Interactions between deep-water gravity flows and active salt tectonics

The sedimentology and stratigraphic architecture of deep-water systems deposited in unconfined basins (e.g., Johnson et al. 2001; Baas 2004; Hodgson 2009; Prélat et al. 2009; Hodgson et al. 2011; Spychala et al. 2017), or in basins with static or relatively static topography (e.g., Kneller et al. 1991; Haughton 1994; McCaffrey and Kneller 2001; Sinclair and Tomasso 2002; Amy et al. 2004; Soutter et al. 2019), are reasonably well established compared to those in basins influenced by active topography (e.g., Hodgson and Haughton 2004; Cullen et al. 2019).

Seafloor topography is generated by a variety of geological processes, including relief above mass-transport deposits (MTDs) (e.g., Ortiz-Karpf et al. 2015, 2016; Soutter et al. 2018; Cumberpatch et al. 2021), syndepositional tectonic deformation (e.g., Hodgson and Haughton 2004; Kane et al. 2010) and salt diapirism (Fig. 1; e.g., Hodgson et al. 1992; Kane et al. 2012; Prather et al. 2012; Oluboyo et al. 2014). Salt-tectonic deformation influences over 120 basins globally (Hudec and Jackson 2007), including some of the world's largest petroleum-producing provinces (e.g., Booth et al. 2003; Oluboyo et al. 2014; Charles and Ryzhikov 2015; Rodriguez et al. 2018, in press; Grant et al. 2019, 2020a, 2020b; Pichel et al. 2020).

Subsurface studies have shown that salt structures deforming the seafloor can exert substantial control on the location, pathway, and architecture of lobe, channel-fill, levee, and mass-transport deposits (Fig. 1; e.g., Mayall et al. 2006, 2010; Jones et al. 2012; Wu et al. 2020; Howlett et al., in press). Turbidity currents that were ponded, diverted, deflected, and confined by salt structures (Fig. 1) are well documented in the eastern Mediterranean (e.g., Clark and Cartwright 2009, 2011), offshore Angola (e.g., Gee and Gawthorpe 2006, 2007), the Gulf of Mexico (e.g., Booth et al. 2003) offshore Brazil (e.g., Rodriguez et al. 2018, in press), the North Sea (e.g., Mannie et al. 2014), and the Precaspian Basin (e.g., Pichel and Jackson 2020). Successions of genetically related growth strata influenced by near-surface diapiric or extrusive salt form unconformity-bounded packages of thinned and folded strata termed halokinetic sequences, which become composite when stacked (Giles and Rowan 2012; Rowan and Giles 2021). The geometry and stacking of composite sequences are dependent on the interplay between sediment accumulation rate and diapir rise rate. Giles and Rowan (2012) recognize two end-member stacking patterns; tapered (stacked wedge) or tabular (stacked hook).

Typically, salt-influenced successions are poorly imaged in seismic reflection data due to ray path distortion at the salt–sediment interface, steep stratigraphic dips, and deformation associated with salt rise (Davison et al. 2000; Jones and Davison 2014). Due to these complications, our understanding of subsurface salt-influenced systems benefits from their calibration to outcrop analogues (Lerche and Petersen 1995). Exposed examples are rare, largely due to dissolution of associated halites (Jackson and Hudec 2017). Exhumed systems typically contain shallow-marine (e.g., Laudon 1975; Giles and Lawton 2002; Giles and Rowan 2012) or nonmarine (e.g., Banham and Mountney 2013a, 2013b, 2014; Ribes et al. 2015) strata. The Bakio diapir in the Basque–Cantabrian Basin (BCB), northern Spain, provides a rare exhumed example of deep-water strata deposited in a syn-halokinetic setting (Figs. 2, 3; Lotze 1953; Robles et al. 1988; Rowan et al. 2012; Ferrer et al. 2014). The overburden displays well-exposed, unconformity-bounded sedimentary wedges that thin towards and upturn against the diapir, supporting the interpretation of syn-halokinetic growth strata (Poprawski et al. 2014, 2016).

Previous studies in the area have focused on carbonate halokinetic sequences in the middle Albian overburden (Poprawski et al. 2014, 2016), hence the salt-influenced deep-water succession remains poorly understood. This study aims to use large-scale outcrops exposed along the Bakio–Guernica coastline to study the bed-scale flow-topography interactions, deep-water facies distribution, and depositional architecture in salt-controlled minibasins. The objectives of this study are to: 1) reappraise the stratigraphy of the study area using specific deep-water sub-environments, 2) document lateral and vertical changes in deep-water facies and architecture with variable amounts of salt-induced confinement, 3) document the evolution of coeval deep-water axial and debrite-rich lateral depositional systems, and 4) distinguish criteria for the recognition of halokinetically influenced deep-water systems.

The BCB is a peri-cratonic rift basin in northern Spain, inverted during the Campanian–Eocene western Pyrenean Orogeny (Fig. 2; Gómez et al. 2002; Ferrer et al. 2008). The basin is located between the Iberian and Eurasian plates and is associated with hyper-extensive rifting and mantle exhumation during the opening of the North Atlantic and the Bay of Biscay (Van der Voo 1969; Brunet 1994; Jammes et al. 2009; DeFelipe et al. 2017; Teixell et al. 2018). The stratigraphy of the BCB is mainly of Mesozoic to Cenozoic age, sourced from a punctuated rift system that existed from Permian–Triassic to Late Cretaceous times (Cámara 2017).

The Mesozoic evolution of the BCB began with the development of a rift system in the Permian–Triassic. During the Carnian–Norian, a thick sequence of mudstones, sabkha evaporites and carbonates accumulated (Keuper Group: Geluk et al. 2018). The Jurassic to Early Cretaceous was characterized by limited subsidence and shallow-water deposition (Martín-Chivelet et al. 2002; García-Mondéjar et al. 2004). Extensional thin-skinned tectonics, controlled by basement faulting, in the Early Cretaceous initiated reactive diapirism across the basin (Bodego and Agirrezabala 2013; Agirrezabala and Dinarés-Turell 2013; Teixell et al. 2018). As rifting continued, the Lower Cretaceous succession preferentially accumulated over downthrown blocks, forming a differential load that triggered a transition into passive diapirism (Agirrezabala and García-Mondéjar 1989; Agirrezabala and López-Horgue 2017). During the Barremian–Albian the flanking minibasins were filled with c. 500 m of mixed carbonates and siliciclastics (García-Mondéjar 1990, 1996). Aptian–middle Albian shallow-water carbonate platforms of Urgonian limestone (García-Mondéjar et al. 2004) formed on the footwalls of tilted normal-fault blocks; these limestones pass abruptly into deeper-water marlstones and mudstones deposited in hanging-wall depocenters (Rosales and Pérez-García 2010). From the late Albian to the early Cenomanian, subsidence combined with early Albian global sea-level rise (Vail et al. 1977; Haq et al. 1987; Robles et al. 1988; Haq 2014) was concurrent with the development of siliciclastic turbidites and redeposited carbonates of the Black Flysch Group (BFG), which are the focus of this study.

As rifting waned, passive diapirs continued to grow at the paleo-seafloor due to minibasin subsidence (Zamora et al. 2017). During the Late Cretaceous to the early Paleogene, subsidence continued and calci-turbidites were deposited (Mathey 1987; Pujalte et al. 1994). Lower Paleocene to Eocene stratigraphy records a gradual transition from mainly calcareous to siliciclastic deposition, with an increase in deposition of siliciclastic turbidites. This change is associated with erosion of the emerging Pyrenean mountain belt (Crimes 1973; Pujalte et al. 1998). Pyrenean NE–SW-oriented compression in Eocene to Oligocene times reactivated Mesozoic–Cenozoic normal faults (Ábalos 2016) and squeezed pre-existing diapirs (Pujalte et al. 1998).

The Bakio diapir is a NE–SW-trending (c. 1 km by 4 km) salt wall of Keuper Group evaporites. Partial exposure of the salt wall occurs at Bakio beach; in other locations the evaporites are easily eroded, typically marked by topographic depressions and/or coastal embayments (e.g., Fig. 3A; the Guernica structure, located c. 9 km to the east). At Bakio beach, the Keuper Group consists of red clays, gypsum, and carbonate, with Triassic-age tholeiitic ophitic inclusions (see Robles et al. 1988; Poprawski et al. 2014). From the middle Albian, the Bakio diapir grew rapidly and reactively in response to regional hyper-extension (Teixell et al. 2018). The diapir then grew passively during the late Albian due to sediment loading, at around 500 m Myr^–1 (Poprawski et al. 2014).

The Guernica structure is poorly understood due to limited exposure, and hence is referred to as a “salt structure” rather than a salt diapir like Bakio. The Guernica structure has previously been interpreted as a salt-cored anticline (Poprawski and Basile 2018). Vintage onshore seismic reflection data suggest that the basal salt layer is present at depth connecting the Bakio and the Guernica structures (Fig. 4; Robles et al. 1988; Poprawski and Basile 2018). The structures were close to the seafloor during the middle Albian creating highs that were capped by isolated carbonate platforms and influenced the deposition of the BFG (Vicente Bravo and Robles 1991a, 1991b; Pujalte et al. 1986; Cámara 2017; Roca et al. 2020). Slope apron facies, deposited at the platform edge, and subsequent stratigraphy formed tapered halokinetic sequences against the west of the Bakio diapir (Fig. 4; García-Mondéjar and Robador 1987; Soto et al. 2017; Roca et al. 2020).

Studies of magnetic anisotropy in the Bakio–Guernica area demonstrate a minimal Pyrenean compressional overprint to the stratigraphy (Soto et al. 2017), as the tholeiitic ophitic inclusions in the diapir acted as buttresses forming shadow areas protected from the compression. Hence the area is used to study syn-halokinetic deposition without a regional tectonic-deformation overprint.

The Aptian–middle Albian Urgonian stratigraphy (middle Albian Sequence 2: H. dentatus Zone of Agirrezabala and López-Horgue 2017) comprises the Gaztelugatxe, Bakio Marls, and Bakio Breccias formations (Fig. 3B). The Gaztelugatxe Formation (GZF) is a massive-brecciated limestone, interpreted as a karstified platform carbonate (García-Mondéjar and Robador 1987; Robles et al. 1988). The Bakio Marls Formation (BMF) (minimum 60 m thick: Poprawski et al. 2016) comprises thin-bedded calci-debrites deposited in a low-energy mud-dominated environment intermittently punctuated by catastrophic debris flows sourced from local, carbonate-capped highs (García-Mondéjar and Robador 1987; Poprawski et al. 2014). The Bakio Breccias Formation (BBF) is up to 550 m thick and unconformably overlies the BMF (Figs. 3B, 4, Table 1). The BBF is primarily composed of poorly sorted, carbonate breccia beds tens of meters thick (Table 1; García-Mondéjar and Robador 1987; Poprawski et al. 2014, 2016) that are interpreted as earliest middle Albian mass failures from carbonate platforms developed on top of salt structures (Poprawski et al. 2014). The abrupt change from carbonate-dominated to siliciclastic-dominated stratigraphy is associated with a middle Albian hiatus (López-Horgue et al. 2009).

The Urgonian section is overlain by the upper Albian–early Cenomanian BFG, which has been subdivided into a lower and upper unit (Fig. 3B). The Lower Black Flysch Group (LBF) corresponds to the upper Albian Sequence 3 (D. cristatum–M. inflatum zones; Agirrezabala and López-Horgue 2017), including the Sollube, Punta de Bakio, and Jata units (Poprawski et al. 2014). This group consists of thin-bedded siliciclastic turbidites, marls, and debrites, and is interpreted to represent a submarine fan system (Robles et al. 1988; Vincente Bravo and Robles 1991, 1995; Poprawski et al. 2014; Roca et al. 2020). The Upper Black Flysch Group (UBF) corresponds to the upper Albian–Cenomanian Sequence 4 (M. fallax zone; Agirrezabala and López-Horgue 2017), and the Cabo Matxitxako unit of Poprawski et al. (2014), which consists of thick-bedded, coarse-grained, siliciclastic turbidites deposited in a submarine fan system (Robles et al. 1988, 1989). Provenance studies indicate that BFG sediment was sourced from the northerly Landes Massif, a c. 100 km × 40 km granitic basement block, presently located c. 10 km offshore in the Bay of Biscay (Fig. 2; García-Mondéjar 1996; Puelles et al. 2014).

The dataset comprises 28 sedimentary logs (totaling 821 m of stratigraphy) collected along the Bakio–Guernica coastline. The logs were collected at a 1:25 scale, with 1:10 scale used locally to capture additional detail. Halokinesis during BFG deposition (García-Mondéjar 1996; Poprawski et al. 2014, 2016; Roca et al. 2020) generated syndepositional basin-floor relief and led to the development of multiple discrete depocenters (Vicente Bravo and Robles 1991a, 1991b, 1995; Agirrezabala 1996). As such, correlating stratal surfaces in and between depocenters is difficult and un-crewed-aerial-vehicle (UAV) photography was used to aid stratigraphic correlations (Hodgetts 2013). Paleocurrent, bedding, and structural data were collected to determine the influence of syndepositional basin-floor relief and to quality-control the pre-existing geological map of Poprawski et al. (2014, 2016). Paleocurrent readings were taken where sedimentary structures were clear enough to permit unambiguous data collection. Sparse biostratigraphic data (Agirrezabala and López-Horgue 2017) hinders correlation across the structures; hence we refer to the Lower (LBF) and Upper (UBF) Black Flysch group only, to avoid further subdivisions based on geographic location (e.g., Robles et al. 1988; Vincente-Bravo and Robles 1991a, 1991b, 1995; Poprawski et al. 2014).

To aid comparison, the study area has been divided into two depocenters: the Jata and Sollube basins (Figs. 3, 4). These are analogous to subsurface minibasins, defined as relatively small (5–30 km) synkinematic depocenters subsiding into thick salt (Hudec and Jackson 2007; Jackson and Hudec 2017). The Jata basin is confined to the east by the Bakio diapir. The Sollube basin is confined on both its western and eastern sides by the Bakio and Guernica structures, respectively (Fig. 3), and hence is more confined than the Jata basin.

This study focuses primarily on the facies variability in the siliciclastic BFG. A description and discussion of the carbonate facies of the BMF and BBF is provided in Poprawski et al. (2016). Here, the carbonate facies are tabulated for reference in Table 1 (and Supplemental Fig. 1) and their depositional process interpreted. The BFG lithofacies presented in Table 2 and in Figure 5 represent “event beds” and are classified based on outcrop observations. “Mud” is used here as a general term, for mixtures of clay, silt, and organic fragments. Where individual facies are heterogeneous, multiple photographs are shown to illustrate this lithological and sedimentological variability (Fig. 5).

Facies associations (Table 3, Fig. 6) and architectures (Table 4, Fig. 7) are integrated to support interpretation of depositional environment. Facies associations are interpreted based on dominant lithofacies (Table 2, Fig. 5) and use lobe (Prélat et al. 2009; Spychala et al. 2017) and channel–levee (Kane and Hodgson 2011; Hubbard et al. 2014) nomenclature that best fit field observations. Facies associations and geometries are described separately, because architecture alone is not diagnostic of the depositional sub-environment, and multiple facies associations can form a similar architecture.

Extensive exposures permit detailed lithostratigraphic analysis (Figs. 3, 8, 9, 10), allowing investigation of the role of salt-induced relief on depositional patterns (Figs. 11, 12, 13). The following sections describe the exposures from oldest to youngest, first focusing on the flanks of the Sollube and Jata basins (Gaztelugatxe Island and Bakio West Bay, respectively) and then the axis of the Sollube basin (Cabo Matxitxako).

The cliff sections to the south of Gaztelugatxe Island (located in Fig. 3) provide a semi-continuous section through 120 meters of the BFG, 2 km northeast of the exposed Bakio diapir, and c. 9 km northwest of the Guernica structure. The stratigraphy is subdivided into five lithostratigraphic units (GX1–5).

GX1 is 8 m thick and consists of bioturbated mudstones, calci-debrites, calci-turbidites, thin-bedded turbidites, and mud-rich debrites. It shows an overall coarsening- and thickening-upwards from centimeter- to meter-scale interbeds of each facies. GX2 is 10 m thick and dominated by carbonate–clastic debrites, with angular clasts of the Gaztelugatxe Limestone, up to 1 m in diameter. GX2 pinches out downslope, forming a triangular geometry (Table 4, Fig. 7E). GX3, has a minimum thickness of 42 m, onlaps GX2 and is recognized as the first purely siliciclastic succession; comprising thin- to medium- bedded turbidites, debrites, hybrid beds, and bioturbated mudstones. GX4 has a minimum thickness of 9 m, and its base is marked by a meter-thick slump, overlain by interbeds (centimeter to decimeter scale) of turbidites, debrites, slumps, slides, hybrid beds, and mudstones.

GX5 is identified on the western side of Cabo Matxitxako (Fig. 8), having a minimum thickness of 30 m. There is approximately 400 meters of missing stratigraphy between GX4 and 5 (Robles et al. 1988), but GX5 is projected to lie stratigraphically above GX4. GX5 comprises predominantly amalgamated medium- to high-density turbidites showing evidence of soft-sediment deformation.

The presence of siliciclastic and calci-turbidite deposits and debrites in GX1 (Fig. 8) suggests a transition from the upper BBF to the LBF (Fig. 12C: Poprawski et al. 2014, 2016). The carbonate deposits could have been remobilized from previous BBF deposits or remnant carbonate highs (Poprawski et al. 2014, 2016). GX2 represents a period of increased mass failure, which is interpreted to be halokinetically driven due to the lentil-shape and diapir-centric distribution of these limestone breccias (Table 4: Fig. 7E; e.g., McBride et al. 1974; Hunnicutt 1998; Giles and Lawton 2002). The thin-bedded nature and presence of hybrid beds in GX3 suggests early BFG deposition in a proximal lobe-fringe environment (Spychala et al. 2017; Soutter et al. 2019). Thin-bedded debrites are interpreted to be delivered axially, based on their association with thin-bedded turbidites that show regional paleocurrents. Thick-bedded, chaotic, clast-rich units are interpreted to be halokinetically driven based on variable slump-axis paleocurrent readings (Poprawski et al. 2014).

At the base of GX4, a meter-scale debrite overlies 30 m of missing section (Fig. 8), which given the low-lying geomorphology is likely mud-rich. The overlying turbidites and debrites suggest deposition in a lobe off-axis setting (Prélat et al. 2009; Spychala et al. 2017) where the seafloor was, at least periodically, unstable (Fig. 12E). Meter-thick beds that stack into 30-meter-thick packages suggest that GX5 represents deposition in the axis of a lobe complex (Fig. 12F: Prélat et al. 2009; Soutter et al. 2019). The absence of debrites or slumps in GX5 (Fig. 8) suggests minimal halokinetic influence, either due to diapir inactivity or sediment accumulation, due to uplift and erosion from the Landes Massif (Agirrezabala 1996), outpacing the rate of seafloor deformation. The presence of amalgamated, laterally extensive medium- and high-density turbidites in GX5 supports deposition in a channel–lobe transition zone (Vincente Bravo and Robles 1991a, 1991b, 1995) or lobe-axis setting.

The coastal cliff section at Bakio West Bay (Fig. 9) exposes c. 150 m of the BFG above its basal contact with the BBF (Robles et al. 1988), c. 1 km west of the Bakio diapir. This section is divided lithostratigraphically into three units (BW1–3), and is further divided by halokinetically driven unconformities into sub-units (Fig. 9; Poprawski et al. 2014).

BW1 is 6-meter-thick, consists of calciturbidites and siliciclastic turbidites, debrites, and mudstones, and is overlain by BW2 across an angular unconformity (U2; Fig. 9A; Poprawski et al. 2014). BW2 is principally siliciclastic, comprising predominantly turbidites, with minor debrites and mudstones. A 10-meter-thick package of fine sand- to pebble-grade turbidites with lenticular geometries and scoured-amalgamated bases is observed to overlie a 2-meter-thick debrite (Fig. 9A). BW3 consists of interbedded meter-scale siliciclastic turbidites and debrites (Fig. 9B). Unconformities 5 and 6 are intra-BW3, and thus BW3 is subdivided into three sub-units (BW3a, b, and c).

At the bases of BW3a, BW3b, and BW3c, 1–12-meter-thick debrites with variable thickness across the exposure overlie the angular unconformity (Fig. 9). Grain size varies from medium sand to boulders and clasts vary from rounded to angular. A more diverse range of clast rock types than elsewhere in the study area are observed, including limestone, sandstone, mudstone, organics, heterolithics, siderite, mafic material, granite, and siderite (Table 3). An undulose contact exists between the debrites and the 2–4-meter-thick amalgamated turbidites which overlie them (Fig. 9). These medium sand- to pebble-grade turbidites are lenticular in geometry, can be divided into meter-scale fining-upwards successions, and contain inclined stratification (Fig. 9).

The angular unconformities are interpreted to be related to salt-diapir movements, and are interpreted as part of a tapered halokinetic sequence (Giles and Rowan 2012; Poprawski et al. 2014). Unit BW1 marks the transition from BBF to BFG, and is interpreted as representing deposition at the base of slope of the carbonate platform, which was growing on the Bakio diapir (Fig. 12D: Poprawski et al. 2014). Coarse-grained sandstones with lenticular geometries, scoured bases, and normal grading, such as those observed in BW2, indicate deposition in a channelized or scoured setting (Figs. 6F, 9, 12E; e.g., Hubbard et al. 2014; Hofstra et al. 2015). The debrites capping unconformities could be halokinetically-derived or related to channel-margin collapse induced by diapir movement (Rodriguez et al. in press). The wide range of clast rock types in these debrites suggests that they are dissimilar to other halokinetically derived debrites and could indicate a different set of mass flows sourced up-dip of the depositional system (Fig. 9C; e.g., Doughty-Jones et al. 2019; Wu et al. 2020).

The deepest point of each lenticular geometry in BW3 appears to step eastward towards the Bakio diapir (Figs. 6F, 7A); this could indicate lateral-accretion deposits from a meandering submarine channel (e.g., Peakall et al. 2007; Kane et al. 2010; Janocko et al. 2013). The concave-upward geometry of the turbidites and the undulose contact with the debrite below (Figs. 6F, 7B, 9) could represent channel fills or scour fills influenced by previous debrite topography (e.g., Cronin et al. 1998; Jackson and Johnson 2009; Kneller et al. 2016). The thick beds, concave-upward geometry, erosional bases, and coarse grain size suggests that these deposits are channel fills rather than scour fills (Hubbard et al. 2008; Romans et al. 2011; McArthur et al. 2020).

The repeated facies change between pebbly chaotic debrites and channelized turbidites is interpreted to represent periods of rapid diapir growth, evidenced by debrites overlying halokinetic unconformities (Giles and Rowan 2012). This is suggested to have been followed by periods of relative diapir quiescence, which permitted submarine channels to infill debrite topography and migrate around the diapir due to reduced seafloor topography (Kane et al. 2012).

Cabo Matxitxako provides an extensive section (c. 600 m) through the BFG. In this locality, we subdivide the group into eight lithostratigraphic units (CM1–8; Fig. 10). There is c. 500 m of missing section between Cabo Matxitxako North and South Beach (Fig. 3). Cabo Matxitxako is located in the Sollube basin, c. 4.5 km northeast and c. 5 km northwest of the Bakio and Guernica salt structures, respectively.

CM1 is a 110-meter-thick package of mudstones, with minor thin- to medium-bedded siliciclastic turbidites and debrites. CM2 is 60 m thick and is dominated by meter-scale debrites with subordinate thin- to medium-bedded turbidites, hybrid beds, and mudstones (Fig. 10). Slump axes, where present, indicate a range of paleoflow directions (forming two clusters: 80–160° and 280–320°; Fig. 3). CM3 is 50 m thick and contains meter-thick packages of stacked medium to thick bedded, dewatered turbidites and slumps, meter to tens of meters thick containing rafts of thin-bedded turbidites. Two beds of granular sandstone (27 and 19 cm thick) with lenticular geometries are observed at the top of CM3. CM4 is 32 m thick, is distinguished from CM3 as it is debrite-poor and mostly comprises thick-bedded, amalgamated high-density turbidites that stack into 3 to 6-meter packages. CM5 is 124 m thick and consists of roughly equal proportions of 1 to 3-meters-thick amalgamated turbidites, which are normally graded on a bed scale, and meter-scale slumps and debrites, which occur every 2–10 m and contain rafts of thin-bedded turbidites. CM6 has a minimum thickness of 18 m, is observed at the northern part of South Beach, and is composed of 1 to 3 m debrites and 1 to 80 cm turbidites and mudstones (Fig. 3, 10). CM7 has a minimum thickness of 38 m, similar to CM6; however, the units are separated by c. 500 m of missing stratigraphy, much of which is assumed to have been removed due to Pyrenean deformation and recent landslides (Vicente Bravo and Robles 1995), so have been separated. CM8 is 40 m thick and consists of predominantly meter-scale, normally graded thick-bedded turbidites with erosional bases, cross-stratification, amalgamation, mud-clasts, and dewatering structures common throughout (Fig. 10).

The Cabo Matxitxako succession (Fig. 10) suggests a broadly basinward-shifting (i.e., progradational) system from CM1 to CM4, followed by a slight back-step (i.e., retrogradational) or lateral shift in CM5 to CM7, and a further basinward shift in CM8 (Fig. 12).

Debrites and slumps with clasts of thin- and medium-bedded stratigraphy are present throughout CM2, 3, 5, 6, and 7 suggesting that the seafloor was periodically unstable, possibly due to relatively high rates of diapir rise and related seafloor deformation. CM1 is dominated by background suspension fallout and dilute low-density turbidites in a lobe-complex distal fringe setting (Fig. 12D). CM2 represents higher-energy, more proximal lobe conditions compared to CM1, based on facies, hybrid beds, geometry, stacking patterns, and thickness and is interpreted as proximal lobe fringe deposition (Spychala at al. 2017). The depositional sub-environment of CM3 is interpreted as an off-axis lobe complex, based on facies and bed thicknesses, with small distributive channel fills, evidenced by lenticular granular sandstones (Normark et al. 1979; Deptuck and Sylvester 2017). CM4 is dominated by stacked, amalgamated, high-density turbidites (Fig. 10) and is interpreted to represent deposition in the axis of a lobe complex (Fig. 12F; Prélat et al. 2009; Spychala et al. 2017). CM5 contains distributions of facies similar to those of CM3, so is interpreted to represent lobe-complex off-axis deposition with some distributive channel fills (Normark et al. 1979; Deptuck and Sylvester 2017). Debrite dominance in CM6 and CM7 suggests remobilization due to diapir growth throughout deposition (Fig. 12F). These deposits are interpreted to represent proximal-fringe to lobe-off-axis deposition (Spychala et al. 2017), which is highly modulated by halokinetic debrites. The coarse grain size, cross-stratification, thick beds, and lack of debrites and mudstones (Figs. 6E, 10), suggests that CM8 was deposited in either a lobe-axis or channel–lobe transition zone. This unit has previously been interpreted as a channel–lobe transition zone (Vincente Bravo and Robles 1995) and shares characteristics similar to channel–lobe transition zones reported elsewhere (e.g., Brooks et al. 2018). This unit shows little evidence for active topography, suggesting that the sedimentation rate had increased with respect to the diapir rise rate, possibly associated with uplift of the Landes Massif (Rat 1988; Martín-Chivelet et al. 2002), or welding of the salt source layer. Any remaining seafloor topography was filled by CM8 (Fig. 12G).

The BW, GX, and CM lithostratigraphic units represent different depositional systems despite their close proximity. Poor biostratigraphic calibration renders stratigraphic correlations between the areas challenging (Agirrezabala and López-Horgue 2017). Using lithostratigraphy, BW1 is correlated to GX1–2, BW2–3 are correlated to GX3–4 and CM1–7, and GX5 is correlated to CM8 (Figs. 8, 9, 10).

There is widespread sedimentological evidence for seafloor topography during deposition of the BFG, which as we discuss below reflects the interplay between active salt growth and depositional processes controlling the available accommodation.

Ripple cross-lamination, cross-stratification, and sole marks indicate a regional southwestward paleoflow direction (Fig. 11). This direction is consistent with a northward source for the BFG, supporting the Landes Massif as a potential regional source area (Rat 1988; Robles et al. 1988; Ferrer et al. 2008; Puelles et al. 2014). At Cabo Matxiatxako, a secondary westward paleoflow orientation (Fig. 11A) is comparable to findings by Robles et al. (1988), who suggest that this reflects the passage of gravity flows that spilled across the Guernica structure into the Sollube basin. Therefore, paleocurrent data (Fig. 11A) suggest modulation of a regional (primarily south-trending) paleoflow by salt-induced topography (west-trending flows off east-facing slopes) (Fig. 12). Analogously, a west–south-westward paleoflow observed at Bakio West Bay (Fig. 3) may reflect the passage of gravity flows that spilled from the Sollube basin, across the Bakio structure into the Jata basin. This west–south-westward paleoflow could alternatively represent the westward deflection of regional paleoflow around the Bakio diapir.

Ripple lamination in opposing directions is common in individual thin-bedded turbidites (Fig. 11B). Such features have been attributed to flow reflection or deflection from seafloor topography (e.g., Kneller et al. 1991; McCaffrey and Kneller 2001; Barr et al. 2004; Hodgson and Haughton 2004). Moreover, hybrid beds seen throughout the distal fringe (Figs. 5L, M, 8, 9, 10) indicate that topography had influenced a transformation of flow from turbulent to laminar (Fig. 14; e.g., Barker et al. 2008; Soutter et al. 2019).

Turbidites that pinch out up depositional slope (Fig. 7C) reflect the thinning towards topography (e.g., Ericson et al. 1952; Gorsline and Emery 1959) as the low-density part of the turbidity current ran up the topography farther than the high-density component (e.g., Al-Ja'aidi 2000; Bakke et al. 2013). Hence, thicker sandstones are more likely to be confined to localized salt-withdrawal minibasins (Figs. 12, 13, 14), whereas thinner sandstones may drape halokinetically influenced slopes (Figs. 12, 13, 14; Straub et al. 2008; Soutter et al. 2019). Based on a bed-scale thinning rate of 10 cm/m at Cabo Matxitxako (Figs. 3, 10), we calculate the slope angle to be 2–3° (Fig. 7C). Due to the distance (c. 5 km) from the present-day Bakio diapir, it is unlikely that this slope is solely related to diapir growth, but rather caused by a combination of salt withdrawal or welding from the salt source layer at depth, and salt-structure growth, as observed in similar-sized subsurface examples (e.g., Doughty-Jones et al. 2017).

Multiple paleoflow directions, hybrid beds, and abrupt pinch-out of beds can suggest the presence of (static) topography. However, the number of debrites intercalated with lobes, and the tapered composite halokinetic sequence observed at Bakio West Bay (Fig. 11D) suggest that this topography and salt growth was active at the time of deposition.

Debrites, slumps, and slides (the vast majority being debrites) account for 23% of stratigraphy across all measured sections, with an average thickness of 111 cm. Assuming that all the debrites (Table 1, Figs. 5K, 7D) are derived from diapir slopes and all turbidites are derived from far field, a 1:4 ratio of halokinetically to axially derived deposition exists. While this is clearly an oversimplification, and we provide evidence for local, diapirically derived debrites and regional, slope-derived debrites, it does suggest that locally, extra stratigraphy may be present in salt-confined basins compared to unconfined settings. Therefore interpreting stacking patterns and correlating between basins may be challenging.

Debrites on the flank of the Jata basin have an average thickness of 140 cm, compared to 119 cm and 73 cm in the axis and flank of the Sollube basin, respectively. 31% of measured stratigraphy on the flank of the Jata basin comprises debrites, compared to 22% and 18% in the flank and axis of the Sollube basin, respectively. Debrite composition shows siliciclastic dominance in the axis of the Sollube basin; debrites with carbonate clasts or matrix become more common on the flank of the Sollube basin and are dominant on the flank of the Jata basin (Figs. 8, 9, 10), in agreement with models of halokinetic sequences (Giles and Rowan 2012). Limestone clasts of similar composition in debrites on both the Jata and Sollube flanks support the presence of a carbonate platform growing on top of the Bakio diapir (García-Mondéjar and Robador 1987; Poprawski et al. 2014, 2016), indicating that these debrites are related to local diapir failures. The proportion of carbonate clasts decreases from the Sollube basin flank to axis (39% in Fig. 8 and < 1% in Fig. 10) due to distance from the carbonate platform growing on top of the Bakio diapir. Isolated limestone megaclasts (Figs. 9F, 11E, F) derived from the Gaztelugatxe Limestone could be out-runner blocks (e.g., De Blasio et al. 2006; Soutter et al. 2018) or fractured blocks of platform limestone that have toppled off during diapiric growth (e.g., Alves et al. 2002, 2003; Martín-Martín et al. 2016). Younger deposits progressively onlap these limestone clasts (Fig. 11E, F), showing that subsequent turbidity currents later interacted with this additional seafloor topography (e.g., Kilhams et al. 2012, 2015; Olafiranye et al. 2013).

Debrites can be sourced from either collapse on top of the diapir or its flanks, or from failures of the shelf-edge and/or slope (Doughty-Jones et al. 2019; Rodriguez et al. in press; Wu et al. 2020). However, the source is difficult to decipher without a dataset covering the coeval shelf and slope succession. The presence of more debrites in the basal active part of the Sollube basin fill (Fig. 8, 9, 10, 13) compared to the upper passive part of the basin fill (Fig. 10) suggests that mass failures are more common during initial development of salt-confined depocenters (Wu et al. 2020). The Sollube basin is more confined than the Jata basin, and therefore can be expected to receive a larger proportion of material derived from diapir growth. In fact, the Jata basin received more and thicker debrites. This could suggest asymmetric growth of the Bakio diapir, or the carbonate platform above it, creating a steeper slope on the boundary of the Jata basin. However, the apparent difference in the number and thickness of debrites could also be due to limitations of the outcrop, in that the Sollube basin flank location (Gaztelugatxe Island) is more axial than the Jata basin flank outcrop (Fig. 3). The absence of carbonate clasts in the axis of the Sollube basin, compared to the Sollube and Jata basin flanks, could suggest that diapirically derived mass failures did not extend into the axis of the basin. However, the exposed minibasin stratigraphy is younger than the flanking stratigraphy, and therefore carbonate clasts are expected to be rarer due to a decrease in exposure and availability to be remobilized through time.

The presence of complicated variations in thickness, clast type, and debrite style across the study area suggests that mass flows are likely to be both locally derived (from the salt structures) and regionally derived (from the shelf), and therefore debrites were likely both allogenic and halokinetic in origin (Moscardelli and Wood 2008; Doughty-Jones et al. 2019; Wu et al. 2020). The proximity to salt structures, reduction in mass- failure deposits away from salt structures, and the remobilized intrabasinal clasts within them suggests that the majority of debrites in the study area are locally derived from the Bakio diapirs. The wide variety of clasts types in Jata basin debrites (Table 3: Fig. 9) and the association of these deposits with channelized turbidites above could suggest that some of the Jata basin debrites were regionally derived, and deposited as part of channel-axis depositional elements. The absence of these possible regionally derived debrites in the Sollube basin could be due to confinement by the offshore part of the Bakio diapir, or different up-dip sediment routing. The difference in thicknesses and numbers of debrites between the Jata and Sollube basins suggests that they developed, at least partially, as separate depocenters influenced by different controls (Figs. 8, 9, 10).

The discussion initially focuses on the Sollube basin, then compares the Sollube and Jata basins, before comparing our observations to similar depocenters developed in other salt-influenced basins.

The Sollube basin is of a similar size and geometry to previously reported subsurface minibasins (Fig. 13; e.g., Pratson and Ryan 1994; Booth et al. 2003; Madof et al. 2009; Doughty-Jones et al. 2017). Therefore, this rare, exhumed example of a halokinetically influenced deep-water succession provides an excellent exposure of fine-scale minibasin depositional architecture, providing an analogue for subsurface minibasins.

The Sollube basin is 8 km wide and confined to the east and west by the Guernica and Bakio structures, respectively (Fig. 4; Robles et al. 1998; Poprawski and Basile 2018). Repeated stratigraphy and facies distribution on either side of Cabo Matxitxako, the change in bedding angle between the LBF and UBF, and sedimentological evidence for syndepositional topography support the presence of a broadly symmetrical basin confined by the Bakio and Guernica structures.

Early stratigraphy in the siliciclastic fill of the Sollube basin is dominated by thin-bedded sandstones, with localized debrites on the flanks (Figs. 8, 10, 13). As the basin developed, thicker-bedded sandstones representing channel fills and lobes were deposited in topographic lows (basin axis), consistent with subsurface analogues (e.g., Booth et al. 2003; Madof et al. 2009; Mayall et al. 2010; Doughty-Jones et al. 2017) and numerical models (e.g., Sylvester et al. 2015; Wang et al. 2017). Towards the flanks, the lower-density parts of the flows responsible for the thick-bedded sandstones may run up topography, depositing thin-bedded sandstones. Therefore, allocyclically controlled, axially derived, and often the thickest stratigraphy is observed in the axis of the minibasin. Halokinetically controlled (e.g., debrites) or -influenced (e.g., thickness variations) stratigraphy occurs towards the basin margins. These interpretations are consistent with subsurface studies (e.g., Doughty-Jones et al. 2017; Rodriguez et al. in press; Wu et al. 2020).

Oluboyo et al. (2014) suggest that a fundamental control on the type of confinement developed is the incidence angle between the strike of the salt structure and the paleoflow direction. “Fill-and-spill” architecture is observed in deep-water environments where topographic highs strike perpendicular to the gravity-flow direction (i.e., at a high incidence angle) (e.g., Piper and Normark 1983; Hay 2012; Prather et al. 2012; Soutter et al. 2019). This study documents a rare example of an exhumed halokinetically influenced deep-water succession where paleoflow is at a low incidence angle to structural strike (i.e., oblique-parallel). In such scenarios, spill between basins is rare, and sedimentary systems are deflected to run broadly parallel to salt walls in minibasins for several kilometers (Figs. 13, 14, 15; e.g., Oluboyo et al. 2014). The four-fold model of the fill of a confined basin (Sinclair and Tomasso 2002) is not appropriate where paleoflow is oblique or parallel to salt structures, and there is a down-dip exit (i.e., not confined in all directions). Our study indicates that the dominant style of interaction between gravity flows and topography is lateral confinement, with channels and lobes in the Sollube basin being thickest in the axis and elongated parallel to the margins of the salt-controlled basin. The presence of MTDs is somewhat overlooked in both the confinement model proposed by Oluboyo et al. (2014), and the earlier “fill-and-spill” model (Winker 1996; Prather et al. 1998; Sinclair and Tomasso 2002). MTDs sourced from either up-dip (i.e., extrabasinal; detached) or from local mass failures (i.e., intrabasinal; attached) related to growing salt structures, can generate additional syndepositional relief and flow confinement (Fig. 14; Moscardelli and Wood 2008; Rodriguez et al. in press).

The hierarchical scheme for classifying deep-water systems developed in the Karoo basin (Prélat et al. 2009) is widely accepted, but must be used with caution, or be adapted for confined systems (Prélat et al. 2010; Etienne et al. 2012; Marini et al. 2015). Prélat et al. (2010) recognized that width-to-thickness ratios and areal extent-to-thickness ratios are different for confined and unconfined systems, with width-to-thickness ratios of 100:1 measured in selected subsurface confined settings, compared to 1000:1 in unconfined settings, and areal extent-to-maximum-thickness ratios 30 times greater in unconfined systems compared to confined systems (Prélat et al. 2010). All examples used in Prélat et al. (2010) are from settings where paleoflow is perpendicular (high angle) to topographic strike.

In terms of areal extent, stratigraphy in the Sollube basin (c. 8 km wide) would be best classified as a lobe element (c. 5 km wide) using the Prélat et al. (2009) framework. However, in terms of thickness each lithostratigraphic unit observed at Cabo Matxitxako (18–124 m thick, Fig. 10) would be classified as a lobe complex (c. 50 m thick). The width:thickness ratio of lobes in the Sollube basin is c. 160:1 (taking a midpoint thickness of 53 m), in agreement with confined examples reported by Prélat et al. (2010). This suggests similar basic geometries for confined lobes regardless of incidence angle between paleoflow and topographic strike. The dimensions observed in the salt-influenced minibasins in the study area are comparable to those of intraslope lobes complexes documented in the Karoo (6–10 km wide, 10–15 m thick; Spychala et al. 2015), which are an order of magnitude smaller than their basin-floor counterparts (Prélat et al. 2009).

Confined-lobe complexes are predicted to have smaller areal extents because radial spreading is minimal due to topographic confinement (e.g., Marini et al. 2015; Soutter et al. 2019). The ratio of axis to fringe deposition is likely to be increased in confined settings where flows stay turbulent for longer, flow deceleration is limited, and development of a wide fringe is hindered due to presence of topography (Etienne et al. 2012; Soutter et al. 2019). The presence of thicker axial deposits due to confinement by topography, and less space for lateral lobe switching to occur, may make axis definition easier in a confined setting; however, this may change through time if topography is healed and depositional systems become less confined (Marini et al. 2015).

This study supports recent work (Oluboyo et al. 2014; Rodriguez et al. in press) which suggests that elongate systems are common adjacent to topography, on all scales. This is in contrast with the roughly equant geometries predicted in unconfined systems (Prélat et al. 2009). Multi-scale analysis suggests that all confined hierarchical elements would have greater lengths than widths, and lesser areal extents and greater thicknesses (lower aspect ratios) than unconfined settings when deposited adjacent to oblique-parallel topography (Booth et al. 2003; Oluboyo et al. 2014; Rodriguez et al. in press).

The overall upward thickening of beds and coarsening of grain size from south to north at Cabo Matxitxako is associated with a transition in depositional environment from lobe distal fringe to channel–lobe transition zone (Figs. 10, 12). Coarsening and thickening upwards elsewhere is widely interpreted to represent progradation (e.g., Mutti 1974; Macdonald et al. 2011; Kane and Pontén 2012); however, this could also represent (a component of) lateral stacking of lobes (e.g., Prélat and Hodgson 2013).

Throughout the Pyrenean, the BFG is interpreted to have been controlled by allocyclic progradation (Robles et al. 1988; Agirrezabala and Bodego 2005), driven by increases in sediment supply following the uplift of the Landes Massif (García-Mondéjar et al. 1996; Martín-Chivelet et al. 2002; Puelles et al. 2014) and/or increased flow efficiency from confinement (Hodgson et al. 2016). This regional progradation, along with our field observations, provides compelling evidence that, on a lobe to lobe-complex scale, the stratigraphic architecture of the study area is controlled primarily by system progradation. Lateral switching may be reduced due to confining topography decreasing the amount of space available for switching to take place (e.g., Mayall et al. 2010; Oluboyo et al. 2014).

By definition, only two lobe elements would be able to fit laterally within the Sollube basin during LBF deposition (Prélat et al. 2009), suggesting that due to confinement lateral stacking in our study area is feasible only at the bed scale (Marini et al. 2015). The apparent retrogradation observed between CM5–7 could be a result of bed to lobe-scale lateral shifting and compensational stacking modulating an otherwise progradational lobe complex (e.g., Gervais et al. 2006; Pickering and Bayliss 2009; Etienne et al. 2012; Morris et al. 2014).

The lack of space for lateral stacking to occur suggests that lateral topography reduces flow loss to overspill and deceleration, and therefore the system remains turbulent for longer. This causes a basinward shift in deposition effectively acting to magnify the effects of progradation (e.g., Kneller and McCaffrey 1999; Talling et al. 2012; Patacci et al. 2014). This concept accounts for numerous, thick, high-density turbidites (UBF) along the axis of the Sollube basin formed by gravity flows that were funneled between the two structures (Figs. 13, 14C, F, 15; e.g., Scott et al. 2010; Oluboyo et al. 2014; Counts and Amos 2016; Howlett et al., in press).

Using observations from Bakio, a range of stacking patterns may form during progradation of a deep-water system in an unconfined, partially confined, and dual-confined setting (Fig. 15). Unconfined fans have a higher aspect ratio, surface area, and avulsion angle than confined systems as the ability of the flows to spread radially was not restricted by topography (Prélat et al. 2009; Spychala et al. 2017). Where only one lateral confinement is present, deposits may be asymmetrical, as flows are confined by diapir topography in one direction but are able to spread radially away from it, as is seen in the deposits of the Jata basin (Fig. 9; Soutter et al. 2021).

In settings with lateral confinement, deep-water systems are elongated axially, subparallel with bounding relief (Figs. 13, 14, 15; Oluboyo et al. 2014; Soutter et al. 2021). Funneling of axial gravity flows, and therefore bed amalgamation, is interpreted to be more enhanced where two salt structures are present, resulting in thicker deposits but areally smaller depositional architectures than unconfined settings (Kneller and McCaffrey 1999; Patacci et al. 2014; Soutter et al. 2021).

Diapir growth is not continuous through time, and phases of rapid growth (e.g., Fig. 5; t2–t3, t5–t6) and quiescence (e.g., Fig. 15; t1, t4) cause destabilization and remobilization of the diapir roof, overburden or flank deposits (Figs. 8, 9, 10). This can drive rerouting of subsequent systems to avoid failure topography, potentially resulting in lateral or compensational stacking (Figs. 9, 12F, 14E, 15; Kane et al. 2012; Doughty-Jones et al. 2017, 2019; Rodriguez et al. 2018, in press). In fully confined settings, there is no space for rerouting and lateral MTDs could be amalgamated with, or eroded away by, flows depositing axial turbidity currents (Figs. 7C, 10, 12, 13, 14, 15).

The geometry and number of the debrites, and thin-bedded sandstones that pinch-out, is controlled by the presence of actively growing topography during LBF deposition. The absence of debrites in the UBF suggest that diapir growth ceased following uplift of the Landes Massif (García-Mondéjar et al. 1996; Puelles et al. 2014).

We infer that, following the cessation of diapir growth, an underfilled synclinal basin remained due to remnant topography of the buried Bakio and Guernica structures, which appears to have constrained UBF deposition until it was filled (Figs. 3, 12G, 13). The LBF represents early-stage “active” deposition, perhaps comparable to synkinematic megasequences observed in the subsurface, whereas the UBF represents late-stage “passive” deposition, infilling antecedent topography, comparable to postkinematic megasequences observed in the subsurface (e.g., Pratson and Ryan 1994; Warren 1999, 2006; Jackson and Hudec 2017). UBF deposits are less confined due to the lesser influence of salt-influenced topography during deposition, and therefore through time may evolve to represent semiconfined or unconfined deep-water systems, more capable of lateral stacking (Marini et al. 2015).

Different facies distributions on either side of the Bakio diapir varied during BFG times according to the degree of confinement and distance from diapir crest (Figs. 12, 13). In the BBF, clast- and matrix-supported breccias are common in the Sollube and Jata basins, respectively (Poprawski et al. 2016), suggesting that minibasin individualization is long-lived. The lack of confining topography to the west of the Jata basin may have caused flows to dilute, resulting in muddier, more-matrix-rich breccias (e.g., Hampton 1972; Sohn et al. 2002; Baas et al. 2009).

LBF stratigraphy in the Jata basin thins towards the Bakio diapir (Fig. 11D), showing more evidence for topography than comparable strata in the Sollube basin, supporting the idea that halokinetic deformation is greatest closest to salt structures (Giles and Lawton 2002; Giles and Rowan 2012). Richness in limestone clasts in LBF MTDs in the Jata basin (Fig. 9C, Table 3) could indicate asymmetric buildup and failure of the carbonate platform above the Bakio diapir, preferentially filling the Jata basin (Rosales and Pérez-García 2010; Li et al. 2016). Asymmetric growth and failure of either the carbonate platform or the diapir itself is further supported by thicker, more prevalent debrites observed in the Jata basin compared to the Sollube basin (discussed above: Figs. 8, 9, 10). The diverse range of clast types in the Jata basin (Table 3; Fig. 9) could suggest different depositional routing relative to the Sollube basin, possibly due to the presence of salt topography causing different source areas to be tapped (e.g., Mayall et al. 2010; Oluboyo et al. 2014).

Another key difference is the architecture of thick-bedded sandstones. In the Jata basin, individual depositional elements are often erosionally based, concave-upwards, and thinner, and show more tractional structures (e.g., ripple lamination and planar lamination) than those in the Sollube basin. Where lateral confinement occurs along one margin, sandstones could represent sinuous low-relief channel fills that ran subparallel to topography (e.g., Mayall et al. 2010; Oluboyo et al. 2014). These channels were able to spread laterally and migrate because they were only partially confined (e.g., Mayall et al. 2010; Oluboyo et al. 2014). Such systems are less modulated by halokinetic controls than those that develop under dual-lateral confinement (e.g., Oluboyo et al. 2014; Rodriguez et al., in press). Subsurface observations indicate that channels migrate away from growing structures (Mayall et al. 2010; Kane et al. 2012); however, those at Bakio West Bay appear to step towards the diapir in 2D (Figs. 6F, 7B). This could suggest a periodic reduction in diapir growth, due to the episodic nature of halokinesis (Kane et al. 2012), which may be unresolvable in subsurface data. Alternatively, the debrites underlying the thick-bedded sandstones could form pathways that controlled sandstone deposition, and therefore the apparent movement towards the diapir was in fact controlled by the deep-water systems infilling debrite-related paleotopography (Armitage et al. 2009). However, deciphering detailed interpretations of 3D sinuous channels from 2D exposure remains challenging (Li et al. 2016).

The Jata and Sollube basins had unique tectonostratigraphic histories throughout the deposition of the BBF and LBF due to the interplay of halokinetic, allocyclic, and autocyclic controls. Inaccessible UBF stratigraphy to the west of Bakio (Fig. 11D), from UAV photographs, appears to exhibit facies and geometries similar to UBF stratigraphy at northern Cabo Matxitxako (Fig. 10: Vincente Bravo and Robles 1991a, 1991b, 1995) suggesting that influence of halokinesis decreased through time. This supports the idea that sediment accumulation rate ultimately outpaced diapir growth rate, possibly due to the increase in sediment supply associated with the uplift and erosion of the Landes Massif (Martín-Chivelet et al. 2002; Puelles et al. 2014). Partial or complete welding of salt bodies could also be, at least partially, responsible for the reduction of influence of halokinesis through time (Jackson and Hudec 2017).

Here, for ease of comparison with subsurface examples, we use mass-transport deposit (MTD), instead of debrite, to describe deposits from varied subaqueous mass flows, including a mixture of slides, slumps, and debris flows in agreement with previous subsurface studies (e.g., Nardin et al. 1979; Posamentier and Kola 2003; Pickering and Hiscott 2015; Doughty-Jones et al. 2019; Wu et al. 2020).

Before this study, most understanding of halokinetically-influenced deep-water systems came from subsurface datasets (e.g., Booth et al. 2003; Madof et al. 2009; Carruthers et al. 2013; Doughty-Jones et al. 2017). Features that are common across several depositional settings where halokinetic movements are observed include multi-scalar thinning and onlap, growth faulting, pebble conglomerates, mixed siliciclastic–carbonate lithologies, MTDs, variable paleocurrents, angular unconformities, and abrupt facies variability (Dalgarno and Johnson 1968; Dyson 1999; Kernen et al. 2012, 2018; Carruthers et al. 2013; Counts and Amos 2016; Counts et al. 2019).

Deposition of thick-bedded sandstones along the axis of the Sollube basin, and thinner beds and mudstones on the flanks of the Sollube and Jata basins, is comparable to fluvial facies distribution (Banham and Mountney 2013a, 2013b, 2014; Ribes et al. 2015) where channel-fill sandstones dominate axial settings and floodplain mudstones are observed closer to the diapir.

Individual beds in the BBF are comparable in size (tens- to hundreds-of-meters packages) and composition to stacked MTDs reported overlying bounding unconformities in halokinetic sequences in the La Popa Basin (10–120 m in thickness) associated with remobilization of diapir roof or cap rock (Giles and Lawton 2002; Poprawski et al. 2014, 2016). Smaller carbonate breccias with wedge-shaped geometries (meter-scale packages; Fig. 7E) are similar in geometry and composition to “lentils” (1 meter to 100s of meters thick) described by McBride et al. (1974), but differ in thickness and areal extent. Lentils, MTDs, and breccias represent talus-like failure from diapir roof stratigraphy (Giles and Lawton 2002; Poprawski et al. 2014, 2016).

Presence of evaporite clasts in fluvial successions (Banham and Mountney 2013b; Ribes et al. 2015), suggest that the nearby diapir was exposed during deposition. Such clasts are not observed in our study area, suggesting that the Bakio and Guernica structures may have only episodically been exposed at the seabed, if at all. This fits the interpretation of carbonate-platform growth above the structures, preventing salt exposure (García-Mondéjar 1990; Rosales and Pérez-García 2010; Poprawski et al. 2014, 2016).

The consistency of our observations and previously described halokinetically influenced settings suggests that the criteria for recognizing halokinetically influenced systems is similar regardless of depositional environment, suggesting that halokinetic controls are dominant over allocyclic ones. Multiple directions of ripple lamination, presence of hybrid beds, range of MTD types, and abrupt juxtaposition of deep-water depositional facies can be used to identify halokinetically influenced deep-water systems in core and outcrop.

The gravity flows responsible for the Eocene to Oligocene Annot Sandstone, SE France, were confined during deposition by Alpine fold-and-thrust belt topography (Apps 1987; Sinclair 1994). When compared with the rate of topographic deformation associated with diapir growth, the rate of orogenic deformation is more minor.

Like the BFG, the stratigraphy of the Grès d'Annot is broadly progradational, and rapid facies changes occur over tens of meters towards pinch-outs (Soutter et al. 2019). Unlike Bakio, where paleoflow was consistently at a low angle to structural trend, sub-basins in the Annot area were eventually filled and bypassed sediment into down-dip basins (Sinclair and Tomasso 2002; Salles et al. 2014), indicating that paleoflow was perpendicular to at least one of the complex structural trends (Oluboyo et al. 2014).

Debrites in the Grès d'Annot were slope-derived and infrequent compared with our study area, which were sourced laterally from failures of stratigraphy above salt structures that are intercalated with axially derived deep-water deposits (Figs. 12, 13, 14, 15). This is a reflection of a more active slope in diapiric settings.

The stratigraphy in this study is characterized by an axial deep-water depositional system and a series of lateral systems dominated by debrites fed from the growing salt structures. This interplay of two distinct depositional systems is common in deep-water environments influenced by active rift topography, such as the Gulf of Corinth, Greece (Leeder and Gawthorpe 1987; Pechlivanidou et al. 2018; Cullen et al. 2019) and the Gulf of Suez, Egypt (Sharp et al. 2002; Jackson et al. 2002, 2005; Leppard and Gawthorpe 2006). Here the continually evolving footwall scarps feed lateral MTD-rich systems coevally with axial, allocyclically controlled depositional systems. Deposits in synrift settings are often narrow and elongated parallel to the strike of normal-fault segments (Carr et al. 2003; Jackson et al. 2005; Cullen et al. 2019), indicating the control on stratigraphic architecture by footwall physiography. Analogous variability of depositional facies occurs due to salt-structure evolution in halokinetically influenced settings.

This study documents deep-water facies distributions, with variable amounts of topographic confinement, adjacent to growing salt structures from a rare exposed example. We compare observations from two minibasins, one confined (Sollube) and one partially confined (Jata), which are comparable in size and facies heterogeneity to subsurface minibasins in salt provinces globally.

Stratigraphic variability and juxtaposition of architectural elements in the Jata and Sollube basins is high and controlled by the interplay of halokinetic, autocyclic, and allocyclic processes. The low angle between the paleoflow and the strike direction of salt structures results in the depositional system being focused between two salt structures in the Sollube basin, and against one salt structure in the Jata basin, but with no evidence of downdip flow confinement. Confinement against topography increases the effects of allocyclic progradation. Failure of carbonate platforms developed above the crests of the active Bakio diapir and Guernica structure created lateral debrites in the flanking basins, and generated local topography to further constrain axial depositional systems. Debrites can also be sourced axially from up-dip failures on the shelf, and the compositional differences of debrites suggests that the Jata and Sollube basins were subject to different influences.

Indicators of active topography include hybrid beds, remobilized strata, lateral thickness changes over short distances, reversal in ripple cross-lamination in beds and intercalation of debrites throughout the stratigraphy. These indicators individually are not diagnostic of salt-influenced topography, but collectively they provide a set of features that support interpretation of halokinetic modulation of a deep-water setting. Following the cessation of diapir growth, topography does not heal instantly, and the “passive” paleotopography continues to confine subsequent depositional systems despite diapir inactivity.

Closely related depositional systems can be highly variable depending on their complete or partial confinement. Stacked, amalgamated sandstones are observed between the confining barriers in the Sollube basin, whereas more variable architectures are observed in the Jata basin, where only partial confinement is present. These observations are due to the modulation of a broadly progradational system by halokinetically influenced lateral barriers and the coeval development of axial allocyclic and lateral debrite-rich depositional systems.

Utilizing outcrop analogues combined with a good regional understanding of source area and salt movement and extracting insights from depositional analogues are advised when exploring in the salt–sediment interface for carbon storage or geothermal or hydrocarbon reservoir targets.

Supplemental Figure 1 us available from SEPM's Data Archive: https://www.sepm.org/supplemental-materials.

This paper contains work conducted during ZCs' Ph.D. study undertaken as part of the Natural Environment Research Council (NERC) Centre for Doctoral Training (CDT) in Oil & Gas (grant number NEM00578X/1). ZC is a recipient of an American Association of Petroleum Geologists (AAPG) Foundation Grant-in-Aid “Gustavus E. Archie Memorial Grant” which supported this fieldwork. Stereonet 10 is acknowledged for data plotting. Dave Lee is acknowledged for building digital outcrop models. Ross Grant is thanked for his comments, figure beautifying, and proofreading. Gemma Doughty-Jones and Yvonne Spychala are thanked for clear and constructive reviews which greatly improved the manuscript, and for providing the foundations for which much of this work is based. Associate Editor Steve Hubbard and Editors Gary Hampson and John Southard are thanked for their handling of the manuscript.