1998Journal of Physics Condensed MatterOpen access

The ratio of small polarons to free carriers in derived from susceptibility measurements

K. A. Müller, Guo‐meng Zhao, K. Conder, Hugo Keller

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Abstract

The normal-state spin susceptibility of was measured as a function of doping x . For , is well described by small-polaron theory. For , a temperature-independent Pauli component is present in as well. These results indicate the coexistence of small polarons and free carriers above the transition concentration . The concentration of the free carriers increases rapidly with , reaching a maximum for optimal doping ( x = 0.15). The large mass anisotropy of the polarons is obtained quantitatively from the -measurements.

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The normal-state spin susceptibility of was measured as a function of doping x . For , is well described by small-polaron theory. For , a temperature-independent Pauli component is present in as well. These results indicate the coexistence of small polarons and free carriers above the transition concentration . The concentration of the free carriers increases rapidly with , reaching a maximum for optimal doping ( x = 0.15). The large mass anisotropy of the polarons is obtained quantitatively from the -measurements.

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Available abstract

The normal-state spin susceptibility of was measured as a function of doping x . For , is well described by small-polaron theory. For , a temperature-independent Pauli component is present in as well. These results indicate the coexistence of small polarons and free carriers above the transition concentration . The concentration of the free carriers increases rapidly with , reaching a maximum for optimal doping ( x = 0.15). The large mass anisotropy of the polarons is obtained quantitatively from the -measurements.

Key concepts: Polaron, Pauli exclusion principle, Condensed matter physics, Doping, Free carrier, Anisotropy, Effective mass (spring–mass system), Spin (aerodynamics)

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