Low temperature properties of some RIn3 compounds

Hale, Lucas Michael; Gschneidner, K. A.; Pecharsky, V. K.; Mudryk, Yaroslav

doi:10.1016/j.jallcom.2008.04.097

Cited by 9 publications

(5 citation statements)

References 20 publications

(26 reference statements)

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“…CeIn 3 has the AuCu 3 structure, which has inspired new studies of the AuCu 3 family of materials. Normal state properties have been measured in YIn 3 via de Haas-van Alphen experiments [6], thermal conductivity [7], and heat capacity [8], leaving it well characterized and a promising candidate for further exploration of the interplay between crystal structure and magnetic superconductivity.…”

Section: Introductionmentioning

confidence: 99%

Superconductivity in single-crystal

Johnson

Young

Zieve

et al. 2012

Solid State Communications

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We measure the superconducting transition of YIn3 by resistivity, susceptibility, and specific heat. Despite using high-quality single-crystal samples, the transitions detected by the three techniques are shifted from each other in temperature, suggesting a region of filamentary superconductivity. We discuss the possible implications for filamentary superconductivity in unconventional superconductors.

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Section: Introductionmentioning

confidence: 99%

Superconductivity in single-crystal

Johnson

Young

Zieve

et al. 2012

Solid State Communications

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“…[25][26][27] REIn 3 shows remarkable features, such as heavy fermion, antiferromagnetism, superconductivity at critical temperature or pressure, crystal field effects, Kondo effect, and multiaxial magnetic structures. [25,[27][28][29][30][31][32][33][34] CeIn 3 belongs to a heavy fermion and shows unique magnetic and electric properties such as antiferromagnetic order at 10 K, superconductivity under applied high pressure, and Kondo effect. [35] GdIn 3 orders antiferromagnetically at 45 K, which is the highest Néel temperature among the REIn 3 intermetallic compounds.…”

Section: Introductionmentioning

confidence: 99%

A review on 3d transition metal dilute magnetic REIn₃ intermetallic compounds

Guo¹,

Guo²,

Yin³

et al. 2022

Chinese Phys. B

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The dilute magnetic intermetallic compound (DMIC) is an extended study of the dilute magnetic semiconductor. The giant magnetic effect and room temperature ferromagnetism are induced by doping minor 3d transition metal into REIn3 intermetallic compound. Owing to the metallic processability, the REIn3-based DMIC might have the potential application as magnetoelectric device. In this review, the structural stability, magnetic and electric transport properties of REIn3 – x Tx (RE = rare earth; T = Co, Mn, Fe; x = 0–0.3) have been systematically summarized and analyzed.

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“…RIn 3 (R = rare earth) intermetallic compound has received much attention due to its interesting magnetic properties such as various magnetic structures, crystal field effect, and heavy fermion behavior . It is known that RIn 3 crystallizes in a cubic AuCu 3 type structure with a space group of Pm

\overset{3}{true}

m .…”

Section: Introductionmentioning

confidence: 99%

Structure and Magnetic Properties of RIn_2.9Co_0.1 (R = La, Ce, Pr, Nd, Gd, Tb, Dy, Ho, Er, Tm, Lu)

Tan

Guo

2019

Crystal Research and Technology

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RIn 2.9 Co 0.1 (R = rare earth) intermetallic compound has been synthesized, and its structure and magnetic properties have been investigated using X-ray diffraction, scanning electron microscopy with energy dispersive spectrum and magnetic measurement. RIn 2.9 Co 0.1 crystallizes in cubic AuCu 3 -type structure for R = heavy rare earths, and a small amount of R(In, Co) 2 metaphase separates from RIn 2.9 Co 0.1 for R = light rare earth. Rietveld's structural refinement confirms that R(In, Co) 2 metaphase is the isomorphism of hexagonal CaIn 2 . The lattice parameters of RIn 2.9 Co 0.1 tend to decrease with increasing atomic number of R due to the shrinking effect of atomic radius in rare earth group. The cubic phase can be stabilized in the range of 1.048-1.133 for the effective atomic radius ratio R A and 0.35-0.41 for the electronegativity difference X. The magnetizing process of RIn 2.9 Co 0.1 shows various characteristics with increasing atomic number of rare earth, and the magnetizing curves follow a ferromagnetic model for R = La, a mixed ferromagnetic and paramagnetic model for R = Ce, Pr, Nd, Gd, Tb, Dy. The formation of ferromagnetic characteristics results from the strong spin-spin interaction between R and Co.

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Low temperature properties of some RIn3 compounds

Cited by 9 publications

References 20 publications

Superconductivity in single-crystal

Superconductivity in single-crystal

A review on 3d transition metal dilute magnetic REIn₃ intermetallic compounds

Structure and Magnetic Properties of RIn_2.9Co_0.1 (R = La, Ce, Pr, Nd, Gd, Tb, Dy, Ho, Er, Tm, Lu)

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Low temperature properties of some RIn3 compounds

Cited by 9 publications

References 20 publications

Superconductivity in single-crystal

Superconductivity in single-crystal

A review on 3d transition metal dilute magnetic REIn3 intermetallic compounds

Structure and Magnetic Properties of RIn2.9Co0.1 (R = La, Ce, Pr, Nd, Gd, Tb, Dy, Ho, Er, Tm, Lu)

Contact Info

Product

Resources

About

A review on 3d transition metal dilute magnetic REIn₃ intermetallic compounds

Structure and Magnetic Properties of RIn_2.9Co_0.1 (R = La, Ce, Pr, Nd, Gd, Tb, Dy, Ho, Er, Tm, Lu)