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Successive phase transitions and phase diagrams for the quasi-two-dimensional easy-axis triangular antiferromagnet Rb4Mn(MoO4)3
Using magnetic, thermal and neutron measurements we show that Rb4Mn(MoO4)3 is a quasi-2D triangular Heisenberg antiferromagnet with easy-axis anisotropy and successive transitions bracketing anExpand
Synthesis, structure and physical properties of LnNi(Sn,Sb)3 (Ln=Pr, Nd, Sm, Gd, Tb)
Abstract Five new analogues of the β- CeNiSb 3 family have been synthesized and found to be Ln Ni(Sn,Sb) 3 and isostructural to the previously reported β -CeNiSb 3 . Ln Ni(Sn,Sb) 3 ( Ln =Pr, Nd, Sm,Expand
Discovery of beta-LnNiSb3 (Ln = La, Ce): crystal growth, structure, and magnetic and transport behavior.
A new polymorph of CeNiSb3 has been grown from a Sn flux and characterized by single-crystal X-ray diffraction. beta-CeNiSb3 crystallizes in the orthorhombic space group Pbcm (No. 57) with Z = 8. TheExpand
Low-dimensional structure and magnetism of the quantum antiferromagnet Rb4Cu(MoO4)3 and the structure of Rb4Zn(MoO4)3.
Single crystals of the quantum low-dimensional antiferromagnet Rb(4)Cu(MoO(4))(3) and the nonmagnetic analogue Ru(4)Zn(MoO(4))(3) have been synthesized by a flux-growth method. Detailed structuralExpand
Magnetization and transport properties of α-CeNi0.78Co0.22Sb3
Abstract Single crystals of α-CeNi x Co 1− x Sb 3 ( x ∼0.8) were synthesized and crystallize in the orthorhombic space group Pbcm with unit cell parameters of a =12.6480(2) A, b =6.2060(4) A, and cExpand
The layered intermetallic compound LaPdSb3
The title compound, lanthanum palladium trianti­mony, adopts a new structure type and is an inter­mediate between the CeCrSb3 and CeNiSb 3 structure types. Expand
Investigation of the effect of Ni substitution on the physical properties of Ce(Cu(1-x)Ni(x))(y)Sb(2).
Single crystals of Ce(Cu(1-x)Ni(x))(y)Sb(2) (x = 0, 0.25, 0.37, 0.46; y∼0.7) were synthesized using a flux growth method and crystallize in the tetragonal P4/nmm space group with lattice parametersExpand
Successive phase transitions and phase diagrams of $S$ = 5/2 quasi-two dimensional triangular antiferromagnet Rb$_{4}$Mn(MoO$_{4})_{3}$
Submitted for the MAR10 Meeting of The American Physical Society Successive phase transitions and phase diagrams of S = 5/2 quasi-two dimensional triangular antiferromagnet Rb4Mn(MoO4)3 RIEKO ISHII,Expand
Magnetotransport properties and the Fermi surface of single crystal VB2
We report the results of magnetotransport and de Haas–van Alphen (dHvA) measurements on high quality single crystals of VB2 grown from a molten aluminum flux. In addition, we compare these results toExpand