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2
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85036219084
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A. P. Vinogradov, Proceedings of the International Seminar on Electrodynamics of Chiral and Bianisotropic Media “Bianisotropics ’93” (Helsinki University of Technology, Espoo, 1993), Rep. 159, p. 22
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A. P. Vinogradov, Proceedings of the International Seminar on Electrodynamics of Chiral and Bianisotropic Media “Bianisotropics ’93” (Helsinki University of Technology, Espoo, 1993), Rep. 159, p. 22.
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3
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0031383811
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C. R. Simovski, S. A. Tretyakov, A. A. Sochava, B. Sauviac, F. Mariotte, and T. G. Kharina, J. Electromagn. Waves Appl. 11, 1509 (1997).
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Simovski, C.R.1
Tretyakov, S.A.2
Sochava, A.A.3
Sauviac, B.4
Mariotte, F.5
Kharina, T.G.6
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5
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A. K. Sarychev and Yu. R. Smychkovich, Actual Problems of Technology of Composite Materials for Microelectronics Information Systems, Proceedings of the first National Conference, Yalta, 1990 (Simferopol State University, Simferopol, 1990) (in Russian);
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A. K. Sarychev and Yu. R. Smychkovich, Actual Problems of Technology of Composite Materials for Microelectronics Information Systems, Proceedings of the first National Conference, Yalta, 1990 (Simferopol State University, Simferopol, 1990) (in Russian)
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6
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85036347819
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MRS, San Francisco, p. L6.14
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I. V. Kukolev, A. N. Lagarkov, S. M. Matitsin, K. N. Rozanov, and A. P. Vinogradov, Proceedings of the Spring Meeting (MRS, San Francisco, 1992), p. L6.14.
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Kukolev, I.V.1
Lagarkov, A.N.2
Matitsin, S.M.3
Rozanov, K.N.4
Vinogradov, A.P.5
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8
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J. C. Garland and D. B. Tanner AIP, New York
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R. Landauer, in Electrical Transport and Optical Properties of Inhomogeneous Media, Ohio State University, 1977, edited by J. C. Garland and D. B. Tanner, AIP Conf. Proc. No. 40 (AIP, New York, 1978).
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Electrical Transport and Optical Properties of Inhomogeneous Media, Ohio State University, 1977 AIP Conf. Proc.
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Landauer, R.1
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9
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0003724744
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L. D. Landau, E. M. Lifshitz, and L. P. Pitaevskii, Electrodynamics of Continuous Media, 2nd ed. (Butterworth Heinemann, Oxford, 1995).
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Landau, L.D.1
Lifshitz, E.M.2
Pitaevskii, L.P.3
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10
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85036428231
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I. E. Tamm, Basic Electricity Theory (GITTL, Moscow, 1956) (in Russian)
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I. E. Tamm, Basic Electricity Theory (GITTL, Moscow, 1956) (in Russian).
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85036153521
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M. M. Bredov, V. V. Rumyantzev, and I. N. Toptyghin, Classical Electrodynamics (Nauka, Moscow, 1985) (in Russian)
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M. M. Bredov, V. V. Rumyantzev, and I. N. Toptyghin, Classical Electrodynamics (Nauka, Moscow, 1985) (in Russian).
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A. N. Lagarkov and A. P. Vinogradov, Advances in Complex Electromagnetic Materials, edited by A. Priou et al., Vol. 28 of NATO Advanced Study Institute Partnership Sub Series 3. High Technology (Kluwer, Dordrecht, 1997), p. 117
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A. N. Lagarkov and A. P. Vinogradov, Advances in Complex Electromagnetic Materials, edited by A. Priou et al., Vol. 28 of NATO Advanced Study Institute Partnership Sub Series 3. High Technology (Kluwer, Dordrecht, 1997), p. 117.
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V. P. Silin and A. A. Rukhadze, Electromagnetic Properties of Plasma and Plasma Like Media (GosAtomIzdat, Moscow, 1961) (in Russian)
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V. P. Silin and A. A. Rukhadze, Electromagnetic Properties of Plasma and Plasma Like Media (GosAtomIzdat, Moscow, 1961) (in Russian).
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21
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85036417007
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Certainly, there are other representations. One example was presented by R. Raab (private communication), (Formula presented)where (Formula presented) (Formula presented) (Formula presented)Unfortunately, contrary to Eqs. (6789), some of the terms have no clear physical sense
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Certainly, there are other representations. One example was presented by R. Raab (private communication), (Formula presented)where (Formula presented) (Formula presented) (Formula presented)Unfortunately, contrary to Eqs. (6789), some of the terms have no clear physical sense.
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23
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85036433651
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We imply that the scale of this level is still much less than the wavelength
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We imply that the scale of this level is still much less than the wavelength.
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24
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0342977187
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A. P. Vinogradov, L. V. Panina, and A. K. Sarychev, Dokl. Akad. Nauk (SSSR) 306, 847 (1989) [Sov. Phys. Dokl. 34, 530 (1989)].
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, vol.34
, pp. 530
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Vinogradov, A.P.1
Panina, L.V.2
Sarychev, A.K.3
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25
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85036283350
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V. M. Dubovik and S. V. Shabanov, Essay on The Formal Aspects of Electromagnetic Theory, edited by A. Lakhtakia (World Scientific, New York, 1993), p. 339;
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V. M. Dubovik and S. V. Shabanov, Essay on The Formal Aspects of Electromagnetic Theory, edited by A. Lakhtakia (World Scientific, New York, 1993), p. 339
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28
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0000600798
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Ya. B. Zeld´ovich, Zh. Éksp. Teor. Fiz. 33, 1531 (1957) Zh. Éksp. Teor. Fiz. 33, 1531 (1957) [ Sov. Phys. JETP 6, 1184 (1958)].
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, vol.6
, pp. 1184
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Zeld´ovich, Ya.B.1
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30
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0028766567
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Busarov, I.G.2
Posudnevsky, O.P.3
Romanenco, V.E.4
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31
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26844547183
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A. P. Vinogradov, A. A. Kalachev, A. N. Lagarkov, V. E. Romanenko, and G. V. Kazantseva, Dokl. Acad. Nauk 349, 182 (1996) [Sov. Phys. Dokl. 41, 291 (1996)].
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, pp. 291
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Vinogradov, A.P.1
Kalachev, A.A.2
Lagarkov, A.N.3
Romanenko, V.E.4
Kazantseva, G.V.5
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33
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85036237990
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R. P. Feynman, R. B. Leghton, and M. Sands, The Feynman Lectures on Physics (Addison-Wesley Publishing Company, Reading, MA, 1996), Vol. I, Chap. 33–35
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R. P. Feynman, R. B. Leghton, and M. Sands, The Feynman Lectures on Physics (Addison-Wesley Publishing Company, Reading, MA, 1996), Vol. I, Chap. 33–35.
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34
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85036301509
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Owing to symmetry of the cell, the mean value of the current (Formula presented) is equal to (Formula presented)
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Owing to symmetry of the cell, the mean value of the current (Formula presented) is equal to (Formula presented).
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35
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85036189886
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The patterns in Figs. 11(b) and 11(c) are of the same order. One can comprise the (Formula presented) pattern employing (Formula presented) and (Formula presented) patterns (see Fig. 22), which is a graphical analog of Eq. (6): Fig. 11(a) =Fig. 11(b) + Fig. 11(c). So, in some sense, Eq. (6) is the presentation of the field as the sum of a part symmetric in (Formula presented) and a part that is antisymmetric
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The patterns in Figs. 11(b) and 11(c) are of the same order. One can comprise the (Formula presented) pattern employing (Formula presented) and (Formula presented) patterns (see Fig. 22), which is a graphical analog of Eq. (6): Fig. 11(a) =Fig. 11(b) + Fig. 11(c). So, in some sense, Eq. (6) is the presentation of the field as the sum of a part symmetric in (Formula presented) and a part that is antisymmetric.
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36
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85036323768
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The restriction to Eq. (17) or even to Eq. (1) does not mean that the fields generated by the current from the PISVE have dipole-quadrupole character. As is shown in 10, multipole expansion of these radiated fields in a source-free region contains, in the general case, all multipole contributions (see Chap. 16.2 in 10
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The restriction to Eq. (17) or even to Eq. (1) does not mean that the fields generated by the current from the PISVE have dipole-quadrupole character. As is shown in 10, multipole expansion of these radiated fields in a source-free region contains, in the general case, all multipole contributions (see Chap. 16.2 in 10).
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