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Giant isotope effect and spin state transition induced by oxygen isotope exchange in (Pr1xSmx)0.7Ca0.3CoO3

G. Y. Wang, X. H. Chen, T. Wu, G. Wu, X. G. Luo, and C. H. Wang
Phys. Rev. B 74, 165113 – Published 20 October 2006

Abstract

We systematically investigate the effect of the oxygen isotope in (Pr1xSmx)0.7Ca0.3CoO3 which shows a crossover with x from ferromagnetic metal to the insulator with spin-state transition. A striking feature is that effect of oxygen isotope on the ferromagnetic transition is negligible in the metallic phase, while replacing O16 with O18 leads to a giant up shift of the spin-state transition temperature (Ts) in the insulating phase, especially Ts shifts from 36 to 54K with isotope component αS=4.7 for the sample with x=0.175. A metal-insulator transition is induced by oxygen isotope exchange in the sample x=0.172 being close to the insulating phase. The contrasting behaviors observed in the two phases can be well explained by occurrence of static Jahn-Teller distortions in the insulating phase, while the absence of them in the metallic phase.

    • Received 6 July 2006

    DOI:https://doi.org/10.1103/PhysRevB.74.165113

    ©2006 American Physical Society

    Authors & Affiliations

    G. Y. Wang, X. H. Chen*, T. Wu, G. Wu, X. G. Luo, and C. H. Wang

    • Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People’s Republic of China

    • *Electronic address: chenxh@ustc.edu.cn

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    Issue

    Vol. 74, Iss. 16 — 15 October 2006

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    Images

    • Figure 1
      The XRD patterns for the samples (Pr1xSmx)0.7Ca0.3CoO3 with x=0.05, 0.175, and 0.30 treated in O216 and O218, respectively.Reuse & Permissions
    • Figure 2
      (Color online) Temperature dependence of resistivity for the O16 and O18 samples (Pr1xSmx)0.7Ca0.3CoO3 with x=0.175, 0.20, 0.25, and 0.30. The data denoted by the solid and open symbols are taken from the samples treated in O216 and O218, respectively.Reuse & Permissions
    • Figure 3
      (Color online) Temperature dependence of susceptibility for the O16 and O18 samples (Pr1xSmx)0.7Ca0.3CoO3 with x=0.175, 0.20, 0.25, and 0.30. The data denoted by the solid and open symbols are taken from the samples treated in O216 and O218, respectively.Reuse & Permissions
    • Figure 4
      (Color online) Temperature dependences of resistivity and susceptibility for the sample (Pr1xSmx)0.7Ca0.3CoO3 with x=0.172 (solid squares for the O16 sample; solid circles for O18 sample). The data denoted by the open symbols were obtained after the oxygen isotope back-exchange (O16O18 and O18O16). The reversibility of the metal-insulator transition induced by oxygen isotope exchange is clear.Reuse & Permissions
    • Figure 5
      (Color online) Temperature dependence of susceptibility for the O16 and O18 samples (Pr1xSmx)0.7Ca0.3CoO3 with x=0.05, 0.10, 0.15, and 0.17: solid lines for O16 samples; dot lines for O18 samples.Reuse & Permissions
    • Figure 6
      The oxygen isotope exponent αc and αs as a function of Sm content x and the average ionic radius rA of the A site (Pr1xSmx)0.7Ca0.3 in (Pr1xSmx)0.7Ca0.3CoO3 system.Reuse & Permissions
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