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Print version ISSN 0001-3765

An. Acad. Bras. Ciênc. vol.82 no.2 Rio de Janeiro June 2010 



Combined U-Pb and Lu-Hf isotope analyses by laser ablation MC-ICP-MS: methodology and applications



Massimo MatteiniI; Elton L. DantasII; Marcio M. PimentelII; Bernhard BühnII

ICNPq and Instituto de Geociências, Universidade de Brasília, Campus Darcy Ribeiro Asa Norte, 70910-900 Brasília, DF, Brasil
IIInstituto de Geociências, Universidade de Brasília, Campus Darcy Ribeiro Asa Norte, 70910-900 Brasília, DF, Brasil

Correspondence to




The Lutetium-Hafnium isotopic system represents one of the most innovative and powerful tools for geochronology and isotopic studies. Combined U-Pb and Lu-Hf in situ analyses on zircon by LA-MC-ICP-MS permit to characterize isotopically the host magma from which it crystallized furnishing significant information for sediment provenance and crustal evolution studies. In this paper e describe the Lu-Hf systematic by LA-MC-ICP-MS developed in the laboratory of Geochronology of the University of Brasilia and report the results obtained by repeated analyses of 176Hf/177Hf isotopic ratio of three zircon standards: GJ-1 = 0.282022 ± 11 (n=56), Temora 2 = 0.282693 ± 14 (n=25) and UQZ = 0.282127 ± 33 (n=11). The 176Hf/177Hf ratio (0.282352 ± 22, n=14) of gem quality zircon used as in-house standard have been also characterized. As a geological application, we analyzed two complex zircons selected from a migmatitic rocks from the Borborema Province, NE Brazil. On the basis of U-Pb and Lu-Hf data, two main crystallization events have been identified in both studied zircons. An older event at ca. 2.05 Ga recognized in the inherited cores represents a well-characterized paleoproterozoic magmatic event that affected the whole Borborema Province. A second crystallization event at ~ 575 Ma, recognized at the rims, represents a Neoproterozoic (Brazilian) high grade metamorphic-magmatic event.

Key words: LA-MC-ICP-MS, Lu-Hf, U-Pb, zircon, Borborema Province.


O sistema isotópico Lutécio-Hafnio representa uma das ferramentas mais recentes e poderosas para estudos isotópicos e geocronológicos. Análises combinadas in situ de U-Pb e Lu-Hf sobre zircão pelo LA-MC-ICP-MS permitem caracterizar iso-topicamente o magma onde ele cristalizou, fornecendo valiosas informações para estudos de proveniência de sedimento e de evolução crustal. Nesse trabalho descrevemos a sistemática de Lu-Hf pelo LA-MC-ICP-MS implantada no laboratório de Geocronologia da Universidade de Brasília e reportamos os resultados obtidos de repetidas análises de três padrões de zircão: GJ-1 = 0.282022 ± 11 (2SD, n=56), Temora 2 = 0.282693 ± 14 (2SD, n=25) and UQ-Z = 0.282127 ± 33 (2SD, n=11). Foi também caracterizada arazão isotópica 176Hf/177Hf(0.282352 ± 22, 2SD, n=14) de um zircão usado como padrão interno do laboratório. Como aplicação geológica, analisamos dois zircões complexos selecionados a partir de uma amostra de migmatito da Província de Borborema, NE do Brasil. Sobre a base dos dados U-Pb e Lu-Hf foram identificados em ambos os zircões dois eventos de cristalização. Um evento mais antigo de 2.05 Ga nos núcleos herdados, representa um evento magmático Paleoproterozoico bem conhecido na Província Borborema. Um segundo evento de ~ 575 Ma, reconhecido nas bordas, representa um evento magmático-metamórfico Neoproterozóico (Brasiliano).

Palavras-chave: LA-MC-ICP-MS, Lu-Hf, U-Pb, zircão, Província de Borborema.




During the last decade, the rapid progresses in Inductively Coupled Plasma mass spectrometry (ICP-MS), combined with the new techniques for in situ laser ablation microanalysis, made the Lutetium-Hafnium isotopic system one of the most innovative and powerful tools for geochronologic and isotopic studies. (Thirlwall and Walder 1995, Vervoort and Blichert-Toft 1999, Blichert-Toft and Albaréde 1997, Gerdes and Zeh 2006, 2009, Griffin et al. 2000, 2002, Hawkesworth and Kemp 2006, Woodhead et al. 2004, Zeh et al. 2007).

The significance of the Lu-Hf method on zircon grains, when combined with the U-Pb method, is the possibility to characterize isotopically the host magma from which they crystallized. The geological applications of this information are numerous. Firstly, in sediment provenance studies the Hf isotopes yield isotopic constrains on the origin of detrital zircons and consequently of the host sediments. The different Hf isotope signatures, found in a zircon population or even in a single zircon, permit to characterize different magmatic or high-T metamorphic events succeeding in time during the crustal evolution of the source regions (Gerdes and Zeh 2006, Zeh et al. 2007).

In this paper we describe in detail the analytical systematic of the Lu-Hf method for LA-MC-ICP-MS on zircon, developed in the Laboratory of Geochronology of the University of Brasília.

We show Hf isotope analyses obtained for three standard zircons (GJ-1, Temora 2 and UQ Z6) and for a gem quality zircon that would represent a potential in-house standard.

We also present an application of this methodology for studying a geological problem in an area of the Borborema Province, Rio Grande do Norte. Combined U-Pb and Lu-Hf analyses, associated with backscattering imaging (BSI), have been carried out on two selected zircons separated from a leucosome portion of a migmatitic rock associated to a paleoproterozoic ter-rane. Several authors (Dantas et al. 1999, 2004) identified in this sector of the Borborema Province multiple orogenic/metamorphic events of archean to paleo- and neoproterozoic ages.




The Lu-Hf isotope system consists of the spontaneous decay of unstable radionuclide 176Lu, by β-emission, to the stable 176Hf with a half-life of 37.2 Ga. The element Lu is the heaviest Rare Earth Element, belonging to the Lantanides group. It has two natural isotopes: the stable isotope 175Lu and the radioactive isotopes 176Lu, representing 97.41% and the 2.59% of the natural Lu isotope abundance respectively. Hafnium is a High Field Strength Element (HFSE) and belongs to the Lithophile group IVa of the periodic table. It has six isotopes: 176Hf, 177Hf, 178Hf, 179Hf and 180Hf, all being stable non-radiogenic except for 176Hf.

The abundance of the isotope 176Hf on Earth is variable due to the radioactive decay of 176Lu, and in the literature it is conventionally compared to the 177Hf. The equation represents the basic age equation for Lu-Hf method, where t is the elapsed time from the closure of the system, and λ is the decay constant of 176Lu. Different values for λ have been proposed in the past by several authors. Patchett and Tatsumoto (1980) proposed the value 1.94 x 10-11 y-1, calculated from the slope of a Lu-Hf isochron for eucrite meteorites of known age. In the following, Sguigna et al. (1982) modified the X value to 1.93 x 10-11 y-1. Recently, Scherer et al. (2001) proposed the new value of 1 .86 x 10_11 y_1 obtained by calibration against the U-Pb decay system, which is in agreement with the value obtained by Nir-El and Lavi (1998) using the decay scintillation counting method.

The application of Lu-Hf systematic to geosciences was developed since 1980 when Patchett and Tatsumoto (1980) and Patchett et al. (1981) used TIMS to measure the respective isotopes. However, due to the high ionisation potential of hafnium (6.65 eV), the TIMS method required large sample sizes and a high purity ion exchange separation in order to achieve acceptable results. In the last decade, the new MC-ICP-MS method, which permits excellent ionisation on impure sample solutions, became the best method for Hf isotope analysis. The laser ablation technique coupled with MC-ICP-MS permitted to analyze solid samples, as mineral grains, with high spatial resolution. The mineral zircon is considered a privileged mineral for isotope analyses of the Lu-Hf system (as for U-Pb system) due to the combination of physical-chemical characteristics and to the capability to host trace and Rare Earth Elements in its crystalline structure (Kinny andMaas 2003, Woodhead et al. 2004). Moreover, zircon is a common accessory mineral, which is present in a great variety of rocks, usually preserving a very complex growing history.

An advantage to use the Lu-Hf method is that Hf, having a geochemical behavior very similar to zirconium, is much more compatible for zircon than Rare Earth Elements (REE), especially Lu. Thus, Hf may reach a higher concentration (up to 3 %) and is retained more easily than Lu in the zircon lattice.

For this reason, zircons are characterized by very low 176Lu/177Hf ratios (< 0.001) and, consequently, the isotopic variations of Hf due to the radiogenic 176Hf are practically negligible. The main corollary of this is that zircons preserve the initial 176Hf/177Hf isotopic ratios inherited by the magma where they crystallized.

This characteristic, together with the high content of Hf and its very low diffusivity in zircon, permits to preserve,in a single crystal,different Hf isotopic composition, generated during crystal growing under the variable P,T and compositional conditions. Experimen-talcalibrations showed that zircon has the closingtem-peraturefo rLu-Hf system 200°C higher than U-Pb system(Cherniak et al.1997,Cherniak and Watson2000), indicating that the Hf isotope system remains closed during most of the thermal events after the crysttalization of zircon.


The Lu-Hf isotope system is utilized to study the history of differentiation of the Bulk Silicate Earth (BSE) that led to the formation of the crust-mantle system. This isotope system has a systematic that is very similar to the Sm-Nd system, with some fundamental exceptions. The first is that, while Sm and Nd are both Rare Earth Elements with very similar chemical characteristics, Lu and Hf are a Heavy Rare Earth Element (HREE) and a HFSE, respectively. This implies in a very different behavior for Lu and Hf during the evolution of the crustmantle system. Hf is more incompatible than Lu during the partial melting processes in the mantle; so, during the first events of juvenile crust generation in the archean time, the crust has been enriched in Hf and depleted in Lu, leaving a mantle enriched in Lu and depleted in Hf. Thus, starting from an unique primordial mantle with chondritic Lu and Hf isotopic composition, which is referred as CHUR (Chondritic uniform Reservoir) composition, two reservoirs with different Lu/Hf ratio were generated: the crust with Lu/ Hfcrust < Lu/HfCHUR and the depleted mantle with Lu/ Hfmantle > Lu/HfCHUR.

As for other isotope systems, the deviation of the 176Hf/177Hf from the chondritic (CHUR) values for a sample is indicated by the Epsilon (@@##) notation:

while the model age is calculated referred to the Depleted Mantle by the following formula:

Whereas a single stage TDM age is commonly calculated for whole rock analyses, for zircon studies a two-stage TDM age is needed (Nebel et al. 2007).

The Lu-Hf isotope system is utilized to study the history of differentiation of the Bulk Silicate Earth(BSE) that led to the formation of the crust mantle system. This isotope system has a system atic that is very similar to the Sm N Whereas a single stage TDM age is commonly calculated for whole rock analyses, for zircon studies a two- stage TDM age is needed (Nebel et al. 2007).

The TDM age in zircon is calculated from the initial Hf isotopic composition of the zircon, using an average crustal Lu/Hf ratio. The initial Hf composition of zircon represents the 176Hf/177Hf value calculated at the time the zircon crystallized, namely the U-Pb age previously obtained on the same crystal. Such model ages indicate the crustal residence time for the rocks that hosted the zircon.

It is evident the importance to carry out U-Pb and Lu-Hf measurements on the same portion of a zircon grain, in order to be able to recalculate the eHf and Hf TDM values at the time of its crystallization.



Instrumentation and LA MC-ICP-Mass Spectrometry

In this study we use a Thermo Neptune MC-ICP-MS instrument equipped with an array of eight moveable Faraday collectors (L4, L3, L2, L1, H1, H2, H3, H4) and one fixed center collector (C), which supports a Faraday and a Secondary Electron Multiplier (SEM). The Neptune is also equipped with six Multiple Ion Counting (MICs), four of these associated to the L4 Faraday and two associated to the L3 and H4 Faradays, respectively.

All the measurements were performed in a static multi-collection and low mass resolution mode. The Far-adays configuration for Lu-Hf measurements are shown in Table I.



Standard Solutions Analyses

In terms of signal stability, the ICP-MS solution system (solution sample) has more accuracy than laser ablation analyses; so, before starting the laser ablation sessions, we routinely calibrate the spectrometer with solutions. For this reason, the first objective in the development of this systematic has been to prepare a Hf standard solution.

For the preparation of the Hf standard solution, the SRM reference material JMC475, available as oxide -Hfo2, has been used. Firstly, we dissolved 100 mg of HfO2 oxide in fluorhydric and nitric acid (HF+HNO3) preserve, in a single crystal, different Hf isotopic composition, generated during crystal growing under the variable P, T and compositional conditions. Experimental calibrations showed that zircon has the closing temperature for Lu-Hf system 200°C higher than U-Pb system (Cherniak et al. 1997, Cherniak and Watson 2000), indicating that the Hf isotope system remains closed during most of the thermal events after the crystallization of zircon.

to complete dissolution. Then, we prepared a 1000 ppm stock solution and, starting from this, a 1 ppm sub-stock solution and a 200 ppb solution for analyses have been produced.

With the aim to test the corrections for Lu and Yb isobaric interference and mass-bias fractionation, a portion of the prepared JMC475 standard solution has been doped with a known quantity of Yb and Lu, obtaining a new standard solution with Yb/Hf=0.02 and Lu/Hf=0.02. At the beginning of each analytical session, the JMC475 standard solution is ran to calibrate the instrument until the reported values of 176Hf/177Hf are achieved.

The JMC475 isotopic values of Hf reported in the literature (Wu et al. 2006, Chu et al. 2002) were reproduced within error margins. In Figure 1 a typical result for a 240 cycles analysis of JMC475 standard solution is shown.

Laser Ablation Analyses — Sample Preparation

Zircons are separated with density and gravimetric methods, and the preparation of polished mounts of epoxy resin with a number of zircon ranging from 10 to 100, depending on the purpose of the analysis, is carried out.

As explained before, the measurement of Lu-Hfisotopes on zircons is made on a crystal previously analyzed by laser ablation U-Pb method to obtain age information. Spatially, the two spot analyses have to be as close as possible in order to analyze portions of the zircon grain with the same isotopic characteristics.

Before the in situ analysis, we should obtain as more information as possible about the structure of the zircon, such as zoning composition, growth pattern and presence of inherited core. It should prevent to analyses of portions of the zircon with different Hf and Pb isotopic compositions that would generate misleading results.

The best methods to obtain images of the internal structure of zircon on polished surfaces are the Cathodoluminescence (CL) and the Back-Scattered Electrons (BSE) techniques. For the Lu-Hf method, the BSE imagery is preferable because the brightness of the image is atomic mass dependent and, for that, it is possible to easily discriminate regions with different Hf content in the same zircon crystal. Higher brightness in the image corresponds to higher Hf contents in the zircon (Hanchar and Miller 1993, Corfu et al. 2003).

Laser Settings

For U-Pb method, we utilized the laser configuration described in Bühn et al. (2009), which employ a a raster ablation generated by a moving laser spot with a diameter of 30 μm. As the raster ablation does not consume much material and produce a low deep hole on the zircon surface, in some case it is possible to do the Lu-Hf analyses in the same local of the previous U-Pb analyses.

For Lu-Hf method, we chose a laser configuration following the most recent literature (Gerdes and Zeh 2006, 2009). The ablation geometry that we used is a laser spot of 40 to 55 μm (Fig. 2), which, while reducing the spatial resolution, permits to ablate more material for a higher signal. To improve the stability of the signal, we chose a low laser frequency of about 5-7 Hz. The power of the laser used during the analytical session depends mainly on the Hf contents of the analyzed zircons, especially the standard one. In our case, using th GJ standard zircon, we used a power of about 40-50%, hich corresponds to an energy of 1-3 J/cm2.



Helium flux is used to transport the ablated material from the zircon in the sample chamber to the MC-ICP-MS: a flux of about 0.38-0.46 lit/min is utilized depending on the values of the other laser parameters. The Helium flux has to be calibrated together with the Sample gas (or Spare gas), which aids the sample to entry the plasma, and, so, obtaining the higher and more stable signal.



Three different standard zircons (GJ-1, TEMORA 2 and UQ-Z) have been analyzed by laser ablation to reproduce their Hf isotopic compositions. The standards are: (i) GJ-1 zircon standard (Jackson et al. 2004) provided by the ARC National Key Centre for Geochemical Evolution and Metallogeny of Continents (GEMOC), Australia; this is a gem-quality zircon crystal of about 0.7 cm in diameter, which was broken and prepared for analysis; (ii) Temora 2 (Black et al. 2004), provided by Lance Black, Geoscience Australia, Australia, which comes from the Middledale gabbroic diorite in the Eastern Australia; the zircon crystals have a size of about 300500 μm and, prior to sample preparation, the concentrate was hand-picked to obtain a high-purity zircon concentrate; iii) UQ-Z (Machado et al. 1996) provided by Alfonso Schrank, UNICAMP, Brazil. With the aim to characterize an in-house standard zircon for U-Pb and Lu-Hf methods, a gem-type zircon from Madagascar (sample MADA) has been also analyzed. This zircon was provided by the Mineralogy Museum of Pisa University, Italy. For an example of geological application, two complex zircons from a paleoproterozoic migmatite from the Borborema Province were analyzed.





The analyses have been carried out using raster ablation method (Bühn et al. 2009) to prevent laser induced mass bias fractionation. The U-Pb raw data are translated to an Excel spreadsheet for data reduction and, when necessary, we corrected the laser induced mass bias using the method of Kosler et al. (2002). Common lead (204Pb) interference and background correction, when necessary were carried out by monitoring the 202Hg and 204 mass (204Hg+204Pb) during the analytical sessions and using a model Pb composition (Stacey and Kramers 1975) when necessary. Reported errors are propagated by quadratic addition [(2SD2+2SE2)1/2] of external reproducibility and within-run precision: the external reproducibility is represented by the standard deviation (SD) obtained by repeated analyses (n=20, ~ 0.8% for 207Pb/206Pb and ~ 1% for 206Pb/238U) of standard zircon GJ-1, performed during analytical session, and the within-run precision is represented by the standard error (SE) that was calculated for each analysis. Concordia diagrams (2@@## error ellipses), concordia ages and lower and upper intercept ages were calculated using Isoplot/Ex (Ludwig 2001).


The acquired Lu and Hf isotope data are corrected online for mass bias fractionation and isobaric interferences. Successively, the isotope ratios are translated to an Excel spreadsheet, for calculation of the parameters of geologic interest, as εHf and Hf Tdm model age. The signals of the interference-free isotopes 171Yb, 173Yb and 175Lu are onitored during the analyses in order to remove isobaric interferences of 176Yb and 176Lu on 176Hf signal (Table I). The 176Yb and 176Lu contribution are calculated using the isotopic abundance of Lu and Hf proposed by Chu et al. (2002). The contemporaneous measurements of 171Yb, 173Yb permit to correct the ass bias fractionation of b using a 173Yb/171Yb normalization factor of 1.132685 (Chu et al. 2002). The Hf isotope ratios are normalized to 179Hf/177Hf value of 0.7325 (Chu et al. 2002). our routine laser ablation measurements consist of 1 block of 40 cycles with an integration time of 1.034 seconds. For solution analyses, 4 blocks of 40 cycles and an integration time of 4 seconds are employed.

The εHf(t) values are calculated using the decay constant λ = 1.86 * 10-11, proposed by Scherer et al. (2001) and the 176Lu/177Hf and 176Hf/177Hf CHUR values of 0.0332 and 0.282772 proposed by Blichert-Toft and Albaréde (1997). The two stages depleted mantle Hf model ages (TDM Hf) are calculated using 176Lu/ 177Hf=0.0384 and 176Hf/177Hf=0.28325 for the depleted mantle (Chauvel and Blichert-Toft 2001) and 176Lu/177Hf value of 0.0113 for the average crust (Taylor and McLennan 1985, Wedepohl 1995).


The GJ-1 zircon standard has been analyzed over a period of about six months. The obtained Hf isotopic compositions yielded 176Hf/177Hf=0.282022±11 (2SD, n=56), reproducing within the error margins the values reported in literature by several authors (Elhlou et al. 2006, Zeh et al. 2007). The Temora-2, UQ-Z zircon standards and MADA zircon have been analyzed in several analytical sessions. The obtained results are listed in Table II. The Temora-2 isotopic composition yielded 176Hf/177Hf=0.282693±14 (2SD, n=25), in agreement with the values reported in the literature by Woodhead et al. (2004), Hawkesworth and Kemp (2006) and Wu et al. 2006.



The analyses carried out on the UQ-Z zircons standard yielded 176Hf/177Hf=0.282127±33 (2SD, n=11), showing a very homogeneous Hf composition. Before the analytical session, the MADA zircon has been previously studied with the BSE technique in order to evaluate a possible growth zoning. The BSE image obtained for the analyzed grain shows that it is very homogeneous in terms of Hf content, do not showing any internal structures. The Hf analyses carried out in different parts of the grain yielded 176Hf/177Hf=0.282352±22 (2SD, n=14), suggesting a very homogeneous Hf isotopic composition.


We present an application study of the in situ combined U-Pb and Lu-Hf systematic on zircons with LA-(MC) ICP-MS technique. This study has been chosen to show the potential of the Lu-Hf LA-MC-ICP-MS systematic on zircon as a powerful tool for reconstructing the tectonic evolution of a cratonic area.

The studied zircons have been separated from a leucocratic portion of migmatitic rock from the Rio Grande do Norte terrain in the Borborema Province. Images of the selected zircons in backscattered electrons (BSE) mode were obtained using a Scanning Electron Microprobe (SEM) in order to have information on the internal structure of the studied zircons. In this contribution, we employ the BSE technique using a Scanning Electron Microscope (SEM) JoEL of the laboratory of the Federal Police of Brasília.

The BSE images permitted us to differentiate Hf-rich and Hf-poor portions of zircons, characterized by high and low brightness response, respectively.

The studied zircons show a typical flat shaped meta-morphic morphology and complex internal structures (Fig. 3), with well developed zoning with an euhedral Hf-rich core rimmed by a Hf-poor rim.

We analyzed the selected zircons with combined U-Pb and Lu-Hf in situ LA-MC-ICP-MS technique (Tables III and IV). Every portion of each zircon grains showing peculiar and distinctive characteristics based on the interpretation of BSE images has been analyzed. Initial Hf composition for each zircon has been calculated using the U-Pb age of the correspondent spot. For old discordant zircons, it was assumed that 207Pb/206Pb age represents the crystallization age, whereas for younger zircons the 206Pb/238U was considered. The Lu-Hf data are shown in Table IV.

In Figure 4 the Concordia diagrams for the obtained data on two zircons are shown. The two analyses of zircon 1 (Fig. 4a) define two crystallization events: an older one defined by a 207Pb/206Pb age of 2057± 14 Ma, and a younger one defined by the concordant age of 578±11. The U-Pb analyses on zircon 12 also define (Fig. 4b) two crystallization events individuated by a concordant analysis of 2024± 11 Ma and a by a slightly discordant analyses with 206Pb/238U age of 606±15Ma. In Figure 4c a graphic interpretation of the slightly discordant rim data for zircon 12 is shown.

The distribution of these younger analyses may be interpreted in two different ways: i) different extreme Pb-loss of Paleoproterozic grains induced by a 575 Ma magmatic event (Dantas et al. 2004) and ii) crystallization event at 575 Ma, with discordance for zircon 12 rim possibly caused by an imperfect sample preparation. In this case, as shown in Figure 4c, it is possible that the laser accidentally ablated a portion ofthe older core. The total signal of such analysis, representing a mixing of two different portions of the zircons, would be plotted on a discordia line defined by the two different (end-members) U-Pb isotopic compositions.

The Hf results are listed in Table IV and shown in the diagram of Figure 5a-b. The zircon 1 shows very homogeneous Hf composition with 176Hf/177Hf ratios of 0.281405 and 0.281401, and εHf(t) of -2.73 and -35.5 for the core and rim, respectively. The analyzed core portions of zircon 12 with Paleoproterozoic 207Pb/ 206Pb apparent ages have homogeneous Hf isotope composition with measured 176Hf/177Hf ratios of 0.281348 and 0.281356, and εHf(t) -6.6 to -6.1, respectively. The rim with neoproterozoic 206Pb/238U age gave similar Hf compositions with 176Hf/177Hf ratio of 0.281331 and εHf of-38). The TDM Hf model ages for the Paleoproterozoic cores of the two analyzed zircons are similar, ranging between 2.68 and 2.82 Ga. The Neoproterozoic rims have been characterized by older TDM Hf model ages of 3.32 and 3.46 Ga for zircon 1 and zircon 12, respectively.



The Hf isotope composition evolution diagram shows that the Paleoproterozoic cores crystallized at ~ 2.05 Ga in magmas characterized by an important crustal signature. These magmas may have been formed by partial melting of an older juvenile crust generated at 2.5-2.8 Ga or, alternatively, may represent juvenile magmas generated at 2.0-2.2 Ga and contaminated by older (Archean) crustal material. in the diagrams of Figure 5a-b, the evolution of Hf isotopic composition (calculated for Lu/Hf = 0.0113) for different types of Paleoproterozoic to Archean juvenile crust are reported.

The Hf isotopic composition of Neoproterozic rims suggests that they could not crystallized in magma derived by partial melting of a 2.0-2.2 Ga Paleoprotero-zoic crust, represented by the older core of the studied zircons. To produce the measured Hf composition ( εHf(t) ~ 35, TDM > 3.2 Ga) of the young rims, a more radiogenic isotopic component, derived from earlier (or older) Archean crust, has to be involved during the crystallization of the outer part of the studied zircons.

On the other hand, the zircons are characterized by practically the same values of 176Hf/177Hf ratio at the rim and the core. In the diagrams of Figure 5a, the Hf composition of the rims plot on the Hf isotopic evolution curve of the core portions of the same zircons, calculated from the measured 176Lu/177Hf. Thus, these younger rims may be interpreted as a recrystallization of the outer part of the zircon grains during a Neoprotero-zoic high metamorphic/migmatitic event. This process would have reset almost entirely the U-Pb system, leaving unaltered the Hf isotopic composition.



In this paper we described the systematic developed in the laboratory of geochronology of the University of Brasília for the combined in situ U-Pb and Lu-Hf analyses on zircons by LA-MC-ICP-MS. The Hf isotopic compositions for three zircon standards have been measured. The 176Hf/177Hf values for GJ-1 and TEMORA-2 reported in the literature by several authors have been reproduced, within error margin. The Lu-Hf isotopic composition for the zircon standard UQ-Z and for a in-house zircon standard is reported.

New U-Pb and Lu-Hf isotopic data were obtained for two zircons selected from a migmatitic rock from the Borborema Province. The U-Pb, Lu Hf in situ analyses, combined with BSE imaging, permitted to study in detail the internal isotopic composition of the zircons and to obtain information about the growing history of each zircon. On the basis of U-Pb and Lu-Hf data, two main crystallization events have been identified in both studied zircons. An older event at ca. 2.05 Ga that was recognized in the core portions of the zircons represents a well characterized Paleoproterozoic magmatic event that affected the whole Borborema Province. A second younger crystallization event at ~ 575 Ma, which generated the rim portions of the zircons, would represent a high grade metamorphic-magmatic, in agreement with previous geochronological data obtained by other authors (Dantas et al. 2004) on monazite (TIMS) from a granite outcropping in the same region.



The LA-MC-ICP-MS facility was installed at the University of Brasília with funds provided by PETROBRAS and the Ministry of Minas e Energia of Brazil. This work is part of the postdoctoral research of the first author. Financial support from Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq), Grant N. 150142/2007-2, is acknowledged. We thank Prof. Roberto Ventura Santos, University of Brasília, for providing JMC475 Hf standard material.



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Correspondence to:
Massimo Matteini

Manuscript received on September 23, 2008; accepted for publication on July 8, 2009

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