2011
DOI: 10.1103/physrevb.84.104105
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Crystallographic superstructure inR2PdSi3compounds (R=heavyrare earth)

Abstract: The R 2 PdSi 3 intermetallic compounds have been reported to crystallize in a hexagonal AlB 2 -derived structure, with the rare earth atoms on the Al sites and Pd and Si atoms randomly distributed on the B sites. However, the intricate magnetic properties observed in the series of compounds have always suggested complications to the assumed structure. To clarify the situation, x-ray and neutron diffraction measurements were performed on the heavy rare earth compounds with R = Gd, Tb, Dy, Ho, Er, Tm, which reve… Show more

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Cited by 54 publications
(54 citation statements)
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“…We used it to systematically derive Lagrangians for bipartite QDMs in 2D and 3D from the corresponding microscopic Hamiltonians. We find good agreement with known results in the literature; namely, calculations up to quadratic order yield a stiffness for the square lattice QDM at the RK point equal to 1/4 compared to the exact result π/18 [5,12]; and they yield a speed of light in the gapless phase of the diamond lattice QDM c = √ J(J − V)/6 S 2 compared to the numerical result c(S = 1) √ 0.8J(J − V) [13,14].…”
Section: Discussionsupporting
confidence: 88%
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“…We used it to systematically derive Lagrangians for bipartite QDMs in 2D and 3D from the corresponding microscopic Hamiltonians. We find good agreement with known results in the literature; namely, calculations up to quadratic order yield a stiffness for the square lattice QDM at the RK point equal to 1/4 compared to the exact result π/18 [5,12]; and they yield a speed of light in the gapless phase of the diamond lattice QDM c = √ J(J − V)/6 S 2 compared to the numerical result c(S = 1) √ 0.8J(J − V) [13,14].…”
Section: Discussionsupporting
confidence: 88%
“…We compare our results against the existing literature, where we find good agreement considering the large-S and quadratic approximations that we employ. For example, we derive the stiffness of the 2D square lattice QDM at a well-known critical point called the Rokhsar-Kivelson (RK) point [2], where the ground-state wave function of the system is known exactly: Our result, 1/4, is comparable to arXiv:1904.12868v2 [cond-mat.str-el] 5 Aug 2019 the exact value, π/18 [5,12]. We use instanton considerations to discuss the fate of 2D phases at finite temperature.…”
Section: Introductionmentioning
confidence: 87%
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“…SAED was indexed using the lattice parameters of hexagonal crystal structure (lattice parameters, a  = 4.032 Å and c  = 4.247 Å). Though some of the earlier reports yield superstructure formation in single crystalline R 2 TSi 3 type of materials 19 , no evidence of any such superstructure formation could be traced from the electron diffraction pattern in the defect structure compound Pr 2 Ni 0.95 Si 2.95 [Fig. 3(b)].…”
Section: Resultsmentioning
confidence: 96%
“…Just as in the 1-2-2 families, wide-ranging anomalies and phenomena have been reported (even in Gd-based systems), including competition between the Kondo effect and magnetic ordering, re-entrant spin-glass phases, geometrically frustrated and low-dimensional magnetism, non-Fermi liquid behavior, giant magnetoresistance, and an anisotropic magnetocaloric effect . One reason for the rich range of properties is that there are several structural variations with this composition, depending on the nature of T and X ions, including hexagonal (space groups P 6/mmm, P62c, P 6 3 /mmc) and orthorhombic (F mmm) materials 31,[34][35][36][37][38] . In particular, a number of these consist of honeycomb layers of T and X separated by triangularly arranged R ions 12,35 , which can give rise to frustration in the presence of nearest neighbor antiferromagnetic interactions.…”
Section: Introductionmentioning
confidence: 99%