Posted on 23 Jun 2023 — The copyright holder is the author/funder. All rights reserved. No reuse without permission. — https://doi.org/10.22541/essoar.168748485.58030882/v1 — This a preprint and has not been peer reviewed. Data may be preliminary.
Contrasting Styles of Salt-Tectonic Processes in the Ionian Zone
(NW Greece and S Albania)
Juan I Soto1 , MARKOS DAMIANOS TRANOS2 , Zamir Bega3 , Tim Dooley4 , Pablo
Hernández5 , Michael R. Hudec1 , Takis Konstantopoulos6 , Ervin Lula7 , Konstantinos
Nikolaou6 , Rubén Pérez5 , Juan Pablo Pita5 , Juan Antonio Titos7 , Constantinos Tzimeas8 ,
and Adela Herra Sánchez de Movellán5
1
University of Texas at Austin
KING FAHD UNIVERSITY OF PETROLEUM AND MINERALS
3
Independent Consultant
4
Bureau of Economic Geology, Jackson School of Geosciences, The University of Texas at
Austin
5
REPSOL Exploración S.A.
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ENERGEAN
7
Granada University
8
Independent Exploration Geoscience Consultant
2
June 23, 2023
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Contrasting Styles of Salt-Tectonic Processes
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in the Ionian Zone (NW Greece and S Albania)
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J. I. Soto1,2*, M. D. Tranos3, Z. Bega4, T. Dooley1, P. Hernández5, M. R. Hudec1, P. A.
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Konstantopoulos6, E. Lula7,8, K. Nikolaou6, R. Pérez5, J. P. Pita5, J. A. Titos7, C. Tzimeas9,
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and A. Herra Sánchez de Movellán5
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Independent consultant, Tirana, Albania.
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5
REPSOL Exploración S.A., Madrid, Spain.
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Energean Oil & Gas, Athens, Greece.
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7
Departamento de Geodinámica, Granada University, Granada, Spain.
19
8
San Leon Energy Plc, Tirana, Albania.
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9
Independent Exploration Geoscience Consultant, Athens, Greece.
Bureau of Economic Geology, Jackson School of Geosciences, The University of Texas at
Austin, University Station, Box X, Austin, TX 78713-8924, USA.
On leave of absence from: Departamento de Geodinámica, Granada University, Avenida de
Fuente Nueva s/n, 18071 Granada, Spain.
Department of Structural, Historical & Applied Geology, University of Thessaloniki,
Thessaloniki, Greece.
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* Corresponding author: Juan I. Soto (juan.soto@beg.utexas.edu)
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Key points
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and the interpretation of new seismic profiles
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The Ionian Zone in Greece and Albania is studied with surface geology, well information,
Triassic salt pillows, isolated thick diapirs, and elongated salt walls condition the style of
this Alpine fold and thrust belt
•
Salt tectonics provides new clues about Alpine orogenic evolution, opening new
opportunities for geologic storage in the region
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Abstract
32
The Ionian Zone (IZ) is one of the key elements of the external zones of the Albanian Hellenides
33
orogen and contains large outcrops of Triassic evaporites. The IZ consists of various thrust sheets
34
with a general westward vergence, stacking over the Apulian and Pre-Apulian zones, and
35
repeating a thick carbonate sequence of Late Triassic or Early Jurassic to Eocene age. Thrusting
36
becomes younger toward the west with a piggyback sequence, starting during the latest
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Oligocene Epoch in the internal Ionian and ending in the Pliocene in the external Ionian. We have
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studied the IZ in southern Albania and northwestern Greece using field observations and borehole
39
data and by fully interpreting a recently acquired 2D seismic data set. Our objectives are to
40
establish the geometry and nature of the contacts associated with the major Triassic outcrops, to
41
unravel precursor salt diapirs, and to assess their role during the Alpine contraction. Salt
42
structures include gentle salt pillows, isolated salt plugs and diapirs, thrust welds, and salt walls.
43
We show how these structures control the geometry and kinematics of the Alpine thrusts or the
44
location of recent strike-slip faults. Salt minibasins have also been identified, demonstrating salt
45
mobility conditioned Mesozoic sedimentation in the Ionian Basin. The use of salt-tectonics
46
principles to evaluate the structural style and evolution of the IZ fold and thrust belt also opens
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new directions for interpreting the subsurface and could help to better define structures that can
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be used as opportunities for geologic storage in the region.
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50
Keywords:
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Fold and thrust belts, salt tectonics, diapirs, seismic interpretation, Hellenides, Albanides.
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1. Introduction
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Within the Alpine belts developed in the eastern Mediterranean Sea, one of them is the fold and
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thrust belt (FTB) that extends from the Alps and the Carpathian arc along the eastern Adriatic
56
coast to Greece and Crete, including the Dinarides, Albanides, and Hellenides. This orogenic belt
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encircles the Aegean extensional basin and faces the Apennines, with a structural vergence
58
opposite that of the Apennines (Figure 1). The general structure of the Dinarides–Albanides–
2
59
Hellenides (DAH) consists of the imbrication of several terrains linked to the Adriatic plate,
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which collided with several elements of the Eurasian plate during the Alpine orogeny, closing
61
and obducting the oceanic domains that separated these plates (Aubouin, 1959a; Aubouin et al.,
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1976; Aubouin et al., 1962; Bernoulli, 2001; Bernoulli & Laubscher, 1972; Cavazza et al., 2004;
63
Channell et al., 1979; Channell et al., 2022; Degnan & Robertson, 1998; Dercourt et al., 1993;
64
Handy et al., 2019; Kilias et al., 2016; Kilias et al., 2001; Mountrakis, 2006; Nieuwland et al.,
65
2001; Papanikolaou, 2013; Papanikolaou, 2021; Papanikolaou, 1996-1997; Robertson & Shallo,
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2000; Schmid et al., 2008; Schmid et al., 2020).
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Specifically, in the present-day region of Albania and Greece, the configuration of the FTB is
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conditioned by several unique features. First, the external domains of the Albanides-Hellenides
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(AH) involved thick Mesozoic carbonate successions. Next, although the AH belt contains
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obducted elements from several preorogenic oceans, its present-day orogenic front lies on a
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domain of strongly-thinned continental crust, in the present-day Adriatic Sea (Hieke et al., 2003;
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Kokinou et al., 2003; Makris et al., 2013). And finally, the curvature of the AH, south of Crete, is
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produced by the superposition of active northward subduction of the African plate and
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simultaneous high-magnitude extension of the AH forming the Aegean Sea (Brun et al., 2016;
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Jolivet & Brun, 2010; Jolivet & Faccenna, 2000; Kilias et al., 2002; Mountrakis, 2006; van
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Hinsbergen et al., 2006)).
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Our study region is located precisely in the outer domains of the AH, between southern Albania
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and northwestern Greece (in the Epirus region; Figure 2). In this particular sector, the zone we
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have studied covers the entirety of one of the main elements of the outer zones of the orogen: the
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Ionian Zone (IZ; (Philippson, 1898) or “adriatisch-ionische Zone” (Renz, 1925, 1955)). For our
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purposes, the structural organization of this FTB consists of thin-skinned thrust systems directed
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westward, whose configuration and nomenclature differ between those proposed in Albania and
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those realized in Greece.
84
Another value in the study region is that there is an active exploration of the resources in these
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countries for the discovery and extraction of hydrocarbons (included in Figure 2) (Arvanitis et al.,
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2020; Bega, 2013; Bega & Soto, 2017; Curi, 1993; David et al., 2014; Kamberis et al., 2022;
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Maravelis et al., 2012; Mavromatidis, 2009; Moorkens & Döhler, 1994; Rigakis et al., 2007;
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Sadekaj et al., 1992; Sejdini et al., 1994; Shehu & Johnston, 1991; Stournaras, 1985; Zelilidis et
3
89
al., 2015; Zelilidis et al., 2003; Zelilidis et al., 2016). In addition, we believe that a precise study
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on the deep and shallow nature of the salt structures and the associated salt-tectonic processes
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will be valuable for the new challenges of geologic storage (e.g., CO2 and Hydrogen) in these
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countries (e.g., (Arvanitis et al., 2020; Hatziyannis et al., 2009; Stournaras, 1985)).
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In the Epirus area, several previous studies have interpreted the existence of diapiric salt bodies,
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nucleated in the evaporitic successions of the Late Triassic Epoch. This has been suggested in
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some specific structures both in Albania and Greece (Aliaj, 1974; Berberi et al., 1990; Jardin et
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al., 2011; Jenkins, 1972; Kamberis et al., 1996; Kamberis et al., 2013; Karakitsios, 1995;
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Karakitsios & Rigakis, 2007; Nikolaou, 1986; Plaku & Murataj, 1974; Prifti et al., 2013;
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Underhill, 1988; Velaj, 2001, 2015; Velaj et al., 1999; Zelilidis et al., 2016). However, we
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believe that major questions remain to be answered completely in the area. For example, what
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kind of observations can we make in such a FTB to confirm that diapiric structures previously
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existed or, on the contrary, that the structural evolution of particular structures can be explained
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uniquely by shortening (e.g, (Kamberis et al., 2022))? What is the internal architecture of the IZ?
103
Can we use a single frame of reference to explain the whole IZ in Albania and Greece? What role
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did the Triassic evaporites play in the IZ during the Alpine shortening? What is the structure of
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the evaporite bodies at surface and at depth? What preorogenic salt structures can we still
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differentiate in this FTB and when did they form?
107
With these general tectonic objectives in mind, our work has consisted of the analysis of three
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different types of data: (1) an extensive reconnaissance of the Triassic structures of the IZ in the
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field; (2) seismic interpretation of a new set of unpublished two-dimensional (2D) seismic
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profiles obtained in the NW onshore region of Greece, and; (3) a review of previous geophysical
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data in the IZ, such as gravity, previous deep-seismic reflection profiles, and a comprehensive
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borehole data set. Our main objective has been to characterize in detail the geometries of the FTB
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and the role played by the Triassic evaporites, using the principles of salt tectonics (e.g., (Jackson
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& Hudec, 2017)). For the overall interpretation of these observations, we will also use a set of
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experimental models with various types of diapiric structures deformed under compression, and
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data from previous studies in the area, such as the distribution of paleomagnetic rotations in the
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IZ.
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2. Tectonic Setting
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The AH FTB consists of a set of terrains linked to the Adria plate, forming various metamorphic
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units and two obducted nappes of ophiolites (Western and Eastern Vardar ophiolites), which
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constitute the inner zones of the orogen (e.g., Pelagonian Massif in Greece and Albania) (Figure
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2) (Kilias et al., 2016; Kilias et al., 2001; Meço et al., 2000; Papa, 1970; Papanikolaou, 2009;
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Papanikolaou, 1996-1997; Plougarlis et al., 2021; Robertson & Shallo, 2000; Schmid et al., 2008;
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Schmid et al., 2020; Smith & Moores, 1974). In the study area, during the Alpine orogeny, these
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terrains were thrusted westward over a deepwater basin infilled by Paleogene–early Neogene
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flysch series (Aubouin, 1959b; Papanikolaou, 2021; Robertson & Shallo, 2000; Skourlis &
127
Doutsos, 2003; Thiébault, 1982). These tectonic elements constitute the external zones of the AH
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FTB and extend under different names from Greece (Pindos and Gavrovo–Tripolitza zones),
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Albania (Krasta–Cukali and Kruja zones), to Montenegro, Croatia, and Bosnia (e.g., Dalmatian,
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Bubdva, Beotian, Pre-Karst, and Bosnian Flysch zones) (for a recent and comprehensive revision
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see (Schmid et al., 2008; Schmid et al., 2020)).
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Underlying these flysch sequences of Oligocene to lower Miocene age is the IZ, formed by a
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Mesozoic (to Eocene) carbonate sequence and large outcrops of Triassic evaporites (Figure 2).
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The IZ is organized in three large thrust sheets, detached along (and possibly within) the Triassic
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evaporites (Institut_Francais_du_Pétrole_Mission_Grèce, 1966; Jenkins, 1972; Karakitsios &
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Rigakis, 2007; Lykakis et al., 2021; Roure et al., 2004; Sadekaj et al., 1992; Sejdini et al., 1994;
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Sotiropoulos et al., 2022; The_B.P._Co_Ltd., 1971; Underhill, 1988, 1989; Velaj, 2001; Velaj et
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al., 1999; Zelilidis et al., 2015).
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The orogenic front of the IZ consists of a thrust system with various salients and reentrants, and
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some oblique structures that are locally known as the Vlora–Dibër (or Vlora–Elbasan; VDL),
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Corfu–Picari (CPL), and Kefallinia–Lefkas–Lixourion (or Cephalonia fault; KLL) lineaments
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(from north to south) (Bega & Soto, 2017; Kokinou et al., 2005; Kokinou et al., 2006; Mehillka
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& Canaj, 1996; Picha, 2002; van Hinsbergen et al., 2006). Beneath this front, detached elements
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of the Mesozoic Apulian carbonate platform are found, forming what is known locally as the Pre-
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Apulian or Sazani–Paxi zones (Aliaj, 1987; Aubouin et al., 1962; Papa & Kondo, 1968; Prifti &
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Uţă, 2012; Underhill, 1988, 1989). To the west, beneath much of the Adriatic Sea, the present-
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day marine basin consists of a Miocene to present-day sedimentary section overlying the thick
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Mesozoic carbonate sequence of the Apulian and the pre-Apulian platforms (Cazzini et al., 2015;
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Fantoni & Franciosi, 2010; Fournillon et al., 2017; Kamberis et al., 1996; Sotiropoulos et al.,
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2022). Existing data show that the AH FTB orogenic front in the offshore region is formed by a
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thrust stack with the IZ over the Pre-Apulian zone (Kamberis et al., 1996), and both lie above the
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Apulian platform that dips eastward by flexure due to the load of the AH orogenic edifice
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(Scrocca et al., 2022). Due to this process, a thick marine foreland basin originates, in which
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post-Messinian sediments can reach thicknesses of more than 4 km in the northern part of the IZ,
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in a domain known as the Albanian foredeep (Figure 2) (Aliaj, 2006; Nieuwland et al., 2001).
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The tectonic situation of orogenic convergence extends to the present day. GPS data in the area
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reflects this, showing that the continental region of the AH FTB is now moving south in northern
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Greece and North Macedonia and WSW in western Greece and southern Albania, with velocities
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of up to 26–32 and 4–5 mm/yr, respectively (see vectors in Figure 2) (Caporali et al., 2020;
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Cocard et al., 1999; D’Agostino et al., 2008; D’Agostino et al., 2020; Pérouse et al., 2016; van
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Hinsbergen et al., 2006). This curved motion of the AH FTB appears to accelerate south of the
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KLL dextral transform (transpressional) fault zone, because further south the orogen is associated
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with an active subduction of the oceanic (or strongly thinned continental) crust of the Ionian
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Basin. Kinematic data from the Apulian and southern Italian domains, on the contrary, show a
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movement against present-day Eurasia, directed NNE (4.2 mm/yr; (D’Agostino et al., 2008;
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D’Agostino et al., 2020; Pérouse et al., 2016)).
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The Alpine tectonic activity, which shaped the AH FTB, therefore extends to the present day,
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with a complex orogenic front in which the northward movement of Apulia and the overthrusting
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of the IZ over both an oceanic crust (Ionian Basin) and elements of the Mesozoic Apulian
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carbonate platform must play a different role. For example, we also suggest that the position of
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the Pre-Apulian Zone, with a thick accumulation of Mesozoic carbonates (e.g., (Fournillon et al.,
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2017; Kokinou et al., 2005; Kokinou et al., 2003; Papa & Kondo, 1968; Sotiropoulos et al.,
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2022)), acted as a tectonic buttress against the westward advance of the IZ (Bega, 2020; Bega &
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Soto, 2017; Underhill, 1989). The role that the geometry of the eastern escarpment of the Apulian
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platform may also have on the dynamics and configuration of the IZ at the FTB front is not the
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subject of our study, but it is worth noting because of the development of complex salients and
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embayments developed by this orogenic front (Argnani, 2013; Underhill, 1989).
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3. General Structure of the Orogenic Front
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The general configuration of the external zones of the AH FTB is illustrated in Figure 3 with two
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crustal-scale cross sections. The cross section in Albania (Figure 3a) is located just north of the
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surface termination of the IZ, also north of the Dumrë diapir, across the central Albanian
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foredeep. This cross section merges surface geological observations from several authors together
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with data from the offshore region (Bega, 2013; Cazzini et al., 2015; de Alteriis, 1995; Fantoni &
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Franciosi, 2010; Kamberis et al., 2022; Moisiu & Gurabardhi, 2004; Scrocca et al., 2022; Xhomo
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et al., 2002). The deep structure, showing the internal crustal structure and characteristics, has
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been drawn by reinterpreting gravity models from previous studies (Frashëri et al., 2009). We
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have also included the density and compressional-wave velocity (Vp) values established there for
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the Triassic evaporites (Velaj, 2002; Velaj et al., 1999) (Table 1). Note, that we propose the
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existence of a thin synrift to postrift succession of Triassic evaporites beneath the Mesozoic
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carbonate succession of the Apulian platform.
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The configuration of the AH FTB in the central region of the IZ in Greece is schematized in the
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cross section of Figure 3b. In this section we have modified previous geological interpretations
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from the Corfu region and the structure from the Pindos Zone to the Mesohellenic trough
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(Doutsos et al., 2006; Ferrière et al., 2004; Monopolis & Bruneton, 1982; Waters, 1994),
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incorporating our interpretations. The deep structure here consists of a moderate subduction of
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the oceanic crust beneath the Apulian shelf, under a thinned continental crust in which a lower
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crust is still preserved (with Vp= 6.9×103 m s-1) (Makris, 1985; Makris et al., 2013). The crustal
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structure, its thickness, and the existence of two large Mesozoic carbonate units (Sazani–Paxi or
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pre-Apuliaz zone versus IZ) separated by a thick evaporite sheet (with Vp= 4.2–4.3×103 m s-1)
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have been taken according to seismic tomography data carried out by several authors recently
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(Makris & Papoulia, 2018; Makris & Papoulia, 2019). Although it has not been sufficiently
202
documented, the thick Apulian Mesozoic carbonate platform must have a thin evaporite sequence
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below it, as it has been suggested by some authors (Cazzini et al., 2015; Fantoni & Franciosi,
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2010; Kamberis et al., 1996; Kokinou et al., 2005; Kokinou et al., 2003). Perhaps the evaporites
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are only composed of anhydrite, as documented by some wells and subsurface data in the
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Gargano area and surroundings in offshore Italy (e.g., Puglia–1 and Gargano–1D wells;
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(Agostinetti et al., 2007; Bosellini & Morsilli, 2001; de'Dominicis & Mazzoldi, 1987; Improta et
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al., 2000; Patacca et al., 2008; Santantonio et al., 2013).
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Two aspects already known and of special interest for our study are also documented in both
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sections. First, the important role played by the Triassic evaporites as a detachment level for thin-
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skinned thrust systems in the IZ. This has been extensively documented in previous studies
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(Institut_Francais_du_Pétrole_Mission_Grèce, 1966; Jenkins, 1972; Kamberis et al., 2022;
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Karakitsios & Rigakis, 2007; Lykakis et al., 2021; Maravelis et al., 2012; Roure et al., 2004;
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Sadekaj et al., 1992; Sejdini et al., 1994; Sotiropoulos et al., 2022; The_B.P._Co_Ltd., 1971;
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Underhill, 1988, 1989; Velaj, 2002; Velaj et al., 1999; Waters, 1994; Zelilidis et al., 2015).
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Second, the existence of a thick body of evaporites in the central sector of the IZ (also
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documented by well data; e.g., Delvinaki–1 and Parakalamos–1 wells in Figure 3b), which may
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have deeper thrust sheets of the Mesozoic carbonate succession, and whose geometry, origin, and
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influence on the orogeny will be explored in this study.
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3.1. Main phases of deformation
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In the external zones of the AH FTB, the age of shortening is well known according to the dating
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of synorogenic sediments, which are flysch sediments filling large synclinal basins, but also
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considering the deformations affecting the offshore foredeep (Figure 3). In Albania and Greece,
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the age of flysch successions, syntectonic sediments affected by IZ thrusts, and age
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determinations in foredeep wells describe a thrust system whose age is progressively younger
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toward the front (to the west) and down the thrust stack. The age succession describes a
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piggyback thrust system, with ages varying progressively from late Oligocene and Aquitanian–
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Burdigalian in its innermost (eastern) part (Institut_Francais_du_Pétrole_Mission_Grèce, 1966;
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Jenkins, 1972; Kamberis et al., 2000; Makrodimitras et al., 2010; Pieri, 1990; Roure et al., 2004;
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Savoyat, 1977; Sejdini et al., 1994; Sotiropoulos et al., 2003; Speranza et al., 1992) to post-
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Messinian (affecting evaporites of this age; see (Aliaj, 2006; Kokkalas et al., 2013; Kosmidou et
232
al., 2018; Lacombe et al., 2009; Papanikolaou, 2021; Schröder, 1986)) and Pliocene in the
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outermost (western) thrusts (e.g., (Kamberis et al., 1996; Karakitsios et al., 2017; Kokkalas et al.,
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2013; Nieuwland et al., 2001; Speranza et al., 1995; Underhill, 1988, 1989)).
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The geometry and age of the foredeep infill also describe that the frontal thrusts are upper
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Miocene to Pliocene in age, in some cases affecting the Messinian evaporites and unconformity
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in the offshore region (Aliaj, 2006; Bega, 2020; Gjika et al., 2001; Karakitsios et al., 2017). Some
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studies suggest the occurrence of three punctuated shortening episodes; one in the lower to
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middle Miocene (Tranos et al., 2020), a second in the Pliocene, and the latest during the
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Pleistocene; (Kamberis et al., 2022; Sorel et al., 1992)), although we do not have the data to
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better refine this suggestion.
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Deformation in the frontal domain of the AH FTB extends to the present day, as evidenced by
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paleomagnetic rotations measured in Pliocene-to-Recent sediments, GPS-derived kinematic
244
vectors (Figure 2), and the seismic activity linked to some of the frontal thrusts (in the vicinity of
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the coastal region from Albania to Greece; e.g., (Caporali et al., 2020; D’Agostino et al., 2020;
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Kokkalas et al., 2013; Louvari et al., 2001; Matraku et al., 2023; Schmitz et al., 2020; Valkaniotis
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et al., 2022)) and to the strike-slip faults affecting the orogenic front (Figure 2). The two main
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seismically active strike-slip faults in this region are the Kefallinia–Lefkas–Lixourion dextral
249
transpressional fault zone in Greece (Bonatis et al., 2021; Kokinou et al., 2005; Kokinou et al.,
250
2006; van Hinsbergen et al., 2005) and in Albania, the dextral strike-slip fault zone associated
251
with the Shkodra–Tropoja (or Shkodra–Peje) Lineament and its offshore continuation with the
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Lezha (or Lezhe) fault (Aliaj, 1999; Aliaj et al., 2004; Caporali et al., 2020; Mehillka & Canaj,
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1996).
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4. Stratigraphy of the Ionian Zone
255
The stratigraphic column of the IZ was established since the first surveys on this domain of the
256
AH FTB. The first detailed biostratigraphic and lithostratigraphic study was carried out in the
257
region of Greece by (Renz, 1913, 1955), to which we must add the studies of (Nowack, 1924,
258
1926) in Albania. We have synthesized in Figure 4 our observations in the study region in
259
Albania and Greece, also using information from multiple authors (Aubouin, 1958; Aubouin et
260
al., 1977; Avramidis et al., 2002; Bellas, 1997; Bourli et al., 2019; Dalipi et al., 1972;
261
Institut_Francais_du_Pétrole_Mission_Grèce, 1966; Jenkins, 1972; Kamberis et al., 2022;
262
Karakitsios, 1995, 2013; Karakitsios & Rigakis, 2007; Meço et al., 2000; Papanikolaou, 2021;
263
Renz, 1913, 1925, 1955; Savoyat, 1977; The_B.P._Co_Ltd., 1971; Triantaphyllou, 2013;
264
Zelilidis et al., 2015; Zelilidis et al., 2003). Along with the synthetic column, lithological
265
variations, thicknesses and chronostratigraphic information, we have also included other useful
266
data, such as the position and characteristics (porosity and total organic [TOC] content) of the
9
267
different elements of the petroleum system of the IZ as well as the position of the structural
268
detachment horizons.
269
Three major lithostratigraphic sequences are present. First, the Upper Triassic evaporites,
270
possibly Carnian–Norian in age (Renz, 1925). Then, a thick carbonate succession that extends
271
from the uppermost Triassic (Norian–Rhaetian) Series to the upper Eocene (Priabonian) Series.
272
And finally, separated by a regional discontinuity, a flysch sequence of upper Eocene and
273
Oligocene to lower Miocene age (Aquitanian and Burdigalian). Several continental sediments
274
from the Burdigalian to the present erosively cover the previous sequences.
275
The Mesozoic carbonate sequence consists of the following lithostratigraphic formations (for
276
which we will use the terminology established by multiple authors in northern Greece). A thick
277
package of dolomites (“Obertriadischer Dolomit” or “Hauptdolomit” of Upper Triassic, Norian-
278
Rhaetian to Hettangian age; (Renz, 1955)), is followed by the dolomitic limestones of the
279
Pantokrator Formation (“Pantokratorkalk”; Sinemurian) and the massive limestone series of the
280
Siniais Formation (Pliensbachian; (Flügel, 1983)). In the lower part of the Pantokrator Limestone
281
(or Formation), thin levels of organic-rich black shales (up to 39% TOC content) have also been
282
described (Renz, 1955). The Middle Jurassic succession (Toarcian to Kimmeridgian) shows
283
important variations in thickness and sedimentary facies (Aubouin, 1958; Bernoulli & Renz,
284
1970; Institut_Francais_du_Pétrole_Mission_Grèce, 1966; Karakitsios, 1995; Nikolaou, 1988;
285
Renz, 1955; Savoyat, 1977). The following members can be distinguished: an “ammonitico
286
rosso” marly limestone member and the marly limestones of the Lower Posidonia mudstones
287
(Toarcian); limestones with filaments (“Calcaires à filaments;” Bajocian) and another package of
288
marls and marly limestones of the Upper Posidonia mudstones (Kimmeridgian). Both marl
289
intervals have high organic contents (up to 3.5% TOC) and constitute regionally the main source
290
rocks of the IZ petroleum system. Overlying these discontinuous successions and with variable
291
thickness and stratigraphic facies is a limestone and white marly limestone package of variable
292
thickness (up to ~800 m) that is the Vigla Limestone (Tithonian to Cenomanian; (Danelian et al.,
293
2004)). Above this formation are two limestone members of approximately uniform thickness,
294
which are the Senonian (~150 m) and Eocene (~800–900 m) limestones, whose ages are
295
Coniacian to Maastrichtian and probable Paleocene to upper Eocene (Priabonian), respectively.
296
Some phosphate- and chert-rich intervals have been found in south Albania and north Greece in
10
297
the transition from the Vigla to the Senonian limestones (Serjani, 1991). Studies conducted by
298
this team and previously by (Karakitsios, 2013; Karakitsios & Rigakis, 2007; Makri et al., 2023),
299
supported by basin thermal models and subsurface data, show that the middle to upper part of the
300
Eocene limestone, where the marly intercalations are more abundant, constitute a regional
301
reservoir sequence in the IZ.
302
The carbonate succession will be abbreviated as Mesozoic in age, although it extends from the
303
Lower Jurassic (Hettangian) to the upper Eocene (Priabonian). Within this formation, it should be
304
noted that all the marls and marly limestone sequences of Middle Jurassic age, constitute a
305
horizon of special interest for our study, both for its lithological and sedimentary facies variations
306
and for constituting an efficient structural detachment horizon.
307
Above this sequence, and separated by a regional discontinuity, are the detritic successions of the
308
flysch units (Aubouin et al., 1977). In this group, three stratigraphic formations can be
309
distinguished. The lower one is the thin level, not always observable, of the “base flysch”
310
formation (upper Eocene in age; Priabonian). Above this level, two flysch series are easily
311
recognized in the field due to their lithological differences, sedimentary facies, and colors, such
312
as the Ayii Pantes (Oligocene) and Upper Flysch formations (late Oligocene to Aquitanian and
313
Burdigalian).
314
Of special interest for our study are the Triassic evaporites. We dedicate a separate section to
315
them, differentiating the observations that can be made at the surface from those derived from
316
subsurface data. We believe that we present for the first time, a novel and extensive set of well
317
data, gathering information from multiple wells in Albania and Greece, bringing together
318
information that is generally not easily accessible to the scientific community.
319
4.1. Characteristics of Triassic evaporites
320
Several authors have analyzed the age of the evaporite sequence in the IZ, and we can assign it to
321
the Upper Triassic (Carnian–Norian) Epoch (Dragastan et al., 1985; Jenkins, 1972; Muhameti &
322
Pejo, 1974; Pomoni-Papaioannou & Tsaila-Monopolis, 1983; Velaj, 2001)), which is in
323
agreement with the age of the Keuper evaporites in much of the Mediterranean Alpine belts (see
324
summary in (Soto et al., 2017)). However, some authors attribute a pre-Carnian (Bornovas,
325
1960), a Lower–Middle Triassic (Pomoni-Papaioannou & Tsaila-Monopolis, 1983) or a
11
326
Permian(?)–Triassic lato sensu age to the evaporites (e.g., (Meço et al., 2000; Moorkens &
327
Döhler, 1994; Papanikolaou, 2021)).
328
Triassic evaporites at the surface are usually covered by a thick layer of dolomitic breccias
329
(Figure 5b), being poorly exposed due to weathering and the occurrence of soil and vegetation
330
cover (“obertriadischer Dolomit” or “Hauptdolomit”; (Renz, 1955)). It is interpreted that these
331
breccias were formed immediately after deposition, in an arid evaporitic environment, also
332
having early diagenetic dissolution processes (Getsos et al., 2004; Karakitsios & Pomoni-
333
Papaioannou, 1998). However, it is possible to find some continuous sections in which a thick
334
section of reddish to green or grayish marls and clays grades upward to a gypsum-rich series
335
below the breccias (Figure 5a). Levels of black oleaginous clays (which may have up to 17%
336
TOC) may also be encountered toward the upper part of the evaporite sequence and within the
337
lower part of the dolomites (Bornovas, 1960; Karakitsios & Rigakis, 1996; Renz, 1955). The red
338
clay and marl sequences usually have abundant intercalations of alabastrine gypsum and thin
339
levels of black dolomites (Pomoni-Papaioannou & Tsaila-Monopolis, 1983), with local lenses of
340
sub-volcanic rocks (Dalipi et al., 1972). Some authors have interpreted that these gypsum layers,
341
with massive and bedded micro-fabrics, are transformed and recrystallized during burial to
342
anhydrite (Bornovas, 1960; Pomoni-Papaioannou & Tsaila-Monopolis, 1983).
343
In the outcropping evaporites, especially toward the base, stratified packages of black limestones
344
with Foustapidima (Alexandridis et al., 2022; Bourli et al., 2022; Renz, 1955) and with Cardita
345
guembeli (Dragastan et al., 1985), known regionally as “Cardita limestone” (“karnischen
346
Fustapidimakalk” and “Carditakalke”; (Jacobshagen, 1986; Renz, 1955)) and which have been
347
dated as Upper Triassic (Carnian–Norian) in age, are also occasionally found.
348
Recognizable structures in the evaporite successions comprise cemented polymictic breccias with
349
abundant centimeter and millimeter clasts of variable lithologies, such as gray limestones,
350
gypsum, dolomites, and marls (inset in Figure 5a). In the evaporite levels it is common to observe
351
structures showing ductile flow, such as asymmetric and sheath folds (Figure 5c–d) or ductile
352
shear zones with gypsum and anhydrite porphyroclasts (Figure 5g–h). When the limestone and
353
dolomitic layers are intercalated within the gypsum-rich sequences, they usually develop boudins
354
and discontinuous clasts, evidencing their fracturing due to layer-parallel extension, while the
355
evaporites show ductile behavior.
12
356
4.2. Borehole information on Triassic evaporites
357
Information of the Triassic evaporites is more complete if borehole data are used (Figure 6). In
358
this figure we have assembled a set of wells that especially document the lithologic and thickness
359
variation of Triassic successions in the IZ in Albania (Figure 6a) and Greece (Figure 6b–c). The
360
thicker evaporite sequences occur in the Filiates–1 (~3.6 km) and Butrinti–1 (>3.9 km) wells. The
361
successions in the more complete wells generally have two sections: an upper one formed by
362
anhydrite and gypsum with various levels of dolomites and clays or marls, and a lower one rich
363
in halite with centimetric to metric intercalations (rarely more than 150–200 m) of anhydrite and
364
gypsum. According to well data, the two sequences have different average densities, varying
365
between 2400 and 2900 kg×m-3 between the gypsum and anhydrite-rich and the halite-rich
366
sequences, respectively (Table 1). Between the two sections (anhydrite- and gypsum-rich above
367
and halite-rich below; also reported by (Pomoni-Papaioannou et al., 2004)) there is always a
368
gradational boundary, possibly due to internal shearing within the evaporites (Velaj et al., 1999).
369
Some wells also show thin intervals of other evaporites, like potassic salts, probably rich in
370
sylvite and carnallite (e.g., Astakos–1 well).
371
As we will document later, the large thickness variations (kilometers) in the evaporite
372
successions are not only stratigraphic but are also due to the existence of precursor diapiric
373
structures.
374
Taking the wells along a W–E transect in northern Greece (from Butrinti–1 and Filiates–1 to
375
Parakalamos–1 and Demetra–1; Figure 6a–b), it can be deduced that halite is more abundant
376
toward the west, whereas the evaporite sequences are richer in anhydrite and gypsum toward the
377
east. This agrees with the estimated average densities in these wells, decreasing westward (richer
378
in halite) from Parakalamos–1 to Delvinaki–1 and Filiates–1 (2950 to 2400 kg×m-3, respectively;
379
Table 1). Likewise, and using information from wells in Albania, a N–S variation in the Triassic
380
evaporites, being progressively richer in anhydrite toward the south (with average values
381
increasing toward the south from 2490 to 2590 kg×m-3; Table 1).
382
In our interpretation, these variations probably reflect a lithological variation of the evaporitic
383
sequences in the Upper Triassic IZ basin, being richer in halite toward the West and toward the
384
center, in a region that lies between Albania and Greece. This idea was also pointed out in the
385
region by some previous authors (Pieri, 1990; Savoyat, 1977; Veizaj & Polo, 1999).
13
386
5. Data and Methods
387
Our study has employed three types of data and methods. On the one hand, we have carried out
388
field observations, reinterpreting the salt structures according to modern concepts of salt tectonics
389
(Jackson & Hudec, 2017). In this way we have revised the cartographic information in the area,
390
including new observations and proceeding to unify with our own criteria the geological maps of
391
Greece and Albania, since they use different chronostratigraphic criteria for the IZ.
392
We have also used all the seismic lines available in the region, from those coming from previous
393
campaigns, which have been converted into digital format, to the new seismic lines acquired in
394
2018–2019 by Repsol and Energean in the continental region of northern Greece. The
395
distribution of these seismic lines is shown in Figure 7. The 2D seismic lines have been depth
396
processed by both companies and we have had access to the prestack depth migration (PSDM)
397
profiles in digital format. The depth conversion has been carried out using the average seismic
398
velocities (Vp) of the main lithostratigraphic successions of the IZ (Table 1).
399
The average density and Vp values have been obtained by averaging the sonic data measured in
400
several of the wells in the region (Ágios Georgios–3, Demetra–1, Filiates–1, Lavdani–1 and
401
Parakalamos–1, see situation in Figure 7), according to the study of (Olaya et al., 2020). The
402
average values obtained in the different stratigraphic successions of the IZ are shown in Table 1.
403
The seismic velocities of the Triassic evaporites that we have thus established range from 5.0 to
404
5.8×103 m s-1 (Table 1). These average velocities are higher than those of halite or rock salt (4.2–
405
4.75×103 m s-1), and also turn out to be higher than those estimated for the Triassic evaporites by
406
seismic tomography in the region of Greece (4.2–4.3×103 m s-1) or those deduced from boreholes
407
in Albania (4.5–5.0×103 m s-1) (Makris & Papoulia, 2014, 2018; Makris & Papoulia, 2019; Velaj,
408
2002; Velaj et al., 1999). Our interpretation is that the estimated mean Vp demonstrates that the
409
evaporite succession has in addition to halite, other higher velocity lithologies such as dolomites,
410
gypsum, and anhydrite (Jones & Davison, 2014). For example, amounts around 50% of gypsum
411
and anhydrite in a saline evaporite can cause the average velocity to be between 4.9 and 5.5×103
412
m s-1 (e.g., (Cornelius & Castagna, 2018)). The abundance of dolomitic layers (mean Vp of
413
6.3×103 m s-1; (Jones & Davison, 2014)) would further elevate the mean velocity of Triassic
414
evaporites in the study area.
14
415
416
417
Table 1. Characteristics of the different seismic units of the IZ. Average densities (ρ) and compressionalwave velocities (Vp) used for seismic processing are according to this study and (Olaya et al., 2020).
Detailed information of the different stratigraphic units is shown in Figure 4.
418
Unit
Lithology
Vp (m s-1) a
ρ (kg×m-3) a
Lower Miocene flysch
mudstones, sandstones
2,500–2,800
–
Oligocene flysch
mudstones, sandstones
2,500–4,500
2,500–2,600f
Eocene limestone
Cretaceous limestones
Jurassic sequences
Triassic evaporites
limestones
b
4,700
limestones, cherty limestones
5,300–6,000
limestonesc with mudstone intervalsd
gypsum, halite, anhydrite, and brecciated
dolostones at the top
5,000–6,700
5,000–5,800(5)
2,600–2,700g
2,400–2,900h
Notes:
a. Average values estimated according to well-log properties.
b. Vigla and Senonian limestones.
c. Pantokrator and Siniais limestones.
d. Lower and Upper Posidonia mudstones.
e. Seismic refraction studies in Greece suggest variable sonic velocities for the evaporites, ranging from 4,200–
4,300 m s-1 (Makris & Papoulia, 2014, 2018; Makris & Papoulia, 2019) to 5,000-5,500 m s-1 (Kokinou et al.,
2003), while in Albania average sonic velocities of 4,500–5,000 m s-1 are commonly used (Velaj, 2002;
Velaj et al., 1999).
f. In Albania, a progressive increase in the density of the flysch sequences from 2,470 km×m-3 at the surface
and up to 2,650 kg×m-3 at 3 km depth has been measured in some wells (Veizaj & Polo, 1999).
g. The average density estimated with wells in Albania is quite uniform and does not show variations with
depth. The mean value is 2,670 kg×m-3 (Veizaj & Polo, 1999). Gravity modeling studies in Greece also
suggest an average density of 2,600 kg×m-3 for the carbonate sequence (Makris et al., 2013).
h. Densities are quite variable in the Triassic evaporites, ranging between 2,400 and 2,900–3,000 kg×m-3 in
gypsum- or anhydrite-rich sequences, respectively. Other studies in Albania document variations between
2,490 to 2,590 kg×m-3, suggesting an average value of 2,550 kg×m-3 (Veizaj & Polo, 1999).
419
420
The deep seismic processing has followed a workflow that started with near-surface modeling
421
(NSM) using first-break arrival times including long offsets (detailed information on the depth
422
migration is in (Olaya et al., 2020)). Diving-wave tomography provided a model that was
423
constrained according to surface geology and available well velocities. Flooding models were
424
later created based on the deepest NSM velocities as permitted by the maximum depth
425
penetration. This model enabled us to image a deeper top of evaporites and carbonates sections.
426
Images corresponding to the flood models were used to provide interpretation for guiding deeper
427
model building in an iterative workflow for KDP–RTM migration, which incorporated the
428
measured dips at the surface and the geological models for the sections.
429
The iterative process allowed us to improve the seismic image, finding that the Triassic evaporite
430
bodies show a strong lateral variation of the sonic velocities (Vp ranging from 5.0 to 5.8–6.0×103
431
m s-1). Tops and bases of evaporites are usually difficult to image, especially because they do not
432
exhibit a strong variation of acoustic impedance with respect to the Jurassic or Cretaceous
433
carbonates (which exhibit Vp from 5.0–6.0×103 m s-1 and locally 6.7×103 m s-1). Another
15
434
problem intrinsic to our seismic images comes from the high-dip areas in some structures and,
435
possibly, the complex internal structure of the evaporite bodies. In the thicker bodies of
436
evaporites, we have identified discontinuous strong reflections with variable dip, which might
437
correspond to intrasalt layering due to other lithologies within the Triassic evaporites. On the
438
contrary, when evaporites are in contact with the underlying flysch units, there is always a strong
439
reflection associated with the boundary, which can be either caused by a strong acoustic
440
impedance between evaporites and the flysch sequences or the occurrence of highly strained
441
fabric associated with thrust surfaces.
442
The seismic interpretation has been carried out based on the information provided by the wells
443
(detailed in Figure 7), of which we have presented a selection in Figure 4. Due to confidentiality
444
issues, we cannot show the seismic image so we have chosen to present line drawings of the
445
seismic profiles. The seismic interpretations have been correlated among the 2D seismic lines,
446
making the structures coherent and compatible at all line intersections.
447
Finally, a series of physical models of shortened salt structures are used to compare with
448
structures we see in the IZ, and postulate on their origins. A detailed description of the physical
449
modeling, the materials used, the experimental setup, and how the data was acquired is presented
450
in the Appendix.
451
6. Observations and Results: Salt Structures in the Ionian Zone
452
6.1. General structure of the Ionian Zone
453
The general structure of the IZ, and its relations with other domains in the external zones of the
454
AH FTB (Kruja and Gavrovo–Tripolitza, Krasta–Cukali and Pindos, and Parnassos–Giona zones)
455
are shown in the tectonic map in Figure 7. This map integrates our observations in a detailed
456
framework that brings together multiple cartographic sources, unifying the different geological
457
criteria used in Albania and Greece (Bornovas & Rondogianni-Tsiambaou, 1983;
458
Institut_Francais_du_Pétrole_Mission_Grèce, 1966; Kamberis et al., 2000; Kamberis et al., 2013;
459
Onuzi & Ymeri, 2020; Sejdini et al., 1994; Velaj, 2001; Xhomo et al., 2002; Zelilidis et al.,
460
2015). This map has greater detail in the onshore region, but we have also integrated the available
461
information in the marine region (Bell et al., 2008; Brooks & Ferentinos, 1984; Cushing, 1985;
462
Fournillon et al., 2017; Kokinou et al., 2005; Kokinou et al., 2006) to have a complete overview
16
463
of the AH FTB orogenic front and of the relationships between the IZ with the Sazani–Paxi (Pre-
464
Apulian) zone, the Apulian platform and the Ionian oceanic basin (Argnani et al., 1993; Argnani
465
et al., 2009; Fantoni & Franciosi, 2010; Finetti & Del Ben, 2005). The structure of the western
466
Hellenic accretionary wedge (or the Mediterranean Ridge) is simplified according to (Polonia et
467
al., 2011). The main active and recent faults are taken from various sources (Brooks et al., 1988;
468
Kassaras et al., 2020; Lekkas et al., 1997; Ntokos, 2018; Roberts & Jackson, 1991; Tranos et al.,
469
2020).
470
In this tectonic map (Figure 7), we have highlighted the Triassic evaporite bodies and the
471
surrounding structures, as well as the distribution of the oil and gas shows (and fields) (Bega,
472
2013; Bega & Soto, 2017; Curi, 1993; David et al., 2014; Mavromatidis, 2009; Moorkens &
473
Döhler, 1994; Rigakis et al., 2007; Sejdini et al., 1994; Zelilidis et al., 2015; Zelilidis et al.,
474
2003). Finally, the map also includes the positions of the seismic lines and wells we have used in
475
our study.
476
Thrusting within the IZ produces kilometric tectonic repetitions of the evaporites (Figures 3, 7–8)
477
(Kamberis et al., 2022; Sadekaj et al., 1992; Sotiropoulos et al., 2022; Underhill, 1989; Velaj,
478
2001, 2015) and their ductile expulsion and flow feeding thick frontal plugs, like for example in
479
the Dumrë diapir (Figure 7) (Bega & Soto, 2017; Velaj et al., 1999). Our interpretation of the
480
general structure of the IZ is given in the two regional cross sections in Figure 8 and is based on
481
historical (from the 60’s to the 90’s) and recent borehole information and the interpretation of
482
two large seismic line transects oriented parallel to the main shortening direction (NE–SW). The
483
seismic transects are built up by joining some of the recently acquired 2D seismic profiles in
484
northern Greece and available seismic profiles in southern Albania. The two sections are
485
constrained by surface observations, such as dip measurements included along the topographic
486
profile.
487
The names given in Greece and Albania to these thrust sheets vary, but we propose the following
488
correlation from innermost (east and higher) to outermost (west and deeper): Berati or internal
489
Ionian, Kurveleshi or middle Ionian, and Ҫika or external Ionian
490
(Institut_Francais_du_Pétrole_Mission_Grèce, 1966; Karakitsios & Rigakis, 2007; Papanikolaou,
491
2021; The_B.P._Co_Ltd., 1971; Zelilidis et al., 2015; Zelilidis et al., 2003). In Albania, another
492
thrust sheet, the Sqepuri thrust sheet (Figure 8a), has been locally differentiated (Bare et al.,
17
493
2001; Meço et al., 2000; Roure et al., 2004; Sadekaj et al., 1992; Sejdini et al., 1994; Velaj, 2001;
494
Velaj et al., 1999; Xhomo et al., 2002). Due to its position and deep structure, we interpret the
495
Sqepuri as an imbricate of the Kurveleshi (middle Ionian) sheet. Stratigraphic variations in the
496
Mesozoic succession between these three thrust sheets have been described in previous studies of
497
the IZ (Aliaj, 1974; Aubouin, 1958, 1959b; Bega & Soto, 2017; Bernoulli & Renz, 1970;
498
Institut_Francais_du_Pétrole_Mission_Grèce, 1966; Karakitsios, 1995; Nikolaou, 1988; Plaku &
499
Murataj, 1974; Prifti et al., 2013; Renz, 1955; The_B.P._Co_Ltd., 1971; Velaj, 2002; Velaj et al.,
500
1999). However, based on our field observations, we believe that these variations, rather than
501
sedimentary facies, are thickness variations toward previous diapiric structures. However, more-
502
detailed field work is needed to resolve this question.
503
Larger accumulations of evaporites also are present. We interpret these to be caused by precursor
504
diapirs where the wells show kilometer thicknesses of the evaporite succession (especially the
505
wells Filiates–1 and Butrinti–1; Figure 6). The shapes of these bodies, their structures, and the
506
relationships with the nearby sequences allow us to differentiate several major types of salt
507
diapiric structures in the IZ. The general structure of some of these is documented by more-
508
detailed mapping in Figures 9 through 11 and in selected field observations (Figure 12).
509
The four types of salt diapiric structures in the IZ are as follows:
510
1. Subcircular- to elliptical-plan diapirs, which appear to be shortened and tectonically
511
translated salt plugs (SP), such as the Dumrë (DSP) (Bega & Soto, 2017; Jardin et al.,
512
2011; Velaj et al., 1999) and Filiates (FSP) (Figure 10) structures.
513
2. Salt walls (SW) of pluri-kilometer length and of preferential orientation subperpendicular
514
to shortening, such as those of Butrinti–Xarra (BSW) (Figures 10 and 11a–b), Delvinaki–
515
Parakalamos (DSW) (Figure 9), and Fyteies–Trífos (FSW) (Figure 11).
516
517
518
3. Gentle unrooted salt pillows (P), which are detached and displaced by thrusts, such as the
Delvinë pillow (DP) (Bega & Soto, 2017).
4. Pinched-off diapirs, which we also found. These exhibit reverse faults cutting the thrust-
519
related anticline and the secondary thrust welds. Anticlines of this type with associated
520
thrust welds (WA) have been identified in Vasiliko (VWA) (Figures 9 and 12c–d),
521
Navarica (NWA) (Figures 9 and 12i–j), the Kassidhiáris Mountains, near the
18
522
Parakalamos–1 well (KWA) (Figures 9 and 12 g–h) and the shortcut thrust seen in Parga–
523
Sarakiniko (PWA) (Figure 10),
524
Our description of these structures will bring together field and cartographic observations
525
(Figures 9–11 and 12, respectively), with the interpretation of selected seismic profiles (Figures
526
13 and 14), in whose interpretation we have integrated a revision of the chronostratigraphic
527
information provided by the wells (Figure 6).
528
6.2. The Butrinti–Xarra salt wall and other salt structures in South Albania
529
On the border between Albania and Greece, an elongate and narrow (20×3–5 km) salt structure
530
extends from the Greek coast near Sayiadha to Lake Butrint, just north of Vrina (or Vrinë) in
531
Albania. The Butrinti–1 well shows that this salt structure is at least 4 km thick and that the
532
evaporites lack a Mesozoic or Neogene overburden (Figure 6a). Our review of the previous
533
mapping of the area is shown in Figures 9 and 10, and we interpret this structure to correspond
534
with an elongate NW–SE salt wall, which we have termed the Butrinti–Xarra salt wall (BSW).
535
Several observations support this interpretation:
536
1. The eastern flank of the wall is formed by an anticline parallel to the salt wall and the
537
Mesozoic successions (the Vigla and the Senonian limestones; Upper Jurassic to Upper
538
Cretaceous) dip westward against the salt structure.
539
540
541
2. A similar fold is found on the western flank of the salt wall and local thrusts are
developed over the evaporites (Figure 12a–b).
3. Successions are progressively younger to the SE on the eastern flank of the wall, with
542
obliquity relations to the salt structure (with the Eocene limestones coming to rest on the
543
salt wall between Konispol and Sayiadha).
544
4. To the north, the wall culmination deepens northward and north–south folds affect only
545
the Upper Triassic dolomitic succession and the Pantokrator Formation (Hettangian to
546
Sinemurian).
547
With these observations, we interpret that the salt wall is shortened in the NE–SW direction,
548
allowing the approach of the two flanks that are deformed with anticlines against the wall, while
549
the salt wall is shortened and probably upbuilds, preventing the deposition of Paleogene or
550
Neogene sediments on top. In addition, according to observations around Sayiadha, we propose
19
551
the wall is resolved toward the SE by a subvertical weld that is partially cut by a thrust sheet to
552
the SW (Figure 10). The connections with the Filiates structure are not visible at the surface,
553
because the whole area is covered by very recent sediments (the Kalamas River delta plain;
554
(Chabrol et al., 2012)). We believe that the BSW is connected to the Filiates structure through a
555
narrow area, where the evaporites are squeezed, forming a weld zone that is also cut by a SW-
556
directed thrust (near Smertos) (Figure 10).
557
According to our seismic interpretation (Figures 13g, 14g), the BSW is displaced to the SW by a
558
basal thrust that lies at about 5.5 km depth beneath the Butrinti–1 well [identified at 2 s two-way
559
travel time (TWT) and using a mean Vp of 5.5×103 m s-1], with evaporites probably detached on
560
the lower Miocene flysch. Beneath the BSW, we identify another IZ sheet, which may have
561
deeper evaporites in a para-autochthonous position (at about 11–12 km depth). The western flank
562
of the BSW corresponds with a listric thrust, detached above the evaporites, in which a strong
563
succession of Upper Triassic dolomites and the Pantokrator Formation, describes a hanging wall
564
ramp of a NE-directed backthrust over the salt wall.
565
Two other salt structures have been studied in southern Albania. In a previous work, we
566
described the Delvinë salt structure (Bega & Soto, 2017) (Figure 9). Because of its geometry, as a
567
gentle culmination of the Triassic evaporites with progressive onlaps of the Upper Triassic
568
dolomites and Pantokrator formations on the two flanks, we consider that this structure
569
corresponds with a salt pillow (the DSP). According to these observations, we infer that the salt
570
pillow emerged in the Mesozoic basin of the IZ during Upper Triassic to Middle Jurassic time.
571
The other structure we have studied in Albania is the Navarica (or Navaricë) structure in the
572
Livinë Mountains (Figures 9 and 12i–j). Here, Triassic evaporites outcrop as gypsum-rich black
573
clays and dolomites at the core of a thrust-cut anticline. Above the evaporites, we find folded
574
onlaps in the Upper Triassic successions and in those of the Pantokrator Formation. We interpret
575
the general geometry as corresponding to a decapitated diapir, with the central conduit still open
576
but not completely welded. It would therefore be an example of a diapiric anticline cut by a thrust
577
weld.
578
6.3. The Delvinaki–Parakalamos salt wall and the Vasiliko pinched-off anticline
20
579
The first major structure we describe in Greece includes two large Triassic outcrops in Delvinaki
580
and Parakalamos (DSW). The overall structure of the salt walls has been reinterpreted, including
581
our observations as shown in Figure 9. Both bodies are linked by a narrow corridor of evaporites
582
just south of Delvinaki. The Delvinaki structure elongates NW–SE until it disappears
583
progressively to the N, where the Vigla Formation is directly in contact with the evaporites. The
584
entire south contact is a low-angle thrust where evaporites overthrust the Aquitanian–Burdigalian
585
flysch. Discontinuous and thin lenses of Cretaceous–Eocene and even Oligocene flysch
586
formations can be found along this contact, almost always in an inverted position and with a thin
587
thickness. On the NE flank of the Delvina structure, oblique W–E folds and progressive onlap
588
relationships to the NW are identified. The Delvinaki–1 well also shows that the evaporites
589
overthrust the Oligocene flysch succession, probably in normal polarity (Figure 6b).
590
The other evaporite body, around Parakalamos, is bounded to the north by W–E-oriented, left-
591
lateral strike-slip faults, while on its eastern edge there are NW–SE folds that run obliquely to the
592
evaporites. The western edge corresponds with a thrust toward the east, which progressively
593
becomes to the south into a subvertical fault zone (or weld), where Cretaceous successions (Vigla
594
and Senonian limestones) collide with opposing thrusts. Continental sediments of Messinian age
595
seal the structure here. The Parakalamos–1 well did not reach the base of the evaporites but
596
shows that this succession is more than 1.5 km thick (Figure 6b).
597
We interpret both outcrops to correspond with a complex salt wall, the DSW, perhaps composed
598
of two close and joined diapirs in plan view and finally thrusting SW over the lower Miocene
599
flysch. Note that between the two diapirs, when the orientation of the salt wall is west–east, and
600
forms a small angle with the shortening direction (NE–SW), a major strike-slip fault system is
601
formed along the salt wall.
602
In this same sector, just west of the Parakalamos wall, in the Kassidhiáris Mountains, we interpret
603
the structure to describe a tight anticline with subvertical flanks, cut by double-vergent, high-
604
angle thrusts (Figures 9 and 12g,h). Surface observations, together with information from wells in
605
the area (Lavdani wells 1 through 3 and Parakalamos–1), allow us to interpret this structure as
606
corresponding to a tight box-like anticline [a detached lift-off fold; (Mitra, 2003)], whose core
607
has a vertical weld, connected with the source layer of evaporites, which do not outcrop (see inset
608
in Figure 12h).
21
609
The deep structure of the DSW is illustrated by two profiles perpendicular to the structure
610
(Figures 13e,f and 14e,f). We interpret this salt wall as part of an allochthonous sheet that moves
611
SW over a tight syncline affecting only the flysch successions so that the basal thrust of the
612
evaporites eventually cuts a thin reverse flank, as attested by data from the Delvinaki–1 well. Our
613
review of the stratigraphy of this well suggests that levels that would be lower Miocene are
614
already beneath the Oligocene flysch. On the other hand, our seismic interpretation suggests that
615
the DSW is compressed and that outside this structure, the evaporites become a constant layer
616
with local highs formed by squeezed anticlines. Below this thrust sheet, which corresponds to the
617
inner IZ (or Berati), we interpret that there is another thrust sheet detached over the Triassic
618
evaporites, with internal imbrications and some backthrust structures (Figure 14f). This lower
619
sheet would therefore be the middle IZ (or Kurveleshi).
620
The Vasiliko salt anticline (VWA) allows a detailed observation of a subvertical secondary weld
621
(Figure 12c–d). In this domain the evaporites are strongly deformed by subvertical brittle shear
622
zones, bounding lenticular domains of gypsum and clays in which an associated cataclastic
623
foliation is found. This weld is the core of a tight anticline deforming successions of the Vigla
624
Formation. Field observations and the development of inverted flanks near the salt weld suggest
625
that the VWA must have a non-outcropping upper bulge (or teardrop), disconnected from the
626
pedestal at the root. This is the geometry we include in seismic interpretations of the area
627
(Figures 13e, 14e).
628
6.4. The Filiates diapir and the Parga–Sarakiniko salt thrust
629
The Filiates structure is shown in the mapping in Figure 10. The plan-view shape of this structure
630
is complex, resembling a rhombus whose boundaries outcrop only to the north, east, and south.
631
Inside, the evaporites generally dip to the north, defined by some thick gypsum package (Figure
632
5a). Given information from the Filiates–1 well, the evaporite thicknesses are about 3.75 km
633
(Figure 6b). We interpret that this structure corresponds to a diapir (or plug) whose present-day
634
contacts are strongly modified by Alpine shortening: the Filiates salt plug (FSP). For example, in
635
the north (near Filiates), Cretaceous successions (especially the Vigla and the Senonian
636
limestones) dip southward against the diapir, and above the diapir, these same successions are
637
condensed and deformed by west–east folds (isolated outcrops between Smertos and Filiates).
638
We interpret the northern contact of the FSP to currently be a high-dipping reverse fault that
22
639
laterally transitions to a WNW–ESE, dextral strike-slip fault. On that flank, we have identified a
640
set of NW–SE folds that affect the entire Jurassic and Cretaceous succession, which is locally
641
thicker here and is deformed by overturned and asymmetric, NE-vergent folds that may be locally
642
cut by folded thrusts (Figure 12e,f and inset). On the eastern edge and to the south, the FSP roof
643
thrusts westward (with sheets involving mainly the Vigla and the Senonian limestones). Some of
644
these thrusts imbricate the diapir evaporites themselves (NE of Igoumenitsa, in the Varathi
645
Mountains). The FSP is terminated to the SE by a narrow shear zone that we interpret as a salt
646
weld, in which the evaporites are characterized by pervasive ductile shearing (Figure 5g,h). This
647
weld is cut by a SE-directed thrust, which in its footwall develops a S–verging anticline with a
648
kilometer-long reverse flank affecting the Vigla Formation (observed between the cape of
649
Vrachonisída Ágios Dionýsios and Plataria; Figure 10).
650
The deep structure of the FSP is shown in four seismic profiles and their interpretation; thus, we
651
have studied two sections subparallel to the shortening direction (NE–SW; Figures 13a,b and
652
14a,b) and two perpendicular (NW–SE; Figures 13c,d and 14c,d). The FSP is a thick salt body
653
with continuous internal reflections (probably from other evaporites) that are folded (Figure 14a),
654
while the base is a gently dipping thrust advancing SW over the Oligocene and lower Miocene
655
flysches (as is confirmed by the well Filiates–1; Figure 6b). The FSP is part of a thrust sheet
656
(external IZ or Ҫika) that is detached over a para-autochthonous succession that may have minor
657
internal imbrications (Figure 14b). Its extension outside the study area, already in the marine
658
region, could contain another salt wall (trending NW–SE) that is the one outcropping on Corfu
659
Island (Figures 3b, 7) (e.g., (Tserolas et al., 2019; Waters, 1994)).
660
The FSP has two flanks with different geometries in the suprasalt series. The SW flank is formed
661
by a backthrust (to the NE) involving a thick Middle Jurassic to Lower Cretaceous limestone
662
succession (including the Vigla Formation). The eastern flank, on the contrary, contains a thick
663
succession of the same sequences but also exhibits deformed disharmonic folds against the
664
parallel succession of Triassic dolomites and the Pantokrator Formation, which might represent a
665
folded megaflap (Figure 12e,f and inset). We interpret this flank to correspond to a minibasin that
666
developed from the Middle Jurassic to the Lower Cretaceous on the NE flank of the FSP and then
667
shortened along with the diapir, developing backthrusts that may incorporate the evaporites of the
668
source layer (Figure 14a–c).
23
669
In this northern sector of Greece, we have also studied the area between Parga, Sarakiniko, and
670
Perdika (Figure 10). Here we interpret that a tight NW–SE anticline develops, with an incomplete
671
secondary weld that is finally displaced to the SW by an out-of-sequence thrust that superimposes
672
the salt anticline (PWA) on the Oligocene flysch (the tectonic window between Parga and
673
Perdika) and finally, at the front (to the SW), on Messinian evaporites, as observed in the cliffs of
674
the Sarakiniko and Arillas beaches.
675
6.5. The Fyteies–Trífos salt wall
676
The other sector studied in Greece contains a large elongated NNW–SSE structure between the
677
gulfs of Arta and Preveza, outcropping from the locality of Paliampela to that of Katochi (Figure
678
11). By its shape and geometrical relationships, this structure corresponds to a relatively narrow
679
(60×6–7 km) salt wall (the Fyteies–Trífos salt wall, FSW), on which multiple doline fields are
680
developed and in which the salt wall is covered by subhorizontal packages of brecciated massive
681
dolomites and small outcrops of the Vigla Formation. Structures within these later outcrops
682
describe small synclinal basins, with progressive unconformities, wedging, and debris flow levels
683
(Figure 12k,l). We interpret these domains as local minibasins, with condensed sequences of
684
Cretaceous sediments whose sedimentation was conditioned by the local movement (uplift and
685
subsidence) of the Triassic evaporites.
686
The FSW exhibits three major structural features. First, the entire eastern contact is a narrow,
687
subvertical, left-lateral strike-slip fault zone, which was cut by the Trifos South–1 well (Figure
688
6c). The deformation associated with the fault is largely produced by brittle faulting, where
689
lenses of hundreds of meters of Mesozoic limestones (Pantokrator, Vigla, and Senonian
690
limestones) are found. No traces of deformation are associated with this fault zone within the
691
FSW, except in rare NW–SE dextral faults that occasionally develop only in dolomitic packages
692
overlying evaporites. This fault zone (the Aitoloakarnania, left-lateral strike-slip fault) has
693
associated seismic activity and constitutes the active western edge for the Kalivia–Lisimakia or
694
Trichonis basin (Tranos et al., 2020; Underhill, 1989).
695
Second, to the north, two windows are developed under the basal salt thrust of the FSW,
696
outcropping the Oligocene flysch in its hanging wall (around the Trifos–2 well). In this same
697
sector, we interpret that the salt wall is losing height and the Neogene sediments of the Drimos
24
698
region come to rest directly on the subsalt sequences, suggesting an almost complete welding of
699
the allochthonous evaporite layer.
700
Finally, the western edge of the FSW presents two types of singular structures. In the north, from
701
Paliampela to Kompoti, the salt wall overthrusts westward, an inverted succession (through a
702
north–south synclinal fold) of the Oligocene flysch, with condensed layers at the top
703
corresponding to the Vigla and the Senonian limestones. In contrast, south of Aetos, the entire
704
western edge of the FSW corresponds with backthrusts to the east, developing two large thrust
705
sheets (one each at Vasilopoulos and Bampini) and associated folds that superimpose a thick
706
Mesozoic limestone succession (from the Pantokrator to the Senonian limestones) on the
707
evaporites. Although none of these thrusts imbricate the Triassic evaporites, one of these folds is
708
nucleated in them (Astakos–1 well; Figure 6c), so the Triassic succession, although being a
709
detachment level for these backthrusts on the western flank of the FSW, must also flow into the
710
anticlinal cores during Alpine shortening.
711
7. Experimental Models of Fold and Thrust Belts with Precursor Diapirs
712
Numerous publications have recently analyzed the role of preexisting salt structures in a thin-
713
skinned FTB (Callot et al., 2007; Callot et al., 2012; Dooley et al., 2009b; Dooley et al., 2015;
714
Duffy et al., 2018; Granado et al., 2019; Rowan et al., 2022; Rowan & Vendeville, 2006;
715
Santolaria et al., 2021; Santolaria et al., 2022). Our goal has not been to perform new experiments
716
that analyze this well-known situation, but rather to gather published and unpublished
717
information from existing experiments that explore some of the main problems we have
718
identified in the IZ. For example, what structural differences can we find between a shortened
719
diapir and a shortened wall? What structural style develops during shortening of variably oriented
720
salt walls? What structural style do shortened salt structures develop in section? And how does
721
deformation vary spatially and temporally?
722
Note that some tectonic processes that are operating in the IZ e have not been analyzed by
723
experimental models, such as the inversion of synrift salt structures (e.g., (Dooley & Hudec,
724
2022; Hudec & Jackson, 2007; Jackson & Hudec, 2017; Letouzey et al., 1995)), the role of salt-
725
layer (and basement) tilting on subsequent shortening (e.g., (Dooley et al., 2007; Santolaria et al.,
726
2022)), and how the deformation evolves having varying shortening directions over time.
25
727
The plan-view evolution in of a system of isolated diapirs and variably oriented salt walls during
728
shortening is illustrated in Figures 15 and 16, respectively. These figures show how the structures
729
on the surface of the models vary under increasing shortening strains.
730
In the case of isolated diapirs (Figure 15), shortening migrates progressively toward the foreland
731
(left in all models), generating initial soft links between neighboring diapirs (Figure 15a), then
732
doubly vergent thrusts in the hinterland (Figure 15b,c), and finally frontal thrusts that can verge
733
toward the hinterland (Figure 15d) (see also (Callot et al., 2007; Callot et al., 2012; Dooley et al.,
734
2015; Santolaria et al., 2022)). The foreland migration of the deformation is caused by the fact
735
that the entire suprasalt succession is detached above the salt layer. Other results of this model
736
indicate: (1) that pop-ups are generated by the linkage of neighboring diapirs; (2) that these
737
structural ridges (pop-up anticlines that have a broad and flat culmination) become narrower
738
around the diapirs and migrate toward the foreland, progressively moving away from their zone
739
of origin and end up displaced with respect to the position of the original diapir, and (3) that the
740
geometries of the thrusts are conditioned by the diapirs. For this last point, all the models
741
preserve an early structural feature, such as the thrust reentrants toward the position of the diapirs
742
(see also (Dooley et al., 2009a; Duffy et al., 2018; Rowan et al., 2022; Santolaria et al., 2021)).
743
In the case of shortened salt walls, the structural evolution is strongly conditioned by their
744
position, but also by their orientation with respect to the shortening direction (Figure 16) (see
745
further details in (Dooley et al., 2009b; Duffy et al., 2018; Jahani et al., 2009)). Some major
746
features are shared with the previous model, such as the advance of the deformation toward the
747
foreland, the nucleation of thrusts and associated folds in the salt structures, and the displacement
748
of the shortening structures as the deformation advances. The novel features are as follows:
749
1. Walls oriented at a high angle to shortening nucleate long thrusts and anticlines (mostly
750
foreland-vergent) associated with the salt high (e.g., walls e and f in Figure 16);
751
2. Walls oblique to shortening develop systems of curved, long faults and folds, and;
752
3. “Relay or stepover” structures form between nearby walls, and also strike-slip faults with
753
variable kinematics, but dominantly transpressional along these walls (wall d in Figure
754
16c–d).
755
Walls oriented parallel to the shortening evolve into a large dome by ductile salt flow, eventually
756
creating a local major diapir with a subcircular shape (wall a in Figure 16c,d). The figure also
26
757
illustrates how the thrusts originate in the salt walls, but as shortening increases, deformation
758
propagates in the salt roofs and the salt walls are squeezed and welded, developing grabens with
759
normal faults along their crests due to outer arc extension above the rising diapiric salt (e.g., wall
760
e in Figure 16d).
761
The final geometry of the structures around salt walls with different orientation is shown with
762
several sections in Figure 17 (using the end result of the model in Figure 16). The walls oriented
763
parallel to shortening (number 1 in Figure 17) become shorter and narrower as the salt flows
764
upwards to form allochthonous salt sheets (Figure 17a). In this case, the salt wall remained open
765
due to its length relative to the amount of shortening it absorbed, and may develop salt wings
766
along the roof bedding. The walls perpendicular to shortening (number 4 in Figure 17), on the
767
contrary, are closed more rapidly, developing subvertical secondary welds that link upwards to
768
allochthonous salt sheets or salt bulbs, and finally end up being cut and displaced by foreland-
769
directed thrusts (Figure 17a,b). Oblique walls (numbers 2, 3, and 5 in Figure 17), after
770
considerable shortening, develop both vertical secondary welds with double-vergent thrusts
771
(number 3 in Figure 16c), as well as secondary welds cut by thrust welds (numbers 2, 3, and 5 in
772
Figure 16b,c).
773
The temporal evolution of a shortened salt wall from an arched roof to upright weld, to finally a
774
displaced secondary weld is shown in Figure 18. Shortening begins by focusing on the weak
775
diapir, resulting in its gradual closure displacing diapiric salt both upwards and downwards
776
(Figure 18a). Once the wall closes, a vertical secondary weld develops (Figure 18). Finally, if the
777
shortening continues, a foreland-vergent thrust develops, cutting and displacing the original
778
vertical weld (Figure 18c), similar to those seen in Figure 17. Other noteworthy processes are the
779
development of pop-ups above the wall crest as salt is forced to upwards during initial
780
shortening, and the existence of two opposing salt flows. Initially, salt flows from the wall into
781
the source layer, inflating it to fill the space created by the rising hangingwall (number 2 in
782
Figure 18a), followed by the development of an upward salt flow from the diapir due to the
783
impingement by approaching wallrocks, which initially feeds the salt bulb at shallow levels and
784
then a salt nappe at the surface after the roof was breached (numbers 3 and 4 in Figure 18b). Both
785
types of flow were characterized by (Dooley et al., 2009a), who called them outward and inward
786
plumes, respectively.
27
787
Finally, we have gathered experiments to explore the geometry of two types of structures. Firstly,
788
the structural configuration that develops in relation to the so-called “Q-tips” (Rowan &
789
Vendeville, 2006) (Figure 19a). And also, the structures that can develop in the vicinity of
790
welded walls (Figure 19d). The models we have chosen to study these structures come from salt
791
walls oriented at a high angle to the shortening direction (80º). These models differ in the
792
thickness of the original source layer, and thus height of the diapir that could be generated.
793
“Q tips” structures are characterized in plan-view by a secondary weld with the orientation of the
794
original salt wall, connecting two isolated salt bodies at their lateral terminations. The structural
795
style can be very variable depending on the orientation of the cross section. In those parallel to
796
shortening, the central weld develops in the source layer, while an upper diapir upwarp the
797
overburden that is also deformed by double-vergent thrusts (Figure 19b). Sections perpendicular
798
to the shortening, however, show a diapir with two large lateral wings, again bounded by
799
opposing thrusts (which in this case would correspond to lateral ramps) (Figure 19c).
800
In our model with higher salt walls and thus thicker diapir-bounding sequence, a secondary weld
801
develops as seen previously, but also two strike-slip faults with opposite displacements that end
802
against the lateral terminations of the wall. These “tear faults” (number 7 in Figure 19d) bound a
803
suprasalt “indentor” that into the wall, displacing diapiric salt and allowing the development of
804
the vertical secondary weld. After advanced stages of shortening this secondary weld is thrusted
805
and displaced (number 5 in Figure 19e).
806
We suggest that many of these structures developed in the experimental models explain cases that
807
we have observed in the IZ, as we will discuss in the next section.
808
8. Discussion
809
8.1. Influence of preexisting diapirs on the orogenic evolution of the Ionian Zone
810
Our study has demonstrated several types of salt structures in the IZ. We have characterized their
811
geometry and relationships with the salt roofs, assessing the role they have played in the
812
shortening of the IZ during the Alpine orogeny. In addition to detailed observations and
813
geological cross sections generated with structural criteria and supported on seismic
814
interpretations, our overview of the diapiric structures and the structural organization of the IZ is
815
summarized in Figure 20. This is a simplified tectonic map of the entire IZ, bringing together our
28
816
own observations and previous mapping information in Albania and Greece. The main tectonic
817
features have been simplified from Figure 7, highlighting the different types of salt diapirs
818
identified.
819
Four types of structures nucleated in the Triassic evaporites exist in the IZ (Figure 20):
820
1. Salt pillows such as the Delvinë (or Delvina) (DSP) and Picari–Kardhiq (PK).
821
2. Diapirs rising from a point source (sensu (Jackson & Talbot, 1991)), and which are often
822
deformed and unrooted/displaced, currently forming part of high-allochthonous thrust
823
sheets, such as the Dumrë and Filiates diapirs (or plugs; DSP and FSP, respectively).
824
3. Salt walls rising from line sources (sensu (Jackson & Talbot, 1991)), such as the Corfu
825
(CSW) and those studied here, the Butrinti–Xarra (BSW) and Fyteies–Trífos (FSW).
826
4. Welded pinched-off anticlines that are finally cut by out-of-sequence thrusts that displace
827
the secondary weld, such as the structures in the Kassidhiáris Mountains (KWA),
828
Navarica (NWA), Vasiliko (VWA), and the shortcut thrust seen in Parga–Sarakiniko
829
(PWA).
830
The Delvina–Parakalamos structure (DSW) can be considered a mixed case, because although
831
globally it is an allochthonous salt wall, it is internally composed of two diapirs connected by a
832
narrow corridor where the suprasalt succession reaches greater thickness (cf. just south of the
833
Delvinaki locality in Figure 9). This type of geometry has been found in other salt walls, for
834
example in the North Sea (e.g., (Tvedt et al., 2016)), so we are inclined to interpret it as a salt
835
wall with two local bulges or diapirs.
836
In light of our observations and experimental models described in the previous section, it is clear
837
that the relief, shape, and orientation of salt structures condition the structural style of the IZ
838
FTB. However, there is a fundamental difference between the geology under study and our
839
models due to the nature of the Triassic evaporites that are formed by many lithologies, and to a
840
lesser extent by halite, which gives them a higher viscosity and heterogeneity than the
841
experimental models. The existence of thin salt levels in an evaporite sequence with abundant
842
competent lithologies that will tend to deform brittlely gives the Keuper evaporites rheological
843
characteristics that have not yet been studied in other Alpine FTBs. For example, it may be that
844
the higher viscosity of the Triassic evaporites here causes the deformation of the salt diapirs to be
29
845
resolved by salt-involved thrusts and with only partial diapir welding as the more mobile units
846
are expelled and the less mobile ones are left behind.
847
The following major features observed in the IZ also appear in the models:
848
849
1. Thrust curvature of thrusts toward the position of diapirs, forming reentrants; e.g., in
DSW and FSP (as in Figure 15b,c).
850
2. Secondary welds and thrust welds, with out-of-sequence thrusts cutting salt bulges (e.g.,
851
KWA, NWA, PWA, and VWA), with double-vergent thrusts also developing from such
852
salt structures (as in Figures 17c, 18).
853
3. Variable structural style depending on the orientation of the salt wall versus the direction
854
of shortening, as may occur in the oblique walls of BSW, DSW, and FSW, as opposed to
855
the perpendicular salt wall of Corfu (as shown in Figures 16, 17). So oblique salt walls
856
develop strike-slip faults only along their edges (e.g., Aitoloakarnania fault in FSW;
857
(Tranos et al., 2020; Underhill, 1989)); in turn, their kinematics depend on the initial
858
orientation of the wall with respect to shortening direction (as in Figure 16).
859
4. Pinching at the centers of the salt walls, creating two salt bodies at their ends (“Q-tips”)
860
joined by a narrow conduit (or even welded in a secondary weld), as found between the
861
Delvinaki and Parakalamos culminations in DSW or the thrust welds found between BSW
862
and FSW (as in Figure 19a).
863
5. Almost complete welding of the salt walls perpendicular to shortening, developing two
864
strike-slip faults with opposite kinematics at their ends, bounding an indentor in the
865
suprasalt succession (as in Figure 19b). This geometry is probably the case for the Corfu
866
wall (with the right-lateral, South Salento strike slip fault in the north of this wall;
867
(Tserolas et al., 2019)), outside the studied area, which also describes a salient of the IZ
868
orogenic front against the Pre-Apulian zone (Figure 20).
869
6. Finally, on the scale of the entire AH orogen, the thrusts of the IZ have a unique shape.
870
The thrusts arc toward the foreland, drawing several salients, such as the one located at
871
the front (and west) of the island of Corfu. The thrust system converges in two lateral
872
branches where the IZ ends, such as in the Zákynthos region, to the south, and in the NE–
873
SW alignment of Vlora–Dibër–Elbasan, around the Dumrë diapir (Figures 7, 20). South
874
of Zákynthos and west of Peloponnesus, in the offshore area, Triassic evaporites are only
30
875
represented by a thin layer (Karakitsios et al., 2017; Kokinou et al., 2005; Kokinou et al.,
876
2003; Kosmidou et al., 2018; Sotiropoulos et al., 2022). To the north of the Vlora–Dibër–
877
Elbasan Lineament, there is no trace of these evaporites in the subsurface (Bega, 2013,
878
2020). The existence of salt walls also conditions the shape of the front, but the lateral
879
terminations and the shape of the IZ FTB may be due to the original distribution of the
880
Triassic evaporites and the evaporite facies distribution (being richer in halite toward the
881
center and West of the basin). So, as described by some experimental models (Cotton &
882
Koyi, 2000; Letouzey et al., 1995), the lateral limits of a salt layer determine that the
883
thrust system develops large lateral ramps as is seen in both regions.
884
We have analyzed the pattern of rotations deduced from paleomagnetic studies. To compare this
885
type of information with our interpretation of salt tectonics in the IZ, we have chosen only those
886
rotations established for the carbonate section (Jurassic to Paleocene), presenting the results in
887
Figure 20 (revising data from (Birch, 1990; Broadley et al., 2006; Horner & Freeman, 1983;
888
Márton et al., 1990; Waters, 1994)). All studies of this type have shown two main features:
889
1. The entire IZ has experienced a variable clockwise rotation that began in an early
890
preorogenic epoch, probably since the Late Cretaceous Epoch (Broadley et al., 2006;
891
Kissel et al., 1985; Speranza et al., 1995; Speranza et al., 1992), and
892
2. Strike-slip faults such as the Kefallinia–Lefkas–Lixourion transpressional fault and the
893
Vlora–Dibër–Elbasan Lineament, have been active during the orogeny and until at least
894
the Pliocene Epoch, producing major local rotations (Duermeijer et al., 1999; Duermeijer
895
et al., 2000; Mauritsch et al., 1995; Speranza et al., 1995; van Hinsbergen et al., 2005).
896
Some authors have also proposed that the rotations vary progressively in the IZ,
897
decreasing toward the foreland (westward) and that there are differential rotations
898
between some thrust sheets and others (e.g., (Broadley et al., 2006; Kondopoulou, 2000;
899
Mauritsch et al., 1995)). However, the distribution of rotations, when compared to diapirs,
900
shows a feature not sufficiently well appreciated previously: many of the salt structures
901
show variable rotations around them (see, for example the data around FSP and DSW).
902
Given the available data, we suggest that the diapiric highs thus conditioned the internal
903
rotation within the same thrust sheet, which would agree with what is shown in the
904
experimental data, where it can be seen not only that the thrusts rotate toward the diapirs,
31
905
but that the suprasalt successions also rotate differentially on either side of these
906
structures (Figure 15). This suggestion is useful for paleomagnetic studies in other FTBs
907
with salt structures.
908
8.2. How to differentiate preexisting diapirs in a fold and thrust belt
909
The case of the IZ differs from some other cases of salt-involved FTBs, because of several
910
peculiarities that should be highlighted.
911
1. The Triassic evaporites (Keuper) are an effective detachment level during shortening, but
912
they have a great lithological heterogeneity, with anhydrite, gypsum, and dolostones
913
(occasionally also weaker potassic salts) predominating many times over halite, and being
914
richer in halite toward the center of the basin and basinward. This heterogeneity confers a
915
greater viscosity to the salt layer undergoing deformations and gives them a complex
916
rheology in which levels of different thicknesses coexist with brittle behavior, as opposed
917
to others that behave in a ductile manner. This is not a singularity of the IZ, as it is a
918
constant in the Keuper evaporites in the Alpine belts of the Mediterranean (see (Soto et
919
al., 2017)) and in other FTBs such as those of the Appalachians (Mount, 2014), the Sub-
920
Andean FTB (Baby et al., 2018), and the Zagros FTB (Najafi et al., 2014; Sherkati &
921
Letouzey, 2004). Although it differs from other FTBs in where the evaporites are
922
dominated by halite (e.g., in Central Sivas Basin; (Kergaravat et al., 2017)).
923
2. In our case, we have not identified structures such as allochthonous salt sheets (e.g.,
924
(Flinch & Soto, 2022)), nor salt wings, nor thick sedimentary sequences filling secondary
925
minibasins that can completely weld the source layer (e.g., (Kergaravat et al., 2017)). This
926
is probably due to a lower thickness of the IZ evaporites, as well as to their
927
aforementioned higher viscosity and complex rheology.
928
3. Another problem that is often discussed in the interpretation of FTBs with evaporites is
929
whether the observed structures can be explained only by thrust and fold tectonics without
930
the need for preexisting diapirs (e.g., (Kamberis et al., 2022; Liesa et al., 2023; Lykakis et
931
al., 2021)). Our interpretation has demonstrated the existence of preorogenic diapirs of
932
different shapes and orientations, conditioning the final style of the FTB. Figure 21
933
schematizes the observations we made to illustrate the criteria we propose to resolve this
934
uncertainty. We compare an idealized preorogenic situation (Figure 21a) and how the salt
32
935
geometries would eventually look in the FTB (Figure 21b). The diagrams idealize a salt
936
basin sloping toward the foreland (left), in which there could be a carbonate platform as
937
represented by the Apulian Zone. In this simple configuration, we ignore the role of the
938
basement (either with normal faults of imbricated by thrusting; e.g., (Kamberis et al.,
939
2022; Kamberis et al., 1996; Kokinou et al., 2005; Kokinou et al., 2003; Kokkalas et al.,
940
2013)) and the existence of local thickness variations in synrift to postrift evaporites.
941
4. The increased thickness of the salt layer toward the foreland could be the cause for the
942
source layer to progressively develop gentle pillows (like those of Delvinë [DP] and
943
Picari–Kardhiq [PK]), punctual-source diapirs or salt plugs (like Filiates [FSP]), and
944
finally salt walls (like those of Butrinti–Xarra [BSW], Corfu [CSW], and Fyteies–Trífos
945
[FSW]). In suprasalt successions such as those represented here by the carbonate
946
sequence (Jurassic to Eocene), preorogenic structures such as those observed (Figure 20)
947
may develop with progressive onlaps over the pillows (as in DP), truncations and
948
important thickness variations around the diapirs (as in the NE edge of FSP), and
949
condensed (or absent) successions over the higher-relief salt walls (as in BSW, FP, and
950
FSW). Diapirs growth occurred during the Middle Jurassic to Lower Cretaceous (i.e.,
951
Lower Posidonia mudstones to the Vigla Formation).
952
5. As for the tectonic inversion by shortening of the salt province (in age that would vary
953
progressively toward the foreland from latest Oligocene to Pliocene), structures such as
954
those described above would develop (Figures 20 and 21): unrooted pillows displaced by
955
thrusts located at their base (as in DP and PK); tight anticlines with vertical welds that
956
may be sheared forming thrust welds (as in Kassidhiáris [KWA], Navarica [NWA], and
957
Vasiliko [VSW]); Q-tips diapirs joined by secondary welds that may become cut and
958
displaced by thrusts (as in between Butrinti and Filiates); opposite-vergence faults on
959
either side of former tight diapirs (as at Filiates [FSP]); strike-slip faults at the lateral
960
terminations of salt walls perpendicular to the shortening direction, similar to the tear
961
faults limiting indentors (as at Corfu [CSW]); and strike-slip (transpressional) faults along
962
the edges of walls oblique to shortening (such as the Aitoloakarnania fault on the eastern
963
edge of FSW; (Tranos et al., 2020; Underhill, 1989)).
964
Our study presents a novel, detailed, and accurate analysis of the shallow and deep structure of a
965
large part of the IZ in Albania and Greece and characterizes the roles of the different types of salt
33
966
diapirs in the orogen. It also provides knowledge that can be useful for the search for resources in
967
these countries as well as for the assessment of what role these structures can play in objectives
968
linked to geologic storage (like CO2 and Hydrogen) in salt diapirs (Arvanitis et al., 2020;
969
Hatziyannis et al., 2009; Stournaras, 1985).
970
9. Conclusions
971
Using field observations, reviews of existing mapping and other tectonic data (such as
972
paleomagnetic rotations), interpretation of PSDM seismic profiles (including those from a recent
973
acquisition campaign), and information from borehole data, we present a tectonic synthesis of the
974
architecture of the Ionian Zone (IZ) in Albania and Greece.
975
We characterize several bodies of salt diapirs nucleated in Upper Triassic (Keuper) evaporites,
976
whose compositions prove to be highly heterogeneous, from both a rheological point and
977
compositional point of view, as they have an upper-level rich in anhydrite, gypsum, and
978
dolomites and a lower, halite-rich sequence. During the Alpine shortening, deformation within
979
the Triassic evaporites is accommodated by simultaneous brittle failure in the more competent
980
layers (e.g., dolostone and anhydrite) and ductile flow in the less viscous lithologies (e.g., halite).
981
The salt bodies identified vary from low-relief salt pillows (e.g., Delvinë and Picari–Kardhiq
982
structures), isolated salt plugs (e.g., at Filiates), and salt walls of varying orientations to the
983
shortening, such as those perpendicular to shortening (e.g., Corfu) and others of variable
984
obliquity (e.g., Butrinti–Xarra and Fyteies–Trífos).
985
We have characterized the structural style around these salt structures, showing that their
986
presence, geometry, relief, and orientation conditioned the shape and kinematics of the thrusts
987
and associated folds and faults. Combining surface observations, borehole data, and seismic
988
interpretations, along with comparison to physical modeling results, we have reconstructed for
989
the first time in the region the deep structure of the different thrust sheets as well as the internal
990
structure and geometry of the main salt diapirs. We interpret that diapirs to have an early growth
991
stage, before the orogeny, most probably from the Middle Jurassic to the Lower Cretaceous
992
Epoch, and then to have been unevenly shortened during the Alpine shortening (from the end of
993
the Oligocene to the upper Miocene–Pliocene Epoch), according to a piggyback sequence of
994
thrusting.
34
995
This global study of the IZ can be used to better target exploration efforts in the region, but we
996
are also confident that it will open new directions of study in the search for geologic storage
997
linked to the energy transition in Albania and Greece (e.g., carbon and hydrogen storage in salt
998
diapirs).
999
1000
Acknowledgments
1001
We thank Nancy Cottington and Pablo Ruiz for initial figure drafting. Repsol and Energean Oil
1002
& Gas are specially acknowledged for their invitation and financial support to conduct the
1003
fieldwork for this study and for giving us access to the seismic data set they recently acquired in
1004
onshore northern Greece. The project was also funded by the Applied Geodynamics Laboratory
1005
(AGL) Industrial Associates program, comprising the following companies: BP, Chevron,
1006
Condor Petroleum Inc., Eni, ExxonMobil, Fairfield Geotechnologies, Hess, Murphy Oil
1007
Corporation, Oxy, Petrobras, Petronas, PGS, Repsol, China National Petroleum Company
1008
Development (RIPED), Rockfield, Shell, Talos Energy, TGS, and Woodside Energy
1009
(https://www.beg.utexas.edu/agl/sponsors). JIS also thanks Spyros Bellas (now at the Technical
1010
University of Crete) and Yannis Bassias from Hellenic Hydrocarbon Resources Management
1011
S.A. for supporting this research in Greece. Publication authorized by the Director, Bureau of
1012
Economic Geology, The University of Texas at Austin.
1013
Data Availability Statement: The original seismic data in digital format used for the study of the
1014
subsurface structure are not included in this article due to restrictions by the Government of
1015
Greece. Readers can request a copy of this data and ask for permission by sending a request to
1016
Repsol and Energean. The 2023 version of Adobe Illustrator used to draw figures was available
1017
through a license agreement between Adobe and the Bureau of Economic Geology (UT Austin).
35
1018
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1644
Appendix: Physical Model Materials, Setup, and Data Acquisition
1645
As with other physical modeling studies of salt tectonics, we simulated rock salt using ductile
1646
silicone polymer and its siliciclastic overburden using brittle, dry sands and hollow microspheres.
1647
The silicone was a near-Newtonian viscous polydimethylsiloxane (PDMS). This polymer has a
1648
density of 970 kg m-3 at room temperature and a dynamic shear viscosity of 2.5×104 Pa s at a
1649
laboratory strain rate of 3×10-1 s-1 (e.g., (Vendeville & Jackson, 1992; Weijermars et al., 1993)).
1650
The salt roof consists of differently colored mixtures of silica sand with a bulk density of ~1,700
1651
kg m-3, grain size of 300–600 µm, internal friction coefficient (µ) of 0.55–0.65, and hollow
1652
ceramic microspheres (“glass beads”) having a bulk density of 650 kg m-3, an average grain size
1653
of 90–150 µm, and a typical µ of 0.45 (e.g., (Dooley et al., 2009a; Rossi & Storti, 2003)).
1654
These mixtures moderated the density of the overburden surrounding the diapirs, and the
1655
suprasalt roof, such that the effects of density-driven loading were minimized and diapir rise,
1656
after downbuilding, was solely a function of the imposed shortening (see (Dooley et al., 2007;
1657
Dooley et al., 2009a), for further details). In all the experiments, there is a realistic density
1658
contrast of 1:1.1 between the salt and the surrounding strata, respectively.
1659
Diapirs (stocks and walls) in the experimental models illustrated in Figures 15–17 and 19 were
1660
grown by downbuilding. A layer of dense granular material was deposited uniformly above our
1661
model salt layer and, with the use of templates, this granular material was removed from
1662
predisposed locations by means of a vacuum. The differential load between covered and
1663
uncovered model salt drove our model salt into areas where the cover was removed. As the
1664
diapirs grew upwards additional layers of granular materials were deposited just cresting the tops
1665
of the growing diapirs, further driving diapir rise. After reaching a sufficient height, primarily
1666
governed by the source-layer thickness, the diapirs were covered with a uniform roof and
1667
shortening was initiated. The diapir in Figure 18 was built using the same methodology as
1668
described in (Dooley et al., 2009a), whereby polymer layers were stacked atop each other and
1669
surrounded by sediments. Again, once a certain height was achieved, the diapir was eventually
1670
covered with a uniform-thickness roof and shortening commenced.
1671
Computer-controlled cameras photographed the obliquely lit upper surface of the models at set
1672
time intervals between 3 and 10 minutes depending on the length of time of the experiment.
1673
Surface height-change maps were generated by means of a spherical laser scanner. This high48
1674
resolution laser scanning mapped topography during each experiment, allowing us to track relief
1675
changes on a millimeter scale. Each scan produces more than 8×106 points, from which CAD
1676
applications and other software to render high-resolution, interactive, 3-D surfaces. In all the
1677
experiments, regional shortening direction occurs westward (toward the left in all the
1678
illustrations). Dip sections are the sliced and photographed cross sections, whereas depth slices
1679
are virtual sections constructed from the voxel model.
49