Magnetic Field Dependence of the Dielectric Behavior of Bound Polarons in Rutile (Ti<span class="aps-inline-formula"><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mrow><msub><mrow><mi mathvariant="normal">O</mi></mrow><mrow><mn>2</mn></mrow></msub></mrow></math></span>)

H. S. Matis; R. K. MacCrone

doi:10.1103/PhysRevLett.25.1715

Magnetic Field Dependence of the Dielectric Behavior of Bound Polarons in Rutile (Ti $O_{2}$ )

H. S. Matis^*

R. K. MacCrone

Department of Physics and Astronomy, Rensselaer Polytechnic Institute, Troy, New York 12181

Division of Materials Engineering, Rensselaer Polytechnic Institute, Troy, New York 12181

^*Present address: Department of Physics, The University of Chicago, Chicago, Ill. 60637.

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Phys. Rev. Lett. 25, 1715 – Published 21 December, 1970

DOI: https://doi.org/10.1103/PhysRevLett.25.1715

Abstract

The electric susceptibility of a two-center bound polaron is discussed as a function of applied magnetic field. Periodic maxima observed in the dielectric constant in rutile are shown to result from zero-field ( $H = 0$ ) splitting induced by impurity ions.

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Physical Review Letters

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Magnetic Field Dependence of the Dielectric Behavior of Bound Polarons in Rutile (Ti $O_{2}$ )

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Magnetic Field Dependence of the Dielectric Behavior of Bound Polarons in Rutile (TiO2)

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Magnetic Field Dependence of the Dielectric Behavior of Bound Polarons in Rutile (Ti $O_{2}$ )