microwave range. Also in , transformation optics were employed to mimic a black hole of Schwarzschild form. Similar properties of photon sphere were also found numerically for the metamaterial black hole. Several reduced versions of the black hole systems were proposed for easier implementations.

The dotted line and the small arrow indicate the trajectory and the exact location of the particle, respectively. It is very interesting to look back at the development of methods for fabricating invisibility cloaks over the past few years. Figure 4 provides a brief chronological roadmap of some milestones towards achieving invisibility cloaking. Each milestone was established by providing a solution to previous limitations.

Milestones established on the path to implementing invisibility cloaks. Figure reprinted with permission: a , Ref. The first invisibility cloak Figure 4a was constructed at microwave frequencies using simplified parameters based on traditional split-ring-resonator SRR metamaterial technologies 69 for a particular polarization. Similar SRR experiments have also been reported for the other polarization. A significant breakthrough subsequently followed, which was able to bypass the bandwidth limitation and push the working frequencies into the optical spectrum.

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Transformation optics

This idea is illustrated in Figure 5a. Quasi-conformal mapping can efficiently generate orthogonal meshes that have almost square shapes, which can be possibly implemented using isotropic materials. The reflected ray is exactly restored as if nothing was on top of the ground plane. This exciting carpet cloak model with quasi-conformal mapping has resulted in a considerable number of subsequent experimental implementations Figure 4b—4f. The first implementation Figure 4b based on this model was also at microwave frequencies, but the traditional SRR structure was changed to a non-resonant but still metallic structure.