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Geological Society, London, Memoirs
doi: 10.1144/M37.15 2013, v.37; p491-510.Geological Society, London, Memoirs
A. Peccerillo, G. De Astis, D. Faraone, F. Forni and M. L. Frezzotti
petrogenesis and geodynamics
Chapter 15 Compositional variations of magmas in the Aeolian arc: implications for
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Chapter 15
Compositional variations of magmas in the Aeolian arc: implications for
petrogenesis and geodynamics
A. PECCERILLO1*, G. DE ASTIS2, D. FARAONE1, F. FORNI3& M. L. FREZZOTTI4
1
Dipartimento di Scienze della Terra, Universita
`di Perugia, Piazza Universita
`1, 06100 Perugia, Italy
2
INGV (Istituto Nazionale di Geofisica e Vulcanologia), Sezione di Sismologia e Tettonofisica,
Via di Vigna Murata 605, 00143 Roma, Italy
3
Dipartimento di Scienze Biologiche, Geologiche e Ambientali, Alma Mater Studiorum,
Universita
`di Bologna, Piazza Porta S.Donato 1, 40126 Bologna, Italy
4
Dipartimento di Scienze dell’Ambiente e del Territorio e di Scienze della Terra,
Universita
`di Milano – Bicocca, Piazza Della Scienza 4, 20126 Milano, Italy
*Corresponding author (e-mail: angelo.peccerillo@unipg.it)
Abstract: The volcanic rocks of the Aeolian arc exhibit important within-island and along-arc compositional variations that testify to
both geochemical heterogeneous mantle sources and different roles and intensities of shallow-level magmatic evolution processes. Calc-
alkaline magmas are present on all islands, but dominate in the western arc and at Lipari and Panarea. Shoshonitic rocks are present on the
central-eastern islands and are particularly abundant at Vulcano and Stromboli. Mafic and intermediate rocks comprise the bulk of older
volcanic sequences for most islands. Rhyolites are restricted to younger activity of the central arc, and become particularly abundant at
Lipari and Vulcano. Regional variations of incompatible trace element ratios and Sr-, Nd-, and Pb-isotope signatures in mafic-intermedi-
ate rocks document the variable composition of mantle sources, which were contaminated by different types of metasomatic fluids
released from an oceanic slab in the western-central sectors and from oceanic slab plus sediments in the east. This metasomatism
was superimposed over a heterogeneous mantle wedge, which had a mid-ocean-ridge basalt (MORB-) to ocean-island basalt (OIB)-
type character passing from the centre to the margins of the arc. The OIB-type component in the external arc is attributed to astheno-
spheric mantle inflow from the Africa foreland, around the borders of a narrow slab during rollback.
Aeolian arc magmatism (Fig. 15.1) exhibits strong within-island
and regional variations in elemental and isotopic compositions.
These are the integrated effects of a variety of different processes
that include heterogeneity of the mantle sources, variable physico-
chemical conditions during magma formation and complex geo-
chemical evolution during magma ascent to the surface (e.g.
Keller 1982; Francalanci et al. 1989, 2004, 2007; Peccerillo 2005).
Intra-crustal magma compositional evolution was the latest
process to occur and therefore left the best evidence in the petrolo-
gical and geochemical signatures of subaerial volcanic rocks. Much
more difficult to understand are the compositional characteristics
and conditions of melting within mantle wedge. This is generally
accomplished by studying the compositions of mafic magmas
erupted along the arc, based on the assumption that these are
reliable proxies of their mantle sources. However, it has been
demonstrated that complex evolution processes in the Aeolian arc
also affected mafic magmas which, in some cases, are more
heavily contaminated by wall rocks than the coexisting intermedi-
ate magmas (see Peccerillo & Wu 1992; Peccerillo et al. 1993,
2004; Santo et al. 2004; Lucchi et al. 2013a). This makes the under-
standing of source composition and evolution processes a parti-
cularly challenging problem, which is still a subject of debate.
This paper is a critical review of the petrology and geochemistry
of the Aeolian arc magmatism and of current ideas regarding the
origin and evolution of magmas, mantle source compositions
and their geodynamic significance. The paper consists of two
parts. The first part is based on literature data and summarizes
the volcanological and structural setting of the arc, describes the
first-order compositional variation of rocks in the single islands
and at the regional scale and discusses the nature and effects of
magma evolution processes. The second part deals with regional
variations of trace elements and radiogenic isotope compositions
of magmas and their mantle sources and discusses the most
popular hypotheses regarding mechanisms and effects of mantle
metasomatism, conditions of formation of shoshonitic and
calc-alkaline magmas and the geodynamic setting of the Aeolian
arc. Along-arc geochemical variations are examined based upon
new LAICPMS (Laser Ablation Inductively Coupled Plasma
Mass Spectrometry) trace element analyses for a large number of
representative samples from across the Aeolian arc. Intermediate
rocks are considered along with mafic rocks, since andesites
from some islands show the most primitive isotopic compositions
across the arc and therefore represent more reliable proxies of
mantle sources than mafic rocks. The new analyses provide an
internally consistent set of data that overcomes the problems of
inter-laboratory analytical bias, a main limitation of data in the lit-
erature. These data offer a better insight into fine-scale regional
geochemical zoning, thus providing a foundation for development
of a comprehensive model of the mantle source composition and
its geodynamic significance.
Structural, volcanological and petrological outlines
The Aeolian volcanism consists of seven main islands (Alicudi,
Filicudi, Salina, Lipari, Vulcano, Panarea and Stromboli) making
up a volcanic arc and several seamounts (Marsili, Eolo, Enarete,
Sisifo, Lametini, Alcione, and Palinuro). These have formed
around and inside the Masili basin (Fig. 15.1), a rapidly expand-
ing back-arc basin (Nicolosi et al. 2006) floored by basaltic
rocks and characterized by thin lithosphere and crust (Trua et al.
2004). The arc exhibits strong lateral variation of structural,
volcanological and petrological characteristics, which make the
Aeolian volcanoes an important case study for subduction-
related volcanism.
From:Lucchi, F., Peccerillo, A., Keller, J., Tranne,C.A.&Rossi, P. L. (eds) 2013. The Aeolian Islands Volcanoes. Geological Society, London, Memoirs, 37,
491–510. http://dx.doi.org/10.1144/M37.15 #The Geological Society of London 2013. Publishing disclaimer: www.geolsoc.org.uk/pub_ethics
Stuctural and volcanological setting
The Aeolian volcanoes are composite structures formed by the
superposition of multiple centres and recurrent volcanic and tec-
tonic events, with many sector and central collapses. Rocks
exposed above the sea level are younger than c. 270 ka (Gillot
1987; Leocat 2011). Vulcano and Stromboli are presently active,
but Lipari and Panarea have also erupted or demonstrated
intense submarine degassing during historical time. Of the sea-
mounts, Marsili and Palinuro are considered active. Marsili rises
for more than 3000 m over the sea floor of the Marsili basin, and
is the best studied among Aeolian seamounts (Trua et al. 2011).
The Aeolian islands are constructed upon the Calabro – Pelori-
tano basement, a block of the European continent which detached
from Sardinia– Corsica and migrated south-westwards during the
Miocene– Quaternary opening of the Tyrrhenian Sea. Crustal
thickness beneath the Aeolian arc is c. 15 – 25 km, and increases
westwards. The Aeolian arc is cut by a complex pattern of fault
systems (Ventura 2013). The NW – SE-trending Tindari –Leto-
janni Fault (TLF) is the most important tectonic lineament in the
area, running from the Salina – Lipari –Vulcano alignment to the
Malta escarpment (Fig. 15.1). In mainland Sicily, the TLF cuts
the Calabro– Peloritano basement near the boundary with the post-
Miocene accretionary prism and the Iblei continental block to the
west (Grasso 2001). It is likely that these geometric relationships
continue in the Aeolian arc. This implies that distinct types of base-
ment rocks are present across the Aeolian archipelago, that is, the
Calabro– Peloritano basement in the central-eastern sectors and
the accretionary prism rocks under the western islands. Such a
hypothesis is supported by the increase in crustal thickness west
of the Tindari– Letojanni Fault (Ventura 2013).
Traditionally, the Aeolian arc has been divided into three main
sectors – the western, the central and the eastern arcs – which are
characterized by first-order volcanological, magmatic and struc-
tural differences (Peccerillo 2005; Ventura 2013). The western
arc is formed by Alicudi and Filicudi, which are situated along
east– west- to WNW –ESE-striking fault systems. A NNW –SSE
compressive strain field due to the Africa – Eurasia convergence
is active in this sector (Ventura 2013). The central islands of
Vulcano and Lipari are located along the TLF, where a strike-slip
strain regime is active. Salina is sited at the intersection between
the east– west-trending structures of the western arc and the
Tindari– Letojanni Fault. Panarea and Stromboli are situated
along SW– NE-trending faults. An extensional tectonic regime
affects this sector of the arc.
Active volcanism occurs along the Tindari – Letojanni Fault and
east of this tectonic line. The compressive tectonic regime in the
western sector inhibits upraise and eruption of magmas, whereas
extensional and strike-slip strain regimes in the central-eastern
arc generate vertical faults that are pathways along which
magmas ascend and erupt at the surface (Ventura 2013).
Geophysical studies (e.g. Panza et al. 2003) indicate that deep
seismicity (up to 550 km) only occurs east of the Tindari – Leto-
janni Fault. This is a consequence of the Ionian slab subduction
beneath the Calabro – Peloritano basement and the southern Tyr-
rhenian Sea. Active Aeolian volcanism is therefore located
above or at the margin of the deep seismicity zone.
Magma compositions
Key geochemical data from the literature are shown in Figures
15.2– 15.6. The important information contained in these diagrams
can be summarized as follows.
(1) Calc-alkaline (CA) and high-K calc-alkaline (HKCA) rocks
occur throughout the arc but dominate at Alicudi, Filicudi,
Salina, Lipari and Panarea (Fig. 15.2). In contrast, shosho-
nites (SHO) are spatially restricted to the central-eastern
islands, where they generally appear during the mature to
late stage of volcanic activity. The Marsili seamount has a
CA basalt to basaltic andesite composition, with a few ande-
sites (Trua et al. 2011). A single sample has ocean-island
basalt (OIB)-type affinity and is not plotted in the diagrams.
The small number of analyses available for the other Aeo-
lian seamounts (not shown) indicates that rocks are predomi-
nantly of calc-alkaline mafic to intermediate composition,
with a few shoshonites (Eolo, Enarete) and arc tholeiites
(Marsili basin margin; Trua et al. 2004; Peccerillo 2005).
(2) The degree of magma evolution increases from the external
to the central islands; rhyolitic volcanism (SiO
2
.70%) is
present at Panarea and Salina, and becomes abundant at
Lipari and Vulcano (Fig. 15.2). Rhyolites characterize the
younger stages of activity for all these volcanoes.
(3) Abundances of elements that are incompatible with main
magmatic minerals (e.g. Th, U, Nb, Ta and Light Rare
Earth Elements - LREE) increase with silica for all the islands
and seamounts (Fig. 15.3). The exception observed is for
Ba, which decreases in the rhyolites of Vulcano and Lipari,
but not in the rhyolites of Salina and Panarea (Fig. 15.3d).
(4) Incompatible trace element (ITE) abundances increase from
CA to SHO volcanics for the mafic-intermediate compo-
sitions (Fig. 15.4). This is observed for both the large-ion
lithophile elements (LILE: Rb, Ba, La, Th, etc.) and for the
high-field-strength elements (HFSE: Nb, Ta, Hf, Zr).
However, there are several differences between islands.
These have important petrogenetic implications, and will
be discussed later (see “Isotope and trace element compo-
sition of mantle sources”).
(5) Incompatible element patterns normalized to primordial
mantle for basalts and basaltic andesites from the Aeolian
islands and Marsili seamount display the typical features of
arc volcanics worldwide, with enrichments in LILE and rela-
tive depletion in HFSE (Fig. 15.5). Most of these features are
also shown by the Calabro – Peloritano basement and the
Ionian Sea sediments (Fig. 15.5d). The Aeolian seamounts
(not shown) show similar patterns as the other Aeolian
rocks, with fractionation and abundances of ITE increasing
from CA to SHO rocks.
(6) Sr-isotope ratios of mafic – intermediate rocks increase from
the western island of Alicudi to the central and eastern
islands, reaching maximum values at Stromboli (Fig.
15.6a). Sr– Nd isotopic ratios display the well-known
Palinuro Smt.
Glauco Smt.
(Pliocene)
Eolo Smt.
Sisifo Smt.
Lametini Smt.
Tyrrhenian
Sea
Marsili
Smt.
MARSILI BASIN
Alicudi Filicudi
Stromboli
Panarea
Lipari
Vulcano
Sicily
Salina
AEOLIAN ARC
Calabria
Tyrrhenian
Sea
Alcione Smt.
Enarete Smt.
Fig. 15.1. Location map of Aeolian islands and seamounts. TLF is the Tindari –
Letojanni Fault system.
A. PECCERILLO ET AL.492
negative correlation. However, a slightly steeper slope
characterizes the western-central islands. Marsili shows a
large Sr– Nd isotope variation that overlaps the western-
central arc domain. Panarea has a variable Sr-Nd isotopic
composition, with CA rocks falling within the field of
western islands and SHO rocks plotting with Stromboli.
At Stromboli there is a considerable increase of Sr- and a
concomitant decrease of Nd-isotopic ratios from calc-alka-
line to shoshonitic rocks (Francalanci et al. 1988, 1989,
2013), which is not observed at Vulcano (De Astis et al. 2000).
Normalized
3
He/
4
He (R/R
a
) ratios (not shown) range from
7.07 (Alicudi) to 2.51 (Stromboli) (Martelli et al. 2008).
(7) Pb-isotope ratios have variable and overlapping values for
most islands except for Stromboli, which has a distinctively
less radiogenic Pb-isotope composition. Overall, Pb-isotope
ratios fall between the highly radiogenic Etna OIB-type
basalts and the continental crust of the Calabro – Peloritano
basement (Fig. 15.6b). Etna is close to the so-called FOZO
(¼FOcus ZOne; Hart et al. 1992) mantle composition,
which is extremely common in anorogenic settings of
Europe and has been termed the European Asthenospheric
Reservoir (EAR) by Wilson & Downes (1991). The
Pb-isotope composition of Marsili overlaps Stromboli and
some of the western-central islands.
(8) Stromboli shows similar radiogenic isotope signatures as
Vesuvio (De Astis et al. 2000, 2013; Peccerillo 2001) and
other volcanoes from Campania. Such a similarity is also
observed for several incompatible trace element ratios, and
led Peccerillo (2001) to conclude that Vesuvio and other
Campania volcanoes represent the northern end of the
Aeolian arc rather than the southern sector of the Roman
Magmatic Province, as generally acknowledged.
Shallow-level magma evolution
Fractional crystallization, crustal assimilation, magma mixing or
some combination of these processes has been documented for
the Aeolian volcanoes. These have been extensively discussed
within individual chapters of this volume, so are only summarized
briefly here.
Fractional crystallization
Fractional crystallization was the predominant process of magma
evolution at several centres. This process was much more
intense for the volcanoes of the central islands, where rhyolitic
compositions were reached. This outcome is likely related to
local tectonics associated with the Tindari – Letojanni transcurrent
fault, where the development of pull-apart basins favoured the for-
mation of large reservoirs (Barberi et al. 1994) in which magmas
ponded and fractionated. Mafic minerals plus plagioclase were
main fractionating phases, as demonstrated by curvilinear trends
for many major and trace elements, especially MgO, Ni, Cr but
also Al
2
O
3
and Sr, against SiO
2
(Fig. 15.3). A decrease of Ba in
the rhyolites of Vulcano and Lipari, but not at Panarea and
Salina, indicates significant separation of alkali-feldspar late in
the evolution stages of the two former islands. Alkali-feldspar
crystallization is related to the HKCA to SHO affinity of late
erupted magmas at Lipari and Vulcano. Fractional crystallization
modifies major and trace element abundances of magmas, slightly
modifies d
18
O‰, but leaves radiogenic isotope compositions and
incompatible trace element ratios unaffected. The values of these
parameters measured in evolved rocks can therefore be used to
infer compositions of primary melts and their mantle sources.
However, the main problem is that magma evolution rarely (if
ever) occurs simply by closed-system fractional crystallization;
wall-rock assimilation and magma mixing usually accompany
fractional crystallization in most cases.
Magma mixing/mingling
Magma mixing/mingling is widespread in the Aeolian volcanoes.
The most striking evidence of this process is seen in the occurrence
of abundant mafic enclaves in many intermediate and silicic lavas.
These enclaves are blobs of mafic magmas that were present within
the volcanic system and were intermingled with the silicic melts
during eruption. The best examples are observed for some Lipari
and Vulcano rhyolites (e.g. De Rosa & Sheridan 1983; Gioncada
et al. 2005; Perugini et al. 2007; De Astis et al. 2013; Forni
et al. 2013), for Panarea dacites and rhyolites (Calanchi et al.
K2O %
0
2
4
6
8
50 55 60 65 70 75 80
8
K2O %
SiO2 %
TH
CA
SHO
45
0
2
4
6
0
2
4
6
8
K2O %
Alicudi
Filicudi
Salina
Lipari
Vulcano
Panarea
Stromboli
Marsili
y
Eastern arc
Western arc
Central arc
(a)
(b)
(c)
Fig. 15.2. K
2
O v. SiO
2
classification diagrams for the Aeolian arc volcanics.
Lines dividing arc tholeiitic (TH), calc-alkaline (CA), high-K calc-alkaline
(HKCA) and shoshonitic (SHO) series are from Peccerillo & Taylor (1976).
Data on Marsili are from Trua et al. (2011). For source of other data see
Peccerillo (2005).
COMPOSITIONAL VARIATIONS OF MAGMAS IN THE AEOLIAN ARC 493
2002; Lucchi et al. 2013d) and at Salina (Perugini et al. 2004;
Lucchi et al. 2013c). Mixing processes also affected most (if not
all) of the magmas however, although physical evidence is less
strong either because of the lack of compositional contrast
between end-members or because near-equilibrium conditions
were reached by hybrid magmas.
Mixing is a complex process of major geochemical and volcano-
logical interest. Detailed studies in the Aeolian arc are however
limited (e.g. De Rosa & Sheridan 1983; De Astis et al. 1997; Gion-
cada et al. 2003, 2005; Perugini et al. 2004, 2007; Davı
`et al. 2008;
Piochi et al. 2009), and the effects on magma compositions for
single eruptions, for individual volcanic centres and at the regional
scale, are still basically unexplored.
Magma contamination
Magma contamination by crustal wall-rocks in the Aeolian volca-
noes took place as a consequence of several different processes.
Assimilation plus fractional crystallization (AFC) is the most
common case, and has been recognized at several islands (e.g.
Salina, Vulcano and Lipari; Crisci et al. 1991; Esperanc¸a et al.
1992; De Astis et al. 2013; Forni et al. 2013; Lucchi et al.
2013c). This is clearly demonstrated by the positive correlations
of
87
Sr/
86
Sr and d
18
O‰ with silica observed for many Aeolian
islands by Ellam & Harmon (1990). More complex processes of
combined fractional crystallization, assimilation, refilling of
magma chambers, mixing and frequent tapping by eruptions
(RFTA: refilling, fractionation, tapping, assimilation) have been
recognized for the lowest exposed volcanic sequences of many
islands (e.g. De Astis et al. 1997; Di Martino et al. 2011; Lucchi
et al. 2013a,b, c). These rocks are generally mafic in composition
and display rather variable trace element and isotopic signatures,
which is typical of RFTA processes (O’Hara 1977). Finally, a par-
ticular type of assimilation is represented by incorporation of
different amounts of crustal rocks by basaltic and andesitic
magmas, with the former being able to assimilate greater
amounts of crustal rocks than andesites. Such a process has been
0
4
8
12
MgO%
0.0
0.4
0.8
1.2
TiO2%
10
15
20
25
A
l2O3 %
45 50 55 60 65 70 75 80
0
SiO2 %
0
100
200
300
400
500
Rb ppm
0
500
1000
1500
2000
Ba ppm
0
1
2
3
4
Ta ppm
45 50 55 60 65 70 75 80
0
50
100
150
La ppm
Marsili (a)(b)
(c)(d)
(e)(f)
(g)(h)
50
100
150
Ni ppm
SiO2 %
Marsili
Fig. 15.3. Variation diagrams of some
major and trace elements v. silica. Source of
data and symbols as in Figure 15.2.
A. PECCERILLO ET AL.494
0
0.5
1.0
1.5
2.0
2.5
Ta p pm
0
500
1000
1500
2000
Sr ppm
0 2 4 6
0
100
200
300
Zr ppm
K2O wt%
0 2 4 6
0
20
40
60
80
100
La ppm
K2O wt%
CA SHO
Alicudi
Filicudi
Salina
Lipari
Vulcano
Panarea
Stromboli
0
50
100
150
200
250
300
Rb ppm
0
500
1000
1500
2000
Ba ppm
2500
Marsili
Marsili
CA SHO
(a)(b)
(c)(d)
(e)(f)
Fig. 15.4. Incompatible trace element
v. K
2
O diagrams for mafic-intermediate
rocks (SiO
2
,56 wt%) from the Aeolian arc
and Marsili seamount, showing increase of
element abundances from calc-alkaline to
shoshonitic rocks. Source of data as in
Figure 15.2.
1
10
100
1000
Rock/Primitive Mantle
1
10
100
1000
Rock/Primitive Mantle
1
10
100
1000
Cs
Rb
Ba
Th
U
Nb
Ta K La
Ce
Pb
Pr
Sr
P
Nd
Zr
Sm
Eu
Ti
Dy
Y Yb
Lu
Rock/Primitive Mantle
1
10
100
1000
Cs
Rb
Ba
Th
U
Nb
Ta K La
Ce
Pb
Pr
Sr
P
Nd
Zr
Sm
Eu
Ti
Dy
Y Yb
Lu
Rock/Primitive Mantle
Calabrian crust
Ionian sediments
Alicudi
Filicudi Lipari
Salina
Local MORB
Etna basalt
Marsili
Vulcano
Panarea
Stromboli
(a)(b)
(c)(d)
Fig. 15.5. Incompatible element patterns
normalized to primordial mantle
compositions for representative
mafic-intermediate rocks (SiO
2
,56 wt%)
from the Aeolian islands and Marsili
seamount (source of data as in Fig. 15.2).
Ionian sediments (average of two samples;
De Astis, unpublished data), averages of the
Calabro– Peloritano basement (Rottura
et al. 1991), Tyrrhenian MORB (Dietrich
et al. 1977) and Etna basalts (Viccaro &
Cristofolini 2008) are also shown.
Normalizing data are from Sun &
McDonough (1989).
COMPOSITIONAL VARIATIONS OF MAGMAS IN THE AEOLIAN ARC 495
well documented at Alicudi, where evolved andesites were less
affected by assimilation and, consequently, exhibit more primitive
isotopic compositions (i.e. lower Sr- and O- and higher Nd – Pb
isotope ratios) than associated basalts (Peccerillo & Wu 1992; Pec-
cerillo et al. 1993; Lucchi et al. 2013a). The same process has been
recognized, although less clearly, at Filicudi (Santo & Peccerillo
2008; Lucchi et al. 2013b).
Several studies on Aeolian volcanoes demonstrated that
magma– wall-rock interaction produced an increase in both
87
Sr/
86
Sr and d
18
O‰ (Ellam & Harmon 1990; Peccerillo et al.
2004; Santo & Peccerillo 2008). However, whereas O-isotope
ratios were increased from typical mantle values of d
18
O‰ c.
þ5.5 to values as high as d
18
O‰ c. þ8.5, Sr isotope ratios were
less strongly modified. Detailed studies of two contaminated
suites of mafic magmas from Alicudi and Vulcano (Primordial
Vulcano and Piano Caldera) have shown that extensive crustal
assimilation generated an increase in Sr isotope ratios by five to
six digits on the fourth decimal place (De Astis et al. 1997,
2013; Lucchi et al. 2013a). This is one order of magnitude lower
than the variation observed over the Aeolian arc. Some incompa-
tible element ratios, such as Rb/Ba, Rb/Sr and Ba/K, are signifi-
cantly correlated with Sr-isotope variation, suggesting they were
modified by contamination. By contrast, other element ratios
such as Ba/La, Rb/Nb, U/Th, Sr/Nd and Tb/Yb do not show
any correlation with Sr isotope ratios, implying that they were
less affected or unaffected by contamination. Such different be-
haviour is related to the variable compositional contrast between
magma and wall rocks for various elements. This changes from
one volcanic centre to another however, and results found at
Alicudi and Vulcano cannot be considered as valid for the entire
Aeolian arc.
Conditions of magma ponding and ascent
Conditions of magma ponding, crystallization and ascent have
been examined using two different approaches. One is based on
measurements of crystallographic parameters of clinopyroxenes,
especially cell dimensions, under the assumption that these
depend on pressure of crystallization (e.g. Nazzareni et al. 1998,
2001). Other work has focused on fluid inclusions in quartz-rich
xenoliths (Frezzotti et al. 2003, 2004; Zanon et al. 2003; Frezzotti
& Peccerillo 2004; Peccerillo et al. 2006; Di Martino et al. 2010,
2011).
Clinopyroxene studies have documented crystallization at
different pressures within the volcanic systems, suggesting the
occurrence of various depths of magma storage and fractionation
at the regional scale. Fluid inclusion studies provided additional
insight into magma evolution, confirming polybaric mineral crys-
tallization and demonstrating that mafic to intermediate magmas
ponded in deep reservoirs sited at depths of 21–18 km in the
lower crust at the mantle-crust boundary. Here, magmas were sub-
jected to fractionation and assimilation processes, plus intensive
feeding by mantle-derived mafic melts (RFTA). At Lipari, long-
lived hot mafic magma reservoirs facilitated partial melting of
the lower continental crust, as testified by the eruption of
cordierite-, garnet-, and sillimanite-bearing lavas (Barker 1987;
Di Martino et al. 2011). By contrast, dacitic and rhyolitic
magmas were generated by dominant fractional crystallization of
mafic parental magmas in reservoirs located at depths of 15 –
12 km. Since felsic magmas are restricted to the younger stages
of activity at many Aeolian volcanoes, an overall upward
migration of the magma chambers with time has been suggested
(Peccerillo et al. 2006). The reasons for such a migration are
still poorly understood. A variation of local tectonic stress may
have allowed formation of mid-crustal reservoirs (Ventura
2013). Another possibility could be that there was a decrease in
the input of mafic magmas into the deep reservoirs during the
mature to latest (and vanishing?) stages of volcanism. This
would have allowed fractional crystallization to become dominant
with respect to input and mixing with fresh mafic magmas, favour-
ing the formation of evolved melts. These were able to rise more
readily than mafic magmas to shallow crustal levels because of
their lower density.
Mantle source composition, magma genesis
and geodynamic setting
Trace element and isotope data are crucial for understanding the
composition and evolution of mantle sources and for exploring
conditions of magma genesis and geodynamic evolution. Many
geochemical studies have therefore been carried out on the
Aeolian volcanoes. Much attention has been focused on mafic
magmas, under the assumption that they represent primary compo-
sitions. However, such a statement has been proven incorrect for
some mafic magma suites such as at Alicudi and Filicudi. The
possible effects of magma contamination have to be considered
before inferring compositions of primary melts and their
mantle sources.
Isotope and trace element composition of mantle sources
Regional variations of radiogenic isotope ratios for mafic rocks in
the Aeolian arc have long been recognized and attributed to
Marsili
Marsili
Calabro-
Peloritano
basement
Calabro-
Peloritano
basement
Etna
0.703 0.704 0.705 0.706 0.707 0.708
0.5122
0.5124
0.5126
0.5128
0.5130
(a)
(b)
87Sr/86Sr
143Nd/144Nd
18.00 19.00 20.00
38.00
39.00
40.00
206Pb/204Pb
208Pb/204Pb
Etna
Vesuvio
Vesuvio
Fig. 15.6. Sr–Nd–Pb isotopic compositions for mafic-intermediate rocks
(SiO
2
,56%) from the Aeolian arc and Marsili seamount. Source of data and
symbols as in Figures 15.2 and 15.4. Alicudi and Filicudi andesites
(SiO
2
¼56–62%) are also plotted, since these represent the least-contaminated
magmas in the Aeolian arc (see text). Average Etna basalts (Viccaro &
Cristofolini 2008) and compositions fields of Vesuvio (for source of data see
Peccerillo 2005) and Calabro–Peloritano basement (Rottura et al., 1991) are
also reported. NHRL (Northern Hemisphere Reference Line) is from Hart
(1984).
A. PECCERILLO ET AL.496
heterogeneities of the mantle wedge (e.g. Ellam et al. 1988; Ellam
& Harmon 1990; Francalanci et al. 1993; De Astis et al. 2000;
Peccerillo et al. 2004). However, the common occurrence of
magma– crust interaction raises the problem of how much of this
variation is due to magma contamination and how much to
source heterogeneity.
Combined O- and Sr-isotope studies can help to discriminate
magma contamination from source contamination processes.
Figure 15.7 represents a d
18
O‰ and
87
Sr/
86
Sr diagram for the
available data on Aeolian rocks and separated phases (Ellam &
Harmon 1990; Peccerillo et al. 2004; Santo & Peccerillo 2008;
De Astis, unpublished data). The solid line describes a model of
bulk mixing between a primordial mantle source and Ionian Sea
sediments. Only a small number of samples from Alicudi and a
few from Filicudi plot on or just above the mantle –sediment
mixing line. By contrast, most of the Filicudi samples are shifted
upwards and show high d
18
O‰, which is typical of contaminated
magmas. Well-defined vertical trends are shown by Salina and
Vulcano samples, whereas Stromboli shows scattering and plots
away from the mantle – sediment mixing line.
Although the above model has to be considered as broadly quali-
tative because of the simplistic assumptions of simple bulk mixing
and uniform compositions for end-members, O – Sr isotope data
indicate that a few of the Alicudi and Filicudi magmas can be con-
sidered as near-primary in composition. Their different Sr-isotope
signatures at the same d
18
O‰ value suggest less radiogenic Sr
compositions for Alicudi magmas and their sources. The vertical
data arrays for Vulcano and Salina highlight strong variation of
d
18
O with a modest increase of
87
Sr/
86
Sr, typical of magma con-
tamination (Ellam & Harmon 1990). However, if these trends
are extrapolated back to the mantle – sediment mixing line,
Sr-isotope ratios similar to those at Filicudi are deduced (i.e.
87
Sr/
86
Sr slightly higher than 0.704). Stromboli does not show
typical magma contamination trends but no samples fall on the
mantle– sediment mixing line, suggesting that the Stromboli
magmas are also contaminated but that Sr-isotope compositions
are more variable and radiogenic than at other islands.
To summarize, the O– Sr isotope data suggest that there are few
uncontaminated magmas in the Aeolian arc. Magma contami-
nation processes had minor effects on Sr isotope ratios however,
in agreement with studies on Alicudi and Primordial Vulcano
discussed previously (see “Shallow-level magma evolution”).
This leads to the conclusion that first-order Sr-isotope varia-
tion along the Aeolian arc is a direct manifestation of source het-
erogeneity. The same can be demonstrated for other radiogenic
isotopes.
Variations of Sr– Pb isotope ratios along the arc are shown in
Figure 15.8, to better highlight regional isotopic zoning. There is
an increase of the
87
Sr/
86
Sr ratio from Alicudi to Filicudi and
the central islands, where the lowest Sr-isotope values are slightly
above 0.704. Another increase in radiogenic Sr is observed at
Stromboli. Nd isotopic compositions exhibit a similar trend,
although anti-corrrelated with Sr-isotope variations. Ranges of
Pb-isotope ratios remain fairly constant across most of the arc,
but become less radiogenic at Stromboli. The back-arc Marsili sea-
mount has a rather wide range of Sr – Nd isotope compositions,
comparable to those observed over the entire western arc. A very
low
206
Pb/
204
Pb is observed for one sample from Lipari (Esper-
anc¸a et al. 1992).
Trace element abundances and ratios provide additional infor-
mation on mantle composition. Here, this issue is examined by
using a new set of trace element data (Table 15.1) for more than
90 mafic– intermediate rocks from different stratigraphic levels
on various islands. The new data have the advantage of minimizing
the inter-laboratory analytical bias that characterizes the data in the
literature, thus providing a confident picture of geochemical
zoning along the arc. Inferences on source composition are
based on trace element contents of both mafic and intermediate
rocks, since andesitic rocks at Alicudi have been shown to rep-
resent the least contaminated magmas across the entire arc (Pec-
cerillo et al. 1993; Lucchi et al. 2013a). Moreover, only trace
element ratios that have not shown systematic variation with
Sr-isotope ratios in the contaminated mafic rocks of Vulcano and
Alicudi are considered, under the assumption that they may
provide reliable information on mantle compositions. The
0.702 0.704 0.706 0.708
4
6
8
10
18
87
Sr/
86
Sr
2 4
10
8
Mantle contamination trend
Mantle
Fig. 15.7. d
18
Ov.
87
Sr/
86
Sr for Aeolian magmas. The solid line represents the
mixing trend between primordial mantle and Ionian sediments (mantle
contamination). Numbers along the line are the amounts of sediments involved
in the mixing. Arrows mimic effects of magma contamination by crustal wall
rocks: note strong oxygen isotope variation and modest increase of Sr isotope
ratios. Data for Filicudi, Alicudi and Vulcano have been determined on
separated clinopyroxene phenocrysts (Peccerillo et al. 2004; Santo & Peccerillo
2008; De Astis, unpublished data) and melt compositions have been calculated
considering high-temperature isotope fractionations. Data on the other islands
are bulk rock determinations (Ellam & Harmon 1990; Gertisser & Keller 2000).
Symbols as in Figure 15.4.
18.0
19.0
20.0
0.703
0.704
0.705
0.706
0.707
0.708
87Sr/86Sr
West East
Alicudi
Filicudi
Salina
Lipari
Vulcano
Panarea
Stromboli
206Pb/204Pb
West East
Alicudi
Filicudi
Salina Lipari
Vulcano
Panarea
Stromboli
(a)(b)
Marsili
Marsili
Fig. 15.8. Regional variation of
Sr–Pb isotopic compositions for
mafic-intermediate rocks (SiO
2
,56 wt%)
from the Aeolian arc. Alicudi and Filicudi
andesites (SiO
2
¼56–62%) are also
plotted, since these represent the least
contaminated magmas in the Aeolian arc
(see text). Data of Marsili seamount are
shown as a dashed line on the left-hand side
of the diagrams. Source of data as in
Figure 15.2.
COMPOSITIONAL VARIATIONS OF MAGMAS IN THE AEOLIAN ARC 497
Table 15.1. Major and trace element data for representative rocks from Aeolian volcanoes. Major element data for Vulcano and Panarea are from De Astis et al. (1997) and Calanchi et al. (2002)
Sample A9 ALI A3 ALI A6 ALI A11 ALI A15 ALI A4 ALI A7 ALI A5 ALI FIL 95 FIL 90 FIL 9 FIL10 FIL 7 FIL 80 FIL101
Alicudi Alicudi Alicudi Alicudi Alicudi Alicudi Alicudi Alicudi Filicudi Filicudi Filicudi Filicudi Filicudi Filicudi Filicudi
SiO
2
51.10 51.42 54.03 55.07 56.27 56.32 56.99 58.84 48.78 50.20 50.58 50.62 50.96 50.99 51.43
TiO
2
0.69 0.72 0.77 0.69 0.92 0.72 0.66 0.77 0.72 0.75 0.77 0.77 0.72 0.83 0.81
Al
2
O
3
16.93 16.98 17.84 16.49 18.94 18.68 18.35 18.86 18.92 18.65 18.47 19.44 18.05 19.30 18.78
Fe
2
O
3
3.96 7.71 1.96 3.24 3.31 2.12 2.27 4.71 9.40 9.84 9.06 8.88 8.73 9.91 9.61
FeO 3.82 0.87 5.26 3.74 3.30 4.19 3.79 0.98 0.00 0.00 0.00 0.00 0.00 0.00 0.00
MnO 0.09 0.10 0.09 0.09 0.09 0.09 0.09 0.07 0.16 0.17 0.16 0.16 0.16 0.16 0.16
MgO 8.20 7.16 6.05 6.49 2.43 4.00 4.48 2.23 5.70 4.92 3.54 3.44 4.73 3.93 3.94
CaO 10.45 10.36 8.61 8.71 7.56 7.43 7.10 5.73 11.44 11.00 11.00 10.67 10.20 9.77 10.48
Na
2
O 2.52 2.25 3.24 3.18 3.78 3.50 3.72 4.20 2.28 2.39 2.72 2.69 2.75 2.65 2.68
K
2
O 0.95 0.94 1.55 1.27 1.75 1.82 1.90 2.15 1.16 1.01 1.01 1.17 1.28 1.27 1.37
P
2
O
5
0.29 0.30 0.33 0.32 0.37 0.34 0.36 0.39 0.22 0.20 0.19 0.18 0.21 0.20 0.23
LOI 0.99 1.19 0.27 0.71 1.28 0.79 0.29 1.07 1.23 0.87 2.51 1.99 2.22 1.00 0.52
V 223 221 221 223 169 180 163 137 330 240 308 290 285 271 331
Ga 13 14 16 15 16 16 13 16 19 19 17 20 17 21 17
Rb 24 23 40 28 48 55 47 52 23 27 23 34 34 32 30
Sr 583 606 598 570 623 667 642 686 679 729 708 763 723 773 713
Y 171718 16 23 19182217181718181918
Zr 63 56 83 83 107 112 107 139 54 60 56 63 63 59 55
Nb 7.4 7.3 10.6 11.0 10.6 14.9 13.1 23.1 4.8 5.8 5.6 7.0 6.9 6.0 4.6
Cs 0.95 1.09 1.12 0.86 0.97 1.32 1.37 1.58 1.18
Ba 343 260 417 499 453 607 593 852 335 402 373 406 410 382 379
La 21 19 25 27 30 40 38 42 15 20 16 20 20 19 19
Ce 40 38 46 49 56 69 67 77 30 37 33 43 41 39 36
Pr 4.0 4.2 4.6 4.7 5.5 6.4 6.1 7.2 3.3 4.1 3.7 4.7 4.4 4.4 4.0
Nd 16 18 20 19 24 26 24 28 16 18 15 19 19 19 18
Sm 3.50 3.54 3.37 3.74 4.51 4.26 4.28 5.43 4.18 4.57 4.24 3.97 4.42 3.89 4.12
Eu 1.06 0.95 1.16 1.11 0.91 1.32 0.87 1.01 1.06 1.01 1.33 1.31 1.14 0.74 1.14
Gd 3.44 4.11 3.53 2.74 4.10 3.43 3.48 4.35 2.87 4.77 3.89 3.42 3.91 4.24 2.12
Tb 0.49 0.50 0.53 0.43 0.62 0.59 0.55 0.57 0.52 0.43 0.45 0.53 0.55 0.55 0.44
Dy 2.86 3.42 3.17 3.01 4.04 3.31 3.28 3.73 3.03 2.76 3.14 3.28 3.33 3.30 3.01
Ho 0.60 0.63 0.64 0.55 0.69 0.63 0.59 0.80 0.60 0.62 0.69 0.66 0.54 0.63 0.63
Er 1.70 1.78 1.83 1.54 2.43 1.80 1.83 2.29 1.62 1.80 1.71 1.75 1.96 1.91 1.50
Tm 0.23 0.26 0.25 0.26 0.36 0.28 0.28 0.32 0.36 0.34 0.37 0.24 0.25 0.40 0.26
Yb 1.48 1.53 1.79 1.30 2.08 1.92 1.47 2.28 1.93 2.16 1.68 1.73 2.11 1.92 1.61
Lu 0.24 0.28 0.20 0.29 0.27 0.25 0.28 0.31 0.30 0.41 0.35 0.30 0.29 0.53 0.27
Hf 1.64 1.34 1.87 1.57 2.26 2.26 2.30 2.99 1.87 1.76 1.24 1.45 1.40 1.67 1.28
Ta 0.44 0.36 0.48 0.50 0.65 0.65 0.67 1.34 0.28 0.26 0.34 0.37 0.35 0.30
Pb 5.1 3.3 5.6 4.9 5.5 5.7 6.1 6.9 3.8 2.9 5.8 6.6 6.8 4.1 4.6
Th 3.78 3.02 4.88 6.14 6.18 9.12 8.77 9.88 2.97 3.70 3.22 4.07 4.20 3.72 3.87
U 1.07 0.89 1.56 1.81 1.61 2.49 2.12 2.24 0.99 1.20 1.01 1.44 1.80 1.17 1.19
A. PECCERILLO ET AL.498
Sample FIL 40 FIL 29 FIL 24 SAL 98a SAL 28 SAL 40 SAL 48 SAL 55 SAL 79 SAL 27 SAL 82 SAL 88 SAL 1 SAL 76 A1 LIP
Filicudi Filicudi Filicudi Salina Salina Salina Salina Salina Salina Salina Salina Salina Salina Salina Lipari
SiO
2
52.38 52.68 53.28 49.50 49.53 49.79 50.02 50.76 50.93 51.03 51.46 51.81 52.03 52.15 52.17
TiO
2
0.70 0.78 0.77 0.73 0.65 0.73 0.74 0.65 0.69 0.74 0.67 0.74 0.65 0.66 0.68
Al
2
O
3
19.56 18.17 17.00 17.84 19.13 17.87 19.77 17.85 20.09 19.32 18.53 17.50 18.07 17.36 17.30
Fe
2
O
3
8.87 9.66 8.30 11.44 9.82 11.56 11.31 10.15 9.83 10.62 9.91 10.95 9.63 9.88 9.58
FeO 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 0.00
MnO 0.16 0.17 0.14 0.21 0.18 0.21 0.21 0.19 0.19 0.20 0.18 0.20 0.19 0.19 0.17
MgO 3.85 3.50 5.34 5.17 3.41 5.01 3.41 5.75 3.49 3.39 4.53 4.43 4.59 5.36 5.84
CaO 10.16 10.35 10.15 11.22 9.40 10.85 10.73 10.95 11.11 10.12 10.95 10.23 10.60 10.12 10.13
Na
2
O 2.82 2.51 2.65 2.39 2.47 2.29 2.58 2.31 2.68 2.78 2.36 2.38 2.34 2.42 2.22
K
2
O 1.28 1.20 1.55 0.96 0.75 0.99 0.97 0.92 0.84 0.91 0.88 1.08 1.18 0.98 1.14
P
2
O
5
0.22 0.15 0.34 0.11 0.12 0.10 0.10 0.12 0.12 0.12 0.11 0.16 0.11 0.14 0.15
LOI 0.00 0.82 0.49 0.45 4.52 0.60 0.16 0.35 0.04 0.76 0.42 0.54 0.62 0.74 0.63
V 291 298 263 304 328 309 310 285 380 266 286 299 294 309 239
Ga 21 20 16 15 19 14 18 16 17 15 17 16 16 18 15
Rb 33 36 45 22 20 23 19 20 21 20 21 26 26 22 38
Sr 656 737 561 717 716 771 762 576 730 770 699 709 732 609 602
Y 17 18 16 15 2716161416171519161517
Zr 57 61 63 42 40 43 57 40 42 46 43 52 49 41 64
Nb 7.1 6.5 10.2 2.3 2.6 2.8 2.5 2.3 2.5 2.2 2.6 2.8 4.3 2.3 4.2
Cs 1.63 1.21 1.26 1.54 2.13 1.74 1.87
Ba 380 407 350 347 334 413 354 266 358 325 331 399 378 343 369
La 19 21 20 14 17 17 14 12 13 13 14 18 15 13 16
Ce 37 40 42 27 40 31 28 24 23 26 27 33 31 26 34
Pr 3.8 4.1 4.3 3.0 4.4 3.3 3.1 2.9 2.8 3.0 3.0 4.0 3.4 2.8 3.6
Nd 16 18 18 13 22 17 15 13 13 15 14 18 15 12 18
Sm 2.87 4.66 3.54 3.80 5.41 3.35 3.29 2.84 3.07 2.93 3.74 4.63 4.01 2.81 3.25
Eu 0.98 1.39 0.87 0.79 1.72 1.05 1.31 0.81 0.97 0.96 0.70 1.08 1.05 0.96 1.01
Gd 4.47 3.31 5.53 2.78 4.22 2.44 3.83 2.61 2.92 4.00 2.91 6.22 3.61 3.65 5.32
Tb 0.50 0.60 0.58 0.44 0.77 0.46 0.60 0.36 0.48 0.48 0.47 0.50 0.57 0.46 0.50
Dy 2.87 3.51 3.14 2.28 4.71 2.94 2.74 2.31 2.85 3.19 2.66 3.32 3.20 2.69 3.43
Ho 0.52 0.61 0.63 0.58 0.94 0.57 0.49 0.49 0.56 0.63 0.57 0.76 0.63 0.57 0.55
Er 1.70 2.03 1.73 1.24 2.78 1.61 1.60 1.56 1.60 1.44 1.40 1.65 1.50 1.33 1.54
Tm 0.28 0.28 0.30 0.31 0.45 0.29 0.23 0.28 0.29 0.25 0.32 0.36 0.37
Yb 2.10 1.85 1.50 2.12 2.76 2.28 1.60 1.51 1.27 1.75 1.55 2.12 2.17 1.48 1.89
Lu 0.25 0.30 0.32 0.30 0.37 0.30 0.24 0.33 0.28 0.25 0.32 0.29 0.39
Hf 1.76 1.58 1.48 1.29 1.18 0.93 1.09 0.89 0.95 1.48 0.86 1.68 1.50 1.14 1.45
Ta 0.30 0.34 0.52 0.21 0.13 0.23 0.21 0.29 0.40 0.23 0.27
Pb 7.4 5.9 4.7 5.8 5.7 6.6 6.2 3.9 4.5 4.0 5.6 5.8 5.5 5.2 7.4
Th 4.30 4.56 3.29 2.51 2.78 3.68 2.85 2.37 2.60 2.56 2.52 3.69 3.58 2.47 4.29
U 1.28 1.43 1.32 0.70 0.93 0.95 0.81 0.78 0.72 0.69 0.66 1.01 1.06 0.91 1.01
(Continued )
COMPOSITIONAL VARIATIONS OF MAGMAS IN THE AEOLIAN ARC 499
Table 15.1. Major and trace element data for representative rocks from Aeolian volcanoes. Major element data for Vulcano and Panarea are from De Astis et al. (1997) and Calanchi et al. (2002) (Continued)
Sample LIP 105 LIP 113 LIP 113B LIP 114 LIP 84 LIP 182 T17 A3 LIP LIP 180 A16 LIP MR6 LIP 122 LIP 143 T9 PN235
Lipari Lipari Lipari Lipari Lipari Lipari Lipari Lipari Lipari Lipari Lipari Lipari Lipari Lipari Panarea
SiO
2
52.31 52.64 52.64 53.38 53.53 53.54 53.59 53.76 53.82 54.08 54.94 55.19 57.05 59.27 47.83
TiO
2
0.55 0.67 0.67 0.68 0.73 0.69 0.77 0.68 0.67 0.81 0.71 0.83 0.62 0.79 0.56
Al
2
O
3
14.90 14.95 14.95 14.97 16.56 17.19 17.00 16.72 17.80 17.25 17.81 16.28 17.41 16.18 17.50
Fe
2
O
3
8.62 9.16 9.16 9.13 9.17 8.99 9.60 9.35 8.59 8.67 9.01 9.35 8.33 8.14 8.94
FeO 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 0.00 0.00
MnO 0.14 0.19 0.19 0.32 0.14 0.17 0.16 0.16 0.15 0.14 0.16 0.15 0.17 0.15 0.14
MgO 7.69 6.48 6.48 5.80 4.60 4.58 4.74 5.24 4.50 4.42 4.03 4.17 3.79 3.42 5.64
CaO 10.83 10.38 10.38 10.04 9.67 8.87 9.42 8.88 8.12 8.89 8.48 8.84 7.62 6.47 9.32
Na
2
O 2.43 2.24 2.24 2.25 2.86 2.65 2.10 2.36 2.46 2.49 2.88 2.01 2.27 2.00 1.83
K
2
O 0.96 1.42 1.42 1.35 1.99 2.07 1.54 1.80 1.91 1.61 1.79 1.61 1.54 2.28 0.55
P
2
O
5
0.16 0.16 0.16 0.18 0.22 0.26 0.18 0.23 0.21 0.23 0.19 0.21 0.13 0.18 0.13
LOI 1.42 1.73 1.73 1.90 0.54 0.98 0.90 0.82 1.79 1.41 0.01 1.36 1.07 1.13 7.57
V 278 242 211 297 269 242 254 271 240 252 269 316 199 220 247
Ga 15 16 14 15 17 16 16 17 16 18 18 15 16 18 16
Rb 27 43 36 35 53 56 54 43 57 54 45 39 63 95 26
Sr 575 597 601 608 853 860 691 804 797 656 815 560 557 488 656
Y 15 20 19 1819 181917 19 21 1719 252319
Zr 45 64 67 62 86 81 90 71 78 91 77 67 75 120 58
Nb 2.3 4.4 3.9 4.0 7.1 6.6 6.1 5.2 6.6 6.2 5.1 4.3 5.8 8.8 4.1
Cs 1.02 2.73 1.31 1.70 1.53 1.35 3.00 2.51 2.09 3.62 0.76
Ba 316 329 344 356 526 481 392 464 444 555 478 366 373 620 281
La 13 17 18 18 24 24 22 22 23 23 20 18 25 27 17
Ce 25 35 36 37 49 48 46 43 45 48 41 37 48 56 33
Pr 2.8 3.7 3.8 4.3 5.3 5.2 5.2 5.0 5.2 5.4 4.7 4.1 5.3 5.9 4.0
Nd 13 17 18 19 23 23 23 21 23 23 21 19 22 26 19
Sm 3.11 3.75 4.14 3.43 5.75 5.14 4.60 3.34 4.85 5.07 3.94 4.83 5.55 4.97 4.20
Eu 0.80 1.16 0.98 0.96 1.14 1.47 1.13 1.03 1.31 1.43 1.23 1.35 1.32 1.17 1.08
Gd 4.01 4.25 3.47 3.83 4.00 4.36 4.67 4.19 4.00 4.60 4.11 3.44 4.35 4.23 3.89
Tb 0.48 0.58 0.61 0.55 0.58 0.58 0.67 0.63 0.59 0.61 0.51 0.43 0.62 0.60 0.51
Dy 2.61 3.50 3.59 3.58 3.81 3.56 4.21 3.63 3.38 3.96 3.26 3.57 4.25 4.15 3.33
Ho 0.55 0.66 0.67 0.61 0.62 0.65 0.89 0.55 0.65 0.83 0.67 0.64 0.74 0.80 0.68
Er 1.56 2.01 1.88 1.93 1.82 1.81 2.16 1.57 1.74 2.13 1.56 2.08 2.21 2.24 1.86
Tm 0.25 0.29 0.34 0.34 0.24 0.32 0.33 0.28 0.40 0.29 0.29 0.42 0.35 0.26
Yb 1.81 1.91 1.85 1.98 1.96 1.67 1.99 1.65 1.67 2.35 1.53 1.97 2.35 2.11 1.61
Lu 0.45 0.29 0.27 0.51 0.29 0.26 0.31 0.35 0.27 0.39 0.32 0.34 0.32 0.28
Hf 1.37 1.59 1.49 1.28 2.39 2.17 2.59 2.05 1.90 2.62 2.35 1.65 1.87 2.87 1.27
Ta 0.32 0.32 0.25 0.36 0.44 0.30 0.54 0.41 0.34 0.53 0.40 0.36 0.52 0.73 0.23
Pb 5.1 4.3 2.4 13.4 4.4 9.8 7.5 6.8 9.2 10.0 6.7 7.1 7.0 16.3 5.0
Th 2.80 3.89 3.85 4.02 5.44 5.70 5.79 6.03 5.45 5.95 5.05 4.28 4.94 8.70 3.90
U 0.86 1.16 0.99 1.25 1.80 1.47 1.61 1.66 1.63 1.54 1.53 1.66 1.41 2.27 0.56
A. PECCERILLO ET AL.500
Sample PF1 PS 11A VL168-10 VL250 VLPC1 VL229/1a 1b VL143-1S VL145/2 VL272 VUL508 VL189/1 VL157/2 VL139-6 VL259/1 VL90/1
Panarea Panarea Vulcano Vulcano Vulcano Vulcano Vulcano Vulcano Vulcano Vulcano Vulcano Vulcano Vulcano Vulcano Vulcano
SiO
2
51.16 52.25 48.54 49.13 49.23 49.81 50.10 50.93 51.21 51.23 51.40 52.27 52.33 52.70 52.88
TiO
2
0.62 0.92 0.77 0.66 0.68 0.68 0.76 0.76 0.67 0.81 0.69 0.70 0.80 0.71 0.71
Al
2
O
3
17.12 17.79 12.51 16.33 15.81 14.27 14.73 17.40 16.49 17.54 15.77 17.53 16.96 15.38 16.20
Fe
2
O
3
9.69 9.20 5.42 5.90 5.18 5.73 6.17 5.19 4.66 6.59 4.52 5.81 5.30 3.81 4.59
FeO 0.00 0.00 6.02 3.79 3.82 4.68 4.33 4.42 4.55 3.59 4.74 3.26 4.81 5.76 3.96
MnO 0.16 0.16 0.21 0.18 0.19 0.19 0.18 0.21 0.15 0.23 0.17 0.18 0.18 0.18 0.13
MgO 6.25 4.23 8.65 6.85 5.56 7.29 6.28 4.09 5.49 3.83 6.00 3.86 3.17 5.38 3.54
CaO 10.24 9.06 12.49 10.51 9.65 11.39 10.50 9.39 8.82 8.57 9.15 8.45 7.23 9.46 7.04
Na
2
O 2.54 2.50 2.20 2.31 3.10 2.40 1.77 2.44 2.83 3.33 2.69 3.13 3.32 2.71 4.35
K
2
O 0.90 2.45 2.08 1.75 3.78 2.04 2.23 2.52 2.47 2.72 2.56 2.63 3.67 2.46 3.36
P
2
O
5
0.08 0.58 0.21 0.25 0.48 0.22 0.22 0.28 0.27 0.28 0.26 0.29 0.40 0.21 0.39
LOI 1.24 0.85 0.90 2.33 2.53 1.30 2.72 2.37 2.39 1.29 2.06 1.89 1.82 1.23 2.83
V 251 341 264 260 228 237 245 208 253 326 245 213 251 211 195
Ga 16 20 15 15 18 19 12 16 20 16 17 18 17 16 16
Rb 21 82 46 17 115 47 58 58 35 51 57 50 113 60 125
Sr 593 893 1135 986 1619 1229 1077 1340 953 1293 1048 1249 1320 913 1303
Y 1321172517 16 17 23152016 303115 21
Zr 40 127 72 67 104 76 74 105 76 94 90 104 138 86 155
Nb 3.1 22.2 6.5 5.6 11.6 5.5 5.2 8.3 8.4 6.7 8.3 12.6 17.5 8.5 16.9
Cs 0.64 3.92 1.25 2.42 2.27 1.97 2.06 1.04 1.01 2.71 9.23 2.14 6.08
Ba 319 1199 578 567 1060 765 638 889 614 816 797 865 1150 630 1137
La 11 38 26 29 42 33 27 41 25 34 35 46 54 28 56
Ce 23 71 52 58 80 62 53 85 50 67 67 84 104 55 108
Pr 2.6 7.4 5.9 6.6 8.0 6.5 5.8 9.3 5.2 7.4 7.3 9.5 10.9 5.8 10.3
Nd 12 34 27 30 34 30 25 41 22 32 30 41 49 24 41
Sm 3.20 6.49 6.21 6.47 6.67 6.46 5.41 8.28 4.38 5.88 5.64 7.78 9.16 4.75 7.68
Eu 0.84 1.74 1.41 1.71 1.57 1.28 1.15 1.85 1.15 1.47 1.52 1.83 1.96 1.25 1.47
Gd 1.68 5.15 4.80 5.47 4.73 2.51 4.10 5.37 3.98 4.17 3.54 6.64 6.73 3.69 6.11
Tb 0.34 0.76 0.66 0.83 0.67 0.55 0.53 0.83 0.51 0.69 0.57 0.87 0.99 0.50 0.74
Dy 2.35 3.87 3.34 4.19 3.46 2.88 3.29 4.44 3.14 3.62 3.21 5.06 5.47 2.80 4.34
Ho 0.46 0.73 0.53 0.77 0.60 0.54 0.63 0.72 0.57 0.67 0.60 0.93 0.96 0.50 0.76
Er 1.41 2.03 1.61 2.08 1.48 1.66 1.62 2.00 1.57 1.96 1.65 2.73 2.66 1.30 1.88
Tm 0.22 0.27 0.23 0.31 0.27 0.38 0.25 0.25 0.27 0.20 0.45 0.33 0.23 0.36
Yb 1.26 1.64 1.19 1.80 1.66 1.16 1.29 1.69 0.97 1.55 1.34 2.17 2.01 1.27 1.87
Lu 0.25 0.26 0.29 0.18 0.23 0.21 0.29 0.30 0.30 0.22 0.40 0.37 0.22 0.30
Hf 1.02 3.16 1.81 1.46 2.01 1.95 2.06 2.25 1.94 2.41 2.37 2.60 3.01 1.99 3.49
Ta 0.16 0.91 0.32 0.27 0.51 0.29 0.23 0.48 0.42 0.47 0.39 0.63 1.14 0.48 1.23
Pb 5.2 13.9 8.3 7.1 13.2 9.3 7.7 13.4 9.5 9.1 11.6 13.7 18.0 11.5 17.9
Th 2.14 11.96 5.92 5.57 10.88 8.35 6.80 9.14 5.85 7.40 9.66 10.14 20.30 7.34 22.14
U 0.61 3.13 1.47 1.62 2.52 2.42 1.77 2.19 1.51 2.26 2.43 2.51 4.97 2.12 6.27
(Continued )
COMPOSITIONAL VARIATIONS OF MAGMAS IN THE AEOLIAN ARC 501
Table 15.1. Major and trace element data for representative rocks from Aeolian volcanoes. Major element data for Vulcano and Panarea are from De Astis et al. (1997) and Calanchi et al. (2002) (Continued)
Sample VL345/1 VL283/10 VL273/1 VL149/1 VL144/2 VL356/20 SC1 LS6 T2a At1 STR 13 LR 5 STR 11 STR 5 LS4
Vulcano Vulcano Vulcano Vulcano Vulcano Vulcano Stromboli Stromboli Stromboli Stromboli Stromboli Stromboli Stromboli Stromboli Stromboli
SiO
2
53.24 53.35 53.44 53.78 54.00 54.62 48.15 48.88 49.40 50.06 50.33 50.64 50.86 50.91 50.94
TiO
2
0.86 0.67 0.63 0.69 0.75 0.66 0.93 0.84 0.99 0.95 0.81 1.00 0.91 0.90 0.97
Al
2
O
3
16.76 16.36 17.60 16.42 14.58 14.23 18.17 17.86 18.38 16.77 17.15 17.54 15.31 17.88 17.22
Fe
2
O
3
4.26 4.45 5.05 6.92 4.47 4.58 7.69 6.97 3.92 3.02 1.49 3.34 2.61 2.63 2.85
FeO 4.90 4.12 2.85 2.14 5.19 4.82 0.73 0.68 4.36 4.91 7.43 4.72 6.16 5.41 4.93
MnO 0.16 0.16 0.13 0.15 0.17 0.17 0.13 0.12 0.13 0.13 0.15 0.13 0.17 0.15 0.13
MgO 4.01 3.61 3.59 4.07 4.18 5.04 5.99 5.82 6.88 7.57 5.95 5.21 6.69 5.71 6.03
CaO 7.60 7.25 7.76 7.45 7.37 8.30 10.89 10.66 10.22 9.19 10.90 9.42 10.95 10.55 8.97
Na
2
O 2.63 4.17 4.38 3.35 2.98 2.84 2.31 2.38 2.77 2.19 2.55 2.59 2.23 2.45 2.49
K
2
O 2.83 4.36 2.53 3.59 4.57 3.39 1.82 1.72 1.81 3.63 2.33 3.53 3.23 2.33 3.77
P
2
O
5
0.27 0.36 0.34 0.30 0.36 0.25 0.48 0.44 0.40 0.63 0.60 0.61 0.65 0.53 0.67
LOI 2.49 1.14 1.70 1.14 1.38 1.11 2.71 3.65 0.74 0.95 0.31 1.26 0.23 0.55 1.05
V 220 199 194 238 231 199 220 220 258 220 262 247 257 247 221
Ga 18 16 15 15 15 15 14 14 13 15 15 15 17 15
Rb 68 144 79 102 136 136 62 60 50 117 70 124 108 64 101
Sr 1115 1162 1275 1041 1345 980 783 707 643 792 674 894 745 662 749
Y 202116232425 242322242227262124
Zr 109 139 100 104 143 145 151 145 106 165 140 168 145 136 165
Nb 11.7 17.4 9.9 12.3 14.2 10.0 17.5 16.2 13.0 19.3 21.5 23.8 27.1 24.3 20.5
Cs 2.57 5.60 1.97 2.04 5.07 5.58 4.91 5.65 2.09 5.44 3.18 4.39 7.30 4.36 7.13
Ba 701 993 862 746 980 600 1030 953 815 1660 995 1851 1553 891 1707
La 32 51 34 41 51 53 43 42 36 47 42 54 53 45 45
Ce 63 95 62 82 99 98 92 86 75 101 91 110 111 88 95
Pr 6.6 9.6 6.2 8.5 10.2 10.0 9.9 9.2 7.5 11.2 9.9 11.5 12.5 9.4 10.5
Nd 29 38 29 37 42 33 40 41 32 47 41 51 49 39 47
Sm 5.70 7.73 5.29 7.22 8.27 7.50 6.90 8.22 6.36 9.95 8.79 10.14 11.36 7.41 9.10
Eu 1.45 1.63 1.44 1.51 1.60 1.39 1.88 1.59 1.50 1.79 2.22 1.87 2.77 2.12 2.04
Gd 4.18 5.41 3.32 4.98 5.68 4.00 5.43 5.90 4.98 7.08 4.78 8.10 8.61 5.71 7.36
Tb 0.65 0.67 0.55 0.76 0.90 0.78 0.89 0.78 0.81 0.99 0.79 1.05 1.15 0.78 0.88
Dy 3.61 3.83 2.90 4.16 4.67 3.95 4.55 4.69 4.34 5.33 4.24 5.47 5.50 4.39 4.91
Ho 0.66 0.64 0.49 0.75 0.77 0.69 0.83 0.80 0.78 0.87 0.94 1.04 1.02 0.86 0.81
Er 1.83 1.81 1.30 1.91 2.20 1.83 2.17 2.16 1.88 2.28 2.35 2.47 2.61 2.05 2.18
Tm 0.28 0.26 0.22 0.25 0.31 0.29 0.27 0.37 0.40 0.32 0.32 0.39 0.36 0.31 0.33
Yb 1.91 1.97 1.18 1.50 1.98 2.20 2.52 2.06 2.08 1.95 2.02 2.12 2.56 2.28 1.48
Lu 0.25 0.25 0.23 0.29 0.29 0.33 0.32 0.26 0.26 0.31 0.34 0.35 0.40 0.30 0.30
Hf 2.91 3.26 2.01 2.51 3.83 3.60 3.40 3.41 2.43 4.11 2.57 3.49 3.87 3.29 3.54
Ta 0.66 0.97 0.42 0.81 0.95 0.90 1.11 1.11 0.52 1.15 0.66 1.52 0.98 0.86 1.32
Pb 12.6 17.4 11.3 16.8 18.7 16.0 26.0 39.5 20.5 23.3 18.3 25.2 25.7 15.8 23.5
Th 8.27 21.06 8.30 14.03 19.73 18.00 15.16 14.69 11.03 19.20 14.48 18.29 15.43 13.58 18.49
U 2.40 6.20 2.26 4.20 5.55 5.30 3.52 3.14 3.08 5.23 3.90 4.96 3.52 3.72 5.14
A. PECCERILLO ET AL.502
Sample STR 9 LS3 STR 12 STR 16 L2e STR 7 STR 6 STR 1 STR 2 STR 4 STR 3 STR 15 T3b1 STR 77 STR 17 STR 10 STR 8
Stromboli Stromboli Stromboli Stromboli Stromboli Stromboli Stromboli Stromboli Stromboli Stromboli Stromboli Stromboli Stromboli Stromboli Stromboli Stromboli Stromboli
SiO
2
50.99 51.10 51.12 51.20 51.31 51.31 51.33 51.70 51.81 52.05 52.32 52.43 52.57 52.63 52.63 53.66 55.36
TiO
2
0.96 0.93 0.89 0.88 0.78 0.95 0.95 0.95 0.83 0.91 0.72 0.90 0.88 0.93 0.95 0.7 0.63
Al
2
O
3
17.92 17.63 16.93 16.70 18.57 18.39 17.33 17.78 17.66 17.88 18.00 16.56 17.43 16.58 16.59 15.45 15.33
Fe
2
O
3
2.55 2.56 2.00 8.99 2.04 2.17 2.55 3.03 1.18 1.90 1.33 8.24 4.35 2.70 2.57 3.01 2.23
FeO 7.11 4.76 6.33 0.00 4.99 7.37 5.91 5.07 6.07 5.53 5.91 0.00 2.93 5.09 6.02 6.11 5.63
MnO 0.18 0.13 0.13 0.16 0.12 0.17 0.16 0.16 0.15 0.16 0.15 0.15 0.13 0.15 0.15 0.19 0.17
MgO 4.10 6.09 5.43 6.30 7.12 3.75 4.28 4.77 5.82 5.10 6.69 4.92 6.18 5.71 4.89 5.88 6.23
CaO 10.21 8.66 9.59 11.24 9.62 8.99 9.32 8.80 8.88 9.00 10.09 9.08 9.17 9.11 9.16 10.2 9.86
Na
2
O 2.43 3.02 2.33 2.47 2.61 3.15 2.55 2.51 2.23 2.43 2.11 2.59 2.89 2.39 2.55 2.31 2.3
K
2
O 2.00 3.43 3.91 2.30 1.69 2.83 4.09 3.49 4.57 3.72 1.77 3.75 2.00 3.63 3.79 1.5 1.55
P
2
O
5
0.32 0.61 0.63 0.52 0.29 0.50 0.71 0.71 0.53 0.62 0.25 0.59 0.36 0.59 0.55 0.15 0.16
LOI 1.23 1.08 0.70 0.23 0.87 0.43 0.83 1.03 0.27 0.71 0.66 0.22 1.11 0.48 0.16 0.83 0.55
V 219 242 242 250 227 227 219 226 225 233 217 243 212 242 246 218 238
Ga 17 14 15 18 13 16 17 16 14 16 13 19 15 16 21 13 16
Rb 59 108 112 68 55 88 113 104 126 113 50 128 56 110 126 44 58
Sr 663 805 848 812 482 709 729 806 627 755 429 741 636 692 764 516 553
Y 21 25242619 242123182216 3324 25281618
Zr 138 159 163 164 95 164 163 173 142 152 85 204 139 161 197 91 106
Nb 19.6 23.2 33.2 22.5 10.8 27.4 28.2 36.8 27.1 30.3 12.3 28.0 13.9 20.1 27.4 10.1 17.7
Cs 3.48 6.73 5.47 3.13 3.65 3.48 7.68 7.72 6.16 7.60 3.48 3.89 1.67 2.07 6.23 2.15 3.28
Ba 757 1722 1815 1226 725 1206 1570 1825 1360 1611 656 1682 812 1450 1683 465 648
La 45 50 57 48 25 50 49 58 43 57 25 54 42 44 54 27 33
Ce 90 102 122 99 52 96 101 116 89 120 49 119 82 89 112 52 62
Pr 9.4 10.8 13.3 10.5 5.2 10.5 11.2 12.5 9.4 13.3 5.5 12.5 8.2 9.7 11.9 5.6 6.9
Nd 38 49 52 47 23 40 47 52 42 53 22 55 35 44 49 22 27
Sm 6.85 9.13 10.08 8.33 4.40 7.95 10.05 9.86 8.02 10.44 4.64 9.95 6.65 8.60 10.12 3.72 5.16
Eu 1.71 2.16 2.48 1.96 1.21 2.10 2.35 2.60 2.39 2.56 1.36 2.40 1.36 1.98 2.39 1.11 1.59
Gd 5.50 7.19 7.25 6.72 4.39 6.75 7.63 7.21 6.71 7.51 4.04 7.54 4.83 5.30 6.54 3.71 4.23
Tb 0.72 1.00 0.97 1.04 0.62 0.81 0.91 0.97 0.83 1.00 0.59 1.20 0.71 0.87 1.11 0.5 0.63
Dy 4.40 5.28 4.89 4.98 3.69 4.52 4.48 5.22 4.14 4.83 3.14 6.82 4.79 5.14 5.09 2.84 3.35
Ho 0.83 0.99 0.98 0.93 0.71 0.87 0.85 0.95 0.69 0.88 0.65 1.15 0.85 0.89 0.94 0.56 0.66
Er 2.30 2.31 2.17 2.28 1.69 2.31 2.11 2.29 1.86 2.27 1.66 3.19 2.15 2.47 2.80 1.6 1.72
Tm 0.35 0.29 0.32 0.51 0.28 0.30 0.28 0.28 0.26 0.31 0.23 0.69 0.38 0.32 0.44 0.25 0.3
Yb 2.32 1.86 2.07 2.04 1.92 2.39 2.05 2.15 1.83 1.80 1.53 2.49 1.99 1.99 2.44 1.68 1.84
Lu 0.33 0.28 0.26 0.38 0.22 0.32 0.25 0.30 0.24 0.32 0.28 0.56 0.39 0.40 0.48 0.26 0.28
Hf 3.19 3.85 4.08 3.30 2.04 3.68 4.09 3.84 3.27 3.51 2.10 5.19 2.77 3.77 4.43 2.51 2.51
Ta 0.72 1.30 1.33 0.79 0.56 0.84 0.91 1.23 0.83 1.06 0.46 1.10 0.89 1.16 1.19 0.34 0.47
Pb 13.3 23.4 29.5 22.0 12.8 19.1 27.5 29.8 19.1 26.1 12.8 21.3 11.2 16.5 25.4 9.9 15.2
Th 12.65 16.17 16.94 17.64 10.34 17.58 18.96 17.85 16.02 15.70 9.19 20.42 14.10 17.43 20.69 7.02 9.51
U 3.06 4.39 5.24 3.96 2.96 4.31 5.63 4.93 5.29 3.86 2.37 5.96 2.98 4.49 5.58 2.04 2.71
Analyses have been carried out by LA-ICPMSat the Department of Earth Sciences, University of Perugia, using a New Wave UP213 LA system coupled with a Thermo Electron X7 (Thermo Electron Corporation, Waltham, USA)
ICP-MS. A 60 micrometres laser beam has been used. Details on analytical methods are reported by Petrelli et al. (2007, 2008). Precision expressed as standard relative deviation is better that 5% foralmost all elements, except Cr
and Ho (.7%).
COMPOSITIONAL VARIATIONS OF MAGMAS IN THE AEOLIAN ARC 503
along-arc variation of some ITE ratios is reported in Figure 15.9.
The predominant features observed on diagrams are as follows.
(1) There is an evident increase of Rb/Nb and several other
LILE/HFSE ratios (e.g. La/Nb, Ba/Nb, U/Nb and, to a
lesser extent, Rb/Ta) from the marginal islands of Alicudi
and Stromboli to the central islands, where a large scattering
is observed for Vulcano.
(2) LILE/LILE ratios also show considerable variation along the
arc. For instance, Ce/Pb decreases eastwards and exhibits a
large scattering at Lipari. Sr/Nd and Sr/Th (not shown)
ratios are lower at the arc margins, especially at Stromboli,
than in the central islands (Fig. 15.9c). Ba/La increases
from Alicudi to Filicudi and other central islands, reaching
a maximum at Stromboli which also shows a large range of
values (Fig. 15.9d).
(3) HFSE/HFSE ratios Nb/Zr (Fig. 15.9e), Zr/Ti and, to a lesser
extent, Nb/Ta (not shown) decrease from marginal to central
islands. Nb and Zr abundances, but also LREE abundances
and La/Yb ratios, show the same type of distribution (not
shown).
(4) Th/LREE ratios (Fig. 15.9f) remain fairly constant in the CA
rocks of the western-central arc and increase in the Vulcano
shoshonitic rocks and at Stromboli.
(5) The Marsili volcano, sited in a back-arc position NW of the
Aeolian archipelago, shows a wide range of compositions but
is close to the western island of Alicudi for many ITE ratios.
Most trace element ratios of Figure 15.9 are not affected by frac-
tional crystallization since they are equally incompatible in the
main igneous rock minerals. Also, they do not show significant
correlation with Sr isotopes in the contaminated Alicudi and
Primordial Vulcano mafic suites. It is therefore reasonable to con-
clude that the observed along-arc variations reflect a compositional
zoning of the mantle source. Understanding the processes that gen-
erated these variations is crucial for clarifying key aspects of the
Aeolian subduction factory.
Mantle metasomatism
At least three different end-members are considered to have con-
tributed to the source composition of the Aeolian magmas.
These include the pre-metasomatic mantle, the Ionian subducted
crust and the Ionian Sea sediments. The composition of each end-
member is internally variable and poorly known. The upper mantle
beneath the southern Tyrrhenian Sea has a mid-ocean-ridge basalt
(MORB-) to OIB-type composition, based on geochemistry of
magmas erupted in and around the Tyrrhenian Sea basin (Trua
et al. 2004, 2011). Subducted Ionian crust has been hypothesized
to have an oceanic to thinned continental character, and a lateral
variation in composition has been suggested (Doglioni et al.
2001). Sediments are abundant on the Ionian seafloor, but inade-
quately characterized compositionally. For this reason, a geochem-
ical study of Ionian sediments has been undertaken and
preliminary data are reported as a spider-diagram in Figure 15.5d.
The concomitant increase of Sr- and decrease of Nd-isotope
ratios from the western to eastern Aeolian arc have been inter-
preted as evidence for eastwards increasing contamination of the
mantle source by subducted upper crustal material, likely
0
5
10
15
Rb/Nb
0
5
10
15
Ce/Pb
0.0
0.1
0.2
0.3
Nb/Zr
Etna basalts Ionian sediments Tyrrhenian MORB
10
20
30
40
Ba/La
10
20
30
40
50
60
Sr/Nd
West East West East
Alicudi
Filicudi
Salina
Lipari Vulcano
Panarea
Stromboli
Marsili
Marsili
Alicudi
Filicudi
Salina
Lipari
Vulcano
Panarea
Stromboli
0.1
0.2
0.3
0.4
0.5
Th/La
(a)(b)
(c)(d)
(e)(f)
Fig. 15.9. Regional variation of trace
element ratios for the newly analysed
Aeolian samples (Table 15.1). Average
compositions of Tyrrhenian MORB
(Dietrich et al. 1977), Etna (Viccaro &
Cristofolini 2008) and Ionian sediments (De
Astis, unpublished data) are also reported.
A. PECCERILLO ET AL.504
sediments (e.g. Ellam et al. 1988, 1989; Francalanci et al. 1993,
2004, 2007; De Astis et al. 2000; Peccerillo 2005). The new ana-
lyses of Ionian sediments show Sr concentrations of c. 200 ppm
and
87
Sr/
86
Sr of c. 0.711. Assuming a bulk mixing between a
primordial-type mantle and such sediments, an addition of less
than 2% contaminant is sufficient to explain the entire range of iso-
topic variation along the western-central Aeolian arc (Fig. 15.7).
Much higher amounts of c. 4– 10% are necessary to explain the
composition of the Stromboli mantle sources. These are
maximum values because shallow-level magma contamination
likely contributed to increase Sr isotope ratios of Aeolian
magmas, including the mafic magmas. Moreover, bulk mixing is
not a viable mechanism of mantle contamination, and hydrous
fluid or melts from sediments have been suggested as the likely
carriers of incompatible elements into the mantle wedge
(Hermann & Rubatto 2009). These are much richer in Sr than
the source rocks because of low solid/fluid partition coefficients
for Sr at high pressures (Hermann & Rubatto 2009). This consider-
ably decreases the amount of contaminant that would be necessary
to explain the Sr-isotope ratios observed along the arc. For
instance, if a melt formed by 30 – 50% sediment melting is
assumed as metasomatic agent, Sr concentration in the melt
would be 2– 3 times higher than the source rock. This reduces
the amount of mantle contaminant by a factor of 2 –3, and less
than 1% melted sediment is sufficient to explain Sr-isotope ratios
of the western-central arc and only 2 – 5% would be needed at
Stromboli.
In conclusion, two types of metasomatic agents, likely fluids, are
suggested by Sr-isotope modelling in the Aeolian arc. One type of
fluid, operating in the western-central arc, had low Sr isotope ratios
and was likely released from an oceanic slab with little or no sedi-
ment involvement. Another fluid was enriched in radiogenic Sr and
requires an important contribution from sediments in the eastern
sector of the arc. Following Hermann & Rubatto (2009), the
term ‘fluid’ is used here in its broadest sense, that is, to indicate
aqueous fluids (water-rich fluid containing low amount of
solute), H
2
O-rich silicate melts and supercritical H
2
O-silicic
fluids (intermediate between the two).
The hypothesis of two compositionally distinct metasomatic
fluids is supported by incompatible trace element ratios such as
Ba/La, Th/Sr, Th/Pb, Th/U, Ba/La, Ti/Zr and Sr/Nd, which
all show diverging trends for Stromboli and for the central-western
islands (e.g. De Astis et al. 2000). Variations for some of these
ratios are reported in Figure 15.10
The nature of metasomatic fluids and the efficiency of element
transfer from slab to the mantle wedge is controversial. This is
true not only for the Aeolian arc, but for subduction magmatism
at a global scale (Brenan et al. 1995; Elliot et al. 1997; Becker
et al. 2000; Kessel et al. 2005; Hermann & Rubatto 2009).
Investigation of MORB-type rocks (Kessel et al. 2005) demon-
strated that the capacity of elemental transport increases with
increasing temperature and pressure from aqueous fluids to
supercritical fluids and melts. LILE/LILE ratios such as Rb/Sr,
Ba/La and Ba/Rb are more easily fractionated by aqueous fluids
than by high-temperature supercritical fluids and melts.
However, hydrous melts and supercritical fluids more efficiently
fractionate other element ratios such as Sr/REE and La/Yb.
LILE/HFSE are fractionated by all types of fluids, but low-
temperature aqueous fluids are less able to transfer large
amounts of trace elements than high-temperature supercritical
fluids and melts. High LILE/HFSE ratios coupled with low ITE
abundances (e.g. Th) have therefore been suggested as useful cri-
teria to recognize aqueous fluid metasomatic modifications (Kessel
et al. 2005).
Hermann & Rubatto (2009) suggested that subducted sediments
are the most important sources of incompatible elements for meta-
somatic fluids in subduction zones. The involvement of sediments
in the subduction processes considerably complicates the process
of slab to mantle element transfer however, due to the possible
occurrence of a large variety of major and accessory residual
phases such as phengite, rutile, allanite/monazite and zircon.
Their stability or breakdown at various pressure/temperature (P/
T) conditions influences the composition of fluids emitted from
the slab and hence the flux of incompatible trace elements into
the overlying mantle wedge. For instance, two- to five-fold Ba/
La variations can be generated in melted sediments and transferred
to the mantle wedge from these, depending on the occurrence or
absence of phengite and monazite in the residue. Note that high
Ba/La is traditionally considered a typical signature of low-
temperature metasomatic aqueous fluids (Brenan et al. 1995;
Elliott et al. 1997).
The intrinsic complexities of element transfer from slab to
mantle wedge, along with the poorly known compositions of end-
members involved in the Aeolian subduction processes, make it
difficult to understand mechanisms of element mobilization and
the contribution of various components to mantle wedge compo-
sition. This has fed much speculation and debate; for example,
Tonarini et al. (2004) suggested an increase of both aqueous
fluid flow and sediment input from west to the east, on the basis
of an eastwards increase of B/Nb and d
11
B of lavas. This is sup-
ported by an eastwards decrease of Ce/Pb, typical of aqueous
fluids, and an increase in Th/La, which is high in the sediments
(Fig. 15.9f). However, LILE/HFSE show a decrease from
central arc to Stromboli, that is, the opposite to that expected for
aqueous fluid metasomatism.
Francalanci et al. (1993, 2007) argued that an increase of LILE/
HFSE from external to central islands was related to a stronger role
of metasomatism by aqueous fluids in the central arc. However,
this idea only holds if a homogeneous composition of pre-
metasomatic mantle wedge is assumed for LILE/HFSE. More-
over, high mobile/immobile element ratios (e.g. Rb/Th) should
be coupled with low immobile element (e.g. Th) enrichments
(Kessel et al. 2005). This is not observed in the central Aeolian
arc, except perhaps at Salina. Finally, variations of HFSE/HFSE
Etna basalts Ionian sediments Tyrrhenian MORB
10 20 30 40
0.703
0.704
0.705
0.706
0.707
0.708
87Sr/86Sr
Ba/La
10
20
30
40
50
60
Sr/Nd
10 30
40
c
20
Ba/La
(a)(b)Fig. 15.10. Ba/La, Sr/Nd and
87
Sr/
86
Sr
variation diagrams for the newly analysed
rocks. Sr isotope data are from the literature
(source of data as in Fig. 15.2) and have been
determined either on the same rocks
analysed in this study or on different rock
samples from the same outcrops.
Composition of the Tyrrhenian MORB,
Etna and Ionian sediments are also reported.
Arrows indicate effects of metasomatic
fluids derived from oceanic crust (grey
arrow) and from sediments (white arrow).
Symbols as in Figure 15.4.
COMPOSITIONAL VARIATIONS OF MAGMAS IN THE AEOLIAN ARC 505
ratios (Fig. 15.9e) are also difficult to explain, in that this group of
elements is immobile during aqueous fluid transfer. Therefore,
aqueous fluid transfer may have been present in the central
Aeolian arc, but it cannot be the only process responsible for the
observed trace element variations.
Many of the issues mentioned above are overcome if a hetero-
geneous OIB- to MORB-type starting mantle composition is
assumed for the Aeolian arc (Ellam et al. 1988). An OIB-type com-
ponent under the external islands could explain enrichment in Nb
and LREE, as well as the relatively high Nb/Zr and low Rb/Nb
and Sr/Nd ratios. By contrast, a MORB-type composition for
the central arc better explains the low Nb/Zr and Zr/Ti.
However, several issues still remain unresolved. For instance,
variations of Ba/La (Fig. 15.10) cannot result from any shallow-
level magmatic evolution process. By contrast, Sr/Nd ratios
can change during crystal fractionation if plagioclase is involved;
however, the positive correlation with Ba/La in the western-
central islands excludes this possibility (Fig. 15.10a). The covari-
ation of Ba/La and Sr/Nd in the central-western arc is therefore
a reproduction of source heterogeneity, and can be attributed to
metasomatic fluids from an oceanic slab (grey arrows in
Fig. 15.10). The slight positive trend between Sr/Nd and
87
Sr/
86
Sr could indicate modest sediment involvement, but
might also reflect a variably altered oceanic crust as source of
fluids. Positive correlation between Ba/La and
87
Sr/
86
Sr at Strom-
boli fits well with the hypothesis of metasomatism by low-
temperature (about 700– 800 8C) hydrous melts from sediments
(white arrows in Fig. 15.10), which have high Ba/La because of
residual LREE-rich accessory phases (Hermann & Rubatto
2009). However, experimental data clearly show that these melts
also have high Sr/Nd, and a positive correlation between the
two ratios should be observed. Instead, the almost flat trend for
Stromboli rocks (Fig. 15.10a) requires a selective Ba enrichment
that increases Ba/La but not Sr/Nd and other ITE ratios. Tomma-
sini et al. (2007) suggested a two-stage enrichment process for the
Stromboli mantle an hypothesis supported by Schiavi et al. (2012)
on the basis of trace element and Pb-B-Li isotope data on melt
inclusions. Early high-P/T supercritical fluids from basalts and
sediments produced a general enrichment in all lithophile
elements, with little element fractionation. An aqueous fluid at
lower P/T selectively enriched the mantle wedge in Ba (see Fran-
calanci et al. 2013). However, other element ratios that are strongly
affected by fluid transport (e.g. U/Nb, Rb/Th, U/Ta, U/Th, etc.)
should be correlated with Ba/La, a feature that is not observed in
the Stromboli rocks.
Conditions of mantle melting and the origin of calc-alkaline and
shoshonitic magmas
The distribution of calc-alkaline and shoshonitic magmas in space
and time has received considerably less attention in the literature
than trace elements and isotope geochemistry. Calc-alkaline rocks
have comparable composition as shoshonites for several major
and trace elements (Fig. 15.3), but shoshonites have higher con-
centrations of K, P and all incompatible trace elements. Some
shoshonites are undersaturated in silica, with up to 10% of nor-
mative nepheline, whereas calc-alkaline rocks are saturated to
oversaturated in silica. These differences can depend either on a
heterogeneous source and/or on variable degrees and physico-
chemical conditions of partial melting.
REE geochemistry can help to clarify this issue. Light REE frac-
tionation (i.e. La/Sm) of primary magmas depends on the degree
of melting and/or on the La enrichment of the source. Heavy
REE (HREE) fractionation (i.e. Tb/Yb) depends essentially on
the presence or absence of residual garnet during mantle
melting. Garnet is a high-pressure mantle mineral that retains
HREE with respect to the light and mid REE. Its occurrence as
residual phase during partial melting therefore results in high
Tb/Yb (and La/Yb) in the magmas. La/Sm increases slightly
with magma evolution; only mafic rocks should therefore be con-
sidered for constraining source processes.
The La/Sm v. K
2
O diagram for the most mafic among the ana-
lysed rocks (MgO .4 wt%) shows that Filicudi, Salina and
Lipari have similar La/Sm ratios, but higher values are observed
at Alicudi and in some CA samples from Stromboli (Fig. 15.11a).
Since all these rocks have the same petrological characteristics, it
is reasonable to assume an origin by comparable degrees of
mantle melting. Higher La/Sm ratios in the CA rocks of the
two external islands therefore point to a stronger enrichment of
LREE in their mantle sources. At Vulcano, there is an increase
of La/Sm from CA to SHO rocks at fairly constant Sr-isotope
ratio (De Astis et al. 1997). By contrast, La/Sm ratios do not
change significantly from CA to SHO rocks at Stromboli,
whereas
87
Sr/
86
Sr ratios increase strongly (Francalanci et al.
1988). These data suggest that HKCA and SHO magmas at
Vulcano could be related to variable degrees of partial melting
of a homogeneous source, whereas CA and SHO magmas at
Stromboli are generated by similar degrees of partial melting of
a isotopically heterogeneous source that was variably contami-
nated by subducted sediments. The obvious conclusion is that
SHO magmas are generated by different processes in the
Aeolian arc as already suggested by Ellam et al. (1988) and De
Astis et al. (2000). Finally, Tb/Yb ratios are generally high in
all shoshonites. This points to the occurrence of residual garnet
in the source during melting and, hence, to a deeper origin for
SHO than the associated CA magmas.
The physical conditions that generated variable degrees of
melting for CA and SHO magmas in the central Aeolian arc are
of interest for petrology and geodynamics. It is well known that
water is crucial to promote partial melting in the subduction
environments (e.g. Ulmer 2001; Grove et al. 2012). Variable
degrees of melting in the Aeolian arc could therefore be related
to different fluxes of water from the slab. These were higher
MgO > 4%
0 1 2 3 4 5
0.1
0.2
0.3
0.4
0.5
0.6
0.7
Tb/Yb
0 1 2 3 4 5
3
4
5
6
7
8
9
10
La/Sm
K2O wt% K2O wt%
(a)(b)
Fig. 15.11. La/Sm and Tb/Yb v. K
2
O
diagrams for the most mafic among the
analysed samples (MgO .4 wt%). Plots
are restricted to mafic compositions to
minimize effects of La/Sm variation related
to fractional crystallization. For further
explanation see text. Symbols as in
Figure 15.4.
A. PECCERILLO ET AL.506
during calc-alkaline magma activity, and were less abundant in
the zones and times of shoshonitic magma formation. Variable
water fluxes could be tentatively attributed to different stages of
subduction process. Noting that shoshonitic magmas appear
during mature to late stages of volcanism, it is reasonable to pos-
tulate a decrease of water flux with time.
Pre-metasomatic mantle composition
Gaining insight into the original composition of the upper mantle
beneath the Aeolian Islands is difficult, due to extensive modifi-
cation produced by metasomatic processes. This is however an
important step to a better understanding of mantle source evolution
and geodynamic setting in the southern Tyrrhenian Sea. Ellam
et al. (1988) hypothesized an OIB- to MORB-type composition
for pre-metasomatic mantle, and suggested that HFSE enrichment
in some islands was evidence for the occurrence of the OIB com-
ponent in the sub-arc mantle. Such a hypothesis also explains the
linear Pb-isotope arrays between the Calabro – Peloritano base-
ment and the OIB-type Etna volcano (Fig. 15.6b), which suggest
contamination of an OIB-type source by subducted crustal
material. By contrast, Francalanci et al. (2007) and Tommasini
et al. (2007) envisage a homogeneous MORB-type pre-
metasomatic mantle along the entire arc, and explain the regional
geochemical and isotopic variations as entirely related to variable
roles of aqueous and supercritical fluids or melts from an altered
oceanic crust and associated sediments. Accordingly, radiogenic
Pb-isotope signatures observed in some islands were explained
as the result of metasomatism by fluids released from sediments
and aged Ionian oceanic crust.
The data and discussion presented in this paper support the
hypothesis of a zoned OIB- to MORB-type pre-metasomatic
mantle for the Aeolian arc. In particular, an OIB-type component
in the marginal islands would explain both high HFSE contents and
LREE abundances and fractionation. Variable HFSE ratios are also
better explained by pre-metasomatic mantle heterogeneities, since
these elements behave as immobile during metasomatism.
Francalanci et al. (2007) argued that the OIB-type nature of the
external islands conflicts with the low Pb-isotope ratios of Alicudi
and Stromboli, as compared to those of the central island of Salina.
However, relatively unradiogenic Pb compositions at Stromboli
are an effect of contamination of the mantle source by sediments,
which completely altered its original Pb-isotope signature. A
decrease of
206
Pb/
204
Pb ratios from Salina to Alicudi is only
observed if the Alicudi basalts are considered as the most primitive
compositions in the island. However, it has long been demon-
strated that the Alicudi basalts are more contaminated than the
associated andesites (Peccerillo & Wu 1992; Lucchi et al.
2013a). Therefore, if more evolved but uncontaminated andesites
are considered, Pb-isotopic values at Alicudi are similar to those at
Salina.
Geodynamic implications
There are important relationships between magma and mantle
compositions and the geodynamic setting of the Aeolian arc. The
diversity of the mantle contamination processes in the western-
central and eastern sectors suggests a different nature for the
subducted material. A basaltic slab, with little or no sediment invol-
vement, is indicated by geochemical data as a source of metaso-
matic fluids in the western-central islands, whereas an important
contribution by subducted sediments or other upper crustal
materials is required for metasomatism at Stromboli. The
Tindari– Letojanni Fault therefore represents the boundary that
divides two distinct compositions of the subducted material. Such
a conclusion is also suggested by Doglioni et al. (2001), although
these authors propose a continental-type crust in the west and an
oceanic-type crust in the east, a conclusion that strongly contrasts
with radiogenic isotope signatures of the Aeolian magmas.
Metasomatic fluids activated extensive modification of the
upper mantle beneath the Aeolian volcanic arc. However, some
geochemical signatures of the pre-metasomatic mantle were pre-
served, and indicate a depleted MORB-type source in the central
sector and a more fertile OIB-type component for the external
islands.
Peccerillo (2001) argued that the OIB-type component at Strom-
boli could have originated by inflow of asthenospheric mantle from
the Africa foreland around the margins of the retreating slab. Trua
et al. (2004, 2011) envisaged the same type of process to explain
the occurrence of MORB and OIB components at Marsili. Franca-
lanci et al. (2007) and Tommasini et al. (2007) consider the
hypothesis of mantle flow as unrealistic, a statement that does
not take into account the particular geodynamic setting of the
Aeolian arc. Here, a narrow Ionian slab is subducting beneath
the southern Tyrrhenian Sea (Fig. 15.12) and is retreating toward
the SE (Gvirtzman & Nur 1999), generating deep seismic activity
beneath the eastern Aeolian arc. In contrast, deep seismicity is
lacking beneath the western Aeolian arc, a feature that could be
related to collision and slab break-off in this sector where a frag-
ment of oceanic slab is suggested to passively sink into the
upper mantle (see Peccerillo 2005; Panza et al. 2007 for further
details).
It is well known that the Benioff zone rollback requires mantle
flow to replace the space left by the retreating slab. Such a replace-
ment can occur by mantle flow from the back-arc area. However,
for a narrow slab such as that in the southern Tyrrhenian Sea
most of the asthenospheric inflow likely occurs from the foreland,
moving around the margins of the retreating slab (Fig. 15.12). The
mantle sources at the margins of the slab are therefore the most
heavily affected by inflow and consequently show the clearest evi-
dence of OIB-type components. It should be recalled that all vol-
canoes situated on the margin of the African plate (e.g. Etna,
Iblei, Linosa, etc.) have an OIB-type composition.
Fig. 15.12. Schematic geodynamic setting of the Aeolian arc. A narrow Ionian
plate is subducting beneath Calabria and the southern Tyrrhenian Sea. This is
associated with deep seismicity and active volcanism, and is bounded to the
west by the Tintari– Letojanni Fault (TLF) system. A detached and passively
sinking oceanic slab is envisaged for the western Aeolian arc. Curved black
arrows indicate asthenospheric mantle inflow from the foreland around the
margins of the subducted slabs. Collision zones are indicated with a dashed line.
For further explanation, see text.
COMPOSITIONAL VARIATIONS OF MAGMAS IN THE AEOLIAN ARC 507
Conclusions
The overall petrological and geochemical features of the Aeolian
arc and the relationships with petrogenesis and geodynamics can
be summarized as follows.
(1) CA and HKCA rocks make up all the western islands and the
largest part of Lipari and Panarea, whereas HKCA and SHO
rocks are dominant at Vulcano and Stromboli. Shoshonitic
rocks from these islands have similar compositions for
many major and many trace elements, but exhibit strong
differences for radiogenic isotopes (Sr– Nd –Pb) and some
trace element abundances and ratios. This suggests that
shoshonitic magmatism in the Aeolian arc is polygenetic. In
particular, decreasing degrees of partial melting of a homo-
geneous source at various depths generated the transition
from high-K calc-alkaline to shoshonitic magmatism at
Vulcano. At Stromboli, calc-alkaline and shoshonitic mag-
mas are related to polybaric melting of heterogeneous man-
tle sources that were variably contaminated by subducted
sediments.
(2) There are distinct Sr-, Nd- and Pb-isotope signatures in
different sectors of the arc. Some incompatible trace
element ratios also show diverging variation trends. Differ-
ent types of mantle metasomatic processes have been respon-
sible for these features. Metasomatic fluids affecting the
western-central arc originated from a subducted basaltic
crust, whereas upper crustal material (likely oceanic-type
crust plus sediments) was a main source of metasomatic
fluids under Stromboli.
(3) Modification by metasomatic fluids was superimposed on a
heterogeneous OIB- to MORB-type pre-metasomatic
mantle wedge. An OIB-type component in the source is
recognized for the external islands of Alicudi and Stromboli
and for the Marsili seamount, but not in the central Aeolian
arc where a depleted MORB-type mantle composition is
suggested by rock chemistry. The OIB-type component
was provided by asthenospheric inflow from the Africa fore-
land, around the edges of the slab during rollback.
(4) Aeolian arc magmas were affected by complex evolution
processes which drove parental basalts towards intermediate
and acidic compositions. The degree of magma evolution
was much more extensive in the central islands of Lipari
and Vulcano, where abundant rhyolites were erupted
during the latest activity stages. This is related to the trans-
tensional tectonics along the Tindari – Letojanni transfer
fault, which favoured the formation of large intra-crustal
magma chambers where magmas ponded and fractionated
for a long time to give abundant rhyolitic melts.
(5) Geobarometric investigations revealed polybaric magma
evolution processes for the Aeolian volcanoes. Early basaltic
activity, which characterized the lowest exposed sequences
on most islands, was fed by deep magma chambers in
which magmatic evolution was dominated by fractional crys-
tallization and assimilation plus continuous mixing with
fresh mafic melts from the source. Younger andesitic and
rhyolitic activity was fed by shallower magma chambers,
where magmatic evolution was dominated by fractional crys-
tallization. An overall upwards migration for magma
chambers of the Aeolian volcanoes is therefore suggested
by geobarometric investigations.
Research on Aeolian orogenic magmatism has been financed by MIUR,
PRIN2008. The authors thank J. Hermann, ANU, R. Harmon and an anonymous
referee for constructive reviews.
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