Abstract
Sea-level fluctuations and changes in sediment grain size are widely thought to be the main factors controlling carbonate platform slope geometries. Two successive clinoform bodies from the Upper Miocene Cariatiz carbonate platform (SE Spain) were selected to analyze geometry and facies distribution in relation to sea-level oscillations. Facies occurring in these clinoform bodies are from top to bottom reef-framework, reef-framework debris, Halimeda breccia, Halimeda rudstone, and bioclastic packstone, as well as siltstone and marl. Slope geometry and facies, composition, and distribution, are significantly different in each clinoform body. These differences are the result of the interaction of several factors such as coral growth, in situ slope carbonate production, rockfalls and sediment gravity flows, hemipelagic rain, reworking of reef-slope facies and siliciclastic input. Changes in accommodation were related to sea-level fluctuations and controlled the relative impact of these factors. A sea-level fall took place in the time between deposition of the selected clinoform bodies and changed the hydrographical conditions of the basin. These changes influenced the presence of Halimeda and the grain-size distribution, and consequently the slope geometries. Reef-slope geometry is not exclusively controlled by changes in grain size. The stabilization by organic binding is proposed to be a significant factor controlling the slope deposition.
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Introduction
Sea-level changes are reported as the main factor controlling productivity, reef-slope geometry, and stacking patterns of clinoform bodies in carbonate platforms (Kendall and Schlager 1981; Bosellini 1984; Eberli and Ginsburg 1989; Pomar and Ward 1994). According to Kenter (1990), carbonate platform slope angles are also closely linked to the grain size of the sediment. This was expanded by Adams and Schlager (2000) and Schlager and Adams (2001) relating the geometry of the slope to the sediment type and consequently to the hydrodynamic energy. Schlager and Reijmer (2009) showed that the type of carbonate mud, i.e., loose needles vs. sand-sized mud clasts, also plays a role in determining the slope of clinoform bodies. In order to test the applicability of these models to Upper Miocene carbonate platforms, two successive clinoform bodies from the latest episodes of reef progradation were selected in the Cariatiz carbonate complex (SE Spain) to calibrate facies distribution and grain-size variations in relation to sea-level oscillations.
Messinian coral reefs are well exposed in the Neogene basins of the Betic Cordillera in southeastern Spain and have been the subject of extensive research (Esteban 1980; Dabrio et al. 1981, 1985; Riding et al. 1991; Martín and Braga 1994; Braga and Martín 1996; Esteban 1996; Franseen and Goldstein 1996; Cornée et al. 2004, Warrlich et al. 2005; Cuevas et al. 2007; Sánchez-Almazo et al. 2007; Rodríguez-Tovar et al. 2013). The Cariatiz carbonate platform in the Sorbas Basin (Almería) in cross section exhibits a progradational pattern with well-developed clinoform bodies. These clinoform bodies show a downslope decrease of grain size, from reef-framework blocks and breccia to fine-grained packstone, and a basinward thinning and flattening. This facies distribution was assumed to be static when performing architecture analyses of the carbonate platform showing the vertical shifts of reef-slope facies during reef progradation following sea-level oscillations (Braga and Martín 1996; Cuevas et al. 2007). Up to now, however, no attempts have been made to study variations in components and fabrics in successive reef-slope clinoform bodies affected by relative sea-level changes.
Mapping of facies distribution, with the support of terrestrial LIDAR data and microfacies analysis, shows that the two selected clinoform bodies exhibit different slope geometries and completely different facies distribution patterns. Changes in slope geometries are linked to changes in grain size and facies distribution. In the clinoform bodies, facies distribution is the result of the interaction of different factors related to carbonate production and its distribution along the reef slope. These factors seem to be linked to sea-level fluctuations. A sea-level fall appears as the main cause for facies variations in the studied clinoform bodies but it cannot completely explain reef-slope geometries. The aim of this research is to discuss the nature, importance, and extent of all the factors affecting the geometry of clinoform bodies and to contribute to the ongoing discussion on carbonate slope systems and their controls.
Geological setting
The studied outcrop is located in the Barranco de los Castaños ravine near the village of Cariatiz, at the northern margin of the Sorbas Basin (SE Spain) (Fig. 1). The Sorbas Basin is elongated in an E–W direction, and is bound by metamorphic rocks from the Internal Betic Zone cropping out in the Sierra de los Filabres to the north and in the Sierra Alhamilla and Sierra Cabrera to the south.
The basin-fill is up to 700 m thick and consists of several stratigraphic units ranging from Middle Miocene to Quaternary in age (Martín and Braga 1994). These stratigraphic units are separated by unconformities (Fig. 2a). The Upper Tortonian Unit comprises neritic to deep-sea siliciclastics and carbonates (Kleverlaan 1989; Martín and Braga 1994). The overlying Azagador Member (Völk and Rondeel 1964) consists of platform packstone and bioclastic sandstone. Basinward, the Azagador Member grades into fine-grained packstone and marl of the Lower Abad Member (Martín and Braga 1994), deposited close to the Tortonian-Messinian boundary (Sierro et al. 1993). The lowest Messinian reef deposits constitute the Bioherm Unit (Martín and Braga 1994), which contains coral and algal bioherms among packstone background deposits grading basinward into silty marl and marl with intercalated diatomite. The unconformably overlying Messinian Fringing Reef Unit is the scope of this study. It comprises carbonate platform deposits and related basinal silty marl, marl, and diatomite from the Upper Abad Member (Martín and Braga 1994). The southern end of the Barranco de los Castaños section is located at the transition from reef carbonates to basinal marl and silty marl (Fig. 2a). A basin-wide erosional surface, with signs of subaerial exposure, bounds the top of the Fringing Reef Unit. The Upper Abad marl and the distal Fringing Reef deposits are onlapped by a series of evaporite, carbonate, and siliciclastic deposits (Ruegg 1964; Riding et al. 1998, 1999).
In the carbonate platform of the Fringing Reef Unit, Riding et al. (1991) and Braga and Martín (1996) differentiated a series of facies belts. From the inner platform to the basin these are as follows (Fig. 2b):
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1.
Lagoon. Deposits from this belt are parallel beds of packstone to rudstone with coral, coralline algal, foraminifera, and mollusc remains. Siliciclastic grains also occur, usually mixed with carbonates. Small patches of the coral Porites occur near the reef crest at the outer margin of lagoon sediments. Lagoonal beds dip 3° to southwest (N216E).
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2.
Reef framework. Deposits from this belt are about 20 m thick including from bottom to top: (a) a Pinnacle Zone dominated by columnar Porites connected by bridges of laminar growths. Coral colonies are grouped in up to 15-m-high pinnacles separated by areas of reef debris. Porites skeletons are covered by thin coralline algal-foraminiferal crusts overgrown by thick stromatolitic crusts. A bioclastic matrix fills in the remaining spaces. (b) A Thicket Zone with a framework similar to the Pinnacle Zone but with more lateral continuity of the coral growths; and (c) a Reef crest made up of Porites colonies with platy to irregular shape.
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3.
Reef slope. These deposits consist of three different facies belts including from upper to lower slope: (a) the reef-talus slope, immediately in front of the Pinnacle Zone, consists of a breccia made up of framework blocks (the size of which decreases downslope) with Halimeda plates, bivalves, serpulids, and coralline algae. The proximal reef slope (b) with packstone and rudstone that are made up of coralline algae, serpulids, and molluscs (Halimeda bioclasts can be locally abundant); and the distal reef slope (c), which consists of silty marl and mudstone to packstone intercalated with basinal marl and diatomite.
Reef-framework and reef-slope facies are arranged into depositional wedges thinning downslope and basinward (Fig. 2b). These wedges, here referred as clinoform bodies, represent different phases of reef growth. In the Cariatiz carbonate platform, it is possible to identify distinct stacking patterns of the clinoform bodies starting with lowstand deposits recorded by inverted wedges. These deposits consist of onlapping rudstone with bivalves, serpulids, and red algae. Inverted wedges are overlain by an aggrading systems tract and highstand systems tract followed by a downstepping–offlapping systems tract (Pomar and Ward 1994; Braga and Martín 1996). Along with this progradation of the reef system, facies shifts occurred in response to sea-level fluctuations.
Methods
The study of the reef-slope facies and architecture relies on detailed outcrop mapping of reef clinoform bodies. This mapping was performed using panoramic photomosaics of the best-exposed parts of the succession. The study was carried out over a distance of more than 1,100 m along reef progradation, but this work focuses on the youngest part of the prograding carbonate platform, which is the most accessible. Two clinoform bodies were selected due to their good exposure. The different reef facies within the two clinoform bodies were described and sampled. A petrographic analysis of 43 thin-sections was conducted to identify microfacies and components. Polished slabs were additionally used for analyzing large bioclasts, sedimentary fabrics, and structures.
The quantification of slope dimensions and slope geometries of the selected clinoform bodies was achieved by laser scanning with an Optech Laser Imaging ILRIS 3D terrestrial LIDAR of the Institute for Geology at Hamburg University. LIDAR data were processed using 3D-Reconstructor (Gexcel). Bedding planes and facies limits were mapped in the digital model. The resulting polylines were exported into AutoCAD software for body-dimension and slope-angle measurements. AutoCAD was also used for converting the 3D model into 2D by projecting the system onto a plane positioned parallel-to-progradation.
Results
Clinoform bodies in the Barranco de los Castaños are intercalated with inverted wedges and fan-delta deposits (Braga and Martín 1996), as shown in Fig. 3. This study is focused on the last episodes of reef advance, which include two clinoform bodies, herein defined as Clinoform Body 1 (CB 1) and Clinoform Body 2 (CB 2), separated by a conglomerate body (Fig. 4a). Detailed analysis shows the differences in clinoform body geometries (Fig. 4b). Diverse facies in the clinoform bodies are documented in Table 1. Facies distribution is shown in Fig. 4c.
Clinoform Body 1
This clinoform body is 80 m high. In the direction of progradation (N160E), it extends for nearly 200 m (Fig. 4b). According to Adams and Kenter (2014), this body has a concave-upward linear profile, including three segments with different angles. The upper segment comprises the upper reef-talus slope with an approximate inclination of 60°. The middle segment includes the lower reef-talus slope and the proximal reef slope with angles between 40° and 30°. The lower segment corresponds to the distal slope with angles between 15° and 10°.
The uppermost part of the body consists of a ~10-m-thick package of reef-framework, which has a lateral extension of 35 m in the direction of progradation. The main volume of preserved reef framework corresponds to the Pinnacle Zone (Fig. 5). The Thicket Zone and the Reef Crest are only locally preserved. The reef-framework debris facies is 22 m thick. The size and the amount of the debris decrease downslope from the outermost reef framework (Fig. 4c). The reef-framework debris gradually changes into the reef-talus slope breccia (Halimeda breccia), which is approximately 20 m thick and spreads basinward 15 m from the last large blocks (Fig. 6a). Up to 1-mm-thick and 6–10-mm-long Halimeda plates usually make up more than 20 % of the rock (Fig. 6b). Plates are usually oriented subparallel to bedding but locally they accumulate in patches with a random orientation. Sediments are floatstone and rudstone with varying amounts of micritic matrix. Within the Halimeda breccia, some patches occur which are formed by serpulid-tube clusters and red algae in a micritic matrix (Fig. 6c).
The good exposure of this clinoform body allows the facies change to be traced from the reef-talus slope into the proximal reef slope, in a transition zone characterized by interdigitation of Halimeda breccia and Halimeda rudstone facies, involving a change in the degree of lithification (Fig. 6d). The change in the degree of lithification parallels the basinward decrease of patches of encrusting organisms. The Halimeda rudstone is bedded in the proximal reef slope. Beds range in thickness from 5 to 30 cm and are grouped into an up to 15-m-thick package. Patches of oysters, with some articulated individuals, occur at the top of this interval.
The transition between the Halimeda rudstone and the basinal facies is gradual. It occurs in an area with an alternation of 5–10-cm-thick Halimeda rudstone beds and 15–25-cm-thick siltstone and marl (Fig. 7). Deposits in this part of the slope are bioturbated. Low-angle tabular cross lamination pointing upslope occurs in the Halimeda rudstone beds (Fig. 7). The alternation of Halimeda rudstone and fine-grained beds in this area is a 15-m-thick fining- and thickening-upward sequence. Siltstone and marl with diatomite layers appear at the top of this alternation. The upper boundary of this sequence is an erosional surface at the base of the conglomerate body. The upper beds are deformed by the loading effect of overlying decameter-scale CB 2 reef-framework blocks (Fig. 8).
Clinoform Body 2
Clinoform Body 2 has a height of nearly 80 m. In the direction of progradation (N160E), it extends for 170 m (Fig. 4b). This body has a concave-upward exponential profile, according to the scheme of Adams and Kenter (2014). The reef-slope angles are approximately 80–60° in the reef-talus slope, 45–30° in the proximal reef slope, and 20–15° in the distal reef slope.
The uppermost part of CB 2 consists of a 10-m-high reef framework (Fig. 5) with a lateral extension of 30 m in the direction of progradation. The preserved framework facies are similar to those in CB 1. The transition from the reef framework to the reef-talus slope is gradual. In the uppermost reef-talus slope facies, there are decameter- to meter-scale reef-framework blocks. The abundance of stick-like Porites colonies indicates that most of the reef-framework blocks are derived from the Pinnacle or Thicket Zones. Locally, there are some patches with bioclastic rudstone to packstone made up of bivalves mostly preserved as molds of articulated valves, gastropods, brachiopods, and coral fragments. The reef-framework debris spreads basinward for 60 m from the lower limit of the reef framework and to the proximal to distal reef slope (Fig. 4c). The average thickness of this facies is approximately 17 m.
A bioclastic packstone (Fig. 6e) occurs at the transition from the proximal to the distal reef slope, where bedding is locally deformed by decametric reef-framework debris (Fig. 9). Between the large blocks, there are also some meter- to centimeter-scale reef-framework blocks. In the distal reef slope, 20-cm-thick siltstone and marl units are interbedded with 20–30-cm-thick bivalve packstone beds. Some layers, usually red to ochre in color, are very rich in coralline algae represented by sand-sized fragments and minor rhodoliths up to 15 cm in size. The entire package of alternating siltstone-marl and bivalve packstone is up to 5 m thick. Marl contains pebbles of quartz, schist, and serpentinite at the most distal reef slope. These deposits are in part intensely bioturbated (Fig. 6f).
Conglomerate body
CB 1 and CB 2 are separated by a 50–100-cm-thick and 110-m-wide conglomerate unit. The conglomerate comprises up to 20-cm-large clasts of quartzite, micaschist, marble, amphibolite, and serpentine, which are derived from the Betic basement in the Sierra de los Filabres to the north. Clasts are supported by a microconglomeratic to sandy matrix. This body spreads from the uppermost part of the CB 1 reef slope to the most distal (lowest) point of the studied section. The largest clasts are located in the upper part of the slope and grain size decreases downward where deposits change into sandstone, basinal siltstone, and marl. The thickness of the conglomerate changes from 50 cm in the upper slope to 100 cm downslope. In the proximal to distal reef slope, CB 1 siltstone and marl occur above and below the conglomerate body. The conglomerate base is an erosional surface over the underlying siltstone and marl (Fig. 8).
Discussion
Facies interpretation
It is proposed that the facies distribution in the clinoform bodies is controlled by the effects of the interaction of several processes. These processes are: (a) carbonate production, linked to coral-reef growth and in situ skeletal generation at the reef slope; (b) physical processes such as rock falls, downslope gravity flows and current reworking; and (c) sediment input from suspension or continental supply.
Coral reef growth
Reef growth is water-depth limited and therefore restricted to the uppermost part of the slope in the shallow part of the photic zone. Porites colonies were early encrusted by stromatolites, which are volumetrically and structurally important components of the reef framework (Riding et al. 1991). The presence of these crusts was crucial to protect and enforce the relatively delicate Porites colonies. The early lithification by stromatolitic crusts is thought to have exerted some sort of control on the way reef-framework facies broke and detached as individual blocks. The reef framework was preferentially broken along the planes of weakness provided by the vertical Porites sticks and the horizontal, laminar coral growths (Riding et al. 1991).
In-situ slope carbonate production
Halimeda plates are the main component in the reef-slope facies. Their major occurrence is in the reef-talus slope. This has also been described from the Messinian Níjar carbonate complex (Fig. 1). Mankiewicz (1988) and Martín and Braga (1989) showed that the most abundant Halimeda algal production area was in the reef-talus slope. Reef-framework blocks located in the reef-talus slope were suggested as ideal substrates for Halimeda growth (Riding et al. 1991). Halimeda plates either accumulated in situ or were exported downslope by sediment flows, forming parautochthonous to allochthonous accumulations. These accumulations were syndepositionally encrusted by microbial biofilms that precipitated micrite contributing to the early lithification of the deposits (Adams and Kenter 2014). This is similar to Halimeda mounds from the Bioherm Unit (Martín et al. 1997). The presence of isolated specimens and clusters of articulated oyster shells in life position, with encrusting serpulids and coralline red algae, indicates that the reef-talus slope was the main skeletal production area together with the reef framework.
Rockfalls and gravity flows
The Pinnacle and Thicket Zones at the base of the reef framework were areas of potential instability by slumping and sliding of the underlying unconsolidated sediment at the top of the reef slope (Riding et al. 1991). Under these conditions, the collapse of the reef framework-originating rocks and debris falls was a frequent phenomenon at the reef front (Hine et al. 1992; Martinsen 1994; Drzewiecki and Simó 2002; Berra 2007; Playton et al. 2010). This resulted in the accumulation of blocks and debris on the reef-talus slope. These accumulations occur as discrete tongues (Playton et al. 2010). These tongues reach meter thickness in CB 1 and decameter thickness in CB 2. Rockfalls and debris falls involved the sediment produced on the reef-talus slope and triggered sediment flows spreading basinward to the distal reef slope. The transport capacity of these sediment flows decayed with increasing distance from the uppermost part of the slope (Adams et al. 1998). The progressive energy decrease in these sediment gravity flows as they moved downslope is proposed to control the grain-size reduction, which occurs in the reef-slope sediments.
Hemipelagic rain
The abundance of siltstone and marl in the distal reef slope reflects the prevalence of deposition from suspension under quiet-water conditions (Drzewiecki and Simó 2002). Quiet-water conditions are also indicated by the extensive bioturbation of the distal reef slope deposits. Thin diatomite layers in the basinal sectors are interpreted as the suspension fall-out of planktic-diatom blooms (Saint Martin et al. 2001).
Reworking of reef-slope facies
The presence of climbing-slope cross lamination in the distal reef slope points toward the existence of upslope-directed northward-flowing bottom currents at the distal reef slope. These upslope currents were not acting continuously as cross-laminated coarse sediment alternates with bioturbated siltstone and marl. The change from cross lamination in CB 1 to parallel lamination in CB 2 suggests that bottom currents became less significant through time.
Siliciclastic input
The advance of the conglomerate body to the south is coeval with the continuous input of hemipelagic rain. This resulted in the mixture of terrigenous grains and basinal sediments in the distal reef slope. Braga and Martín (1996) identified this conglomerate as part of the middle-fan facies of a fan delta prograding southward from the Sierra de los Filabres and juxtaposed to the reef at some points.
Clinoform development and sea-level change
The facies distribution and depositional geometries along the 1,100-m Cariatiz carbonate platform section reveal that a long-term cycle of relative sea-level rise and fall took place throughout reef advance (Braga and Martín 1996; Cuevas et al. 2007). According to Braga and Martín (1996) and Rodríguez-Tovar et al. (2013), the relative sea-level cycles reflect glacio-eustatic sea-level changes, as tectonic oscillations of the substrate can be discarded. Obliquity and precession controlled sea-level fluctuations are superimposed onto this general long-term trend (Rodríguez-Tovar et al. 2013). Precessional cycles (C2 cyclicity of Braga and Martín 1996; and RGP in Cuevas et al. 2007) are separated by lowstand deposits represented by the inverted wedges. Clinoform bodies reflect a higher-frequency cyclicity within the precessional cycles.
CB 1 occurs at the beginning of a sea-level fall in the last precession-forced cycle of the Cariatiz carbonate platform (C2.7 in Braga and Martín 1996; and RGP 8 in Cuevas et al. 2007). Rockfalls, in situ carbonate production, gravity flows, and hemipelagic rain were the main processes controlling facies distribution (Fig. 10a). Despite the relative sea-level fall and the decreasing accommodation space, the reef slope was large enough for the development of different subenvironments and successive facies belts, as in the examples shown by Adams et al. (1998, 2004) and Playton et al. (2010). At the distal reef slope, hemipelagic rain and upslope-directed bottom currents were the factors controlling the facies distribution. The occurrence of upslope-directed bottom currents alternates with quiet periods of basinal deposition (Fig. 10b). There was a period of bottom current inactivity recorded by bioturbated siltstone and marl during the last stages of development of CB 1. The conglomerate reached the reef slope while the siltstone and marl accumulated in the basin (Fig. 8).
A significant sea-level fall marked the end of CB 1 and the beginning of CB 2 development. This sea-level fall caused a major exposure of CB 1, which resulted in increasing erosion and breakage of CB 1 reef-framework. Rockfalls dominated the sedimentation and reef-framework debris piled up on the CB 1 reef slope (Fig. 10c). The upper part of the reef-framework debris is the substrate, where CB 2 reef-framework developed. As a result of a lower sea level, this new reef framework grew downslope with respect to the position of reef growth in CB 1. The downstepping trend of the reef-framework base (Fig. 4c) indicates a continuous sea-level fall during the development of CB 2, whereas the accommodation during CB 1 formation was enough to allow for a classical reef-slope facies partitioning. This was significantly reduced in CB 2 where the facies distribution exhibits a completely different pattern. The proximity of the source area of the debris and a shorter reef slope did not allow for an adequate energy decay (Schlager and Adams 2001), and the reef-framework debris could be more easily exported, spreading down to the distal reef slope (Fig. 10d). Facies distribution at the distal reef slope therefore was controlled by sediment gravity flows and eventual rockfalls (Fig. 10e). These sediment gravity flows resulted in well-laminated bioclastic packstone in the distal reef slope. Hemipelagic rain affected the distal reef slope but was less significant than in CB 1.
Composition and sea-level change
Halimeda is a major component in CB 1 and is absent, or almost absent, in CB 2. In general, the facies with high concentrations of Halimeda (Halimeda breccia and Halimeda rudstone) are common in most of the Cariatiz reef-slope deposits including CB 1. The amount of Halimeda algae in reef-slope facies increased during reef progradation reaching its maximum value during the highstand and beginning of sea-level fall of the last precession-forced cycle (C2.7 of Braga and Martín 1996).
Facies with a high proportion of Halimeda plates also occur in other Messinian carbonate platforms (Esteban 1980; Mankiewicz 1988; Franseen and Mankiewicz 1991; Braga et al. 1996; Franseen and Goldstein 1996; Martín et al. 1997). Most of the Messinian Halimeda facies are found in the coral-bearing fringing-reef slope. Halimeda was also the main constituent in some bioherms located on non-rimmed platform slopes as in the bioherms described by Martín et al. (1997). Widespread and extensive Halimeda growth needs a relatively high nutrient environment (Drew and Abel 1983; Franseen and Mankiewicz 1991; Martín et al. 1997), which can ultimately be related to upwelling currents (Mankiewicz 1988).
Sánchez-Almazo et al. (2007) described stable oxygen and carbon isotope variations in shells of benthic and planktic foraminifera from the distal reef slope and basinal deposits adjacent to the analyzed Cariatiz carbonate platform. In deposits laterally equivalent to CB 1, planktic and benthic δ 13C values are different, which was interpreted to reflect a pronounced water-stratification. Up-section, in deposits coeval to CB 2, the carbon isotope signals converge. According to Sánchez-Almazo et al. (2007), this indicates an important nutrient-content decrease and the disappearance of water stratification as a result of the mixing of deeper and shallower water masses.
This change in water stratification can be linked to the falling sea level during the last precession-forced cycle (Sánchez-Almazo et al. 2007). Gill and Clarke (1974) related the occurrence of upwelling in modern equatorial areas to sea-level fluctuations: upwelling takes place in stratified-water conditions during sea-level rise and highstand. Therefore, it is proposed that upwelling of nutrient-rich waters during sea-level rise and highstand stages also promoted the flourishing of Halimeda in the analyzed carbonate platform. These upwelling conditions persisted at the beginning of the sea-level fall in the last precession-forced cycle, as recorded by the presence of Halimeda breccia and Halimeda rudstone facies in CB 1. This is corroborated by upslope-pointing, low-angle cross-lamination indicating the occurrence of upslope-directed bottom currents at the CB 1 distal reef slope. The decreasing water depth with continued sea-level fall finally caused water mixing and consequently the interruption of upwelling. The end of upwelling conditions probably explains the absence of Halimeda algae in CB 2 facies.
Geometry of clinoform bodies
The factors that control the geometry of carbonate platform slopes are summarized in Schlager (2005). These are the volume of sediment and platform height (Schlager 1981), the grain size (Kirkby 1987), and the erosion–deposition balance (Schlager and Camber 1986). Schlager (1981) pointed out that the volume of sediment must decrease with decreasing height of the platform to keep the same geometry of the slope. At the studied section, platform height changed as a response to falling sea level, but the volume of sediment, as deduced from clinoform body size (Fig. 4), does not varies significantly from CB 1 to CB 2. The variation in the platform height from CB 1 to CB 2 seems to be more significant for changing the erosion–deposition balance and, consequently, facies distribution. Schlager and Camber (1986) described variations in slope geometries as a result of changes in the erosion–deposition balance during slope evolution. Erosional and depositional processes, as described in the previous section, were approximately the same in both clinoform bodies but acted with different intensity. Depositional processes are dominant during CB 1 formation while erosion is more relevant in CB 2, at least during the first stages of clinoform body development. Changes in the erosion–deposition balance therefore explain the different facies distribution, but not CB 1 and CB 2 geometries. Kirkby (1987) suggested that grain size controls the angle of stability of the slope. Our study shows that facies, and subsequently grain-size patterns, are completely different in each segment of the linear slope of CB 1, explaining changes in angles of these segments. These slope-angle changes related to grain size are also recorded in the transition from reef-framework debris to bioclastic packstone and basinal deposits in CB 2.
Adams and Kenter (2014) proposed additional factors controlling the steep angles in carbonate slopes. The major factors are the response to higher shear strengths in fine-grained carbonate slope sediments (Kenter 1990; Kenter et al. 2005; Schlager 2005; Playton et al. 2010), processes of early lithification and cementation of the slope sediments, and in situ carbonate production and stabilization (Kenter 1990; Della Porta et al. 2003, 2004; Kenter et al. 2005).
Several factors contribute to the studied clinoform geometries in Barranco de los Castaños. In CB 1, with a linear profile, the different slope segments are characterized by different facies, with different grain sizes, and consequently different angles of repose (Kenter 1990; Adams and Schlager 2000). The uppermost segment consists of an accumulation of reef-framework debris. The large debris blocks were nearly deposited in situ and their imbrication allowed the high angle accumulation of 60°. The slope angles of 40–30° in the proximal and 15–10° in the distal reef slope correspond to the angles of repose of sand-gravel and mud, respectively (Kenter 1990). Although these angles of repose are theoretically possible, field and seismic examples usually show lower angles than those described for CB 1 (see Table 1 in Kenter 1990; and Adams and Schlager 2000).
Carbonate slopes with angles steeper than 30–45°, as in the studied section, were described by Kenter (1990) as the result of stabilization by organic framebuilding or by early lithification. That is the case of CB 1, where patches of serpulids and red algae as well as the abundant microbial micrite matrix and micritic envelopes in most of the bioclasts definitely contributed to the stabilization of the steep reef slope. This binding favored the sediment accumulation in such steep angles of repose (Adams and Kenter 2014). Stabilization by microbial micrite was also suggested as an important factor controlling slope geometries in Paleozoic and Triassic platforms (Keim and Schlager 2001; Della Porta et al. 2003, 2004; Kenter et al. 2005; Schlager and Reijmer 2009). In these platforms, organic binding is more significant than grain size in determining the slope geometry.
In CB 2, decametric reef-framework blocks are the main component of the reef slope. The accumulation of blocks at the base of CB 2 occurred on top of the inherited CB 1 steep reef slope. The imbrication of such large blocks and the development of reef framework on top contributed to stabilize the reef slope despite its high angle. When the steep slope collapsed, reef debris reached the proximal to distal reef slope (Adams and Kenter 2014). Inheritance of substrate topography was suggested by Franseen and Goldstein (1996) as the dominant factor controlling slope geometries in Messinian reefs in the Molata de las Negras, coeval with the Cariatiz reef.
Conclusions
Two clinoform bodies, CB 1 and CB 2, were studied in the Messinian carbonate platform of Cariatiz. CB 1 has a concave-upward linear slope with facies represented by reef framework, reef-framework debris, and Halimeda breccia in the reef-talus slope deposits. A Halimeda rudstone characterizes the proximal reef slope, and bioclastic packstone together with siltstone and marl the distal reef slope. Microbial micrite and micritic envelopes are common in this clinoform body. CB 2 has an exponential profile and its facies consist of reef framework, reef-framework debris from the reef-talus to distal reef slope, and bioclastic packstone and hemipelagic sediment in the distal reef slope.
This facies distribution is the response to the interaction of coral reef growth, in situ slope carbonate production, rockfalls, sediment gravity flows, hemipelagic rain, reworking of reef-slope facies, and siliciclastic input from the basement cropping out to the north. Changes in accommodation space, ultimately related to sea-level fluctuations, controlled the relative impact of these processes as well as their intensity, and, in this respect, the type of sediment that finally accumulated along the reef slope. The vertical shift of facies shows that a sea-level fall took place from CB 1 to CB 2. This sea-level fall also changed the hydrographical conditions of the basin eliminating water stratification and upwelling, which prevailed during formation of CB 1 and promoted the abundance of Halimeda algae that do not occur in CB 2.
Facies distribution and changes in grain size are widely thought to be the main factors controlling slope geometries. However, geometry and facies analysis of CB 1 and CB 2 suggest that additional factors are needed to explain the steep angles of these slopes. The presence of microbial micrite, micritic envelopes, and patches of encrusting organisms such as red algae and serpulids in CB 1 stabilized the steep angle of the reef slope. In CB 2, the heavy decametric reef-framework blocks deposited on top of an inherited, steep, prior topography were fixed there by the reef framework that settled and grew on top of them.
This study proposes two new considerations to the ongoing discussion on carbonate slope systems: (a) The dynamic behavior of slope-facies changes related to sea-level fluctuations, in contrast to the classic static models; and (b) the importance of organic binding in Neogene reef-slope geometries, similar to Paleozoic and Triassic examples.
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Acknowledgments
JR, CB, and SL thank the Deutsche Forschungsgemeinschaft for financial support through the grant Be 1272/21-1 (NEOCARPS). JCB and JMM were funded through the project CGL2010-20857 of Ministerio de Ciencia e Innovación of Spain. JR thanks the VU-SMG Industrial Associates Programme for additional support. All the authors want to thank editor Prof. Maurice Tucker and reviewer Dr. Erwin Adams for their very valuable suggestions and comments, which helped us to improve this paper.
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Reolid, J., Betzler, C., Braga, J.C. et al. Reef slope geometries and facies distribution: controlling factors (Messinian, SE Spain). Facies 60, 737–753 (2014). https://doi.org/10.1007/s10347-014-0406-4
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DOI: https://doi.org/10.1007/s10347-014-0406-4