Yttrium /Holmium Ratio and Lanthanide Observed in Pre-Cenozoic Limestones

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Yttrium /Holmium Ratio and Lanthanide Observed in Pre-Cenozoic Limestones Geochemical Journal, Vol. 25, pp. 31 to 44, 1991 Non-chondritic yttrium /holmium ratio and lanthanide tetrad effect observed in pre-Cenozoic limestones IWAO KAWABE, YOKO KITAHARA and KOH NAITO Department of Earth Sciences, Faculty of Science, Ehime University, Bunkyo-cho 2-5, Matsuyama 790, Japan (Received July 27, 1990; Accepted March 26, 1991) REE and Y in limestones have been determined by ICP-AES method coupled with pre-concentra tion chemical procedures. The lanthanide tetrad effect has been clearly observed in the REE patterns of two Permian limestones. It is the W-type tetrad effect seen in seawaters. Y/Ho ratios for the limestones show large positive deviations from the chondritic ratio. Similar non-chondritic Y / Ho ratios are seen in a Precambrian limestone from South Africa, seawaters, and marine phosphorites. Their REE patterns are well characterized by the W-type tetrad effect. These facts and recent results of aquatic geochemistry of REE and Y strongly suggest that the positive Y anomalies are intimately associated with the W-type tetrad effect of REE in natural aquatic solutions including seawaters and in some hydrogenous deposits from the solutions. Y is not a pseudo lanthanide that behaves like Ho in natural conditions where the lanthanide tetrad effect is operative. This must be a thermochemical effect related to the absence of 4f electron in Y3+ and the systematic differences in 4f electronic configurations in the REE3+ series. The REE plus Y patterns with positive Y anomalies and the W-type tetrad effect are important for the gochemical studies of limestones and other hydrogeneous deposits. and related materials. The other one called the INTRODUCTION M-type is observed in solid materials that are Masuda and Ikeuchi (1979) first probably having remained after leaching by demonstrated that the lanthanide tetrad effect in aqueous media. They emphasized the com nature is recognized in peculiar REE abundance plementary relationship between the W and M patterns for seawaters and a marine phosphate tetrad effects. nodule. Subsequently, Masuda and his The tetrad effect itself was proposed original coworkers further found that such tetrad effects ly by Peppard et al. (1969 and 1970) on the basis are detectable in other natural substance in of their studies on solvent extraction of trivalent cluding limestones, valves of living shellfish, lanthanides and actinides. According to their fresh groundwaters, siliceous ores, leucogranites works, when the logarithmic distribution and so on (Kamioka and Masuda, 1986; Masuda coefficients for trivalent REE between organic et al., 1987; Masuda and Akagi, 1989). On the and aqueous phases are plotted against the other hand, detailed studies on REE distribution atomic number of the lanthanide, the plot ap in Pacific and Atlantic ocean water columns pears to consist of four distinct smooth curves. made by De Baar et al. (1983 and 1985a, b) pro The fifteen REE are grouped by the curves into vide further evidence for the lanthanide tetrad four tetrads with Gd being common to the sec effect in seawaters. Recently, Masuda et al. ond and third tetrads. The extended smooth (1987) proposed to distinguish two types of curves for the first and second tetrads and those tetrad effects in nature: The first one called the for the third and fourth tetrads intersect respec W-type by them is observed in natural waters tively between Nd and Pm and between Ho and 31 32 I. Kawabe et al. Er. In a similar plot for trivalent actinides, they plasma-atomic emission spectrometry (ICP showed that an analogous tetrad effect is ap AES) after the group separation of these parent with Cm being common to the second elements from matrix major elements. The and third tetrads. They wrote that, if the geochemical importance of intimate association lanthanide tetrad effect should be valid, the of non-chondritic Y/Ho ratios with the W-type "half -filled" shell effect would be joined by the lanthanide tetrad effect in limestones and "one -quater-filled" shell effect and "three seawaters is discussed. quaters-filled" shell effect because of the discon tinuities occurring respectively between the third and fourth and between the tenth and eleventh SAMPLES 4f electron additions. Two limestones (EL-1 and EL-2) were sam In response to the proposal of tetrad effect, pled from the Lower to Middle Permian lime Jorgensen (1970) and Nugent (1970) put forward stone body in Ohnogahara, Nonura-cho, Ehime quantum mechanical interpretations for the Prefecture. The limestone body occurs together tetrad effects in terms of the interelectron repul with greenstones, cherts, and clastic rocks. They sion energy of the q electrons in each 4f" or 5f' are collectively designated the Ohnogahara electronic configuration for trivalent lanthanides Group and one of the key pre-Cenozoic and actinides. geological units that constitute the Northern If the lanthanide tetrad effect is related to the Chichibu Belt in the western part of Shikoku ground state electronic configurations in which Island, Japan. The other is a calcareous gneiss the 4f sub-shell is successively filled by an addi sampled in Nishisetodani area along Ohnagatani tional electron, the relationship between Ho and River, Yatsuo-cho, Nei-gun, Toyama Prefec Y is important because the trivalent ionic radii ture. This is a typical sample of the most for Ho and Y are almost the same despite no 4f calcareous member of the calc-silicate gneiss of electron in Y. In this respect, Peppard et al. the Hida metamorphic rocks. The calc-silicate (1969) themselves noted that Y does not always gneiss is characterized as alternations of marbles behave as a pseudo lanthanide in solvent extract and quartzites. This sample was taken from a ions for REE. The distribution coefficient for Y marble-rich portion. It consists of calcite in a solvent extraction system involving H[DOP] mainly, and accessory amounts of quartz , (benzene) and HC1(aqueous) is comparable with clinopyroxene, and tremolite are present. This that for Ho or Er. However, in the other extrac sample differs petrographically from the two tion system utilizing DEH[CIMP] (benzene) and samples of the Ohnogahara limestone in having LiBr plus HBr (aqueous), such a coefficient for Y silicate impurities in it. differs greatly from any values of the coefficients for all the REE. In this context, it is interesting and important EXPERIMENTAL to study the lanthanide tetrad effect and the frac The aliquots of each powdered sample tionation between Y and Ho or other heavy REE weighing 10-30g have been used for repeated together even in natural substance. However, analyses of three to six times, because the REE almost all previous analytical results relevant to and Y contents were expected to be as low as the tetrad effects in natural samples include chondrite levels. Two methods for sample neither Y data nor the information as to Y/Ho decomposition were used in order to ensure the fractionations, because the mass spectrometric presence or absence of non-carbonate impurities isotope dilution method (MSID) has been used that may have those elements and resist the principally. In this paper, we report REE and Y chemical dissolution by mineral acids or by HF determinations for some Japanese pre-Cenozoic plus mineral acids. The first method is the limestones using the inductively coupled Ar dissolution by HC1 alone. The solution is filtered Y/Ho ratio and lanthanide tetrad effect in limestones 33 to remove insoluble materials if present. Only rections for spectral interferences among the the filtrate is used in subsequent procedures for measured elements were made in calculating the the group separation of REE and Y. The other final results of the concentrations of REE and Y method includes additional decomposition pro in samples. The linear correction factors for spec cedures to make all the constituent materials tral interferences among REE, Y and Ca have soluble as completly as possible. The filtered in been re-determined for this study, and the soluble materials after dissolution by HC1 are previous set by Kawabe et al. (1988) was slightly ignited in a Pt-crucible, and then dissolved by revised. The blank tests for all the chemical pro HF + HNO3 + HC1O4 twice. It is filtered again, cedures indicate that the blank correction is un and this filtrate is combined with the first filtrate necessary. after dissolution by HCI. The filterd insolubles, As a result of REE and Y analyses in stan after being ignited in a Pt-crucible again, are fur dard rocks and clastic rocks enriched in heavy ther fused with 300 mg of (2:1) mixture of minerals, we confirmed that the residues after Na2CO3 and H3BO3. If necessary, this fusion is the dissolution by HF-mineral acids can be com repeated twice. The fusion product is then pletely dissolved by the fusion procedure using dissolved in HCl and added to the combined solu Na2CO3 and H3BO3 (Kawabe et al., in prepara tion of the first and second filtrates. This is the tion). So that we believe that all materials in each sample solution obtained by the second decom sample are satisfactorily decomposed into the position method. solution by the second method. By using the sam Both of the sample solutions by the two diges ple solution spiked with the standard solution tion methods are used in the same procedures for having 1001cg of La, Eu, Lu and Y each, the group separation of REE and Y, in which co recovery in the group separation was checked. precipitation with Fe(OH)3 is followed by the ca The recovery of more than 99 % was found for tion-exchange purification. The co-precipitation each spiked element. The alkali earth elements is made at pH = 6.5 by adding 20 mg Fe 3+ and and trivalent major elements are negligible in the ammonia water.
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