Low‐Temperature Studies on Spin‐Ice Behavior in Frustrated Pyrochlore‐Dy <sub>2</sub> Ti <sub>2</sub> O <sub>7</sub>

Dy 2 Ti 2 O 7 is a well‐known member of the pyrochlore family, having an exotic ground state like spin ice, as the weakly interacting Ising spins of each tetrahedron follow the two‐in, two‐out ice rule. A low‐temperature study to understand this novel ground state is carried out using heat capacity and magnetization with no noticeable magnetic ordering. Heat capacity shows a broad anomaly around 1 K, indicative of short‐range interactions. Residual entropy of the spin‐ice state in zero magnetic field is 1.36 JK −1 mol −1 which is close to the Pauling prediction. Kagome‐ice state is to be formed when a magnetic field is applied, and residual entropy is 0.56 JK −1 mol −1 between 0.3 Tand 0.6 T, which matches the literature. A magnetic field–temperature (H–T) phase diagram has been visualized for the spin‐ice configuration. Observation of small yet clear peak structures around 0.2 K may be assigned to the first‐order (gas–liquid) transition below 0.4 K inside the Kagome‐ice state.

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Publication Details

Journal
physica status solidi (b)
Published
2025-12-18
DOI
https://doi.org/10.1002/pssb.202500314
Primary Topic
Advanced Condensed Matter Physics
Type
article
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article

Low‐Temperature Studies on Spin‐Ice Behavior in Frustrated Pyrochlore‐Dy 2 Ti 2 O 7

Uday Deshpande, ShikharG Vyas, R. Rawat, V. Ganesan et al.
physica status solidi (b)
Advanced Condensed Matter Physics
article

Low‐Temperature Studies on Spin‐Ice Behavior in Frustrated Pyrochlore‐Dy 2 Ti 2 O 7

Uday Deshpande, ShikharG Vyas, R. Rawat, V. Ganesan, R. Venkatesh, Manju Mishra Patidar, L. S. Sharath Chandra, Ashok Kumar, Satyendra Singh, P. Saravanan
article en

Abstract

Dy 2 Ti 2 O 7 is a well‐known member of the pyrochlore family, having an exotic ground state like spin ice, as the weakly interacting Ising spins of each tetrahedron follow the two‐in, two‐out ice rule. A low‐temperature study to understand this novel ground state is carried out using heat capacity and magnetization with no noticeable magnetic ordering. Heat capacity shows a broad anomaly around 1 K, indicative of short‐range interactions. Residual entropy of the spin‐ice state in zero magnetic field is 1.36 JK −1 mol −1 which is close to the Pauling prediction. Kagome‐ice state is to be formed when a magnetic field is applied, and residual entropy is 0.56 JK −1 mol −1 between 0.3 Tand 0.6 T, which matches the literature. A magnetic field–temperature (H–T) phase diagram has been visualized for the spin‐ice configuration. Observation of small yet clear peak structures around 0.2 K may be assigned to the first‐order (gas–liquid) transition below 0.4 K inside the Kagome‐ice state.

physica status solidi (b)Vol. 263(3)
Homi Bhabha National Institute (IN), High Magnetic Field Laboratory (CN), Medi-Caps University (IN), UGC DAE Consortium for Scientific Research (IN), AML Superconductivity and Magnetics (United States) (US), International House (PT)
Openalex Percentile: Top 73%
Advanced Condensed Matter Physics
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