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155

176

Lu/

177

Hf ratios of domain II zircon are

extremely low and vary from

c.

0.00001 to

0.00005 (Fig. 35b).

176

Lu/

177

Hf ratios of domain

I zircon are low and vary from

c.

0.00025 to

0.00037 (Fig. 35b).

Nd whole-rock experiments failed to calculate

a model-age, because the

147

Sm/

144

Nd ratio

calculated for this sample has a negative slope

in the

H

Nd

(t)

v.

age plot (higher value than

CHURs

147

Sm/

144

Nd value of 0.1967; Jacobsen &

Wasserburg, 1980). Epsilon value for present day

is:

H

Nd

(t=0)

= +9.4.

7.3.2.2. Discussion

The majority of the U–Pb ages from this

sample are grouped at 390 Ma (domain II; Fig.

32a), and only three zircon grains (domain I)

show ages older than 420 Ma.

Domain I zircon is very scarce (

n

= 3/19; zircon

analysed with U–Pb and Lu–Hf systematics)

and seem to be the remnants of the magmatic

protolithic zircon. This assumption is favoured

by the fact that they are the older zircon grains in

the sample and that they have higher Th/U ratios

(from

c.

0.1 to 0.8) than the younger domain II

zircon (Fig. 35a). Their ages are 455, 469 and

482 Ma. Due to their very low U content these

analysis are very poor quality and show very high

errors. This is most probably due to an intense

solid-state Pb-loss process triggered by the HP

post-protolith metamorphism. Therefore their

ages are not considered to establish a protolith

age.

Domain II (

c.

390 Ma) zircon have low U

content (but higher than domain I zircon) and

very lowTh/U ratios (< 0.01; Fig. 35a). They have

lower

176

Lu/

177

Hf ratios (

c.

0.00001; Fig. 35b) and

also lower

176

Yb/

177

Hf ratios (average:

c.

0.0015;

Appx. 4) than domain I zircon.

176

Hf/

177

Hf

(t)

ratios for all analysed zircon grains plot within

error at 0.282821 ± 0.000061 (domain II) and

0.282859 ± 0.000016 (domain I; ±2 SD; Fig.

34b). These very similar

176

Hf/

177

Hf

(t)

ratios

between domain I magmatic zircon and domain

II metamorphic zircon seem to clearly indicate

that domain II zircon was formed by a solid-

state recrystallisation process of domain I zircon.

This is due to the high immobility of Hf in Zrn,

basically because Hf has the same ionic radius

than Zr (155

p

m; Hoskin & Schaltegger, 2003).

The lower amount of Lu and Yb with respect to

Hf and also of Th with respect of U of domain

II zircon in relation to domain I zircon are

explained as a consequence of the intense and

extreme solid-state recrystallisation process. This

process purged from the crystal structure the

cations with ionic radii and chemical properties

(such as oxidation state) significantly different

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Fig. 33.

CL (cathodoluminescence) images of representative zircons from the studied sample. Laser ablation pits for U–Pb

analyses (red line circles) have 23, 33 and 50

μ

m diameters. Laser ablation pits for Lu–Hf analyses (green line circles) have

26 and 33

μ

m diameters. White numbers are the reference number of the analysis, red numbers are the U–Pb age and its 2

σ

error (Ma) and the green numbers are the

H

Hf values for the U–Pb age.

CL images of A007 and A008 were taken with diffe-

rent SEM parameters than the rest of the Zrn of this sample. Textures of A007 and A008 are the same than A006 and A009.

7.3. ECLOGITES