Extensional tectonics on Sardinia (Italy): insights into the arc–back-arc transitional regime
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Transcript of Extensional tectonics on Sardinia (Italy): insights into the arc–back-arc transitional regime
Extensional tectonics on Sardinia (Italy): insights into
the arc–back-arc transitional regime
Claudio Faccenna a,*, Fabio Speranza b, Francesca D’Ajello Caracciolo a,Massimo Mattei a, Giacomo Oggiano c
aDipartimento di Scienze Geologiche, Universita di ‘‘Roma Tre,’’ Largo San Leonardo Murialdo 1, 00146 Rome, ItalybIstituto Nazionale di Geofisica e Vulcanologia, Rome, Italy
cIstituto di Scienze Geologico–Mineralogiche, Universita di Sassari, Sassari, Italy
Received 4 December 2001; accepted 17 May 2002
Abstract
Although the tectonic features and stress regime typical for accretionary complexes and back-arc domains have been widely
documented so far, few are known on the transitional zone separating these two systems. Here we report on structural analysis
and anisotropy of magnetic susceptibility (AMS) results from Eocene–Pliocene sediments exposed in western Sardinia. From
late Oligocene to middle Miocene, the studied area was located between the Alpine–Apennine wedge to the east, which was
undergoing shortening and accretion, and the Liguro–Provenc�al basin, undergoing extension and spreading. We find that, prior
to the formation of the Liguro–Provenc� al basin, the middle Eocene– lower Oligocene sediments cropping out at the
southwesternmost edge of Sardinia were subjected to NE–SW shortening (in present-day coordinates), in agreement with
recently reported geological information. Conversely, the upper Oligocene–Pliocene sedimentary sequences record a different
evolutionary stage of extensional processes. Upper Oligocene–middle–upper Burdigalian sediments clearly show a N–S-
oriented magnetic lineation that can be related to extensional direction along the prevalent E–W-oriented normal faults. On the
other hand, no magnetic lineation has been detected in upper Burdigalian–Serravallian sediments, which mark the end of the
first rifting process in Sardinia, which likely coincides with the rift-to-drift transition at the core of the Liguro–Provenc�al basin.Finally, a NE–SW extension is observed in two Tortonian–Pliocene sites at the northwestern margin of the NNW–SSE-
oriented Campidano graben. Our study confirms that AMS may represent a valuable strain-trajectory proxy and significantly
help to unravel the characters of temporally superimposed tectonic events.
D 2002 Elsevier Science B.V. All rights reserved.
Keywords: Back-arc basin; Magnetic anisotropy susceptibility (AMS); Sardinia; Mediterranean area
1. Introduction
The subduction process is associated with contrast-
ing styles of back-arc deformation that produces
mountain chains or extensional basins (Uyeda and
Kanamori, 1979; Jarrard, 1986). In the latter case, the
state of stress is expected to switch from compression
near the trench, where accretion of underthrusted
0040-1951/02/$ - see front matter D 2002 Elsevier Science B.V. All rights reserved.
PII: S0040 -1951 (02 )00287 -1
* Corresponding author. Tel.: +39-654-888-029; fax: +39-654-
888-201.
E-mail addresses: [email protected] (C. Faccenna),
[email protected] (F. Speranza).
www.elsevier.com/locate/tecto
Tectonophysics 356 (2002) 213–232
sediments predominates, to extensional process near
the volcanic arc. In addition, extensional and com-
pressional directions in the different sectors of the
trench–arc system are expected to be subparallel and,
when subduction zones is not oblique, back-arc basins
usually extend perpendicularly to the direction of
trenches. The transition between those two domains
is poorly documented. Nakamura and Uyeda (1980)
first describe the presence of an ‘‘intermediate’’ strike-
slip regime in the area located between the trench and
the back-arc region. This is theoretically consistent
with a gradual change in the magnitude of the stress
tensor, but with one of the principal axes always
oriented parallel to the main direction of tectonic
motion.
In this paper, we will focus on a well-documented
example of a transitional regime, between compres-
sion at the trench and extension in the back-arc area.
Our analysis has been carried out in Sardinia. Sardinia
is located in the middle of the Mediterranean region
(Fig. 1) and has been extended and rifted apart from
the Iberian Peninsula during the opening of the
Liguro–Provenc�al basin, between 30 and 15 Ma
(Cherchi and Montadert, 1982). The southeastward
lateral drift and simultaneous counterclockwise rota-
tion of Sardinia is the consequence of the retreat of the
trench, presently active below Calabria (Malinverno
and Ryan, 1986), contemporaneously with accretion
and thrusting of the Apennine chain units (Patacca et
al., 1990).
We reconstruct the extensional direction during
the drifting and rotation of the Sardinia block
using the anisotropy of magnetic anisotropy sus-
ceptibility (AMS) and the analysis of fault popu-
lations, affecting Eocene–Pliocene sedimentary
deposits.
Fig. 1. Map of the central–western Mediterranean region showing volcanism and the Oligocene-to-present kinematics derived from the analysis
of deformation. Numbers describe the age of initiation and end of extension in the various basins. For a review of the data shown here, see
Jolivet and Faccenna (2000).
C. Faccenna et al. / Tectonophysics 356 (2002) 213–232214
Confirming previous reconstruction (Thomas and
Gennesseaux, 1986; Funedda et al., 2000), our results
show that western Sardinia was subjected to two main
extensional episodes. The first was between 25 and 18
Ma (late Oligocene–middle late Burdigalian) where
the island extended roughly NS (in present-day coor-
dinates), along an overall direction oriented parallel to
the trench and orthogonal to the back-arc extension in
the more internal Liguro–Provenc�al area. This epi-
sode was followed since 18 Ma (late Burdigalian–
Messinian) by another extensional episode different
from the previous not only in the direction (extension
EW and NS elongated basins) but also in that sub-
sidence is less intense. Afterwards, during the last 10
my, Sardinia underwent again a SW–NE extensional
episode, inducing the formation of the present-day
depression of the Campidano graben. These results
basically confirm that the Sardinia rifted area (the so-
called Sardinia trough) is the result of superimposed
extensional/transtensional episodes (Thomas and Gen-
nesseaux, 1986; Carmignani et al., 1995). However,
the direction of extension inferred here and the related
interpretation are in conflict with previous studies
(e.g., Cherchi and Montadert, 1982; Letouzey et al.,
1982), which propose that the first extensional (and
main) event was E–W directed.
2. Geological setting
Sardinia is a continental block surrounded by Neo-
gene ocean-floored basins: the Liguro–Provenc�albasin to the west and the Tyrrhenian Sea to the east
(Fig. 1). They opened in different times, first the
Liguro–Provenc�al (between 30 and 15 Ma) and then
the Tyrrhenian Sea (between 10–12 Ma and present).
The two basins share characters of back-arc basins
(Malinverno and Ryan, 1986), as attested by anom-
alous heat flow (Cataldi et al., 1995; Chamot-Rooke
et al., 1999), depth, volcanic suite (Beccaluva et al.,
1985, 1989), the presence of a Wadati–Benjoff zone,
presently active below Calabria (Selvaggi and Chiar-
abba, 1995), and by the fact that extensional process
occurred contemporaneously to wedge accretion in
the Apennine chain (Patacca et al., 1990). Geological
and paleomagnetic data indicate that Corsica–Sardi-
nia drifted apart from the Catalan–Provenc� al coastduring the opening of the Liguro–Provenc�al basin and
the retreat of the trench occurring between 21 and 15
Ma (Van der Voo, 1993; Vigliotti and Langenheim,
1995; Speranza, 1999; Deino et al., 2001). Over the
course of this rapid migration (up to 4–5 cm/year), the
Corsica–Sardinia block was left back in its present-
day position whereas the Calabrian block was carried
along with the retreating trench.
The presence of a continental block in the middle
of the Mediterranean offers an opportunity to inves-
tigate the way the extensional process related to back-
arc opening evolved with time during the episodic
rifting and drifting, and the way the deformation
evolved from the trench area towards the back-arc
region.
The Sardinia ‘‘trough’’ zone is a 55-km wide, 220-
km long roughly N–S elongated depression (Fig. 2),
filled up by more than 1000 m of clastic and carbonate
sediments, epiclastic, and volcanic rocks consisting of
andesites and dacitic–rhyolitic ignimbrites and tuffs
(Cherchi and Montadert, 1982; Assorgia et al., 1997).
Most of the pre-rift basement rocks are constituted of
Paleozoic metamorphic rocks deformed during the
Hercynian orogeny, upper Carboniferous–Permian
granitoids and Mesozoic platform carbonates deposits.
The trough itself results from by the interferences of
several, half-graben and strike-slip basins, mainly E–
W-oriented (Oggiano et al., 1995). Conversely, in the
eastern Sardinia, the pre-rift basement is cross-cut by
E–NE- and N–S-oriented faults with mainly strike-
slip and normal motion, respectively (Carmignani et
al., 1994).
The oldest marine sedimentary cycle, upper Pale-
ocene in age (Barca and Costamagna, 2000), uncon-
formably overlying the Mesozoic units, has been
drilled in the southwesternmost Sardinia (Sulcis). It
is followed by a slow regression and deposition of
lower–middle Eocene supratidal and paralic facies
limestones (Cherchi, 1983), affected by a system of
thrusts likely related to the Pyrenean orogeny (Barca
and Costamagna, 1997). These deposits are uncon-
formably covered by continental deposits of the
Cixerri Formation, formed by middle Eocene (Lute-
tian)– lower Oligocene conglomerates, sandstones,
and reddish silty sandstones sealing the main thrust
system (Barca and Costamagna, 1997), and covered
by volcanics dated between 28 and 30 Ma (Bellon et
al., 1977). The paleotectonic framework of the Cixerri
Formation is still debated, even if it is commonly
C. Faccenna et al. / Tectonophysics 356 (2002) 213–232 215
considered as a ‘‘molassic’’ deposits related to the
Pyrenean orogenic system (Cherchi, 1983; Barca and
Costamagna, 1997, 2000).
Four marine sedimentary cycles mark the onset of
the extensional process in Sardinia. All of them are
accompanied by volcanic activity.
Fig. 2. Geological map of Sardinia. The sites of structural and AMS analysis and the in situ magnetic lineation direction are also shown.
C. Faccenna et al. / Tectonophysics 356 (2002) 213–232216
The first cycle started in the late Oligocene with
continental deposition followed by a local marine
ingression during the late Oligocene–early Aquita-
nian (Marmilla, Anglona, Funtanazza basins), with a
maximum deepening during the Aquitanian–Burdiga-
lian boundary. This sedimentary cycle lasted up to the
middle–upper Burdigalian and until lower Burdiga-
lian in the Anglona area (Francolini and Mazzei,
1991) where it is sealed by continental and pyroclastic
flow and lacustrine deposits (Assorgia et al., 1997,
and references therein). Most of the deposition of
these sediments occurred within E–W to E–NE-
trending basins, as Funtanazza in southwestern Sardi-
nia (site 03 in Fig. 2) or the Castelsardo basin in
northern Sardinia (site 30–35 in Fig. 2) (Francolini
and Mazzei, 1991; Oggiano et al., 1995; Cipollari and
Cosentino, 1997; Sowerbutts and Underhill, 1998). In
NE Sardinia, fine-grained lacustrine sediments with
marine intercalations and continental deposits of the
same age are deposited in the Chilivani–Berchidda
basin (site 36 in Fig. 2), which formed in correspond-
ence of a releasing bend along a major E–NE-trend-
ing strike-slip fault (Oggiano et al., 1995). Gravel and
boulder-sized continental conglomerates were depos-
ited in a similar strike-slip setting, at the border of
positive transpressive structure along the E–NE strik-
ing strike-slip faults of Mt. Albo (Carmignani et al.,
1994; Oggiano et al., 1995).
Upper Burdigalian–lower Serravallian sediments
forming the second marine cycle unconformably over-
lay the older sediments. The maximum deepening of
the sedimentary basin occurred during the early–
middle Langhian–early Serravallian, before a regres-
sive phase, causing the deposition of fluvio-marine
and infralittoral sediments (Martini et al., 1992). This
cycle corresponds to the ‘‘post-rift’’ succession of
Cherchi and Montadert (1982), although NNW–
SSW- and N–S-bearing normal faults control its
deposition within some relatively deep half-grabens.
Such grabens in northern Sardinia cross-cut the pre-
vious extensional/transtensional structures (Sower-
butts and Underhill, 1999; Funedda et al., 2000).
The third marine sedimentary cycle was deposited
during late Serravallian–early Messinian times in a
shelf environment, whereas the fourth and last short
cycle of marine sedimentation consists of by shelf-
environment Pliocene–Pleistocene marls and sandy
clays cropping out in few localities. The last sedi-
mentary cycle is related to the formation of the NNW
narrow and deep Campidano graben (Fig. 2), filled
by several kilometers of Pliocene–Pleistocene sedi-
ments.
In synthesis, the sedimentary cycles appear to be
related with various tectonic regimes, characterised
by different styles and orientation of the main
structures. The detailed reconstruction of these de-
formation episodes and their relationship with the
tectonic framework of the area is far from clear.
Some authors suggest that the first sedimentary cycle
was deposited in a strike-slip environment, related to
N–S compression (Carmignani et al., 1994), whereas
others (Cherchi and Montadert, 1982), relying on
microstructural analyses, proposed a sequence of
compressional and extensional events differently ori-
ented. The difficulty of unraveling the tectonic
evolution is due to the fact that the different de-
positional cycles and superimposed deformational
events obscure the structural architecture of the
basin.
In this framework, AMS results coupled with
microstructural analyses can provide key pieces of
evidence to reconstruct the structural history of this
area. The magnetic fabric has proven to be closely
related to the strain ellipsoid, both in compressional
and extensional regimes (e.g., Sagnotti and Speranza,
1993; Sagnotti et al., 1994, 1998; Scheepers and
Langereis, 1994; Mattei et al., 1997, 1999; Speranza
et al., 1999). Such analyses are of crucial importance
where the rocks are poorly deformed given the
absence or paucity of classical strain markers, and
they can be performed even in small outcrops (Lowrie
and Hirt, 1987). It has been shown that the magnetic
fabric is acquired a short time after the sediment
deposition, during the first tectonic events, and is
hardly modified by subsequent brittle deformational
events (Mattei et al., 1997). This AMS allows us to
separate tectonic phases, occurring in different times,
because it highlights each tectonic event synchronous
to (or shortly following) the deposition of a given
sedimentary unit. Conversely, such partition is often
difficult or impossible by solely using structural
analysis.
We sampled the Eocene–Oligocene Cixerri For-
mation and all the four sedimentary cycles in 36
different sites spread over Sardinia for AMS analyses
(Fig. 2). Seven sites have been drilled in the Cixerri
C. Faccenna et al. / Tectonophysics 356 (2002) 213–232 217
Formation, 16 in the first sedimentary cycle, 11 in the
second cycle, 1 in the third, and 1 in the fourth (Table
1). In each site (apart from site Sa02), we drilled 7 to
17 cores with an ASC-280E petrol-powered drill, and
oriented them in situ with a magnetic compass. In site
Sa02, 87 cores were sampled (Table 1).
3. Results
3.1. Anisotropy of magnetic susceptibility
The low-field magnetic susceptibility (k) of each
sample was measured with a KLY-2 bridge in the
Table 1
List of anisotropy factors computed at each site
Site Age N km L F PV
Sa01: I depositional cycle Lower Burdigalian 13 76.3 (33.3) 1.004 (0.002) 1.052 (0.022) 1.063 (0.026)
Sa02: I depositional cycle Lower Burdigalian 87 112.2 (50.3) 1.004 (0.002) 1.021 (0.012) 1.027 (0.014)
Sa03: I depositional cycle Aquitanian 17 4503.1 (3481.3) 1.004 (0.002) 1.052 (0.022) 1.063 (0.013)
Sa04: II depositional cycle Serravallian–Langhian 12 144.4 (3.5) 1.003 (0.002) 1.030 (0.004) 1.037 (0.005)
Sa05: II depositional cycle Upper Burdigalian 10 108.4 (11.1) 1.002 (0.001) 1.028 (0.004) 1.034 (0.005)
Sa06: II depositional cycle Serravallian 12 135.8 (7.7) 1.003 (0.001) 1.026 (0.005) 1.032 (0.006)
Sa07: Cixerri Formation Eocene–Oligocene 10 201.8 (14.1) 1.008 (0.002) 1.008 (0.002) 1.016 (0.003)
Sa08: Cixerri Formation Eocene–Oligocene 12 225.6 (31.9) 1.004 (0.003) 1.007 (0.002) 1.012 (0.003)
Sa09: Cixerri Formation Eocene–Oligocene 10 115.2 (16.2) 1.003 (0.002) 1.088 (0.249) 1.109 (0.303)
Sa10 Eocene 10 114.2 (10.6) 1.023 (0.003) 1.003 (0.001) 1.029 (0.004)
Sa11: I depositional cycle Lower Burdigalian 12 54.3 (5.7) 1.006 (0.002) 1.061 (0.007) 1.075 (0.008)
Sa12: I depositional cycle Lower Burdigalian 11 67.8 (2.9) 1.004 (0.002) 1.041 (0.003) 1.050 (0.004)
Sa13: I depositional cycle Lower Burdigalian 8 90.0 (18.6) 1.003 (0.002) 1.015 (0.002) 1.020 (0.003)
Sa14: III depositional cycle Tortonian 12 108.5 (3.3) 1.003 (0.002) 1.023 (0.002) 1.029 (0.003)
Sa15: IV depositional cycle Pliocene 8 88.7 (3.3) 1.002 (0.001) 1.024 (0.002) 1.029 (0.003)
Sa16: II depositional cycle Langhian 12 123.4 (8.6) 1.065 (0.007) 1.004 (0.002) 1.078 (0.008)
Sa17: Cixerri Formation Eocene–Oligocene 8 63.9 (15.3) 1.003 (0.002) 1.003 (0.001) 1.006 (0.002)
Sa18: Cixerri Formation Eocene–Oligocene 10 79.7 (7.8) 1.002 (0.001) 1.004 (0.002) 1.006 (0.002)
Sa19: Cixerri Formation Eocene–Oligocene 10 150.4 (21.8) 1.008 (0.004) 1.056 (0.010) 1.070 (0.011)
Sa20: II depositional cycle Upper Burdigalian 9 121.7 (9.7) 1.003 (0.002) 1.019 (0.002) 1.024 (0.002)
Sa21: I depositional cycle Oligocene–Aquitanian 10 201.5 (17.1) 1.003 (0.001) 1.042 (0.014) 1.050 (0.016)
Sa22: I depositional cycle Aquitanian 12 14.6 (3.7) 1.005 (0.003) 1.007 (0.005) 1.012 (0.007)
Sa23: I depositional cycle Oligocene–Aquitanian 10 77.3 (6.7) 1.003 (0.002) 1.030 (0.006) 1.036 (0.007)
Sa24: I depositional cycle Oligocene–Aquitanian 9 140.9 (32.5) 1.005 (0.001) 1.023 (0.003) 1.030 (0.003)
Sa25: I depositional cycle Upper Burdigalian–Langhian 10 81.3 (7.3) 1.003 (0.001) 1.037 (0.003) 1.044 (0.004)
Sa26: II depositional cycle Langhian 11 77.5 (8.6) 1.010 (0.004) 1.029 (0.013) 1.040 (0.017)
Sa27: II depositional cycle Langhian 12 126.4 (4.7) 1.003 (0.001) 1.049 (0.004) 1.058 (0.005)
Sa28: II depositional cycle Langhian 12 79.9 (9.0) 1.002 (0.001) 1.028 (0.003) 1.034 (0.004)
Sa29: II depositional cycle Langhian 10 140.3 (4.5) 1.004 (0.002) 1.031 (0.004) 1.039 (0.004)
Sa30: I depositional cycle Aquitanian 10 88.4 (6.6) 1.004 (0.001) 1.052 (0.005) 1.063 (0.006)
Sa31: I depositional cycle Aquitanian 12 134.1 (20.1) 1.006 (0.009) 1.051 (0.008) 1.064 (0.016)
Sa32: I depositional cycle Oligocene 10 50.1 (12.7) 1.006 (0.005) 1.008 (0.004) 1.014 (0.007)
Sa33: I depositional cycle Aquitanian 9 3137 (436) 1.005 (0.002) 1.033 (0.011) 1.042 (0.013)
Sa34: I depositional cycle Aquitanian 10 131.5 (8.1) 1.001 (0.001) 1.001 (0.000) 1.002 (0.001)
Sa35: I depositional cycle Oligocene–Aquitanian 7 95.7 (7.2) 1.001 (0.001) 1.006 (0.001) 1.008 (0.001)
Sa36: I depositional cycle Oligocene–Aquitanian 7 127.6 (14.8) 1.002 (0.001) 1.014 (0.003) 1.017 (0.002)
N= number of specimens; km=(kmax + kint + kmin)/3 (mean susceptibility, in 10� 6 SI units); L= kmax/kint; F = kint/kmin; PJ = exp{2[(g1� g)2+(g2�g)2+(g3� g)2]}1/2 (corrected anisotropy degree; Jelinek, 1981); T= 2(g2� g3)/(g1� g3)� 1 (shape factor; Jelinek, 1981); S0 = bedding
attitude (azimuth of the dip and dip values); g1 = ln kmax; g2 = ln kint; g3 = ln kmin; g=(g1 + g2 + g3)/3, E1 – 3, E2 – 3, E1 – 2 = semiangles of the 95%
confidence ellipses around the principal susceptibility axes. For each locality, the arithmetic means of the individual site mean values are
shown (standard deviation in parentheses).
C. Faccenna et al. / Tectonophysics 356 (2002) 213–232218
paleomagnetic laboratory of the Istituto Nazionale di
Geofisica e Vulcanologia. The AMS at both the speci-
men and the site level was evaluated using Jelinek
(1978) statistics. In each site, the anisotropy degree and
the shape of the susceptibility ellipsoids were evaluated
by means of the PV and T parameters (Jelinek, 1981),
respectively. The k values are always low ( < 250�10� 6 SI, Fig. 3a and Table 1), except in sites Sa03 and
Sa33 (both Aquitanian in age), where they are as high
as 4503� 10� 6 and 3137� 10� 6 SI, respectively.
As for previous studies performed in clayey–marly
sediments in the Italian peninsula and Sicily (e.g.,
T S0 D, I (kmin) D, I (kmax) E1 – 3 E2 – 3 E1 – 2 Structural analysis
and notes
0.821 (0.141) 310, 15 246, 83 358, 3 3.7 3.1 17.3 no
0.642 (0.214) 64, 21 318, 76 165, 13 5.4 5.3 11.7 yes
0.751 (0.086) 269, 33 97, 59 294, 30 1.6 2.1 11.6 no
0.792 (0.082) not visible 293, 78 146, 10 2.1 2.3 17.4 no
0.885 (0.080) 88, 10 7, 78 277, 0 7.4 2.8 36.4 no
0.815 (0.073) 190, 25 213, 82 111, 2 9.2 4.2 23.0 yes
0.039 (0.244) not visible 22, 82 132, 3 9.0 3.7 26.0 yes
0.342 (0.362) subhorizontal 213, 7 304, 8 6.1 28.0 22.0 yes
0.273 (0.436) not visible 79, 1 348, 40 8.4 19.7 34.0 no
0.757 (0.090) 240, 9 63, 0 154, 77 3.7 19.1 11.3 no– inverse fabric
0.811 (0.073) subhorizontal 162, 89 355, 1 2.1 4.6 11.4 yes
0.839 (0.099) subhorizontal 162, 88 350, 2 2.3 3.9 15.6 no
0.683 (0.189) subhorizontal 295, 80 139, 9 4.6 12.6 72.2 yes
0.756 (0.095) not visible 106, 82 222, 4 2.4 3.3 10.2 yes
0.828 (0.048) 57, 32 313, 59 215, 5 8.9 13.6 26.2 yes
0.886 (0.051) subhorizontal 264, 1 6, 84 2.8 13.5 5.6 no– inverse fabric
0.117 (0.354) not visible 352, 77 102, 5 18.6 26.6 21.8 no
0.285 (0.417) subhorizontal 39, 81 169, 9 6.1 13.8 19.3 yes
0.753 (0.124) subhorizontal 245, 85 360, 2 3.4 6.4 10.8 yes
0.751 (0.141) not visible 278, 29 125, 10 3.6 6.5 53.9 no
0.846 (0.092) 330, 15 231, 73 27, 16 3.4 8.5 25.1 yes
0.118 (0.366) 4, 15 144, 61 31, 12 21.0 45.2 31.0 no
0.819 (0.106) subhorizontal 314, 8 161, 5 2.7 4.7 43.1 no
0.635 (0.12) 2, 24 216, 62 346, 19 2.1 4.2 12.8 no
0.871 (0.064) 76, 8 280, 87 64, 3 2.5 9.6 38.4 no
0.485 (0.123) subhorizontal 299, 68 185, 9 4 12 18 no
0.894 (0.038) subhorizontal 175, 86 56, 2 4 7 59 no
0.840 (0.068) subhorizontal 40, 81 174, 6 4 2 22 no
0.762 (0.137) subhorizontal 186, 83 59, 5 4 4 45 no
0.863 (0.054) subhorizontal 61, 88 186, 1 6 3 21 yes
0.829 (0.174) subhorizontal 187, 87 335, 3 3 4 36 yes
0.118 (0.355) 221, 12 156, 84 269, 2 10 16 21 no
0.699 (0.123) 321, 15 278, 69 62, 17 7 5 49 yes
0.171 (0.427) 332, 15 130, 74 249, 8 15 22 37 no
0.656 (0.249) 326, 18 33, 84 182, 5 9 8 42 yes
0.777 (0.182) subhorizontal 136, 82 243, 2 5 6 11 yes
C. Faccenna et al. / Tectonophysics 356 (2002) 213–232 219
Scheepers and Langereis, 1994; Sagnotti et al., 1998;
Speranza et al., 1999), the question arises as to
whether the measured fabric reflects the anisotropy
of the clay matrix minerals, the ferrimagnetic miner-
als, or both. Sagnotti et al. (1998) and Speranza et al.
(1999) observed that the low-field susceptibility (and
AMS) is likely to be significantly influenced by the
ferrimagnetic susceptibility only when the k values are
higher than 200� 10 � 6 to 300� 10 � 6 SI. The
ferrimagnetic mineral susceptibility adds to the sus-
ceptibility ‘‘base level’’ due to the paramagnetic clays,
which seems to be dominant in the samples having
k < 200� 10� 6 to 300� 10� 6 SI.
The dominant role of the paramagnetic minerals as
carriers of the susceptibility and AMS is confirmed by
the hysteresis properties measured using a Molspin
VSM in three samples from three different sites (Fig.
4). One of these sites (Sa09) shows the highest PVvalue (1.109, Table 1), and another one (Sa16) shows
an inverse fabric (see below). Both the high aniso-
tropy and the inverse fabric might, in principle,
suggest a significant ferromagnetic contribution to
the low-field susceptibility (single-domain magnetite
commonly carries the inverse fabric). All the three
samples show no hysteresis (i.e., a line passing
through the origin, Fig. 4), showing a typical para-
magnetic behaviour. Given the sole paramagnetic
contribution, the inverse fabric shown at two sites
(see below) is likely due to Fe-bearing carbonates, as
also documented elsewhere in Italy (e.g., Winkler et
al., 1996), and not to single-domain magnetite.
The ferrimagnetic contribution is likely significant
only in the sites Sa03 and Sa33, showing k values
much higher (of about one order of magnitude) than
the other sites (Table 1). Site Sa03 was sampled in
porous calcarenite beds cut by calc–alkaline dykes.
Therefore, we infer that in such site hot fluids from the
dykes saturated the adjacent porous sediments and
Fig. 3. (a) Frequency distribution of the mean susceptibility (km) in the sediments investigated in this study; (b) L/F plot for all the studied
samples; (c) lower hemisphere, equal area plots for an example of a site showing a subvertical lineation orthogonal to bedding (inverse magnetic
fabric, e.g., Rochette et al., 1992); (d) example of a site showing a well-defined magnetic foliation parallel to bedding and a well-defined
tectonic-related magnetic lineation.
C. Faccenna et al. / Tectonophysics 356 (2002) 213–232220
filled with material that includes ferrimagnetic miner-
als. Conversely, site Sa33 was sampled in a sedimen-
tary–volcanoclastic succession containing several ash
layers. Here the high k value likely arises from the
volcanic fraction, rich in ferrimagnetic minerals.
The anisotropy degree PVis always low (Table 1),
with values typical of weakly deformed sediments
(PVV 1.109). The shape of the AMS ellipsoids is
predominantly in the oblate field (T>0 or F>L, Fig.
3b) except at sites Sa10 and Sa16, where it is almost
purely prolate (T=� 0.757 and � 0.886, respectively,
Fig. 3b and Table 1). In these two sites, the magnetic
lineation is vertical (Fig. 3c) and orthogonal to bed-
ding (and the sediments are almost undeformed),
implying that here the magnetic fabric is inverse,
and no simple correlation between the magnetic fabric
and the rock fabric exists (e.g., Rochette et al., 1992).
In almost all sites (except Sa08, Sa09, Sa10, and
Sa16), despite the low magnetic anisotropy, the mag-
netic foliation plane is generally well defined and
parallel to the bedding plane (Fig. 3d), as it is
commonly observed in weakly deformed sediments.
The magnetic foliation is perpendicular to the bedding
plane only in the sites Sa08 and Sa09 (Fig. 2),
sampled in the Cixerri Formation. These are the oldest
sediments studied by us and underwent a more com-
plex tectonic history than the other formations (see
Discussion).
The magnetic lineation is well defined in 21 sites
(Figs. 2 and 3 and Table 1), where the e12 confidence
angle of the kmax in the kmax–kint plane is < 30j. Theremaining 13 sites have a purely oblate fabric with
virtually no lineation (e12>30j).The tectonic implications for the presence and
direction of the magnetic lineation in the different sites
will be fully discussed in Sections 4 and 5. We will
present in detail the magnetic fabric characters shared
by the sites from each sedimentary cycle, below,
together with the results of the fault population anal-
ysis carried out on the same sites sampled for AMS.
3.2. AMS and structural analysis of the Cixerri
Formation
The Cixerri Formation crops out in the Iglesiente
and Sulcis areas, in southwestern Sardinia (Figs. 2 and
5A). Two sites, Sa08 and Sa09, close to the south-
western coast, show magnetic foliation subvertical
and perpendicular to the bedding plane (Fig. 6). The
magnetic foliation perpendicular to the bedding planes
has been generally related to the passive displacement
and rotation of hematite and clay minerals within
cleavage planes (Graham, 1966; Kligfield et al.,
1981; Pares et al., 1999). In these cases, it was
demonstrated that magnetic foliation is perpendicular
to the maximum shortening direction (r1). We found
Fig. 4. Hysteresis loops measured using a Molspin VSM for three
samples coming from three different sites. All the three plots show
no hysteresis and a typical paramagnetic behaviour.
C. Faccenna et al. / Tectonophysics 356 (2002) 213–232 221
Fig. 5. Detailed geological map and in situ magnetic lineation from the Marmilla–Campidano (A) and Anglona–Logudoro (B) areas.
C.Faccen
naet
al./Tecto
nophysics
356(2002)213–232
222
microstructural evidence of low angle reverse faults
(striae azimuth oriented N40–50j, Fig. 6b) cross-cutby subsequent extensional faults at site Sa08 (Fig. 6c).
Barca and Costamagna (1997, 2000) describe Eocene
thrusting spread over the area. In compressional set-
ting, the magnetic lineation forms parallel to fold
axes, and thrust sheet, that is almost perpendicular
to the maximum horizontal shortening. The two sites
show a lineation ranging between N–S and NW–SE,
even if Sa09 lineation is not well defined (e12 = 34j,Table 1). Four other sites (Sa07, Sa17, Sa18, and
Sa19) of the Cixerri Formation have a foliation
parallel to bedding and magnetic lineation ranging
from N to NW (Figs. 2 and 5a). Site Sa18 is also
affected by a set of E–Wextensional joints orthogonal
to the kmax axis. As a whole, the Cixerri Formation
sites in the Iglesiente–Sulcis area define an average
N146j magnetic lineation suggesting a NE compres-
sion, as also confirmed by structural data (Barca and
Costamagna, 1997, 2000).
3.3. AMS and structural analysis of the first
sedimentary cycle
The units belonging to the first cycle crop out
along the Sardinian trough (Fig. 1) in the Marmilla
(Fig. 5A) and Anglona areas (Fig. 5B), and tradition-
ally have been considered as a marker for the onset of
the ‘‘rifting’’ episode. Nine sites have been sampled in
the Marmilla area (Fig. 5A) in both continental upper
Oligocene–Aquitanian basal units (Sa21 and Sa24)
and in the marine lower–middle Burdigalian marls.
Five sites yield a well-defined N–S lineation, in
agreement with structural analysis results from some
sites (for example, site Sa02 or Sa11; Fig. 7a,b),
showing that syn-sedimentary faults and extensional
joints are E–W to E–NE striking. The computed
extensional direction, between NS and N10jW, is in
good agreement with the orientation of the kmax axis.
Six sites have been drilled in the Anglona area
(Fig. 5B) and in the Chilivani basin (Fig. 2) in both
continental upper Oligocene–Aquitanian sediments
(Sa32 and Sa36) and in marine Aquitanian–Burdiga-
lian marls interbedded with volcanoclastic debris. In
the continental sediments, the magnetic lineation is
EW in site Sa32 and NE in site Sa36. The latter site
has been drilled in a releasing bend along a major NE
strike-slip fault (Oggiano et al., 1995). One site has
been drilled in the EW striking half-graben Funta-
nazza basin (Sa03; Fig. 2).
Two out of the five sites drilled in the marine units
show a well-defined magnetic lineation, N–S striking
(Figs. 2 and 5b). Microstructural analysis in those
sites systematically showed EW striking syn-sedimen-
Fig. 6. Magnetic fabric (a) and structural analysis (b,c) from site Sa08 (Cixerri Formation, middle Eocene– lower Oligocene). Normal faults
shown in the diagram (c) cross-cut the reverse faults shown in diagram (b). AMS and structural data are reported on equal-area, lower
hemisphere net.
C. Faccenna et al. / Tectonophysics 356 (2002) 213–232 223
tary normal faults and a N–S extensional direction. In
many of the sampled sites, this first deformational
episode is followed by system of NNW–SSE-oriented
normal faults and joints (see, for example, site Sa30,
Fig. 7c).
3.4. AMS and structural analysis of the second
sedimentary cycle
Four sites (Sa04, Sa05, Sa06, and Sa20) were
sampled in Langhian–Serravallian marine marls from
southern Marmilla region (Figs. 2 and 5a). Only site
Sa06 showed a WNW–ESE lineation, whereas the
remaining three showed a purely oblate fabric. In the
Anglona area and east of Monte Ferru, six sites were
sampled in clayey–marly beds interbedded with a
monotonous and thick sequence of coastal sandstones,
Langhian in age (Figs. 2 and 5b). One site (Sa16)
shows an inverse fabric (Fig. 3c), with the magnetic
lineation subvertical and perpendicular to bedding.
Out of the remaining six sites, two (Sa26 and Sa28)
show a N–S magnetic lineation, while the other four
(Sa25, Sa27, Sa29, Sa34) have a purely oblate fabric.
3.5. AMS and structural analysis of the third and
fourth sedimentary cycles
Two sites (Sa14 and Sa15) were sampled in Torto-
nian and lower Pliocene marine clays, respectively, in
the northwestern margin of the Campidano graben
(Fig. 2). These two sites show a well-defined NE–SE
magnetic lineation, in agreement with structural anal-
ysis data documenting NW–SE-oriented joints (Fig.
7).
4. Interpretation of the magnetic lineation
directions and structural data
The magnetic lineation direction has been widely
used in many Miocene to Pleistocene clay deposits
from the external Apennines (Sagnotti and Speranza,
1993; Sagnotti et al., 1998; Scheepers and Langereis,
1994; Mattei et al., 1997) and the extensional margin
of the central Apennines (Sagnotti et al., 1994) and
Calabria (Scheepers and Langereis, 1994; Mattei et al.,
1999) to understand the tectonic history. Here the
magnetic lineation has proven to be a faithful strain-
trajectory proxy and to represent a fundamental struc-
tural tool to unravel the strain history in sediments
lacking other visible structural elements (e.g., faults,
cleavage, fractures). It has been shown that in foredeep
clays interbedded in turbidite sequences and in thrust-
top deposits, the magnetic lineation forms shortly after
compression and faithfully represents the local fold
axis direction (e.g., Mattei et al., 1997, with referen-
ces). Conversely, in extensional syn-rift deposits, the
magnetic lineation is orthogonal to the extensional
faults and parallel to the stretching direction.
On the base of our AMS and structural data set, we
are able to characterise the tectonic regime that
accompanied the deposition of the different sedimen-
tary cycles. Our data show that:
(a) The Eocene–Oligocene Cixerri Formation was
deposited during the final stages of a compressional
episode, which is in agreement with the hypothesis of
Barca and Costamagna (2000). A mean magnetic
lineation, oriented on average NW–SE (Figs. 2, 5a,
and 9a), should reflect the maximum compression,
oriented NE–SW. To imagine its original orientation
Sardinia has to be clockwise rotated back clockwise
by about 30j restoring the island to its previous pre-
drifting position (e.g., Van der Voo, 1993; Speranza,
1999). Our data set can be interpreted in the light of
two different models proposed for the area. In the first
model, the Cixerri Formation was deposited in the
distal part of a continental foredeep basin, tentatively
correlated with the southernmost continuation of the
Pyrenean foredeep basin (Barca and Costamagna,
2000). Alternative model is that the Cixerri Formation
was deposited in transpressional basin, related to
large-scale strike-slip faults (Carmignani et al., 1999).
(b) The first upper Oligocene– lower Miocene
marine transgression in Sardinia marked the onset of
extensional process (Assorgia et al., 1997). The direc-
tion of magnetic lineation, from several sites scattered
Fig. 7. AMS and structural analysis results from (a) site Sa02 (lower Burdigalian), from (b) site Sa30 (Aquitanian) and (c) site Sa30 (upper
Oligocene–Aquitanian). In the latter site, we also show the structural analysis of two different deformative episodes, characterized by syn-
sedimentary normal fault (middle) and, successively, by N20jW striking normal faults and joints (right). AMS and structural data are reported
on equal-area, lower hemisphere net.
C. Faccenna et al. / Tectonophysics 356 (2002) 213–232 225
over the entire island, is well clustered around N10–
20jW (Fig. 9b). In addition, fault population analysis
and the presence of E–W-oriented extensional sedi-
mentary basins, suggest that the deposition of the
upper Oligocene–lower Miocene sedimentary succes-
sions occurred under a roughly N–S extensional
regime. In agreement with Carmignani et al. (1995),
we then confirm that the present-day N–S orientation
of the ‘‘Sardinian trough’’ axis does not reflect the
trend of the main upper Oligocene to middle–late
Burdigalian sedimentary basins.
Oggiano et al. (1995), by studying one of the
extensional basins (Chilivani–Berchidda, site 36 of
Fig. 2), suggested that the E–W normal fault are
related to a releasing bend along a E–NE-trending
strike-slip fault (Fig. 1). These faults cross-cut all the
eastern side of the island and are marked by both
releasing and restraining bends (Carmignani et al.,
1994, 1995; Oggiano et al., 1995). Some of them
show a main sinistral sense of motion (as the one
bordering Mt. Albo, Carmignani et al., 1994, 1995),
though careful analysis of kinematics indicators along
the major fault planes (e.g., Mt. Albo) indicates that
dextral motion is locally superimposed on the sinistral
one. Syn-tectonic continental deposits, in addition,
indicate that the activity of these major strike-slip
faults occurred during the sedimentation of the first
marine cycle and are possibly reactivated as transfer
faults connecting different NNW-trending upper Bur-
digalian basins (Funedda et al., 2000).
Our data set indicates that the first upper Oligo-
cene–lower Miocene marine cycle filled E–W striking
Fig. 8. AMS and structural analysis of sites Sa14 (Tortonian) and Sa15 (Pliocene). AMS and structural data are reported on equal-area, lower
hemisphere net.
C. Faccenna et al. / Tectonophysics 356 (2002) 213–232226
(N–S extensional direction in present-day orientation)
transtensional basin is mainly located along the west-
ern side of the island. Conversely, a strike-slip regime
was predominant at the same time over the eastern side
of the island. We then confirm previous suggestion
(Carmignani et al., 1995) that an overall late Oligo-
cene–early Miocene N–S extensional episode evolved
from transtension in western Sardinia to strike-slip
deformational style moving towards the east.
Different models can be proposed in order to
explain the apparent contradiction between the exten-
sional direction, as estimated in the western side of
island inside the E–W extensional basin and the one
estimated along the major strike-slip fault zones
present in the eastern side of the island. The first
model interpreted the origin of the E–W extensional
basin as kinematically related to releasing bend along
NE-bearing sinistral strike-slip faults (Carmignani et
al., 1995; Oggiano et al., 1995). An alternative
hypothesis proposed here suggests that the whole
region is subjected to a N–S extensional episode
parallel to the strike of the island and that complex
interplay between the strike-slip fault system locally
generates the sinistral sense of motion along the E–
NE-bearing faults, as observed along the Mt. Albo
area (Pasci, 1997). The overall trend of the fault
zone, showing a sinistral ovestepping restraining
bend, and the presence of superimposed dextral kine-
matic indicator could suggest a more complex kine-
matic history of the Mt. Albo fault zone than pre-
viously supposed.
The data set collected here cannot discern between
the two models and further investigations are needed.
For example, it would be interesting to integrate our
data set with other sites located far away from the
main shear zones and in Corsica. More detail of the
kinematic analysis along the eastern Sardinia strike-
slip structures would also be useful.
(c) The second upper Burdigalian–lower Serraval-
lian depositional cycle occurred in less subsiding
basins, i.e., during Sardinian drift and oceanic spread-
ing in the Liguro–Provenc�al basin. The direction of
the magnetic lineation is dispersed, implying lack of a
well-defined stretching regime during the sediment
deposition (Fig. 9c). Microstructural and geological
data show, especially in the northern region, that N–S
high-angle normal faults and joints characterised the
second deformational episode in that area (Funedda et
Fig. 9. Frequency histograms of the magnetic lineation direction for all the studied samples.
C. Faccenna et al. / Tectonophysics 356 (2002) 213–232 227
al., 2000). It is then possible that the present-day N–S
striking orientation of the ‘‘Sardinian trough’’ formed
during the deposition of this second sedimentary
cycle. It is worth noting, however, that the lack of
well-defined magnetic lineations indicates that this
stretching episode has minor relevance over the
island.
(d) The Tortonian (site Sa14) and Pliocene (site
Sa15) sites sampled at the northwestern margin of the
Campidano graben (Fig. 2) show both a well-defined
magnetic lineation clustered around the direction
N40jE (Figs. 8 and 9d). This direction is parallel to
the pole to extensional joints observed in both sites
(Fig. 8) and almost orthogonal to the orientation of the
Campidano graben. These data show that the Campi-
dano graben formed in a pure NE–SW extensional
regime. Moreover, the Tortonian age of site Sa14 may
suggest that extension in the Campidano graben
begun already during Tortonian, i.e., significantly
earlier than the Pliocene age considered so far.
5. Insight into tectonic evolution of the
Mediterranean trench–arc–back-arc system
The microstructural analysis and the study of the
magnetic fabric of the Eocene–Pliocene sedimentary
sequences from Sardinia have tectonic implications in
the framework of central Mediterranean evolution.
The Tertiary evolution of the area started in the late
Paleogene with the deposition of thick sequences of
continental deposits. Our analysis confirm the pre-
vious interpretation that related these deposits to a
compressional setting in the foreland of the Pyrenean
belt or further east, in strike-slip transpressional basins
(Fig. 10, stage a). Our data confirm that Sardinia was
subjected to rifting from Oligocene to middle–late
Burdigalian times during the deposition of the first
sedimentary cycle. The systematic pattern of magnetic
lineation oriented between N–S and N20jWobserved
over the entire western side of the Island, coupled
with systematic microstructural observation and large-
scale basin geometry reconstruction (Oggiano et al.,
1995), indicate that transtensional tectonics affected
western Sardinia, with a maximum extension axis
oriented N–S (in present-day coordinates). The exten-
sional stretching axis, prior to the Sardinia counter-
clockwise rotation, was therefore oriented NE–SW.
This pattern of deformation is in contrast to what
observed along the western shoulder of the basin, that
is the Catalonia–Provenc�al area, i.e., along the west-
ern shoulder of the Liguro–Provenc�al basin. Here,
microstructural observation and large-scale basin
architecture (Seranne, 1999) indicate that a main
NW–SE extensional direction controlled the deposi-
tion of the first sedimentary cycle. This deformational
pattern is also in contrast with that observed in the
fragmented Alpine chain from Corsica to Calabria,
where interval accretion and high-pressure metamor-
phic units were forming at the same time (Carmignani
and Kligfield, 1990; Jolivet et al., 1998; Rossetti et al.,
2001). The depicted scenario thus shows a progressive
change in the deformational regime from compression
in the accreting wedge of Calabria, to strike-slip and
transtension in moving from eastern to western Sardi-
nia, to pure extension in the back-arc area (Fig. 10,
stage b). Carmignani et al. (1995) interpret this change
of the style of deformation as due to lateral escape
processes related to a collisional event. Here we
proposed an alternative interpretation related to the
change in the deformational regime as due to a
permutation of the stress axis. The minimum compres-
sional axis, vertical in the accretionary prism, be-
comes horizontal in the back-arc area where it
strikes perpendicularly to the trench. The Sardinia
region is located between these two well-defined
deformational regimes and is dominated by an inter-
mediate state of deformation and of stress character-
ised by a strike-slip to transtensional regime with a
minimum compressional axis oriented parallel to the
trench. This transitional regime can be compared to
the one describe for the Japan area by Nakamura and
Uyeda (1980) where a progressive transition from
accretion in the trench area to back-arc extension
was documented. Our data also indicate that the
present-day major geomorphic features of Sardinia
have been acquired only during the last extensional
episodes. They occurred during and after the drifting
of the Island, with a passive subsidence and formation
of the main N–S-oriented depression that controlled
the deposition of the second sedimentary cycle (Fig.
10, stage c). The last tectonic episode, probably
started during the late Miocene, caused the formation
of the Campidano basin filled up by the third and
fourth sedimentary cycles. The origin of this deep
half-graben structure is poorly understood as it cannot
C. Faccenna et al. / Tectonophysics 356 (2002) 213–232228
Fig. 10. Schematic block-diagrams showing the inferred tectonic scenario of the arc–back-arc system in the central–western Mediterranean at
three stages, from 35 to 15 Ma.
C. Faccenna et al. / Tectonophysics 356 (2002) 213–232 229
be directly related to the dynamic of the subduction
system.
6. Conclusions
We have shown that AMS, coupled with classical
structural analysis, represents a powerful tool to
define the characters of tectonic episodes affecting
in subsequent times a given region. The magnetic
fabric is sensitive to the strain trajectories produced
by a regime acting during or shortly after the sedi-
ment deposition. Therefore, use of AMS data is
advisable when structural analysis alone is unable to
unravel features of temporally superimposed tectonic
events.
Our structural/AMS data set demonstrates that
the arc–back-arc transition in western Sardinia was
accompanied by orogen-parallel extension. This tec-
tonic regime involved both NE–SW strike-slip faults
close to the Alpine–Apennine accretionary wedge
and N–S extension (both in present-day coordinates)
in the western part of the island, close to the
contemporaneously rifting Liguro–Provenc�al basin.
Therefore, we document here that the accretionary
wedge, the arc domain, and the back-arc basin were
characterised by a progressive shift from orogen-
normal shortening, orogen-parallel extension, and
orogen-normal extension, respectively. We also show
that in western Sardinia a N–S elongated volcanic
arc did not form along an E–W extending basin, the
so-called Sardinia trough, but was spatially super-
imposed over several coalescing N–S extending
grabens of Aquitanian–lower Burdigalian age. The
pre-upper Burdigalian sediments are unconformably
covered by virtually underformed middle–upper
Miocene successions, lacking any visible and mag-
netically retrievable deformation. We interpret this
late Burdigalian tectonic regime change as the inland
reflection of the rift-to-drift transition in the Liguro–
Provenc�al basin.
Acknowledgements
We thank R. Funiciello, for having encouraged this
work, and M. Musacchio, for help in the field. Fault
population analysis has been performed using the
Daisy programme, kindly provided by F. Salvini.
Thanks also to A. Winkler for performing the
hysteresis loops. The paper benefited from careful
reviews by A.M. Hirt and L. Carmignani.
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