Atomic Polarization - Integrated Circuits and Materials - - An Online Book - |
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| Integrated Circuits and Materials http://www.globalsino.com/ICsAndMaterials/ | ||||||||
| Chapter/Index: Introduction | A | B | C | D | E | F | G | H | I | J | K | L | M | N | O | P | Q | R | S | T | U | V | W | X | Y | Z | Appendix | ||||||||
================================================================================= The polarization in materials can be due to several mechanisms: [1-7] The mechanisms of electronic, ionic and atomic polarizations and depolarizations are much faster (<10-12 sec) than the others. This deformational polarization process is also referred to as the resonance process since it involves vibrating modes. The time required for orientational, hopping, or space charge polarization and depolarization is very long and varies in a wide range, depending on the dielectric systems; such polarization processes are sometimes referred to as relaxation processes because they involve a relaxation time. A relaxation phenomenon occurs when restoring action tends to bring the excited system back to its original equilibrium state. Depending on the time scale, the fast polarizations together can be considered as an instantaneous polarization P0. On the other hand, the polarization is to be finite at longer times, P(t →∞) = Ps, because an infinite amount of electrical energy cannot be stored in a dielectric (or a capacitor). [8] Figure 4553a shows the approximate time required for polarization.
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[1] A. K. Jonscher, Diebtric Relnlnration in Solids. Vol. London, pp. Chelsea Dielectric,
London, 1983.
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