CLOSURE TEMPERATURES OF ACCESSORY MINERALS

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DR2005002 Flowers et al. CLOSURE TEMPERATURES OF ACCESSORY MINERALS The range of Pb diffusivity in accessory minerals provides the opportunity to reconstruct detailed thermal histories using the U-Pb isotopic system. Closure temperature (Tc) is a function of diffusivity, cooling rate, and effective diffusion radius (Dodson, 1973), and can be constrained by experimental and field-based empirical studies. The estimates below are ranges for typical diffusion radii (25-100 µm) and cooling rates (1-100 C/m.y.). Zircon and monazite with high Tc > 1000 C (Cherniak and Watson, 2001; Cherniak et al., 2004) are widely used to determine the timing of intrusive and metamorphic events. Titanite is increasingly recognized as a useful geochronometer because it is reactive mineral that readily grows during metamorphism (Frost et al., 2000; Aleinikoff et al., 2002), with closure temperature of 600-650 C constrained by both experimental and field-based studies (e.g. Cherniak; 1993; Verts et al., 1996). In contrast with these minerals that commonly grow below their closure temperatures, the U-Pb systematics of apatite and rutile are typically dominated by volume diffusion (e.g. Mezger 1989; Chamberlain and Bowring, 2000). Experimental and field studies of apatite provide consistent closure temperature constraints of 450-500 C (e.g. Cherniak et al. 1991; Krogstad and Walker, 1994; Chamberlain and Bowring, 2000). Field estimates for closure temperature in rutile are 400-450 C (Mezger, 1989), with somewhat higher experimental determinations (Cherniak, 2000). ANALYTICAL METHODS Mineral separation was carried out using standard crushing, water table, magnetic, and heavy-liquid techniques, with subsequent hand-picking of single and multigrain fractions. Titanite, apatite, and rutile grains were ultrasonically washed in high-purity water or ethanol and rinsed in acetone, followed by a second washing in high-purity water and rinsing with double-distilled acetone. Selected rutile fractions were abraded without pyrite and washed briefly with dilute HNO 3. Sample spiking with a mixture of 205 Pb- 233 U- 235 U was followed by dissolution in 29M HF (titanite, rutile) or 12M HCl (apatite), conversion to 6M HCl, and chemical separation of U and Pb using HBr-HCl anion-exchange chemistry. Pb and U analyses were carried out on the Massachusetts Institute of Technology VG Sector 54 mass spectrometer. Pb isotopic ratios were measured by peak jumping using an axial ion-counting Daly detector or dynamically with Faraday cups and the Daly detector. U was measured as an oxide in static mode on three Faraday cups. Details regarding isotopic ratio corrections are provided in Table DR1 1. The incorporation of significant common Pb of uncertain isotopic composition into apatite and rutile during crystallization, resulting in low ratios of radiogenic Pb to common Pb, is a particularly acute problem for U-Pb age determination in young, less radiogenic samples. Initial common Pb compositions of apatite and rutile were corrected by using the Pb isotopic composition of leached coexisting feldspar (Table DR2 1 ). Titanite data were corrected by using the isotopic composition of feldspars in a Western Fiordland Orthogneiss granulite (F03-61). Feldspar Pb isotopic determination was accomplished by handpicking 1 3 mg plagioclase fractions, sequentially leaching separates with 7M HNO 3, 6M HCl, and 1M HF, separating Pb using HBr anion-exchange

chemistry, and statically analyzing Pb in four Faraday cups. Ultimately, the 206 Pb/ 238 U dates calculated using the initial common Pb composition of coexisting leached feldspars differed little from those calculated using the standard method of correcting with the Stacey-Kramers (1975) model for terrestrial Pb evolution. The maximum effect was on an apatite fraction characterized by the lowest radiogenic Pb to common Pb ratio of the dataset (sample F03-1, analysis a1, Pb*/Pbc = 0.1). The date calculated using coexisting leached feldspars for the initial common Pb composition was 3.7 m.y. younger than the date calculated using the Stacey-Kramers model. In contrast, the effect on the rutile dates (sample F03-61) was 0.15 m.y. REFERENCES CITED Aleinikoff, J.N., Wintsch, R.P., Fanning, C.M., and Dorais, M.J., 2002, U-Pb geochronology of zircon and polygenetic titanite from the Glastonbury Complex, Connecticut, USA: an integrated SEM, EMPA, TIMS, and SHRIMP study: Chemical Geology, v. 188, p. 125-147. Chamberlain, K.R., and Bowring, S.A., 2000, Apatite-feldspar U-Pb thermochronometer: A reliable, mid-range (~450 C), diffusion-controlled system: Chemical Geology, v. 172, p. 73-200. Cherniak, D.J., 1993, Lead diffusion in titanite and preliminary results on the effects of radiation damage on Pb transport: Chemical Geology, v. 110, p. 177-194. Cherniak, D.J., 2000, Pb diffusion in rutile: Contributions to Mineralogy and Petrology, v. 139, p. 198-207. Cherniak, D.J., Lanford, W.A., and Ryerson, F.J., 1991, Lead diffusion in apatite and zircon using ion implantation and Rutherford Backscattering techniques: Geochimica et Cosmochimica Acta, v. 55, p. 1663-1673. Cherniak, D.J., and Watson, E.B., 2001, Pb diffusion in zircon: Chemical Geology, v. 172, p. 5-24. Cherniak, D.J., Watson, E.B., Grove, M., and Harrison, T.M., 2004, Pb diffusion in monazite: A combined RBS/SIMS study: Geochimica et Cosmochimica Acta, v. 68, p. 829-840. Dodson, M.H., 1973, Closure temperature in cooling geochronological and petrological systems: Contributions to Mineralogy and Petrology, v. 40, p. 259-274. Frost, B.R., Chamberlain, K.R., and Schumacher, J.C., 2000, Sphene (titanite): phase relations and role as a geochronometer: Chemical Geology, v. 172, p. 131-148. Hanson, G.N., Catanzaro, E.J., and Anderson, D.H., 1971, U-Pb ages for sphene in a contact metamorphic zone: Earth and Planetary Science Letters, v. 12, p. 231-237. Krogstad, E.J. and Walker, R.J., 1994, Higher closure temperatures of the U-Pb system in large apatites from the Tin Mountain pegmatite, Black Hills, South Dakota, USA: Geochimica et Cosmochimica Acta, v. 58, p. 3845-3853. Mezger, K., Hanson, G.N., and Bohlen, S.R., 1989, High-precision U-Pb ages of metamorphic rutile: application to the cooling history of high-grade terranes: Earth and Planetary Science Letters, v. 96, p. 106-118. Stacey, J.S. and Kramers, J.D., 1975, Approximation of terrestrial lead isotope evolution by a two-stage model: Earth and Planetary Science Letters, v. 26, p. 207-221.

Verts, L.A., Chamberlain, K.R., and Frost, C.D., 1996, U-Pb sphene dating of contact metamorphism: the importance of sphene growth in the contact aureole of the Red Mountain pluton, Laramie Mountains, Wyoming: Contributions to Mineralogy and Petrology, v. 125, pl. 186-199. Figure DR1. U-Pb concordia diagrams showing (A) F03-72 titanite, (B) F03-76 titanite, and (C) P69120 titanite.

206 Pb/ 238 U 0.0505 0.0495 0.0485 A. 300 Titanite Data from calcsilicate east of Doubtful Sound (F03-72) 304 308 312 316 t1 t2 320 t4 t3 0.0475 0.342 0.350 0.358 0.366 207 Pb/ 235 U 206 Pb/ 238 U 0.020 0.019 B. Titanite Data from biotite granite east of Doubtful Sound (F03-76) 118 122 126 t1 t5 t6 t4 130 t3 0.018 114 0.017 0.114 0.122 0.130 0.138 207 Pb/ 235 U 206 Pb/ 238 U 0.045 0.035 0.025 C. Titanite Data from Caswell Sound calcsilicate (P69120) 160 200 t3 t4 240 280 t2 120 t1 0.015 0.08 0.16 0.24 0.32 207 Pb/ 235 U Figure DR1 Flowers et al.