Field induced spin freezing and low temperature heat capacity of disordered pyrochlore oxide Ho$_{2}$Zr$_{2}$O$_{7}$

Sheetal; A. Elghandour; R. Klingeler; C. S. Yadav

doi:10.1088/1361-648X/ac5fd8

paper

Field induced spin freezing and low temperature heat capacity of disordered pyrochlore oxide Ho $_{2}$ Zr $_{2}$ O $_{7}$

arXiv:2110.04555 · doi:10.1088/1361-648X/ac5fd8

Abstract

Spin ice materials are the model systems that have a zero-point entropy as \textit{T} $\to$ 0 K, owing to the frozen disordered states. Here, we chemically alter the well-known spin ice Ho $_{2}$ Ti $_{2}$ O $_{7}$ by replacing Ti sites with isovalent but larger Zr ion. Unlike the Ho $_{2}$ Ti $_{2}$ O $_{7}$ which is a pyrochlore material, Ho $_{2}$ Zr $_{2}$ O $_{7}$ crystallizes in disordered pyrochlore structure. We have performed detailed structural, ac magnetic susceptibility and heat capacity studies on Ho $_{2}$ Zr $_{2}$ O $_{7}$ to investigate the interplay of structural disorder and frustrated interactions. The zero-field ground state exhibits large magnetic susceptibility and remains dynamic down to 30 mK without showing Pauling's residual entropy. The dynamic state is suppressed continuously with the magnetic field and freezing transition evolves ( $\sim$ 10 K) at a field of $\sim$ 10 kOe. These results suggest that the alteration of chemical order and local strain in Ho $_{2}$ Ti $_{2}$ O $_{7}$ prevents the development of spin ice state and provides a new material to study the geometrical frustration based on the structure.

7 pages, 6 figures

Field induced spin freezing and low temperature heat capacity of disordered pyrochlore oxide Ho $_{2}$ Zr $_{2}$ O $_{7}$

Abstract

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Cited by in corpus (2)

Field induced spin freezing and low temperature heat capacity of disordered pyrochlore oxide Ho2​Zr2​O7​

Abstract

References in corpus (7)

Cited by in corpus (2)

Field induced spin freezing and low temperature heat capacity of disordered pyrochlore oxide Ho $_{2}$ Zr $_{2}$ O $_{7}$