Sorolla, Metamaterials with Negative parameters: Theory, Design and Microwave Applications, John Wiley, Hoboken, NJ, 2008. Javier Mata-Contreras was born in 1976 in Malaga (Spain). He received the Ingenieria de Telecomunicacion Degree from the Universidad de Malaga (UMA) in 2000 and the PhD ...
R.Marques, F.Martin, and M.Sorolla, Metamaterials with Negative Parameters: Theory, Design and Microwave Applications, John Wiley & Sons, Inc., Hoboken, New Jersey, 2008.Marqués, R.; Martin, F.; Sorolla, M. Metamaterials with Negative Parameters: Theory, Design and Microwave Applications...
In Metamaterials with Negative Parameters: Theory, Design and Microwave Applications (Wiley, Hoboken, NJ, 2008). Acknowledgements This work has been supported by MINECO-Spain (project TEC2013-40600-R COM-SEN-RFID, project RTC- 2015-4385-7 META-ACCESS, project RTC-2015-3709-7 META-STOCK), ...
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Monopolar and dipolar res- onances are the two basic forms of resonance, with rotational and polarizing symmetry, respectively. Moreover, in the context of acoustic metamaterials, the spatial symmetry of resonance has special impli- cation in creating negative effective constituent parameters. A ...
3 偏光性与负材料参数(Chirality and Negative Material Parameters) 参数全负的各向同性的左手材料可以以有趣的方式调节电磁波的行为。但是,如果材料结构的手性也参与到了这些材料中,那么材料的偏光性也会影响电磁波的行为。偏光性会导致电磁耦合与双折射(birefringence)。如此前述的负折射现象再次就必须进一步推广。 3....
However, by creating metamaterials with a negative Poisson’s ratio, it is possible to generate new properties that enable the material to react differently than expected, or what is even considered possible. For a rubber band, this could result in widening of the band upon pulling its ends, ...
A Novel Broadband Metamaterial Resonator with Negative Permittivity It is well known that the properties of a metamaterial are usually determined from the geometrical structure and material parameters rather than composition. One of the problems of resonant types of metamaterials is that they usually hav...
These parameters along with the inclined angle θ characterize the geometric feature of the material. 4.1. Negative Poisson's ratio With the expression of α, it can be proved that k1 − k2(cos2θ + 2α sin 2θ) > 0in light of k1 > k2. Then it is seen from Eqs. (10), (11)...
These rotations can compensate the expansion of the all positive constituents, leading to an effectively near-zero thermal length-expansion coefficient, or over-compensate the expansion, leading to an effectively negative thermal length-expansion coefficient. This evidences a striking level of thermal-...