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GEOLOGICA CARPATHICA
GEOLOGICA CARPATHICA
GEOLOGICA CARPATHICA
GEOLOGICA CARPATHICA
GEOLOGICA CARPATHICA
, OCTOBER 2012, 63, 5, 383—398
doi: 10.2478/v10096-012-0030-6
Vertical zonality of fractionated granite plutons reflected in
zircon chemistry: the Cínovec A-type versus the Beauvoir
S-type suite
KAREL BREITER
1
and RADEK ŠKODA
2
1
Institute of Geology AS CR, v.v.i., Rozvojová 269, CZ-165 00 Praha 6, Czech Republic; breiter@gli.cas.cz
2
Geological Institute, Masaryk University, Kotlářská 2, CZ-611 37 Brno, Czech Republic
(Manuscript received March 22, 2012; accepted in revised form June 13, 2012)
Abstract: We studied vertical changes in the chemical composition of zircon from two contrasting Variscan granite
systems. The Beauvoir system (Massif Central, France) composed of three successive intrusions (B1, B2, B3) represents
typical peraluminous S-type granite extremely enriched in P, F, Li, Rb, Cs, Be, Sn, Nb, Ta, and poor in Zr, Th, REE and Y.
The Cínovec system (Krušné hory Mts/Erzgebirge, Czech Republic/Germany) composed of two successive intrusions
(protolithionite granite, zinnwaldite granite) is only slightly peraluminous, P-poor, F, Li, Rb, Cs, U, Th, REE, Y, Sc, Sn,
W, Nb, Ta-rich granite, which may be classified as A-type. In both localities, the most fractionated intrusions are located
on the top of the system. Samples from borehole GPF-1 (Beauvoir) represent an 800 m long vertical section through the
entire granite stock, while CS-1 borehole (Cínovec) reached a depth of 1600 m. Chemical compositions of zircons from
both granite systems show distinct vertical zonality, but their shape and elemental speciation is highly contrasting. At
Beauvoir, zircon shows a remarkable increase in Hf-content from 2—4 wt. % HfO
2
( ~ 0.03 apfu Hf) in the deepest B3-unit
to 15—19 wt. % HfO
2
(up to 0.18 apfu Hf) in the uppermost B1-unit. The highest contents of F, P, and U were detected in
the intermediate unit B2 at a depth of 400—600 m. At Cínovec, Hf shows only moderate enrichment from ca. 2 wt. % HfO
2
in the deeper protolithionite granite to 5—10 wt. % HfO
2
in the uppermost part of the zinnwaldite granite. High contents of
Th (3—8 wt. % ThO
2
) are entirely bound in the uppermost section of the granite copula to a depth of 200 m, but below this
level the contents only sporadically exceed 1 wt. % ThO
2
. Concentrations of U, Y, HREE, Sc and Bi also reach their
highest values in the uppermost parts of the zinnwaldite granite, but their decrease downward is much gentler. Extreme
enrichment of outer zones of zircon crystals from some granites with Hf or high contents of Th, U, REE, Y, Nb and of some
other elements in zircons from other localities is not considered to be a specific phenomenon characterizing melts of A- or
S-type granite, but reflects a high degree of fractionation of systems rich in Na and F.
Key words: zircon, Cínovec, Beauvoir, trace elements analyses, S-type granite, A-type granite, fractionation.
Introduction
Zircon is almost a ubiquitous and relatively stable accessory
mineral in the majority of types of granitoids. Its grains that
show no obvious metamictization provide information about
the chemical composition of the melt, which the granite crys-
tallized from. In common I- and S-type granite, zircon belongs
among the first crystallizing minerals, although some slightly
Hf-enriched grains may precipitate during the final stage of
rock crystallization. Zircon is frequently embedded in biotite
and its crystallization results in the decrease of contents of not
only Zr (and Hf), but also of Th, Y and HREE in the melt. On
the contrary, in strongly fractionated peraluminous S-granites,
generally low in Zr, zircon is one of the late-crystallizing min-
erals. It is interstitial and strongly to extremely enriched with
U, P, F and with a number of “ore” elements (Nb, Ta, W, Bi).
In the A-type granites, zircon crystallizes during the whole
process of the melt differentiation, so that in relatively less
differentiated intrusions the zircon crystallized as an early min-
eral, while in later highly differentiated intrusions it may also
be filling interstices.
The contents of trace elements in zircon have been exten-
sively investigated since the early 1960s (summary in Görz
1974). However, only the routine use of electron probe mi-
cro-analysis and LA-ICP MS methods during the last 20
years has produced reliable data concerning the contents of
many elements (Uher et al. 1998; Wang et al. 2000; Huang
et al. 2002; Rubatto 2002; Hoskin & Schaltegger 2003;
Finch & Hanchar 2003; Pettke et al. 2005; Johan & Johan
2005; Breiter et al. 2006; Péréz-Soba et al. 2007; Grimes et
al. 2007; Van Lichtervelde et al. 2009). So far, the most
comprehensive study of the chemical composition of zircons
from various types of magmatic rocks obtained using the
ICP-MS method was published by Belousova et al. (2002).
The following average contents (medians) were established in
zircons from granites: ca. 0.1 wt. % P
2
O
5
, 0.25 wt. % Y, tens
ppm of LREE, hundreds ppm of HREE, 4 ppm Nb, 2 ppm
Ta, 9 ppm Pb, 368 ppm Th and 764 ppm U. Zircon from
fractionated granites was found to be relatively rich in REE
(total 1.5—2 wt. %). Metamict zircon can be LREE enriched.
A positive Ce-anomaly is common. Belousova et al. (2002)
also report contents of 100—1000 ppm Nb and 10—100 ppm Ta
in zircon. The average Nb/Ta ratio in zircon is 3, whereas the
chondrite value is 17. The Th/U ratio in zircon usually corre-
sponds to 0.1—1.0, while the ratio of these elements in the
Earth’s crust is equal to ca. 4. Contents of Th and U show a
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positive correlation with Y and increase with increasing frac-
tionation of magmas from ultramafic rocks up to granites.
Belousova et al. (2002) consider high contents of P to be pri-
mary because phosphorus is compensated by the sum of
REE+Y as a consequence of xenotime substitution.
The majority of published analyses of zircons have been
obtained using the electron microprobe (see below). However,
only a few of the most abundant elements occurring in zircon
were analysed using this technique (in addition to Zr, Hf and
Si also U, Th, Y, some REE, Al and Ca). Complete analyses
for the 20 or more trace elements that contribute to the chem-
ical composition of individual zircon grains are still scarce
(Förster 2006; Breiter et al. 2006, 2009; Uher et al. 2009;
Förster et al. 2011).
The Zr/Hf ratio in chondrites is 37 (Hoskin & Schaltegger
2003), but this ratio in zircons varies considerably. There is a
general rule that the Zr/Hf ratio in crystallizing zircon de-
creases with progressive fractionation of the melt. The con-
tent of Hf in zircon from rocks ranging from kimberlites to
common granites remains almost the same (0.8—1.7 wt. %)
and increases significantly only in strongly fractionated
granites (Belousova et al. 2002). The highest concentrations
of Hf in zircon were found in pegmatites. Černý & Siivola
(1980) found 13.3—17.9 wt. % HfO
2
(0.136—0.166 apfu Hf)
in zircon from the Tanco pegmatite in Manitoba (Canada).
Recently, Van Lichtervelde et al. (2009) reported from this
locality late zircon with up to 38.9 wt. % HfO
2
. Raimbault
(1998) reported 5.5—12.8 wt. % HfO
2
(0.055—0.116 apfu Hf)
and up to 11.67 wt. % P
2
O
5
(0.33 apfu P) in a zircon from the
Li-F pegmatite at Chedeville (France), while contents of UO
2
do not exceed 3 wt. % and those of ThO
2
are 0—11.9 wt. %.
Contents of Y and Sc are a few tenths of a percent. Contents of
REE are not given. Uher & Černý (1998) found in beryl-
columbite pegmatites fron Slovakia up to 22 wt. % HfO
2
.
Hafnon, the Hf-dominant member of the zircon group was
found in rare-metal pegmatite at Zambezia, Mozambique
(Correia Neves et al. 1974).
Wang et al. (2000) analysed zircons from granites of I- and
A-type in Laoshan, P.R.China. Zircons from the I-type gran-
ites are generally poor in trace elements (HfO
2
< 2 wt. %,
UO
2
, ThO
2
, Y
2
O
3
< 1 wt. %), while zircons from the more
fractionated facies of A-type granites contain as much as
12.4 wt. % HfO
2
and 4.3 wt. % ThO
2
, but only small
amounts of UO
2
(< 0 .4 wt. %), Y
2
O
3
(< 1.4 wt. %) and P
2
O
5
(< 0 .75 wt. %). Contents of REE were not analyzed here ei-
ther. Wang et al. (1996) found an extremely high content of
Hf (up to 34.8 wt. % HfO
2
, 0.353 apfu Hf) in zircon from an
A-type granite at Suzhou, P.R.China. This zircon is U- and
Th-free, and Y-, P-poor (< 0 .5 wt. % Y
2
O
3
, < 1 wt. % P
2
O
5
).
Other elements were not reported. Huang et al. (2002) found
up to 22.0 wt. % HfO
2
in zircon from Yichun topaz-lepidolite
granite, P.R. China.
Uher et al. (1998) described a zircon rich in Hf and P, but
very poor in U, Th, Y and REE from the strongly peralumi-
nous Homolka muscovite granite of the South Bohemian
Pluton. Hoskin et al. (2000) analysed zircon from the zoned
I-type Boggy Plain pluton, Australia, and found 0.30—
3.98 wt. % HfO
2
. Péréz-Soba et al. (2007) were able to dis-
tinguish two types of zircon in Spanish peraluminous
granites: older prismatic crystals with low contents of trace
elements and high Zr/Hf ratio embedded mostly in biotite,
and younger, mostly interstitial zircon enriched with U, Th,
Y and REE and having a low Zr/Hf ratio.
Kempe et al. (2004) pointed out that extreme Hf-enrich-
ment is typical of zircons with patchy structure from P-poor
granites. This observation contradicts the results of analysis
of zircons from European Variscan rare-metal granites ob-
tained by us. The highest contents of Hf we found in zircons
from the peraluminous P-rich granites at Beauvoir (this
study) and at Argemela in Portugal (Breiter & Škoda 2010).
Zircons from peralkaline rocks contain in general less trace
elements. De Liz et al. (2009) described zircons from shosho-
nite association of the Lavras do Sul intrusive complex in Bra-
zil to contain on average 1.0—1.4 wt. % HfO
2
, 3—75 ppm Nb,
195—414 ppm Th, 400—800 ppm U and 700—2000 ppm Y.
Nardi et al. (2012) found zircons from several intrusions of
peralkaline granites of A-type near the tin-bearing deposit of
Pitinga in Brazil to contain on average 1.8—5.0 wt. % HfO
2
,
8—825 ppm Nb, 200—6649 ppm Th, 456—2975 ppm U and
2003—9211 ppm Y.
The chemistry of zircon from the Beauvoir granite was in-
vestigated by Wang et al. (1992). The published compositions
are as follows: 2.4—8.1 wt. % (one grain with 18 wt. %) HfO
2
,
UO
2
up to 7.6 wt. %, ThO
2
max. 0.35 wt. % and PbO up to
0.55 wt. %. Elements such as P, Y and REE were not analysed.
Johan & Johan (2005) analysed the following 16 elements
in zircon from Cínovec: P, Si, Zr, Hf, Th, U, Pr, Sm, Dy, Er,
Yb, Y, Sc, Fe, Ca, and F and found significant differences in
the compositions of zircons from the zinnwaldite and pro-
tolithionite granites. Their interpretation is based on the idea
that the zinnwaldite granite is of metasomatic origin. This
view, however, is different from that of the majority of other
investigators (Breiter et al. 1999; Föster et al. 1999; Thomas
et al. 2005).
This paper on an example of two geologically well-docu-
mented small ore-bearing granites – the Beauvoir and the
Cínovec is intended to demonstrate the different behavior of
zircon during the crystallization of fractionated magma of
S- and A-type granites and to show differences in zircon
chemistry with depth and its relationship to an overall chem-
istry of the granite pluton.
Geology and samples
The late Variscan Cínovec granite lies on both sides of the
Czech-German border in the eastern sector of the Krušné
hory/Erzgebirge Mts. Here, the late Variscan tin-bearing gran-
ites form ca. 20 km long NW-SE- oriented belt intruded into
the Upper Proterozoic paragneisses and Upper Carboniferous
rhyolites. Only a few small exposures less than 1 km
2
in size,
in the form of small copulas (Cínovec, Altenberg) or vertical
stocks (Krupka, Sadisdorf), are exposed on the surface. The
pluton consists of two main types of granite: (i) the older me-
dium- to fine-grained mostly distinctly porphyritic biotite to
protolithionite granites compose the majority of the known
volume of the pluton; (ii) the younger medium- to fine-
grained not porphyritic albite-topaz-zinnwaldite granites ac-
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companied by Sn-W (Nb, Ta, Mo, Sc) mineralization of greisen
type form small separate intrusions. The spatial relationship be-
tween the two types of granite is different: the younger ore-
bearing granites can form stocks or stock-works with steep
contacts which intrude in older granites proved by numerous
boreholes and underground workings made at Krupka (Eisen-
reich & Breiter 1993), or intruded in the form of tongue-like
bodies along the upper contact of older granites having formed
rather flat copulas in their roof (Cínovec and its surroundings).
Contacts of both types of granite are evidently intrusive.
The Cínovec granite copula exposure 1.4 0.3 km large was
studied to a depth of 1596 m by borehole CS-1 (Štemprok &
Šulcek 1969). An albite-topaz-zinnwaldite granite (hereinafter
“zinnwaldite granite”, ZiG) was proved to exist in several tex-
tural varieties to a depth of 735 m, while an albite-pro-
tolithionite granite (hereinafter “protolithionite granite”, PrG)
continues to greater depths (Fig. 1). A fractionation in situ can
be observed in the zinnwaldite granite showing increasing
concentrations of volatile and lithophile elements upward. The
apical part of the copula has been eroded, but a facies with
mica corresponding to lepidolite is preserved to a depth of ca.
80 m below the present surface (Rub et al. 1998). From the
viewpoint of geochemistry, the Cínovec pluton represents
Fig. 1. Vertical zonality of granite
types in Cínovec from borehole CS-1
(modified according to Štemprok &
Šulcek 1969) with indication of posi-
tion of studied samples.
strongly fractionated A-type granites: it is only slightly peralu-
minous, enriched with F, Li, Rb, Zr, Th, HREE, Sc, Sn, W, Nb
and Ta, and depleted of P, Ti, Mg and Ca (Table 1). Common
accessory minerals comprise fluorite, topaz, cassiterite,
columbite, microlite, pyrochlore, Nb-rutile, zircon, thorite,
xenotime, fluorides, oxo-fluorides and carbonates of REE
(Cocherie et al. 1991; Rub et al. 1998; Breiter et al. 1999;
Förster et al. 1999; Johan & Johan 2005; Breiter 2011).
The Beauvoir granite forms a small body (< 0 .2 km
2
) at the
southern edge of the late Variscan Echassieres granite pluton
in the northern part of the Massif Central, France. Geochemi-
cally it is a highly specialized, strongly peraluminous (S-type),
rare metal-bearing granite enriched with P, F, Li, Rb, Nb, Ta,
Sn, and W, and depleted of Si, Fe, Ti, Mg, Sr, Y, REE etc.
(Cuney et al. 1992; Raimbault et al. 1995). The Beauvoir
granite is the latest intrusion in a peraluminous granitic com-
plex composed of three successively emplaced units: the hid-
den more or less hypothetical La Bosse granite, the Colettes
two-mica granite, and the Beauvoir topaz-lepidolite-albite
granite (Cuney & Autran 1987; Cuney et al. 1992). All gran-
Unit ZiG
ZiG
PrG
PrG
Depth (m)
60 559 749 1579
SiO
2
72.22
74.69
75.56
75.53
TiO
2
0.01
0.03
0.05
0.07
Al
2
O
3
15.92
13.21
12.76
12.54
Fe
2
O
3
0.20
0.32
0.32
0.60
FeO
0.45
0.58
0.79
0.78
MnO
0.09
0.06
0.05
0.05
MgO
0.09
0.03
0.06
0.07
CaO
0.38
0.35
0.45
0.64
Li
2
O
0.216 0.167
0.061
0.055
Na
2
O
4.83
4.02
3.66
3.49
K
2
O
2.39
4.53
4.78
4.73
P
2
O
5
0.015 0.012
0.009
0.011
F
0.79
0.75
0.46
0.51
LOI
1.95
0.78
0.72
0.87
Total
99.55
99.54
99.73
99.98
Rb
1440
1900
1133
802
Sr
72
6
12
13
Ga
54
40
31
25
Zr
44
58
125
124
Hf
9.1
6.8
8.1
6.9
Th
15
32
52
58
U
4
8.6
39
32
Nb
109
74
56
52
Ta
52
31
8
7
W
13
41
14
12
Y
7.5
49
114
103
La
3.9
22.5
42
34
Ce
13.5
62
105
83
Pr
1.84
7.2
12.4
10.3
Nd
4.9
22
44
40
Sm
1.54
6.4
12.6
10.4
Eu
<0.02 <0.02
0.08
0.12
Gd
1.03
5.4
12.4
40.5
Tb
0.33
1.4
2.8
2.3
Dy
2.4
10.1
19
15.5
Ho
0.51
2.1
3.9
3.4
Er
1.9
7.2
12.6
11.1
Tm
0.46
1.6
2.3
1.9
Yb
4.2
12.4
16.3
13.1
Lu
0.65
1.9
2.4
1.9
Table 1: Whole-rock chemical composition of granites from
Cínovec (major elements in wt. %, trace elements ppm).
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ite types intruded into lower-Paleozoic micaschists. The
900 m deep borehole GPF-1 allowed study of the vertical evo-
lution of the Beauvoir granite over a section more than 700 m
long (Fig. 2). Three granitic units marked B1 to B3 were dis-
tinguished by Rossi et al. (1987) and Raimbault & Azencot
(1987). Later, a detailed geochemical study divided the
Beauvoir granite into two major units: B and B
’ (Raimbault
et al. 1995). The B-unit forms the upper part of the stock rep-
resenting geochemically more evolved, more fluid-enriched
part of the Beauvoir initial magma. The B
’-unit, smaller in
volume, represents a relatively less evolved and later em-
placed portion of the Beauvoir magma. Separation of the
B- and B
’-melts occurred at the early stage of evolution of the
granite system. Later, both melts in fact fractionated indepen-
dently. Thus, the upper B-unit can be divided into three sub-
units, from the uppermost ultimately fractionated B1-unit (at a
depth of 98—423 m), through the B2-unit (at a depth of ca.
423—571 m), to the B3-unit (in a depth of 765—790 m). Within
the lower B
’-unit, the relatively more fractionated B’2-unit
(at a depth of ca. 571—746 m), and less fractionated B
’3-unit
(at a depth of ca. 850—870 m) can be distinguished. All granite
units are built of quartz, K-feldspar, albite and Li-mica.
Chemical composition of the latter mineral ranges from lepi-
dolite (B1) to Li-enriched biotite (B
’3). Amblygonite and al-
kalifeldspars (Breiter et al. 2002) are the main hosts of
phosphorus. Common accessory minerals include apatite, to-
paz, cassiterite, minerals of the columbite group and zircon.
A number of other minerals were also identified (Raimbault
et al. 1995). Comprehensive whole-rock chemical data from
Beauvoir were published by Cuney & Raimbault (1991) and
Raimbault et al. (1995).
Altogether 15 samples from borehole CS-1 drilled at
Cínovec, representing mineralogical and chemical develop-
ment of the pluton to a depth of 1596 m, were collected and
analysed. A total of 10 samples from borehole GPF-1 drilled
at Beauvoir, representing all intrusive units defined by
Raimbault et al. (1995), except for the B3-unit, were collected
and analysed.
Analytical methods employed
In order to study zircon grains in relation to rock-forming
minerals polished thin sections were made from all collected
samples. Back-scattered electron (BSE) images were taken
prior to analysis to study the internal zoning of individual
mineral grains and their relative position to rock-forming min-
erals. Zircon and associated minerals such as monazite, xeno-
time, thorite, and other similar mineral phases were analysed
using the identical set-up and included all of the chemical ele-
ments identified in at least one of the above-mentioned miner-
als. Elemental abundances of W, P, As, Nb, Ta, Si, Ti, Zr, Hf,
Th, U, Y, La, Ce, Pr, Nd, Sm, Gd, Dy, Er, Yb, Al, Sc, Bi, Mn,
Fe, Ca, Pb, S, and F in oxide minerals were determined using
a CAMECA SX100 electron microprobe (Masaryk University
and Czech Geological Survey, Brno) equipped with five WD
spectrometers. Minerals were analysed at an accelerating volt-
age and beam current of 15 keV and 40 nA, respectively, and
with a beam diameter ranging from 1 to 5 µm. The following
standards were used: U – metallic U, Pb – PbSe, Th – ThO
2
,
P – fluorapatite, Y – YAG, La – LaB
6
, Ce – CeAl
2
, Pr –
PrF
3
, Nd – NdF
3
, Sm – SmF
3
, Gd – GdF
3
, Dy – DyP
5
O
14
,
Er – YErAG, Yb – YbP
5
O
14
, Al – almandine, Si, Ca,
Fe – andradite, Mn – rhodonite, W – scheelite, S – barite,
F – topaz, As – InAs, Nb – columbite, Ta – CrTa
2
O
6
,
Ti – titanite, Zr – zircon, and Sc – ScVO
4
. Empirical for-
mulae of zircon were calculated on the basis of 4 atoms of ox-
ygen in a formula unit (4 O apfu).
Contents of major elements in whole rock samples from
Cínovec were established using the standard methods of wet
chemistry at the Laboratory of the Czech Geological Survey,
Praha, while the trace elements were analysed in the ACME
Laboratory, Vancouver, Canada using the ICP-MS method.
Results
Position of zircon crystals in granite and its internal structure
In Cínovec, zircon in the zinnwaldite granite forms tiny iso-
metric crystals 10—50 µm in size (Fig. 3). They are enclosed in
quartz and feldspars, but some of the grains that crystallized
later occupy the interstices between the other minerals. Some
crystals contain µm-sized inclusions of quartz and feldspars
and numerous tiny cavities. Most of the crystals are not zoned
in the BSE image. The internal composition is patchy with do-
mains enriched in Hf, Y and Th. In the few zoned grains, the
Fig. 2. Geological cross-section of the Beauvoir granite stock along
the borehole GPF-1 Eschassieres (modified according to Raimbault
et al. 1995) with indication of position of studied samples.
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cores are patchy and heterogeneous, porous and enriched with
uranium, whereas the rims are compact, homogeneous and en-
riched with Hf. Individual analyses of crystal cores give totals
significantly lower than 100 wt. %, usually 90—95 wt. % that
indicate a high degree of hydratation due to metamict state.
On the other hand, analyses of the compact rims give totals
close to 100 wt. %. The majority of zircon crystals in the pro-
tolithionite granite are enclosed in mica. They are of similar
size (10—50 µm), but crystals showing a distinct zonal struc-
ture and contrasting blebs of exsolved mineral phases close to
xenotime and thorite in composition are relatively more abun-
dant. However, even in this case, the crystal cores are porous.
In spite of low concentrations of Zr in the rock, all studied fa-
cies of the Beauvoir granite contain abundant hypidiomorphic
Fig. 3. Typical crystals of zircon from the Cínovec granite (BSE-images), scale bars in all cases 20 µm: a – zinnwaldite granite depth 97 m,
two zircon grains with bright inclusion of Yb-rich xenotime-(Y); b – zinnwaldite granite depth 336 m, partly altered patchy zoned zircons
(grey) with younger grains of Yb-rich xenotime-(Y) (bright); c – zinnwaldite granite depth 413 m, zircon with Hf-enriched rim; d – zin-
nwaldite granite depth 735 m, group of zircon crystal; e – vacuolized zircon with xenotime-(Y) rim, zinnwaldite granite, depth of 735 m;
f – zoned zircon crystal embedded in protolithionite (black) with younger Yb-rich xenotime-(Y) (bright), xenotime-(Y) penetrates the
protolithionite along cleavage, protolithionite microgranite, depth of 741 m; g – zoned zircon crystal with younger grain of thorite
(bright), protolithionite microgranite, depth of 741 m; h – protolithionite microgranite depth 749 m, two patchy zoned and vacuolized zir-
cons; i – protolithionite granite depth 1579 m, zircon (grey) with patchy domains enriched in Y (light grey) and inclusions of thorite (bright).
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to idiomorphic zircon grains 10—50 µm large, rarely as much
as 80 µm in size (Fig. 4). Zircon grains showing irregular
spotty texture without any observable zoning or with only in-
distinct zoning in outer part of crystals prevail in more frac-
tionated facies. The number of grains with distinct zoning in-
creases with growing depth in relatively less fractionated
granite facies. Only a few relatively broad zones always exist,
but a thick oscillatory zoning, which is common in zircon
Fig. 4. Typical crystals of zircon from the Beauvoir granite (BSE-images): a – distinctly zoned zircon crystal with metamictized core and
homogeneous Hf-rich rim, granite B1, depth 130 m; b – distinctly zoned zircon crystal with patchy U-rich core and Hf-rich rim, granite
B1, depth 130 m; c – zircon crystal with irregular patchy texture, granite B1, depth 228 m; d – shady zoned zircon crystal with patchy
texture, granite B
’2, depth 573 m; e – well zoned zircon crystal with 4 Hf-rich and 3 U-rich metamictized zones, granite B’2, depth
637 m; f – complex zircon crystal with patchy core, well zoned transition zone and patchy rim, granite B3, depth 858 m.
Fig. 5. Typical zircon crystal from the deeper part of the Beauvoir granite (depth of 583 m, unit B
’2): BSE-image (scale bar 20 µm) and
distribution of Hf in the outer part of the crystal, and U mainly in the core.
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from other types of granite, has
never been found. Zoning of sev-
eral crystals was studied by X-ray
mapping which showed that the
bright colour of rims, commonly
observable in BSE, is caused par-
ticularly by an increased content of
Hf (Fig. 5).
Chemical composition of zircon
Approximately 120 microprobe
analyses of zircon from Cínovec
and 90 from Beauvoir were per-
formed (Table 2; Figs. 6—8). Chem-
ical compositions of zircons from
both granite systems show distinct
vertical zoning, but their shape
and elemental speciation is highly
contrasting.
Hafnium
tends to accumulate in
both systems in their uppermost
highly fractionated parts. The in-
crease in Hf concentration can be
seen not only between individual
subsequent intrusions but also in
situ within one single intrusion.
Greater ability of Hf, compared
with Zr, to remain in the melt re-
sults in distinctly zonal structure of
late zircon crystals with Hf-rich
rims. At Cínovec the zircon crys-
tals from the most fractioned facies
of granite attain max. 8—10 wt. %.
The area of high Hf contents ex-
tends to a depth of ca. 100 m below
the surface. Zircon crystals from
Beauvoir are even more Hf-en-
riched. Concentrations of HfO
2
in
zircon from the uppermost part of
the Beauvoir stock increase from
8 wt. % in crystal core up to
19.3 wt. % (0.184 apfu Hf, Fig. 6)
in its marginal zones. The contents
of HfO
2
in deeper parts of both plu-
tons only rarely exceed 5 wt. %.
Uranium
: contents of U range
mostly between 0—2 wt. % UO
2
,
but concentrations of up to 4 %
weight are relatively frequent at
both localities, at Cínovec may
occasionally reach as much as ap-
proximately 6 wt. % UO
2
. The
vertical distribution of U in zircon
was found to be random (Fig. 6).
At Cínovec the higher contents of
uranium were detected in the up-
per parts of both types of granite,
at depth levels of 0—200 m and
Fig. 6. Vertical distribution of selected chemical elements in zircon: Hf, U, Th, Y, Dy, Yb, Sc, Bi.
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Table 2: Representative electron-microprobe analyses (wt. %) and structural formula (apfu) of zircon from Cínovec (ZiG, PrG) and Beauvoir
(B1, B2, B
’2, B3).
0.0 = below detection limit.
Unit ZiG
ZiG ZiG ZiG
PrG
PrG
PrG B1 B1 B2 B2 B´2 B´2 B3 B3
Depth (m)
24 97 413 559 860 988 1580 107 228 396 522 600 657 858 858
Sample
4672 4683 4687 4688 4802 4692 4693 3059B 3061 3062 3063 3066 3067 3069 3069
SO
3
0.00 0.01 0.01 0.03 0.02 0.01 0.01 0.04 0.03 0.02 0.33 0.04 0.04 0.01 0.02
P
2
O
5
2.48 2.72 0.44 1.10 0.61 0.38 0.22 0.29 5.97 0.30 7.35 0.21 4.50 0.02 1.95
As
2
O
5
0.76 0.33 1.09 1.30 0.17 0.20 0.07 0.56 0.22 0.20 0.06 0.09 0.07 0.11 0.29
SiO
2
23.26 24.04 25.46 24.76 29.95 29.76 30.65 30.60 23.31 31.15 19.11 29.92 20.93 32.02 26.49
Al
2
O
3
0.60 0.57 0.83 0.75 0.22 0.16 0.13 0.02 1.41 0.04 1.23 0.10 2.64 0.02 0.67
WO
3
0.03 0.47 0.64 0.67 0.03 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.02 0.00 0.00
Nb
2
O
5
0.84 0.89 0.45 0.39 0.01 0.00 0.00 0.00 0.02 0.00 0.00 0.00 0.00 0.00 0.00
Ta
2
O
5
0.00 0.22 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00
TiO
2
0.02 0.02 0.03 0.03 0.02 0.01 0.00 0.02 0.05 0.00 0.00 0.00 0.05 0.00 0.02
ZrO
2
39.54 40.98 44.24 45.12 54.30 59.84 61.25 48.16 53.37 60.29 46.75 57.93 51.74 62.94 55.32
HfO
2
10.27 3.53 2.01 3.18 2.42 2.80 1.74 19.15 4.82 6.78 2.15 2.66 2.69 4.39 2.84
ThO
2
2.19 1.86 1.63 0.51 0.14 0.23 0.27 0.34 0.06 0.03 0.07 0.00 0.01 0.03 0.03
UO
2
3.46 2.19 7.00 1.35 3.37 0.54 1.03 0.12 0.74 0.14 9.69 4.62 4.25 0.17 2.11
Sc
2
O
3
1.27 0.86 0.30 0.80 0.08 0.04 0.01 0.00 0.04 0.00 0.02 0.02 0.06 0.01 0.03
Y
2
O
3
3.27 4.41 2.67 3.89 1.08 1.07 0.33 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00
La
2
O
3
0.00 0.00 0.00 0.03 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.00 0.03
Ce
2
O
3
0.20 0.37 0.34 0.52 0.05 0.02 0.02 0.00 0.03 0.00 0.00 0.00 0.00 0.02 0.00
Pr
2
O
3
0.00 0.06 0.02 0.00 0.02 0.10 0.00 0.00 0.00 0.00 0.07 0.00 0.00 0.00 0.00
Nd
2
O
3
0.00 0.05 0.03 0.07 0.04 0.01 0.00 0.05 0.00 0.03 0.03 0.00 0.00 0.00 0.06
Sm
2
O
3
0.11 0.13 0.00 0.01 0.02 0.02 0.00 0.00 0.03 0.00 0.00 0.00 0.02 0.00 0.00
Gd
2
O
3
0.22 0.25 0.02 0.11 0.00 0.00 0.01 0.00 0.00 0.02 0.00 0.00 0.02 0.00 0.00
Dy
2
O
3
0.76 1.48 0.34 0.89 0.21 0.22 0.13 0.02 0.19 0.00 0.16 0.04 0.17 0.03 0.21
Er
2
O
3
0.72 1.41 0.64 0.92 0.26 0.20 0.05 0.18 0.03 0.03 0.02 0.02 0.00 0.05 0.01
Yb
2
O
3
1.47 4.46 1.99 2.97 0.86 0.32 0.15 0.00 0.00 0.06 0.00 0.00 0.02 0.04 0.00
Bi
2
O
3
0.09 0.46 0.06 0.93 0.11 0.05 0.10 0.07 0.05 0.01 0.09 0.06 0.10 0.10 0.01
MnO
0.08 0.09 0.14 0.80 0.25 0.16 0.33 0.01 0.74 0.07 0.57 0.06 0.45 0.02 0.98
FeO
1.19 0.19 0.50 1.13 0.38 1.12 0.23 0.04 0.45 0.00 0.30 0.06 0.28 0.05 1.52
CaO
1.18 0.87 1.73 1.93 0.61 0.44 0.48 0.05 2.36 0.12 2.83 0.10 2.27 0.02 0.59
MgO
0.00 0.01 0.01 0.00 0.03 0.01 0.01 0.00 0.14 0.02 0.17 0.01 0.30 0.00 0.03
PbO
0.00 0.00 0.04 0.02 0.01 0.03 0.10 0.00 0.01 0.02 0.00 0.21 0.02 0.03 0.04
F
2.39 2.09 0.50 0.66 0.33 0.16 0.09 0.00 0.97 0.00 1.09 0.31 1.97 0.00 0.85
Total
96.37 95.09 93.17
94.87 95.60 97.91 97.41 99.75 95.04 99.35 92.02 96.43 92.60 100.07 94.12
S
0.000 0.000 0.000 0.001 0.000 0.000 0.000 0.001 0.001 0.000 0.009 0.001 0.001 0.000 0.000
P
0.076 0.084 0.014 0.033 0.017 0.010 0.006 0.008 0.167 0.008 0.222 0.006 0.134 0.001 0.056
As
0.014 0.006 0.021 0.024 0.003 0.003 0.001 0.010 0.004 0.003 0.001 0.002 0.001 0.002 0.005
Si
0.845 0.873 0.925 0.877 0.993 0.959 0.981 1.011 0.769 0.986 0.681 0.988 0.735 0.997 0.896
Al
0.026 0.024 0.036 0.031 0.009 0.006 0.005 0.001 0.055 0.001 0.052 0.004 0.109 0.001 0.027
B-site
0.961 0.987 0.996 0.966 1.022 0.978 0.993 1.031 0.996 0.998 0.965 1.001 0.980 1.001 0.984
W
0.000 0.004 0.006 0.006 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000
Nb
0.014 0.015 0.007 0.006 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000
Ta
0.000 0.002 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000
Ti
0.000 0.000 0.001 0.001 0.000 0.000 0.000 0.000 0.001 0.000 0.000 0.000 0.001 0.000 0.001
Zr
0.701 0.726 0.784 0.780 0.878 0.940 0.956 0.776 0.858 0.931 0.813 0.933 0.886 0.956 0.913
Hf
0.107 0.037 0.021 0.032 0.023 0.026 0.016 0.181 0.045 0.061 0.022 0.025 0.027 0.039 0.027
Th
0.018 0.015 0.013 0.004 0.001 0.002 0.002 0.003 0.000 0.000 0.001 0.000 0.000 0.000 0.000
U
0.028 0.018 0.057 0.011 0.025 0.004 0.007 0.001 0.005 0.001 0.077 0.034 0.033 0.001 0.016
Sc
0.040 0.027 0.010 0.025 0.002 0.001 0.000 0.000 0.001 0.000 0.001 0.001 0.002 0.000 0.001
Y
0.063 0.085 0.052 0.073 0.019 0.018 0.006 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000
La
0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000
Ce
0.003 0.005 0.005 0.007 0.001 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000
Pr
0.000 0.001 0.000 0.000 0.000 0.001 0.000 0.000 0.000 0.000 0.001 0.000 0.000 0.000 0.000
Nd
0.000 0.001 0.000 0.001 0.000 0.000 0.000 0.001 0.000 0.000 0.000 0.000 0.000 0.000 0.001
Sm
0.001 0.002 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000
Gd
0.003 0.003 0.000 0.001 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000
Dy
0.009 0.017 0.004 0.010 0.002 0.002 0.001 0.000 0.002 0.000 0.002 0.000 0.002 0.000 0.002
Er
0.008 0.016 0.007 0.010 0.003 0.002 0.001 0.002 0.000 0.000 0.000 0.000 0.000 0.000 0.000
Yb
0.016 0.049 0.022 0.032 0.009 0.003 0.001 0.000 0.000 0.001 0.000 0.000 0.000 0.000 0.000
Bi
0.001 0.004 0.001 0.008 0.001 0.000 0.001 0.001 0.000 0.000 0.001 0.001 0.001 0.001 0.000
Mn
0.002 0.003 0.004 0.024 0.007 0.004 0.009 0.000 0.021 0.002 0.017 0.002 0.013 0.001 0.028
Fe
0.036 0.006 0.015 0.034 0.011 0.030 0.006 0.001 0.012 0.000 0.009 0.002 0.008 0.001 0.043
Ca
0.046 0.034 0.067 0.073 0.021 0.015 0.016 0.002 0.083 0.004 0.108 0.003 0.085 0.001 0.021
Mg
0.000 0.001 0.001 0.000 0.001 0.000 0.000 0.000 0.007 0.001 0.009 0.000 0.016 0.000 0.001
Pb
0.000 0.000 0.000 0.000 0.000 0.000 0.001 0.000 0.000 0.000 0.000 0.002 0.000 0.000 0.000
A-site
1.096 1.071 1.077 1.138 1.004 1.048 1.023 0.968 1.035 1.001 1.061 1.003 1.074 1.000 1.054
F
0.274 0.240 0.058 0.074 0.034 0.016 0.009 0.000 0.101 0.000 0.123 0.032 0.219 0.000 0.091
Zr/Hf at. 6.6
19.8
37.6
24.2
38.4
36.5
60.1
4.3
18.9
15.2
37.2
37.2
32.9
24.5
33.3
Zr/Hf wt. 4.4
13.3
25.2
16.3
25.7
24.5
40.3
2.9
12.7
10.2
24.9
24.9
22.0
16.4
22.3
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740—800 m, while at the Beauvoir locality the highest values
were detected in B2 and B
’2 units at a depth of 550—650 m.
Thorium
: it is one of the elements for which the concents
differ most in the two plutons studied (Fig. 6). In the upper
part of zinnwaldite granite in Cínovec, to a depth of 200 m,
Th-content in zircon commonly reach 1—5 wt. % (max.
8 wt. %) but in deeper parts of the pluton fluctuate only
around 0.5 wt. % ThO
2
. Contents of Th in the Beauvoir plu-
ton are almost always lower than 0.05 wt. % ThO
2
, and only
in B1 unit sporadically exceed 0.1 wt. % ThO
2
.
Yttrium
: it is another element behaving differently at both
localities (Fig. 6). At Cínovec the contents of Y
2
O
3
in zir-
cons are generally high, fluctuating in zinnwaldite granite
mostly between 0.3—5 wt. %, in the upper part of pro-
tolithionite granite, they range mostly between 0.2—3 wt. %,
whereas in its deeper section only 0.1—1 wt. % Y
2
O
3
(but
here the zircon is associated with xenotime). Conversely,
contents of Y in zircon from Beauvoir are negligible (only
sporadically exceed 0.05 wt. % Y
2
O
3
).
HREE
: due to the dimensions of its crystal lattice, zircon
is able to absorb the heavy REE in particular (Figs. 6, 8). The
most abundant elements are Yb and Dy, the former element
correlates well with Y and its distribution at both localities is
similar as that of Y as far as attains its absolute contents (up
to 5 wt. % Yb
2
O
3
at Cínovec) and also regarding differences
in its vertical distribution. Dy at Cínovec behaves like Yb,
but its contents are ca. 3 times lower than those of Yb (max.
1.7 wt. % Dy
2
O
3
). Dy at Beauvoir compared to Y is markedly
enriched reaching 0.3 wt. % Dy
2
O
3
at a depth interval of
400—650 m (units B2 and B
’2). Anomalous enrichment of Dy
in relation to other REE is well demonstrated in the Dy/Yb
ratio the values of which range between 0.1 and 0.9 at
Cínovec, but between 4 and 9 at the above mentioned depth
interval in borehole GPF1. It is to be pointed out, that chon-
dritic Dy/Yb ratio is 1.15.
LREE
: contents of light REE in zircon are commonly low
(Fig. 8), usually near the detection limits of the microprobe.
When comparing both localities studied, the LREE-contents
are slightly higher in Cínovec (0.2—0.7 wt. % Ce
2
O
3
and
0.1—0.20 wt. % Nd
2
O
3
).
Scandium
: it is another element exhibiting significantly
higher concentrations in zircon from Cínovec (Fig. 6). The
contents of Sc
2
O
3
reach 0.6—1.5 wt. % in the upper 100 m
thick section of lepidolite and zinnwaldite granite, but its
contents decrease randomly with depth. Contents of Sc in
protolithionite granite at Cínovec and in all types of granite
at Beauvoir are markedly lower, mostly not exceeding
0.1 wt. % Sc
2
O
3
.
Bismuth
: it is a characteristic trace element occurring in a
number of European Variscan tin-bearing granites. While
some zircons from the upper section of zinnwaldite granite
(from a depth of 50—100 m) at Cínovec contain as much as
1.0—1.2 wt. % Bi
2
O
3
, zircons from Beauvoir usually contain
only around 0.05—0.10 wt. % Bi
2
O
3
, (Fig. 6).
Phosphorus
: it is a common minor element incorporated in
zircon (Fig. 7). At Cínovec, contents up to 4 wt. % P
2
O
5
were
detected in the upper 200 m of the granite copula. However,
with increasing depth the concentration of P only rarely ex-
ceeds 1 wt. % P
2
O
5
. Although the Beauvoir granite system is
strongly P-enriched, zircons from the uppermost B1 unit in
Beauvoir contain only 0.5—1 wt. % P
2
O
5
; higher contents up
to 8 wt. % P
2
O
5
were found only scarcely. In the deeper units
B2 and B
’2 at a depth interval of 500—700 m the contents of
5—8 wt. % P
2
O
5
were often found more frequently.
Arsenic
: it is only rarely analysed in zircon, although it is
likely to be a relatively common minor or trace element
bound in this mineral. Arsenic at Cínovec appears to be more
abundant when its contents of 0.2—1.0 (max. 1.6) wt. %
As
2
O
3
were detected to a depth of 1000 m, but at greater
depths its concentration again decreases to 0.1 wt. % As
2
O
3
(Fig. 7). Zircons from the Beauvoir locality contain mostly
0.1—0.2 wt. % As
2
O
3
and close to the upper granite contact
as much as 0.8 wt. % As
2
O
3
.
Fluorine
: it is a substantial component of fractionated gran-
ite magmas and at the end of crystallization it enters crystal
lattice of numerous silicates where it replaces oxygen or OH
radical. High contents of fluorine in zircons from Cínovec
were established to a depth of ca. 200 m (1.0—2.5 wt. % F,
Fig. 7), and then gradually decrease to 0.0—0.2 wt. % F at a
depth of 1600 m. At the Beauvoir locality the highest concen-
trations of F in zircon, similar to phosphorus, were detected in
lower sections of borehole GPF-1 with a maximum of
1.5 wt. % F at a depth interval of 500—700 m. Zircons in the
uppermost section of the borehole contain surprisingly only
0.0—0.8 wt. % F.
Niobium, tantalum and tungsten
: these elements form in
granites individual minerals such as columbite/tantalite and
wolframite but they also enter the crystal lattice of zircon.
Tungsten and niobium were commonly detected in zircons
from Cínovec to a depth of ca. 800 m (up to 1 wt. % WO
3
and
1.3 wt. % Nb
2
O
5
). Tantalum was found only rarely in contents
of 0.1—0.4 wt. % Ta
2
O
5
. Contents of all three elements at
depths below 800 m are below their detection limits. Their
concentrations at the Beauvoir locality are markedly lower: Ta
and W always below their detection limits, Nb was detected
only in one sample from a depth of 573 m (top of the B
’2
unit) showing a content of 0.1—0.8 wt. % Nb
2
O
5
.
Titanium
: its contents at both localities are low and its
distribution similar: 0.0—0.06 (up to 0.1) wt. % TiO
2
and
tends to decrease with depth.
Lead
: contents of this element at both localities are low,
mostly below the detection limit, only rarely exceeding
0.1 wt. % PbO with no signs of any vertical zoning. No cor-
relation exists between U and Pb or between (Th + U) and Pb
either. If all lead in zircon is considered to be of radiogenic
origin then a substantial part of it in the studied zircons must
have been leached out.
Sulphur
: was detected in measurable amount only in zir-
cons from the uppermost section of the Cínovec granite copula
to a maximum depth of 80 m (0.5—4 wt. % SO
3
).
Aluminum
: contents of Al at Cínovec range between 0.0
and 1.2 wt. % Al
2
O
3
and tend to decrease gently with depth.
At Beauvoir the highest concentrations (1—3 wt. % Al
2
O
3
)
were found at a depth interval of 500—700 m. Its contents
both upward and downward are slightly lower (Fig. 7).
Iron, manganese, calcium and magnesium
: iron in zircons
from both localities shows contents of 0—1.5 wt. % FeO re-
gardless of the depth which the samples were collected from.
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Manganese was found to be more abundant at the Beauvoir locality (up to
1.5 wt. % MnO) relative to the Cínovec locality (max. 0.8 wt. % MnO).
The highest contents of this element were detected in zircons from medi-
um depths of 400—800 m. Calcium is also more abundant at Beauvoir (up
to 3 wt. % CaO) than in zircons from Cínovec (max. 2 wt. % CaO). The
highest concentrations of Ca, similar to Mn, were detected in zircons from
medium depths. On the contrary, the contents of Mg differ significantly:
while at Cínovec they do not exceed 0.07 wt. % MgO, at Beauvoir they at-
tain 0.5 wt. % MgO in the middle section of borehole GPF-1. Divalent ele-
ments Ca, Mg, Fe and Mn, due to their ionic radii, are unsuitable to enter
the crystal lattice of zircon. Elevated Ca-, Fe-, Mn- and Mg- contents were
found mainly in metamict areas of analysed zircon grains, we suppose that
these elements were incorporated in zircon after its metamictization.
Associated U, Th, Y, REE-minerals
Xenotime-(Y) was found to be the major host for Y and HREE in the
granites from Cínovec. In the zinnwaldite granite, this mineral is abun-
dant. It forms homogeneous subhedral crystals with a maximum size of
10 µm. Whenever this mineral is in direct contact with zircon, xenotime-(Y)
is always younger. Thin coatings of xenotime-(Y) enveloping whole zir-
con grains were observed in deeper parts of the zinnwaldite granite.
A substantial proportion of Y and HREE is located in the primary mag-
matic fluorite. Thorite is rather sporadic in the zinnwaldite granite, but
secondary minerals of the bastnäsite group containing Th, U and REE
are abundant and mostly occur in contact with fluorite.
Thorite and xenotime-(Y) are relatively abundant accessories in the
Cínovec protolithionite granite, occurring together with zircon as inclu-
sions in mica, but monazite-(Ce) is rare. Zircon was not found in direct
contact with these minerals so it is difficult or impossible to establish
their relative age of crystallization in relation to zircon. Neither uraninite
nor coffinite was identified at the Cínovec locality. Uranium at Cínovec,
apart from zircon, is bound in minerals of the bastnäsite group, which
crystallized at the later stages of granite evolution.
Separate REE, Y and Th minerals were not found in either of the types
of granite at Beauvoir because contents of these elements are generally
low (Cuney et al. 1992; Raimbault et al. 1995). Rossi et al. (1987) de-
scribed only scarce uraninite in some samples from a depth exceeding
475 m (deeper part of unit B2, and units B3, B
’2, B’3).
Discussion
Aluminum and divalent elements in zircon, metamictization and hydra-
tion, low totals of analyses
The position of Al, Ca, Fe, Mn and Mg in the zircon structure can be
explained in two ways: (i) by primary incorporation of these elements in
the lattice sites to compensate the substitution of Nb, Ta, and W for Zr
and/or substitution of P and As for Si, (ii) through secondary entry of
these elements into metamictized parts of zircon crystal lattice in the fluids
responsible for alteration.
Geisler et al. (2002, 2003) and Schmidt et al. (2006) demonstrated that
there is significant removal of Si, Zr, U, Th, Pb and uptake of Al, Mg and
Ca due to the interaction of chloride-bearing fluids with metamict zircon.
This means that the present chemical composition of porous metamictized
Fig. 7. Vertical distribution of selected chemical elements in zircon: P, As, F, Al.
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cores in zircons may be quite different from those produced by
crystallization from the initial magma. Moreover, the reaction
of zircon with fluids accelerates the restoration (annealing) of
the lattice structure in amorphized domains (Geisler et al.
2003). Nevertheless, rational evaluation of the primary and
secondary contents of Al, Ca, Fe, Mn and Mg remains prob-
lematic. For instance, Geisler & Schneider (2000) consider
contents of CaO exceeding 2 wt. % to be strongly indicative for
post- metamictization chemical changes in zircon. Ca-enriched
zircons from Cínovec usually show to high occupancy of the
A-site (Table 2), which is a strong argument for late, post-
metamict input of Ca. Nyman et al. (1984) and Crichton et al.
(2005) found similarities in structures of CaSO
4
, CePO
4
and
ZrSiO
4
and proposed so-called clinoanhydrite substitution
(Ca
2+
+ S
6+
REE
3+
+ P
5+
) as a possible way to incorporate
Ca into monazite lattice. In Cínovec, occasionally 1—4 wt. %
SO
3
was found, but there is no correlation between Ca and S.
So, in the case of the studied zircons, existence of the
(Ca
2+
+ S
6+
Zr
4+
+ S i
4+
)-substitution is unlikely. On the other
hand, the Al bound in tetrahedral position according to berlin-
ite substitution (Al
3+
+ P
5+
Si
4+
+ S i
4+
) is believed to by pri-
mary magmatic (Breiter et al. 2006).
Analytical totals for zircon obtained using EMPA are of-
ten significantly lower than 100 wt. %. The deficit in the
analyses is commonly interpreted as being due to the OH ion
in the mineral structure or to molecular H
2
O in the amor-
phous domains of the metamict zircon structure. This is only
partly true because a substantial part of the missing matter
may be accounted for other elements that were not analysed.
For instance, As, Bi, Nb and Ta, that are analysed only spo-
radically, may constitute as much as a several wt. % of zir-
con. The direct determination of the water content in zircon
is rare but analyses do exist. For instance, Nasdala et al.
(2009) found up to 8.8 wt. % H
2
O in Archaean zircon from
Jack Hills, Australia. Caruba & Baumer (1985) synthetised
zircon with as much as 0.8 apfu (OH,F)
4
replacing the (SiO
4
)
group in the structure of the mineral. These authors predict
that hydration takes place only in tetrahedral sites (SiO
4
)
without affecting the occupancy of the Zr position.
Remarkable contents of As (Breiter et al. 2009; Förster et
al. 2011) and Bi (Breiter et al. 2006, 2009) reported recently
from granitic zircons from Krušné Hory/Erzgebirge are sup-
posed to be a product of high-temperature hydrothermal
overprinting taking place shortly after granite crystallization,
and so prior to metamictization.
High contents of fluorine in many zircon grains from
Beauvoir and Cínovec correlate with enhanced content of U,
thus with grade of metamictization. Contents > 0 .5 wt. % F in
Beauvoir and > 1 .5 wt. % F in Cínovec were found mainly in
zircons with > 2 wt. % UO
2
. On the other hand, there is no
correlation between F and Hf: the Hf-enriched rims of zircon
crystals crystallizing from residual F-rich melt are actually
poor in F. In that case, strong enrichment of F in some zircons
should be interpreted as results of reaction of late F-enriched
fluids with U-rich parts (dominantly cores) of some zircon
grains. Enrichments of W, Nb, Ta and Sc in zircons from
Cínovec correlated well with enrichment of F. Thus, entry of
all these elements in the zircon structure may also be better ex-
plained via reaction of zircon with high-temperature F- and
metal-rich fluids after granite solidification. All fractionated
granites in the Erzgebirge intruded at a very shallow subvolca-
nic level and were fast cooled after intrusion (Jarchovský &
Pavlů 1991; Seltmann & Schilka 1991; Breiter et al. 1999,
2005). Thus, the question of whether the short-lived high-tem-
perature hydrothermal fluids reacted with still fully-ordered or
already metamictized zircons, remains unresolved.
Taken together, high contents of Hf, U, Th, Y and REE in
studied zircons are probably primary magmatic and mirror
high grade of fractionation of evolved granitic melt, while
unusually high contents of F, As, W, Nb, Ta, Ca, Fe and Mg
resulted from later hydrothermal overprint. In the case of
phosphorus and alumina, P in xenotime substitution and
P + Al in berlinite substitution are primary magmatic in ori-
gin. The additional P in pretulite and ximengite substitution
(Breiter et al. 2006) and the additional Al are very probably
of secondary hydrothermal origin.
Comparison between the studied zircons and whole-rock
chemical composition
The differences in the geochemical character of the granites
from Beauvoir and Cínovec enables conclusions to be drawn
about which features of the chemistry of the zircons inves-
tigated are governed by the type of granite magma involved
(S- or A-type) and which resulted because of the high degree
of fractionation of residual melt regardless of the magma type.
Strongly fractionated rare metal-bearing granites and peg-
matites are in general enriched with F, Li, Rb, Sn, W, Nb and
Ta, but differ markedly in contents of Zr, Th, REE and Y.
The A-type granites are Zr, Th, REE, Y-rich, while granites
of S-type are poor in these elements. Similarly, pegmatites
are classified as LCT-type (strongly peraluminous, enriched
with Li, Cs, Ta, Rb, P, Ga, etc.) and NYF-type (enriched
with Nb, Y, F, REE, Sc, Zr, U, Th, etc., Černý & Ercit
2005). Zircon from fractionated and F-rich granites was of-
ten found to contain high concentrations of minor and trace
elements. A high content of complex-forming fluorine in
particular, and also high concentrations of sodium in the
magma are reported to enable the entry of “exotic” elements
into the crystal lattice of zircon (Kempe et al. 2004). Al-
though many authors (cf. Raimbault et al. (1995) and refer-
ences therein) pointed out the high activity of F-rich fluids in
Beauvoir, the zircons from Beauvoir are nearly pure stoichio-
metric (Zr,Hf)SiO
4
. In contrast, at Cínovec, zircon absorbed
not only “common” minor and trace elements such as Y,
HREE, U and Th, from the melt, but also contains significant
amounts of “exotic” elements like W, Nb, Ta, Sc, Bi, As. For
example, the content of W in granites from Beauvoir is about
40 ppm, while in Cínovec the content is about 20 ppm. Zir-
cons from Cínovec generally contain 0.5—1.0 wt. % WO
3
,
while zircons from Beauvoir are W-free. The content of Nb
in granites from both localities is similar, ca. 100—150 ppm,
but zircon from Cínovec contains about 0.5 (up to 2) wt. %
Nb
2
O
5
, whereas zircon from Beauvoir is Nb-free. Entry of
elements like Sc, Bi, Nb, Ta, and W into the structure of zir-
con from Cínovec are thought not to be due to the specific
type of melt (A-type vs. S-type), while zircons from some
fractionated S-type granites from the Erzgebirge are also Nb,
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Ta, W, Bi, Sc-enriched (cf. Breiter et al. 2006). Concentra-
tions of Ta in zircon crystallizing from Li-rich pegmatite
melt may be occasionally as high as 4.7 wt. % Ta
2
O
5
(Van
Lichtervelde et al. 2009); contents of Nb are usually much
lower (Van Lichtervelde et al. 2011).
High contents of Th, Y and HREE in zircon from Cínovec
and very low contents of all these elements in zircon from
Beauvoir correlate well with concentrations of these elements
in all granite varieties from both localities (10—60 ppm Th,
7—114 ppm Y and 4—16 ppm Yb in Cínovec, < 1 ppm Th,
< 10 ppm Y, < 0 .05 ppm Yb in Beauvoir).
At Beauvoir, high contents of U, P and F in zircons from the
interval 500 to 700 m deep do not correlate with the chemical
composition of the whole-rock. Contents of F in granite at a
depth of about 520 m decrease from 2.0 to 1.6 wt. %, while
contents of P
2
O
5
below the depth of 550 m decrease from 1.3
to 0.8 wt. %. Contents of U are stable at around 15 ppm. En-
richment of zircon with U, P and F is believed to have resulted
from intensive mineral-fluid reactions taking place in the B2
and B
’2 granite units in the interval from 500 to 700 m deep
(compare also Raimbault et al. 1995). It is also worth men-
tioning that high contents of U are found in the cores of zircon
crystals from both Beauvoir and Cínovec, while their outer
zones and rims are poor in uranium. Consequently, uranium is
thought to have entered the zircon structure particularly at
higher temperature at the beginning of its crystallization. Dur-
ing the final stages of crystallization uranium preferentially
entered the minerals of the bastnäsite group crystallizing from
water-saturated melt or aqueous fluids.
The content of any trace element in crystallizing mineral is
theoretically determined by its concentration in the melt and
by partition coefficient Kd
mineral/melt
for the given trace ele-
ment. Partition coefficients Kd
mineral/melt
for zircon were es-
tablished experimentally (Thomas et al. 2002; Luo & Ayers
2009) or by comparison of their contents in zircon and in
bulk rock (de Liz et al. 2009; Nardi et al. 2012), zircon and
surrounding glass (Sano et al. 2002) or zircon and surround-
ing leucosome (Bea et al. 1994). However, results obtained
and referred by the above-mentioned authors differ signifi-
cantly (Table 3). The reason for such large differences in the
determination of Kd lie only partly in analytical inaccuracies
when establishing low contents of the given trace elements.
Different composition of the parent rock melt is considered
to play a fundamental role in distribution of trace elements in
zircon, specifically its peraluminity or otherwise its peralka-
linity, the content of water, fluorine and other fluxing agents.
Temperature and pressure are also believed to affect the par-
tition coefficient. Moreover, the relative older zircons (or
their cores) crystallized from parental melt, while their rims
and the late, interstitial zircons in the whole crystallized
from residual melt; nevertheless the chemical composition
(trace-element content) of parental and residual melt differ
substantially. In such complex cases, the determination of
real Kd
zircon/melt
is impossible. Therefore, we at least deter-
mined empirical enrichment factors (hereafter Ef) of zircon/
whole rock for elements of which concentrations in zircon
from Cínovec and Beauvoir could be established with suffi-
cient accuracy (Table 3). Contents of Y, HREE and Th in
whole-rock samples of granites from Cínovec correlate well
with the content of Zr which indicates that the Th/Zr, Y/Zr
and HREE/Zr ratios in the melt were stable during the major
part of fractionation. In spite of this, the enrichment factor
for all the above-mentioned elements and also for Ce and Nb
was found to be higher in more differentiated zinnwaldite
granite than in protolithionite granite. The Ef values deter-
mined by us are also higher than the Kd established by the
above-mentioned authors in less differentiated granites.
As emerges from the comparison of Kd and Ef shown in Ta-
ble 3, both coefficients for all the studied elements in slightly
to strongly peraluminous rocks are higher than those in alka-
line rocks. In this context the occurrence of solid solutions zir-
con-xenotime and zircon-thorite found at some localities in
the Krušné hory/Erzgebirge area (Förster 2006; Breiter et al.
2009; Förster et al. 2011) indicates that zircon under specific
conditions of fractionated melts rich in water and F is able to
absorb by order of magnitude higher contents of Th, U, Y,
HREE, than would correspond to Kd coefficients established
in granitoids of “common” composition. In the case of enrich-
ment of some zircons in Nb, Ta, Sc and Bi, the ratio between
the primary magmatic and secondary fluid-induced portion of
particular element remain unresolved.
Based on the above-mentioned analyses and consider-
ations the zircons from strongly differentiated granites and
pegmatites can be divided into two basic types:
1. zircons strongly enriched with Hf ( > 10 wt. % HfO
2
,
(particularly in rims), and poor in all other HFS-elements.
This type was reported from some Europen Variscan strongly
peraluminous granites (Beauvoir and Argemela/Portugal
(Breiter & Škoda 2010)), LCT pegmatites (Tanco/Canada
(Van Lichtervelde et al. 2009), Chedeville/France (Raimbault
1998)), but also from some A-type granites (Suzhou, China
(Wang et al. 1996));
Source
Remark
Ce Dy Yb Y Nb U Th
Bea et al. 1994
peraluminous leucosome
2.04
38.8
278
71.4
354
22.1
Sano et al. 2002
melt of dacite glass
0.36
45.9
277
Thomas et al. 2002 melt inclusions in zircon from tonalite 0.43–2.06
12.4–73
14–97
2.4–191
204–312
Luo & Ayres 2009 melt of peralkaline rhyolite
0.14–3.3
11–83
6.8–66
2.1–32
2–18
de Liz et al. 2009
shoshonitic rocks
1.6–3.0
29–64
150–544
54–114
0.2–3.6
71–168
14–19
Nardi et al. 2012
peralkaline A-type granites
1.5
73
307
106
2.1
168
23
this work
Cínovec protolithionite granite
1–10
49–147
118–914
43–158
<10
192–742
32–106
this work
Cínovec zinnwaldite granite
9–144
140–3451 595–6212 106–2694
13–66
307–2807 63–1412
this
work Beauvoir
270–1760
210–650
Table 3: Partition coefficient Kd
zircon/melt
from laboratory experiments (Sano et al. 2002; Thomas et al. 2002; Luo & Ayres 2009) and natural
granitoids (Bea et al. 1994; de Liz et al. 2009; Nardi et al. 2012) and empirical enrichment factors Ef
zircon/whole rock
calculated in this work.
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2. zircons moderately enriched with Hf ( < 10 wt. % HfO
2
),
as well as moderately to strongly enriched with Th, Y,
HREE, (Nb, Sc, Ta, Bi). This type is typical of the Krušné
hory/Erzgebirge area: A-type granites at Cínovec (Förster
2006) and Hora Svaté Kateřiny (Breiter et al. 2009), S-type
granites at Podlesí (Breiter et al. 2007). A similar type of zir-
con, but with lower absolute contents of Th, Y and REE, was
also described from peralkaline A-type granites in Eastern
China (Wang et al. 2000; Xie et al. 2005), peraluminous
granites from Spain (Pérez-Soba et al. 2007), granites and
pegmatites from Japan (Hoshino et al. 2010) and leucogran-
ites from Slovakia (Uher & Ondrejka 2009).
Consequently, it is evident that high contents of minor ele-
ments in zircon are not determined only by their concentra-
tions in the melt or by the type of melt as such or even by the
degree of its peraluminity and or alkalinity, and the degree of
melt fractionation, but other phenomena or parameters of the
crystallizing system seem to play a decisive role in this case.
For instance, the concentration of Li (up to 1 wt. % Li
2
O in
rocks with HFSE-poor zircon and only 0.1—0.2 wt. %. in
granites with HFSE-rich zircon) may play some role or the
pressure can also affect the process of crystallization. All
granites in the Krušné hory/Erzgebirge area containing
HFSE-rich zircons are of subvolcanic nature and underwent
explosive degasation and resurgent boiling followed by in-
tensive F-rich fluid percolation (Breiter et al. 2005).
Some authors (e.g. Kempe et al. 2000; Pettke et al. 2005;
Uher et al. 2009) argued for post-magmatic origin of the
HFSE- and- REE-enriched late zircons or rims of zoned zir-
con crystals. But in case of zircon from the Cínovec borehole
(this study) and similar A-type granites from the Krušné
hory/Erzgebirge Mts (Breiter et al. 2009; Förster et al. 2011),
during the fluid-related processes zircons are enriched in As,
P, and F, while released REEs form secondary minerals like
chernovite and bastnäsite.
Fractionation of HREE
Zircon preferentially concentrates HREE. Experiments car-
ried out by Hanchar et al. (2001) showed that zircon crystals
doped with REE + P displayed an increase of approximately
1000-fold in contents of REE from La through Lu as a result
of shrinking ionic radii. Of the LREE, zircon tends to selec-
tively accumulate Ce
4+
, which often results in a distinct posi-
tive Ce anomaly. Negative Eu anomalies are typical of zircon
from slightly to strongly peraluminous granites (cf. summary
in Hoskin & Schaltegger 2003), but absent in zircon from sub-
alkaline and shoshonitic rock (de Liz et al. 2009); relative con-
centration of Eu in zircon mimic those in the whole rock.
The distribution of HREE at Cínovec is homogeneous.
HREE are more abundant than LREE and there is a distinct
positive Ce-anomaly (Fig. 8). Granites from Cínovec are
characteristic of a distinct “tetrad effect” in chondrite-nor-
malized distribution of REE (Cocherie et al. 1991). Imprint
or transfer of tetrad effect from a melt into zircon has been
interpreted as a proof of late crystallization of this mineral
after separation of fluid phase from F-rich melt (Nardi et al.
2012). However, because of the applied analytical method
only contents of even-numbered elements (more abundant in
Fig. 8. Chondrite-normalized distribution of REE in zircons from
Cínovec (normalized according to McDonough & Sun 1995).
=
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nature) were established in zircon, it would be inappropriate
to comment the above-mentioned phenomenon.
Contents of REE in zircon from Beauvoir are very low,
usually near or below the detection limit of the microprobe.
Phosphorus in the zircon crystal lattice
Kimura & Hironaka (1936) first described zircon enriched
with P and Y, and Hata (1938) explained this as the result of
zircon-xenotime miscibility. Hanchar et al. (2001) experi-
mentally confirmed the tendency for zircon to accommodate
Y and REE in its lattice dominantly by the xenotime substi-
tution (YPO
4
ZrSiO
4
). This may explain the P-enrichment
in zircons from the generally P-poor, but Y, REE-enriched
A-type granites. In peraluminous P-rich and Y, HREE-poor
granites, the high P-contents can be explained by the berlin-
ite substitution Al + P
Si + Si (Breiter et al. 2006). In special
cases of Sc-enriched zircons, pretulite-type substitution
(Sc + P
Zr + Si) also plays a role (Breiter et al. 2006).
Among the zircons studied, the Beauvoir zircons are Y-free
and follow the berlinite substitution with P predominant over
Al, particularly in the B2 and B´2 units. Zircons from
Cínovec generally follow the xenotime substitution with sig-
nificant predominance of Y + REE over P (Fig. 9). Surpris-
ingly, the excess of Y + REE is greater in the deeper part of
the pluton relative to the upper section that was rich in fluo-
rine and fluids. The occurrence of trivalent elements in zir-
con from the uppermost part of the cupola must be explained
by another type of substitution. One possibility is the substi-
tution (Y,REE) + (Nb,Ta) Zr + Zr (Van Lichtervelde et al.
2011) or perhaps even the incorporation of lithium or other
small ions in interstitial positions apart from the main lattice
sites. Lithium is abundant in fractionated granites and its ion,
due to its small size, can enter a number of minerals not only
in the principal lattice sites but also in their interstices. Lithi-
um cannot be analysed using the electron probe so that data
on its content and distribution in mineral structures is spo-
radic. Ushikubo et al. (2008) found as much as 259 ppm Li
in zircons from granitoids, and suggested that the coupled
substitution (Y, REE) + Li
interstitial
Zr was responsible for
accommodation of trivalent ions in zircon crystal lattice.
Conclusions
The main results of the present study can be summarized
as follows:
The chemistry of zircons from the highly fractionated
S-type and A-type granites at Beauvoir and Cínovec differ
significantly from one another. Zircons from the A-type
granite at Cínovec are markedly enriched with Th, Y, REE
and Sc, while zircons from the S-type granite at Beauvoir are
more enriched with P and Hf;
A distinct vertical zoning of zircon compositions was
found in both granites with a tendency for the content of Hf
to increase at higher levels of the crystallizing system more
enriched with fluids;
High contents of uranium at both localities were always
detected in the cores of zircon crystals, while their rims are
enriched with Hf;
Enrichments of F and U in zircons at Cínovec correlate with
the concentration of these elements in the parent rock and in-
crease systematically upwards in the granite body. At Beauvoir,
these elements are mostly concentrated in the middle part of the
profile and show no correlation with their contents in the parent
rock. The chemistry of zircons at Beauvoir correlates more with
the initial vertical division of the system into B1, B2 and B3
units (Cuney et al. 1992) rather than the classification into B
and B
’units later proposed by Raimbault et al. (1995);
Zircons from highly differentiated granites can generally
be divided into two chemical types: (i) zircons strongly en-
riched with Hf ( > 10 wt. % HfO
2
, particularly in rims), and
poor in all other HFS-elements. These zircons are typical of
peraluminous strongly Li-enriched granites and LCT pegma-
tites, but also of some A-type granites; (ii) zircon moderately
enriched with Hf ( < 10 wt. % HfO
2
), as well as moderately
to strongly enriched with Th, Y, HREE, (Nb, Sc, Ta, Bi).
These zircons are characteristic of moderately Li-enriched
Fig. 9. Crystallochemical relations in zircon: a) correlation between P
and Y: zircon from the uppermost 100 m interval in Cínovec follows
xenotime-(Y) substitution (Y+P Z r+Si) with only small deficiency
of Y, while in zircon from the Cínovec deeper part yttrium markedly
prevails and is probably compensated byh Nb and Ta (Y+Nb Zr+Zr)
or by Li (Y + Li Zr). Zircon from Beauvoir is Y-free and phosphorus
enters the lattice mainly acc. to berlinite substitution (Al + P Si + Si);
b) taking into account all trivalent elements, there is clear deficiency
of P in all samples from Cínovec, and still overabundance of P in
Beauvoir.
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and strongly F-enriched subvolanic granites of both S- and
A-types of the Krušné hory/Erzgebirge area, but occasionally
were found in evolved S- and A-type granites and granitic
pegmatites worldwide.
High contents of minor elements in zircon are not directly
determined by their concentrations in the melt, but by combi-
nation of enrichment of the melt with water, Al, F, Na and
Li, and the pressure. High degree of peraluminity and high
content of Li seem to be favourable phenomena facilitating
crystallization of zircon rich in Hf, whereas subvolcanic con-
ditions of the intrusion linked with explosive degasation and
secondary boiling support the crystallization of zircon high in
Th, U, Y, REE, Nb and W. Influence of late- to post-magmatic
fluid-driven zircon alteration also play a role.
Acknowledgments: It is a very pleasant duty for the authors
to thank Louis Raimbault for providing the samples from
borehole GPF1 drilled at Beauvoir. Thanks are also due to
Zuzana Korbelová and Vlasta Böhmová (Laboratories of the
Geological Institute AS CR Praha) for technical assistance in
producing the excellent EBS photomicrographs used to illus-
trate our paper. Constructive reviews by J. Leichmann (Brno)
and P. Uher (Bratislava) helped to improve the manuscript
significantly. L.V.S. Nardi (Porto Alegre), I. Broska (Bra-
tislava) and J.F. Molina (Granada) are thanked for comments
on the older version of the manuscript. This study was made
possible thanks to the Czech Science Foundation – Projects
P210/10/1105 and P210/10/1309, and also to the Czech IGCP
Committee.
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