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[198]. - PolyU
[198]. - PolyU

... Yet, when surface effects from polarization gradients, near-surface lattice relaxation [27], and depolarization field Ed are involved, the accuracy of the Landau approach suffers, particularly when Ed is significant such as under opencircuit boundary conditions. Very often [7], the depolarization fi ...
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Low-field microwave absorption in pulsed lased deposited FeSi thin films

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... I have here a weight on a spring. If we pull it down, it will oscillate up and down. T h a t is what we call a mechanical oscillation. T o get an electrical oscillation, suppose we take, as I have here, a metal ball connected by a wire t o another metal ball. Now suppose you have positive electricit ...
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... Let the folowing experiment be considered: a glass rod is rubbed against a piece of fur and the two objects are afterwards placed in their previous positions, waiting for them to regain their previous thermal state as well. It easy to see that the two objects exibit a new state, called electrificati ...
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Advanced Solid State Physics

... The atoms arrange in particular patterns because the patterns minimize the energy in a binding, which is typically with more than one neighbor in a solid. An ordered (periodic) arrangement is called crystal, a disordered arrangement is called amorphous. All the macroscopic properties like electrical ...
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Superconductivity



Superconductivity is a phenomenon of exactly zero electrical resistance and expulsion of magnetic fields occurring in certain materials when cooled below a characteristic critical temperature. It was discovered by Dutch physicist Heike Kamerlingh Onnes on April 8, 1911 in Leiden. Like ferromagnetism and atomic spectral lines, superconductivity is a quantum mechanical phenomenon. It is characterized by the Meissner effect, the complete ejection of magnetic field lines from the interior of the superconductor as it transitions into the superconducting state. The occurrence of the Meissner effect indicates that superconductivity cannot be understood simply as the idealization of perfect conductivity in classical physics.The electrical resistivity of a metallic conductor decreases gradually as temperature is lowered. In ordinary conductors, such as copper or silver, this decrease is limited by impurities and other defects. Even near absolute zero, a real sample of a normal conductor shows some resistance. In a superconductor, the resistance drops abruptly to zero when the material is cooled below its critical temperature. An electric current flowing through a loop of superconducting wire can persist indefinitely with no power source.In 1986, it was discovered that some cuprate-perovskite ceramic materials have a critical temperature above 90 K (−183 °C). Such a high transition temperature is theoretically impossible for a conventional superconductor, leading the materials to be termed high-temperature superconductors. Liquid nitrogen boils at 77 K, and superconduction at higher temperatures than this facilitates many experiments and applications that are less practical at lower temperatures.
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