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E. M. Chudnovsky, “Theory of spin Hall effect: Extension of the Drude model,” Phys. Rev. Lett. 99, 206601 (2007).
S. Takahashi and S. Maekawa, “Spin current in metals and superconductors,” J. Phys. Soc. Jpn. 77, 031009 (2008).
N. Nagaosa, J. Sinova, S. Onoda, A. H. MacDonald, and N. P. Ong, “Anoumalous Hall effect,” Rev. Mod. Phys. 82, 1539 (2008).
S. A. Mikhailov and K. Ziegler, “Nonlinear electromagnetic response of graphen: Frequency multiplication and the self-consistent-field effects,” J. Phys.: Condens. Matter 20, 1 (2008).
J. D. Jackson, Classical Electrodynamics, 3rd ed. (Wiley, New York, 1999), p. 549.
R. Karplus and J. M. Luttinger, “Hall effect in ferromagnetics,” Phys. Rev. 95, 1154 (1954).
J. Smit, “The spontaneous Hall effect in ferromagnetics I,” Physica 21, 877 (1955).
J. Smit, “The spontaneous Hall effect in ferromagnetics II,” Physica 24, 39 (1958).
J. Kondo, “Anomalous Hall effect and magnetoresistance of ferromagnetic metals,” Prog. Theor. Phys. 27, 772 (1962).
G. Y. Guo, S. Maekawa, and N. Nagaosa, “Enhanced spin Hall effect by resonant skew scattering in the orbital-dependent Kondo effect,” Phys. Rev. Lett. 102, 036401 (1970).
L. Berger, “Side-jump mechanism for the Hall effect of ferromagnets,” Phys. Rev. B 2, 4559 (1970).
L. Berger, “Hall effect of a compensated magnetic metal proportional to MB2 in the high-field limit,” Phys. Rev. 177, 790 (1969).
M. Sakai, D. Kodama, T. Sakuraba, Z. Honda, S. Hasegawa, A. Kitajima, A. Oshima, K. Higuchi, and O. Nakamura, “Negative magnetoresistance generated by combination of spin-orbit interaction and applied magnetic field,” Jpn. J. Appl. Phys. 51, 023001 (2012).
M. Sakai, D. Kodama, Y. Okano, T. Sakuraba, Z. Honda, A. Kitajima, A. Oshima, K. Higuchi, S. Hasegawa, and O. Nakamura, “Magnetoresistance generated by combination of spin-orbit interaction and applied magnetic field in bipolar conductors,” Jpn. J. Appl. Phys. 52, 093001 (2013).
J. M. Lavine, “Alternate current apparatus for measuring the ordinary Hall coefficient of ferromagnetic metals and semiconductors,” Rev. Sci. Instrum. 29, 970 (1958).
S. Sikorski and A. Kobus, “Influence of the skin-effect on Hall voltage in semiconductors,” Solid-State Electronics 10, 1063 (1967).
A. H. MacDonald, T. M. Rice, and W. F. Brinkman, “Hall voltage and current distributions in an ideal two-dimensional system,” Phys. Rev. B 28, 3648 (1983).
H. Akera, “Crossover of the Hall-voltage distribution in ac quantum Hall effect,” Physica E 43, 1240 (2011).
F. L. A. Machado and S. M. Rezende, “A theoretical model for the giant magnetoimpedance in ribbons of amorphous soft-ferromagnetic alloys,” J. Appl. Phys. 79, 6558 (1996).
L. V. Panina and K. Mohri, “Magneto-impedance effect in amorphous wires,” Appl. Phys. Lett. 65, 1189 (1994).
Y. Aharonov, P. Pearle, and L. Vaidman, “Comment on “Proposed Aharonov-Casher effect: Another example of an Aharonov-Bohm effect arising from a classical lag”,” Phys. Rev. A 37, 4052 (1988).
W. Schockley and R. P. James, ““Try simplest cases” discovery of “hidden momentum” forces on “magnetic currents”,” Phys. Rev. Lett. 18, 876 (1967).
A. L. Kholmetskii, O. V. Missevitch, and T. Yarman, “Reply to comments on ‘Electromagnetic force on a moving dipole','' Eur. J. Phys. 33, L7 (2012).
V. Hnidzo, “Comments on ‘Electromagnetic force on a moving dipole','' Eur. J. Phys. 33, L3 (2012).
K. Ohta, “Maxwell Riron no Kiso,” Fundamentals of Maxwell’s Theory: Electrodynamics via Relativity (University of Tokyo Press, 2002), pp. 3358 [in Japanese].
S. Sunagawa, Riron Dejikigaku, 3rd ed. (Kinokuniya Shoten, 1999), pp. 2425 [in Japanese].
A. Fert and I. A. Campbell, Phys. Rev. Lett. 21, 1190 (1968).

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The relativistic effect on electromagnetic forces yields two types of forces which depend on the velocity of the relevant particles: (i) the usual Lorentz force exerted on a moving charged particle and (ii) the apparent Lorentz force exerted on a moving magnetic moment. In sharp contrast with type (i), the type (ii) force originates due to the transverse field induced by the Hall effect (HE). This study incorporates both forces into a Drude-type equation with a fully spin-polarized condition to investigate the effects of self-consistency of the source and the resultant fields on the HE. We also examine the self-consistency of the carrier kinematics and electromagnetic dynamics by simultaneously considering the Drude type equation and Maxwell equations at low frequencies. Thus, our approach can predict both the dc and ac characteristics of the HE, demonstrating that the dc current condition solely yields the ordinary HE, while the ac current condition yields generation of both fundamental and second harmonic modes of the HE field. When the magnetostatic field is absent, the simultaneous presence of dc and ac longitudinal currents generates the ac HE that has both fundamental frequency and second harmonic.


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