13569-80-7Relevant articles and documents
Optically active uniform potassium and lithium rare earth fluoride nanocrystals derived from metal trifluroacetate precursors
Du, Ya-Ping,Zhang, Ya-Wen,Sun, Ling-Dong,Yan, Chun-Hua
, p. 8574 - 8581 (2009)
This paper reports the first systematical synthesis of near-monodisperse potassium and lithium rare earth (RE) fluoride (K(Li)REF4) nanocrystals with diverse shapes (cubic KLaF4 and KCeF4 wormlike nanowires, nanocubes and
Greis, O.,Cader, M. S. R.
, p. 145 - 150 (1985)
Russo, R. C.,Haendler, H. M.
, p. 763 - 770 (1974)
The sodium fluoride-lanthanide trifluoride systems
Thoma,Insley,Hebert
, p. 1222 - 1229 (1966)
Phase diagrams are reported for the NaF-LnF3 binary systems. Hexagonal phases of the formula NaF·LnF3 are formed in all NaF-LnF3 systems. Above 700° the hexagonal phases NaF·PrF3 to NaF·LuF3 become converted to disordered fluorite-like cubic phases of variable composition. The composition limits of the cubic phase region are extended in proportion to the difference in ion size between Na+ and Ln3+ and vary in breadth ranging from 9 mole % (NaF-PrF3) to 25 mole % (NaF-LuF3). In each case, the LnF3-rich phase boundary was found empirically to be 5NaF·OLnF3 as the interstitial positions for allions become filled. Values of the fluorite unit-cell constants were calculated from ionic radii and found to be in good agreement with measured values. Unit-cube dimensions, a0, range from a maximum value of 5.720 A for the LnF3-rich phase in the system NaF-PrF3 to 5.425 A for the NaF-rich phase in the system NaF-LuF3. Lattice constants for the hexagonal phases NaF·LaF3 to NaF·LuF3 vary for a0 from 6.157 to 5.907 A and for C0 from 3.822 to 3.523 A. At high temperatures the 5NaF·9LnF3 phase displays disordering characteristic of the fluorite-like solid solutions; at lower temperatures cationic ordering takes place in the 5NaF·OLnF3 phases where Ln = Dy to Lu, transforming the cubic phase to an orthorhombic phase. Hexagonal NaF·LnF3 and orthorhombic 5NaF·OLnF3 compounds are partially miscible in the solid state. In the series Dy to Lu, the hexagonal phase is increasingly soluble in 5NaF·OLnF3, stabilizing the 5:9 phase to the extent that the lutetium compound is stable at temperatures below 300°, the lower temperature limit of this study. Optical properties and refractive indices of the intermediate crystalline phases in the NaF-LnF3 systems were determined as part of this investigation. Minimum liquidus temperatures in the NaF-LnF3 systems are associated with an NaF-NaF·LnF3 eutectic which varies in composition only from 25 to 29 mole % LnF3 and in temperature from 733 to 595°.
Banks, C. V.,Bruke, K. E.,O'Laughlin, J. W.
, p. 239 - 243 (1958)
Thermochemical studies on the lanthanoid complexes of trifluoroacetic acid
Yoshimura,Ohara
, p. 573 - 576 (2006)
The thermal decomposition of the lanthanoid complexes of trifluoroacetic acid (Ln(CF3COO)3·3H2O; Ln = La-Lu) was studied by TG and DTA methods. The Ln(CF3COO) 3·3H2O complexes decompose in several stages; first dehydrate to the anhydrous state, then followed by decomposition of the anhydrous salt to a stable product of LnF3. From the endothermic and exothermic data of Ln(CF3COO)3·3H2O complexes, pyrolysis behavior of the complexes is classified into three groups: (1) La-Pr salts; (2) Nd-Gd salts; (3) Tb-Lu salts. It has been shown that all the final decomposition products were found to result in the formation of LnF3.
X-ray magnetic circular dichroism (XMCD) study of a methoxide-bridged DyIII-CrIII cluster obtained by fluoride abstraction from cis-[CrIIIF2(phen)2]+
Dreiser, Jan,Pedersen, Kasper S.,Birk, Torben,Schau-Magnussen, Magnus,Piamonteze, Cinthia,Rusponi, Stefano,Weyhermueller, Thomas,Brune, Harald,Nolting, Frithjof,Bendix, Jesper
, p. 7842 - 7847 (2012)
An isostructural series of dinuclear chromium(III)-lanthanide(III) clusters is formed by fluoride abstraction of cis-[CrF2(phen) 2]+ by Ln3+ resulting in LnF3 and methoxide-bridged Cr-Ln clusters (Ln = Nd (1), Tb (2), Dy (3)) of formula [CrIII(phen)2(μ-MeO)2Ln(NO3) 4]?xMeOH (x = 2-2.73). In contrast to fluoride, methoxide bridges in a nonlinear fashion, which facilitates chelation. For 3, X-ray magnetic circular dichroism (XMCD) provides element-specific magnetization curves that are compared to cluster magnetization and susceptibility data acquired by SQUID magnetometry. The combination of XMCD and SQUID is able to resolve very small magnetic coupling values and reveals a weak Cr III-DyIII coupling of j = -0.04(3) cm-1. The DyIII ion has a ground-state Kramers doublet of mJ = ±13/2, and the first excited doublet is found to be mJ = ±11/2 at an energy of δ = 57(21) cm-1. The Cr III ion exhibits a uniaxial anisotropy of DCr = -1.7(1.0) cm-1. Further, we observe that a weak anisotropic coupling of dipolar origin is sufficient to model the data, suggesting that methoxide bridges do not play a significant role in the magnetic coupling for the present systems.
Wartenberg, H. v.
, p. 771 - 771 (1941)