The Island Arc (2004) 13, 432–451 Research Article Character of sediments entering the Costa Rica subduction zone: Implications for partitioning of water along the plate interface GLENN A. SPINELLI1,* AND MICHAEL B. UNDERWOOD2 1 Department of Earth and Environmental Science, New Mexico Tech, Socorro, New Mexico 87081, USA (email: [email protected]) and 2Department of Geological Sciences, University of Missouri, Columbia, Missouri 65211, USA Abstract Sediments deposited off the Nicoya Peninsula advect large volumes of water as they enter the Costa Rica subduction zone. Seismic reflection data, together with results from Ocean Drilling Program Leg 170, show that hemipelagic mud comprises the upper ~135 m of the sediment column (ranging from 0 to 210 m). The lower ~215 m of the sediment column (ranging from 0 to 470 m) is pelagic carbonate ooze. We analyzed samples from 60 shallow (<7 m) cores to characterize the spatial variability of sediment composition on the incoming Cocos Plate. The bulk hemipelagic sediment is 10 wt% opal and 60 wt% smectite on average, with no significant variations along strike; the pelagic chalk contains approximately 2 wt% opal and <1 wt% smectite. Initially, most of the water (96%) in the subducting sediment is stored in pore spaces, but the pore water is expelled during the early stages of subduction by compaction and tectonic consolidation. Approximately 3.6% of the sediment’s total water volume enters the subduction zone as interlayer water in smectite; only 0.4% of the water is bound in opal. Once subducting strata reach depths greater than 6 km (more than 30 km inboard of the subduction front), porosity drops to less than 15%, and temperature rises to greater than 60∞C. Under those conditions, discrete pulses of opal and smectite dehydration should create local compartments of fluid overpressure, which probably influence fluid flow patterns and reduce effective stress along the plate boundary fault. Key words: biogenic silica, Costa Rica, opal, seismogenic zone, smectite, subduction. INTRODUCTION The deposition, compaction and diagenesis of sedimentary rocks controls the distribution of fluids, fluid pressures and fluid flow patterns within subduction zones. High fluid pressures probably affect fault strength along various types of plate interface (Sibson 1981; Byerlee 1990; Unsworth et al. 1997). Cyclic dissipation of fluid pressure and commensurate increases of effective stress might control the spatial distribution and timing of seismicity (Byerlee 1993; Magee & Zoback 1993). Sediments constitute a small volumetric fraction of the oceanic lithosphere, but they host a large frac*Correspondence. Received 26 November 2003; accepted for publication 24 March 2004. © 2004 Blackwell Publishing Asia Pty Ltd tion of the total water volume that enters subduction zones. On a global average, the volume of pores and sediment grains each account for approximately 2.5% of the total slab volume, but approximately 40% and approximately 5%, respectively, of the mass of subducting water (Peacock 1990). Mechanical compaction and diagenesis control the release of fluids from sediments (e.g. Athy 1930; Trask 1931; Powers 1967; Bekins & Dreiss 1992; Moore & Vrolijk 1992). The distribution of sediment-derived fluid sources in any sedimentary system depends upon 3-D variations in sediment composition, pressure and temperature (Raymond 1983; Langseth & Moore 1990; Swarbrick et al. 2002). Sedimentary strata gain strength when porosity is lost, so the amount of consolidation decreases exponentially as effective stress Costa Rica sediment: Fluid partitioning 433 increases (Moore & Vrolijk 1992; Bahr et al. 2001; Holbrook 2002). Therefore, the volume of fluid expelled from sediment during compaction decreases with depth in a sedimentary basin (or distance into a subduction zone). In deep levels of a basin, water stored within minerals (e.g. opal and smectite) comprises a greater proportion of the total fluid budget. Transformations of opal to quartz and smectite to illite are controlled by reaction kinetics (Ernst & Calvert 1969; Pytte & Reynolds 1988; Huang et al. 1993). The activation energies are low for both opal to quartz and smectite to illite (Ernst & Calvert 1969; Pytte & Reynolds 1988), so the reactions usually progress quickly from initiation to completion. However, the smectite-to-illite reaction can be slowed or halted if the supply of K+ is limited (Hower et al. 1976; Boles & Franks 1979). Opal-toquartz diagenesis goes to completion at temperatures of 50–100∞C (Murata et al. 1977; Behl & Garrison 1994). Smectite dehydration involves three discrete stages at temperatures less than approximately 140∞C (Perry & Hower 1972; Bird 1984; Bruce 1984; Colten-Bradley 1987). Consequently, one might expect opal and smectite dehydration to trigger two or three discrete pulses of fluid release within narrow windows of temperature and depth. When unconsolidated sediment first enters a subduction zone, most of the water is stored in pore spaces, but the pores collapse rapidly near the deformation front due to vertical compaction and tectonic consolidation (e.g. Moore & Vrolijk 1992; Kimura et al. 1997; Screaton et al. 2002). Therefore, hydrous mineral can convey a relatively large volume of water deep into subduction zones. The loci of diagenetic dewatering reactions within a subduction zone depend upon a margin’s thermal structure and its subduction–accretion geometry (i.e. stratigraphic position and dip of decollement, offset along out-of-sequence faults, underplating via duplex structures). Smectite and opal dewatering are merely two of several low-grade reactions that influence pore pressure, effective stress and frictional properties within subduction zones (Moore & Saffer 2001). Geochemical evidence of diagenetic dewatering is substantial within many active margins (e.g. Kastner et al. 1991). The starting composition and temperature history of the subducting sediments, however, vary dramatically both within and among individual systems (e.g. Tribble 1990; Underwood & Pickering 1996; Deng & Underwood 2001; Underwood 2002; Steurer & Underwood 2003a). Because of that heterogeneity, linkages between diagenetic reactions and their chemical or physical effects must be established independently, and in 3-D, within each study area. The need for sitespecific assessment applies to compositional factors that might, in theory, control the up-dip limit of seismicity on subduction megathrusts (Vrolijk 1990; Hyndman et al. 1997). Substantial volumes of sediment-hosted water enter the Costa Rica subduction zone off the coast of the Nicoya Peninsula (Fig. 1). Leg 170 of the Ocean Drilling Program (ODP) demonstrated that the entire package of incoming sediment is subducted beneath the frontal toe of the margin (Kimura et al. 1997), but deeper-seated subduction processes remain poorly documented. In addition, various interpretations have been offered to explain profiles in pore water chemistry near the margin toe (Chan & Kastner 2000; Silver et al. 2000; Saffer & Screaton 2003), but those efforts have been hampered by a lack of detail regarding the actual composition of sediment inputs. To help fill this void in our knowledge of the Costa Rica subduction system, we completed compositional analyses of near-surface sediments on the incoming Cocos Plate, with the goal of gaining insight into how water is partitioned among pore space, opal and smectite. The nature of fluid partitioning at the subduction front, and the down-dip evolution of fluid sources, are also important geotechnical considerations, because of their potential control over fluid pressure and shear strength along the plate interface. COSTA RICA MARGIN Our study focused on the sediment on the incoming Cocos Plate off the Nicoya Peninsula, Costa Rica (Fig. 1). Along the Pacific margin of Costa Rica, the Cocos Plate subducts beneath the Caribbean Plate at the Middle America Trench at approximately 85 mm/year (DeMets 2001). Offshore of the Nicoya Peninsula, a triple junction trace divides the subducting Cocos Plate into crust formed at the East Pacific Rise (EPR) to the north, and crust formed at the Cocos–Nazca Spreading Center (CNS) to the south (Barckhausen et al. 2001). Seaward of the Middle America Trench, seafloor heat flow on the CNS crust is 105–115 mW/ m2 (Fisher et al. 2003), consistent with conductive lithospheric cooling models (e.g. Parsons & Sclater 1977; Stein & Stein 1994). Heat flow on the EPR crust is 20–40 mW/m2. The lateral transition between the warm and cool crust is abrupt, occurring over a lateral distance £5 km (Fisher et al. 434 G. A. Spinelli and M. B. Underwood -40 00 10 o Costa Rica m Nicoya Peninsula study area -1 00 0 9.5 -2 o m 00 0 -3 00 0 m m o ar /ye o mm 8.5 EPR CNS crust crus t 9 o -87.5 85 50 km -87 o o -86.5 -86 2003). The low heat flow on the EPR crust likely results from hydrothermal circulation, facilitated by numerous basaltic outcrops that allow rapid transfer of water between the ocean and the crust (Fisher et al. 2003). The location of shallow earthquakes along the plate interface also changes along-strike, coinciding with the transition from CNS to EPR crust. Earthquakes occur shallower (~10 km) and closer to the trench (~60 km from the trench) on the warm CNS crust than on the cool EPR crust (~20 km depth and ~75 km from the trench) (Newman et al. 2002). Ocean Drilling Program Leg 170 included a reference site on the floor of the Middle America Trench (Site 1039) and at two sites at the toe of the margin wedge (Sites 1043 and 1040, ~0.5 and 1.6 km landward of the trench, respectively). The stratigraphic section at Site 1039 consists of approximately 225 m of pelagic sediment, primarily composed of siliceous and calcareous nannofossils, overlain by approximately 150 m of hemipelagic mud containing abundant clays and diatoms (Kimura et al. 1997). Reflection seismic profiles, litho-stratigraphy, core-scale geological structures and borehole logs (gamma-ray, resistivity and density) collectively indicate that very little sediment (~1%) is scraped off into the wedge (Kimura et al. 1997; Saito & Goldberg 2001). o -85.5 o Fig. 1 Map showing the location of the 60 gravity and piston cores used in this study from sediments on the incoming Cocos Plate, offshore northwestern Costa Rica (). Ocean Drilling Program (ODP) Sites 1039 and 1040 (✩) are approximately 1.5 km seaward and 0.5 km landward of the Middle America Trench, respectively. Site 1039 spans the entire incoming sediment section (~350 m thick); Site 1040 penetrates the margin wedge and the entire underthrust sediment section. Tracklines of reflection seismic data are shown with the solid gray lines. A triple junction trace (bold dashed line) separates crust formed at the Cocos–Nazca Spreading Center (CNS) in the southeastern portion of the study area from crust formed at the East Pacific Rise (EPR; northwestern portion of the study area). During the TicoFlux program (Fisher et al. 2003), gravity and piston cores, reflection seismic data and heat-flow data were collected in an area approximately 120 ¥ 120 nmi offshore of the Nicoya Peninsula (Fig. 1). The coring program was designed to capture geochemical evidence of basement-related fluid flow (e.g. Friedmann et al. 2001), so there is a bias in sample distribution toward locations where total sediment thickness is at a minimum. METHODS Sediment samples were taken from 60 nearsurface piston and gravity cores distributed throughout the TicoFlux study area, plus five intervals at ODP Site 1040 (Fig. 1). Sediment composition was quantified by a combination of chemical and X-ray diffraction (XRD) analyses of bulk samples and the <2 mm fraction. OPAL ANALYSIS We used an alkaline leaching method to determine opal content, as outlined by DeMaster (1981). When sediment is placed in an alkaline solution, siliceous material is dissolved, and amorphous sil- Costa Rica sediment: Fluid partitioning 435 at a rate of 1∞ 2q/min, and MacDiff software was used to determine the areas and intensities of a composite clay mineral peak (smectite + illite + kaolinite), quartz, plagioclase and calcite (Fig. 3). Relative percentages of each were calculated using a set of normalization factors specific to the Costa Rica mineral assemblage (Table 1), following the singular value decomposition (SVD) method of Fisher and Underwood (1995). Preparation of the clay-sized fraction (<2 mm) for clay mineral identification started with 3% H2O2 digestion of organic matter, addition of Nacarbonate and Na-hexametaphosphate dispersant, and washing by centrifugation at ~6000 g for 20 min. Suspensions were dispersed in de-ionized water using an ultrasonic cell disruptor, and split into size fractions by centrifuging at ~320 g for 2.4 min. Preparation of oriented clay slides followed the filter-peel transfer method (Drever 1973), and the clays were saturated with ethylene glycol vapor before analysis. The clay slides were scanned at 40 kv and 30 mA over 2q angles ranging from 3 to 23∞, at a rate of 1∞ 2q/min. We calculated relative abundances of smectite, illite and kaolinite (area%) using basal reflections (Fig. 3) and Biscaye (1965) peak-area weighting factors (1¥ smectite; 4¥ illite; 2¥ kaolinite). The percent expandability of smectite was determined using the saddle-peak method and the empiric curve for ‘pure’ smectite (Rettke 1981). ica (opal) is digested more rapidly than clay minerals. Therefore, the concentration of silica in the alkaline solution increases over time, with a rapid initial increase overprinted by gradual dissolution of clay minerals. For each sample analyzed, we digested approximately 30 mg of freeze-dried sediment in 40 mL of 0.0316 M NaOH (pH 12.5) at 85∞C. A 12.5 pH solution was used to minimize digestion of clay minerals (Schlüter & Rickert 1998). Aliquots (0.200 mL) of the leachate were collected 5, 15, 30, 60, 90, 120, 200 and 300 min after digestion began. The concentration of silica in the leachate was determined by spectrophotometry (e.g. Grasshoff et al. 1983). The contribution of opal to the leachate was determined by projecting the flattened tail of the concentration curve back to time = 0 (Fig. 2). In determining the weight percent of opal in the bulk samples, we assumed the water content of opal to be 11% by weight (Kastner 1981). X-RAY DIFFRACTION Bulk sediment samples were analyzed by XRD to determine relative abundances (wt%) of total clay minerals, quartz, plagioclase and calcite. Freezedried specimens were powdered for 5 min with a ball mill and analyzed with a Scintag PAD V diffractometer. Bulk powders were scanned at 40 kv and 35 mA over 2q angles ranging from 3 to 35∞, Contribution from opal to Si concentration of leachate Fig. 2 Examples of data from the sediment leaching procedure used to determine the opal content of sediment samples. After all the opal has been extracted from the sediment in a hot alkaline solution, silica continues to be extracted from clays at a slow, constant rate. This rate is extrapolated back to time = 0 to determine the amount of silica extracted from the opal alone. The dark olive gray hemipelagic muds have the highest opal content of the sediments encountered in the study area; the brown clays have intermediate opal content; the pelagic sediments have the lowest opal content. Leachate Si concentration (mM) Mass sediment sample (g) 0.8 (h M05gc 88–90 cm emipelagic; 8.1% opal) Si extracted only from clays (at constant rate) 0.6 All Si from opal has been extracted Si extracted from both opal and clays 0.4 M18gc 0.2 8–10 c m clay (brown M24gc 68–70 cm (calca ; 2.8% opal) reous ooze; 0.6% opal) 0.0 0 60 120 180 Time (min) 240 300 436 G. A. Spinelli and M. B. Underwood (a) 500 Counts 400 plagioclase calcite 300 quartz 200 halite clay 100 0 5 10 15 20 o (b) 600 30 35 2q smectite (001) 400 300 illite (001) 200 kaolinite (001) saddle 100 zeolite 0 4 6 8 10 12 14 o 16 18 20 22 2q (c) 2000 GRAIN SIZE Counts 1500 calcite 1000 500 0 TOTAL INORGANIC CARBON Error analysis of the SVD method shows that calculated abundances of minerals within standard mixtures are usually within 5% of their true percentages by weight (Fisher & Underwood 1995; Underwood et al. 2003). To verify the accuracy of XRD data in an absolute sense, we analyzed for calcium-carbonate content by acid digestion and a coulometer using a diverse subset of 18 hemipelagic samples. The absolute wt% of calcite for each was determined from the total inorganic carbon content. peak 500 Counts 25 To discriminate between dioctahedral and trioctahedral varieties of expandable clay, we identified the d(060) value using randomly oriented powders of the <2 mm size fraction (Brown & Brindley 1980). Those clay powders were scanned from 48 to 64∞ 2q at 1∞ 2q/min after adding a spike of quartz powder to correct for drifts in peak position caused by misalignments of the goniometer and/or sample holder. halite 5 10 15 o 20 25 30 35 2q Fig. 3 Example of X-ray diffraction (XRD) analysis of sediment samples off Costa Rica. Analysis of the bulk sediment powder for a hemipelagic sample indicates that the relative percentage of clay (77%) is much greater than quartz (4%), plagioclase (16%) or calcite (3%) (a; M17gc 43–45 cm (hemipelagic mud)). Results from an ethylene-glycol solivated, oriented slide for the same sample indicate that the <2 mm grain size fraction of the sample is dominated by smectite (b; 84% smectite, 1% illite, 15% kaolinite). The ratio of the number of counts at the ‘saddle’ and ‘peak’ is used to estimate the proportion of expandable layers in the smectite. Pelagic samples are dominated by calcite (92%), with very little clay (<1%), quartz (4%) or plagioclase (4%) (c; M22gc 50–52 cm (calcareous ooze)). The percentages of sand (>63 mm), silt (4–63 mm) and clay (<4 mm) were determined by wet sieving and a Spectrex laser particle counter (LPC). Before wet sieving, the bulk samples were freezedried, digested with 3% H2O2, and dispersed in 0.01 M Na2CO3. Because of the typical abundance of biogenic silica, Na-hexametaphosphate (Calgon) was ineffective as a dispersant. Output from the LPC (counts/cm3) needs to be converted to equivalent spherical settling diameter (wt%) using a calibration curve established by pipette analysis (Steurer & Underwood 2003b). We report here the average values of percentage silt and percentage clay (as spherical equivalents) derived from three replicate LPC analyses. SEDIMENT THICKNESS Approximately 1800 km of reflection seismic lines were collected during 2001 (TicoFlux I expedi- Table 1 Normalization factors for bulk powder X-ray diffraction (XRD) analysis Indicator mineral Target mineral Total clay Total clay Quartz Plagioclase Calcite Quartz -2 1.3267 ¥ 10 3.8598 ¥ 10-5 2.1620 ¥ 10-4 -5.4600 ¥ 10-5 Plagioclase -4 -2.3590 ¥ 10 7.9700 ¥ 10-4 -9.6200 ¥ 10-5 6.9900 ¥ 10-5 -4 -4.3760 ¥ 10 5.2500 ¥ 10-5 3.3377 ¥ 10-3 8.5107 ¥ 10-5 Calcite -1.4851 ¥ 10-3 -2.9600 ¥ 10-6 -5.4700 ¥ 10-5 1.7801 ¥ 10-3 Costa Rica sediment: Fluid partitioning 437 3100 3200 Fig. 4 On reflection seismic lines, the hemipelagic sediment is acoustically more transparent than the underlying pelagic sediment. Reflection seismic data is used to map the thickness of both the hemipelagic sediment and the pelagic sediment. TWT, two way travel time. TWT (s) hemipelagic sediment 4.5 pelagic sediment 3300 3400 3500 3600 5.0 tion). The source was a 10-gun array with a frequency bandwidth of approximately 20–120 Hz. The receiver was a 6 km long hydrophone streamer array with 480 channels. An additional 1200 km of reflection seismic data were acquired during 2002 (TicoFlux II expedition) using a pair of GI guns with a frequency bandwidth of approximately 20–200 kHz and a four-channel, 200 hydrophone streamer. The pelagic and hemipelagic sections of the sediment column on Cocos Plate were differentiated by differences in their acoustic signatures. As noted during previous geophysical surveys of this margin (e.g. Shipley et al. 1990), the pelagic section is characterized by numerous internal reflections with high degrees of lateral continuity, whereas the hemipelagic section is relatively transparent acoustically (Fig. 4). We measured the two way travel times at the boundaries between hemipelagic and pelagic intervals and acoustic basement. We converted to sediment thickness using average velocities of 1541 m/s for the hemipelagic section and 1581 m/s for the pelagic section (Kimura et al. 1997). Sediment thickness was determined along the reflection seismic tracklines, then gridded and contoured over the entire study area. RESULTS SEDIMENT THICKNESS Reflection seismic data and high-resolution swath mapping indicate that seamounts are more common on crust formed at the EPR than on crust formed at the CNS to the southeast (e.g. Fisher et al. 2003). Sediment is thin or absent on the seamounts (Fig. 5). As a result, there is greater spatial variability in total sediment thickness in the northwestern part of the study area than in the southeastern part. Aside from the basement highs, the hemipelagic interval is similar over the EPR crust and the CNS crust, reaching up to 213 m, with a median thickness (for the gridded data) of basaltic basement 3700 Approximate depth (m) seafloor 135 m. Pelagic sediment is consistently thicker on the EPR crust than on the CNS crust. The pelagic interval is 0–472 m thick on the EPR crust (median = 233 m) and 0–372 m thick on the CNS crust (median = 193 m). SEDIMENT COMPOSITION Shipboard descriptions of split cores and smear slides led to a classification system with four basic lithologies: dark olive gray hemipelagic mud (with abundant biogenic silica); variegated clay (with low biogenic silica); mixed sediment (with variable carbonate content); and light gray nannofossil chalk. Many of the cores also contain thin layers of volcanic ash, fragments of Mn-oxide and pieces of basalt. Apart from five deeper intervals at ODP Site 1040, our specimens come from within 7 m of the seafloor. Hemipelagic mud is, by far, the most common lithology throughout the study area. Exposures of variegated clay and chalk are restricted to basement highs (e.g. seamounts and smaller basalt outcrops) where total sediment thickness is at a minimum and the overlying hemipelagic sediment section is thin or absent (Fig. 5). Cores with pelagic chalk are clustered in the southwestern portion of the study area and around outcrops, primarily on the crust northwest of the triple junction trace indicated on Figures 1 and 6 (Fisher et al. 2003). Winnowing by bottom currents may have hampered deposition of hemipelagic mud in those localities. In some cores, the basal chalk interval grades upward through mixed sediment into hemipelagic mud. One piston core was collected from the floor of the Middle America Trench, and it contains turbidites and debris-flow deposits with remobilized fragments of mudstone. Grain size analyses show that the hemipelagic sediment consists primarily of clay-sized particles (~67% by weight as equivalent spherical diameters). Smaller components are silt-sized (~30% by weight) and sand-sized (~3% by weight, largely composed of foraminifers) particles. The pelagic 438 G. A. Spinelli and M. B. Underwood -87.5o -87o -86.5o -86o -85.5o 50 km -87.5o -87o -86.5o -86o -85.5o o 10 9.5 9 o 8.5 Total sediment thickness (m) 0 200 400 600 o o Hemipelagic sediment thickness (m) 0 50 100 150 200 Fig. 5 Gridded and contoured total sediment thickness and thickness of the hemipelagic sediment section. Sediment thickness (both total and hemipelagic) is more variable overlying the East Pacific Rise crust in the northwest (where there are more seamounts and rougher basement topography) than over the Cocos–Nazca Spreading Center crust in the southeast. E09gc M38gc E27gc Opal = 7% 1m 2m E21gc E34gc Clay = 70% Qtz = 4% Plag = 13% Calc = 13% SMEC = 75% ILLITE = 4% KAOL = 21% Opal = 2% Clay = 81% Qtz = 2% Plag = 17% Calc = trace SMEC = 90% ILLITE = 0% KAOL = 10% Opal = 8% Clay = 77% Qtz = 3% Plag = 20% Calc = trace SMEC = 97% 2m ILLITE = 0% KAOL = 3% Clay = 79% Qtz = 5% Plag = 16% Calc = trace Clay = 79% Qtz = 3% Plag = 11% Calc = 7% SMEC = 81% ILLITE = 2% KAOL = 17% Clay = 55% Qtz = 4% Plag = 14% Calc = 27% Clay = 55% Qtz = trace Plag = 45% Calc = trace 3m SMEC = 100% ILLITE = 0% KAOL = 0% Clay = 35% Qtz = 3% Plag = 16% Calc = 46% M02gc Dark olive gray hemipelagic mud Brown clay M38gc M02gc Clay = 85% Qtz = 2% Plag = 13% Calc = trace SMEC = 90% ILLITE = 0% KAOL = 10% 1m Opal = 7% E34gc E09gc Mixed sediment Carbonate ooze E21gc E27gc Ash Mn nodule Fig. 6 Representative core logs and results from opal and X-ray diffraction (XRD) analyses. Clay, quartz, plagioclase and calcite percentages are relative percentages determined by XRD of bulk powder samples. Smectite, Illite and kaolinite percentages are relative percentages of the <2 mm fraction. Opal percentages are weight percentages determined by sediment leaching. Hemipelagic sediments (which contain most of the opal and smectite within the sediment column) are thin in the southwest and around local basement highs. Costa Rica sediment: Fluid partitioning 439 plagioclase (a) total clay opal calcite (b) total clay smectite chalk appears to be coarser than the hemipelagic mud, but our LPC results may have been affected by interference among nannofossils. The average size distribution for the pelagic sediment is 30% clay, 47% silt and 23% sand (mostly foraminifers). Within each sediment type, there is very little spatial variation in mineralogy (Fig. 6). Of the samples analyzed by XRD (Table 2; Fig. 7), hemipelagic mud has the highest opal content (mean (m) = 10% by weight; standard deviation (s) = 3%; number of samples (n) = 23). Variegated clay (olive brown) is intermediate in opal content (m = 5%; s= 2%; n = 11), and the opal content of pelagic chalk is lowest (m = 2%; s= 1%; n = 4). The hemipelagic mud and variegated clay have similar relative abundances of total clay minerals, quartz, plagioclase and calcite. The mean values for hemipelagic mud (n = 39) are 77% total clay minerals, 3% quartz, 19% plagioclase and <1% calcite. The nannofossil chalk contains mostly calcite (n = 6; 1% total clay minerals, 4% quartz, 5% plagioclase, 90% calcite), whereas the mixed sediment ranges from <1 to 46% calcite. Most of the clay-sized fraction is smectite (Fig. 7). Relative percentages of smectite average 87% and range from 75 to 100% (Table 2). The average content of kaolinite is 13%, with a trace contribution of illite (~1%). The clay mineral content of pelagic chalk is too small to analyze accurately by XRD. calcite ABUNDANCE OF HYDROUS PHASES (c) illite Dark olive gray hemipelagic mud Olive brown mud Calcareous ooze Mixed sediment Altered ash kaolinite Hemipelagic mud has relatively high total clay and opal contents, so a considerable volume of fluid must be contained within the hydrous phases. We quantified the opal content as an absolute wt%, but the clay mineral content is relative only to three other constituents (quartz, plagioclase and calcite). To determine how closely such relative abundances match absolute weight percentages, we compared the contents of calcite (from Coulometric analysis) to equivalent XRD values after correcting for the wt% opal. Linear regression shows that the two sets of values match to within approximately 10 wt% (Fig. 8). The fit would improve if Fig. 7 Summary of bulk sediment compositional data (a and b) and <2 mm fraction clay mineralogy (c). The hemipelagic sediment is dominated by clay minerals. The pelagic sediment is mostly calcite. The mixed sediment samples are mixtures of hemipelagic and pelagic sediment. The clay minerals in the <2 mm size fraction are mostly smectite. Number of samples: (a) 39 hemipelagic, 16 olive brown, 6 calcareous, 6 mixed; 1 altered ash; (b) 23 hemipelagic, 11 olive brown, 2 calcareous, 3 mixed; and (c) 29 hemipelagic, 15 olive brown, 3 mixed, 1 altered ash. 02GC 05GC 05GC 07GC 11GC 12GC 14GC 16GC 17GC 18GC 20GC 21GC 22GC 24GC 25GC 26GC 28GC 33GC 38GC 38GC 40GC 42GC 44PC 45PC 45PC 45PC 48PC 54GC 48–50 45–47 88–90 38–40 42–44 208–210 238–240 35–37 43–45 8–10 40–42 20–22 50–52 68–70 62–64 170–172 198–200 78–80 28–30 112–114 60–62 90–92 520–522 370–372 536–538 686–688 657–659 100–102 Sample ID Core Interval (cm) 9.6855 9.3109 9.3109 9.3408 9.6795 9.6799 9.6066 8.4973 8.5369 8.5303 8.4959 8.7367 8.7391 8.6209 8.7425 8.7420 8.7405 9.0876 9.0828 9.0828 9.0841 9.0809 9.6800 9.8657 9.8657 9.8657 8.4967 8.8191 -86.3937 -86.1877 -86.1877 -86.1740 -86.5711 -86.5718 -86.6524 -85.9677 -85.9042 -85.9149 -85.9675 -87.2125 -87.2107 -87.2845 -87.2150 -87.2137 -87.2146 -87.0963 -87.0999 -87.0999 -87.0989 -87.0965 -86.5718 -86.3547 -86.3547 -86.3547 -85.9668 -87.1688 7 5 8 8 7 14 17 8 7 3 4 5 3 1 7 2 2 10 7 8 6 7 12 8 14 14 10 8 85 80 – – 84 84 84 – 77 82 79 – Tr – 82 – – 82 – 81 83 – 83 78 79 77 – 83 2 2 – – 2 3 3 – 4 3 4 – 4 – 2 – – 2 – 2 2 – 3 3 3 2 – 3 13 18 – – 14 13 13 – 16 15 17 – 4 – 16 – – 16 – 17 15 – 14 19 18 21 – 14 Tr Tr – – Tr Tr Tr – 3 Tr Tr – 92 – Tr – – Tr – Tr Tr – Tr Tr Tr Tr – Tr – – – – 3.0 – – – 8.8 – 9.1 – – – – – – – – – – – – – – – – – † 90 91 88 87 – 90 87 88 84 – 87 91 – – 88 93 – 91 91 90 90 90 89 81 82 86 88 88 0 0 1 1 – 0 0 1 1 – 0 1 – – 1 0 – 0 0 0 1 1 0 0 1 1 1 0 10 9 11 12 – 10 13 11 15 – 13 8 – – 11 7 – 9 9 10 9 9 11 19 17 13 11 12 62 60 68 61 – 67 59 70 59 – 59 64 – – 68 51 – 58 63 57 59 61 60 54 51 53 64 59 Y Y Y Y – N Y Y Y – Y Y – – Y N – Y Y N Y Y Y Y Y Y Y Y – 1.503 – – – 1.502 1.506 – 1.509 – – – – – – – – 1.506 – – – – – – – 1.505 – 1.507 3 – – 1 – 2 3 2 1 4 2 18 15 36 14 – 17 12 3 8 3 – 2 – 3 4 3 – 25 – – 22 – 16 24 18 52 39 42 46 34 56 51 – 52 20 20 28 46 – 34 – 26 42 32 – 72 – – 77 – 82 73 80 47 57 56 36 51 8 35 – 31 68 77 64 51 – 64 – 71 54 65 – Latitude Longitude Opal Relative % from XRD % Relative % from Smectite Zeolite Smectite Sand Silt Clay (wt%) Clay Quartz Plagio- Calcite Calcite XRD (<2 mm) % peak† 060 (%) (%) (%) clase from Smectite Illite Kaolinite expanpeak, TIC dibility d-value –, No data; TIC, total inorganic carbon; Tr, trace (<1%); XRD, X-ray diffraction. Y, there is a peak ~10∞ 2q in the <2 mm XRD data, likely indicating the presence of zeolite; N, no peak. ‡ Hemipelagic mud = dark olive gray hemipelagic mud. MV0209 MV0209 MV0209 MV0209 MV0209 MV0209 MV0209 MV0209 MV0209 MV0209 MV0209 MV0209 MV0209 MV0209 MV0209 MV0209 MV0209 MV0209 MV0209 MV0209 MV0209 MV0209 MV0209 MV0209 MV0209 MV0209 MV0209 MV0209 Cruise Table 2 Summary of sediment composition Hemipelagic mud Olive brown clay Hemipelagic mud Hemipelagic mud Hemipelagic mud Hemipelagic mud Hemipelagic mud Hemipelagic mud Hemipelagic mud Olive brown clay Hemipelagic mud Olive brown clay Calcareous ooze Calcareous ooze Olive brown clay Mixed sediment Calcareous ooze Hemipelagic mud Olive brown clay Olive brown clay Olive brown clay Olive brown clay Hemipelagic mud Hemipelagic mud Hemipelagic mud Hemipelagic mud Hemipelagic mud Olive brown clay Sediment type‡ 440 G. A. Spinelli and M. B. Underwood 55GC 59GC 01GC 02GC 05GC 05GC 08GC 09GC 09GC 10GC 11GC 12GC 13GC 14GC 15GC 16GC 17GC 18PC 18PC 19PC 19PC 19PC 19PC 20GC 21GC 21GC 22GC 23GC 24GC 25GC 26GC 26GC 27GC 273–275 88–90 10–12 53–55 10–12 30–32 4–6 72–74 170–172 68–70 108–110 10–12 90–92 176–178 58–60 78–80 30–32 14–16 261–263 110–120 285–295 395–405 540–560 48–50 24–26 140–142 12–14 55–57 96–98 36–38 105–107 262–264 14–16 8.7890 9.1703 7.8601 8.6237 8.6240 8.6240 8.7374 8.7420 8.7420 9.4364 9.4358 9.4808 9.4812 9.4713 9.4710 9.4741 9.4759 9.6762 9.6762 9.6768 9.6768 9.6768 9.6768 8.5156 8.5060 8.5060 8.5014 8.4966 8.2554 8.2553 8.2429 8.2429 8.2433 -87.1970 -87.2582 -85.2732 -87.2770 -87.2800 -87.2800 -87.2081 -87.2137 -87.2137 -86.9320 -86.9332 -86.9966 -86.9964 -86.9946 -86.9975 -86.9959 -86.9937 -86.5687 -86.5687 -86.5613 -86.5613 -86.5613 -86.5613 -85.9867 -85.9765 -85.9765 -85.9718 -85.9670 -86.2432 -86.2426 -86.2322 -86.2322 -86.2323 5 14 – – – – – – – – 10 – – – – 12 – – 6 – – – 9 – – – 2 – 3 – – – 2 81 88 72 Tr 69 6 Tr 79 35 74 78 72 77 77 75 76 72 80 59 76 75 73 80 75 79 55 79 – 54 74 75 Tr 70 2 3 5 4 3 3 3 3 3 3 4 4 3 4 4 4 3 3 3 4 3 3 3 4 5 4 4 – 5 2 4 4 4 17 9 18 4 28 8 5 11 16 23 18 24 20 19 21 20 25 17 35 20 22 24 17 21 16 14 17 – 16 24 18 4 13 Tr Tr 5 92 Tr 83 92 7 46 Tr Tr Tr Tr Tr Tr Tr Tr Tr 3 Tr Tr Tr Tr Tr Tr 27 Tr – 25 Tr 3 92 13 1.2 – 6.3 – 0.2 – – 6.1 31.6 – – – – – 2.8 – – – 2.3 – – – – – – 20.4 5.3 – 18.9 – 6.6 – 13.5 † 82 89 – – – – – 81 – 91 92 – 80 90 – 86 81 85 – – – 76 – 90 – – – 89 87 – 86 – 75 0 0 – – – – – 2 – 1 1 – 1 1 – 0 3 0 – – – 5 – 0 – – – 1 1 – 1 – 4 18 11 – – – – – 17 – 8 7 – 19 9 – 14 16 15 – – – 19 – 10 – – – 10 12 – 13 – 21 48 58 – – – – – 59 – 63 61 – 55 59 – 61 60 54 – – – 57 – 62 – – – 65 64 – 64 – 56 Y Y – – – – – Y – Y Y – Y Y – Y Y Y – – – N – Y – – – Y Y – Y – Y – – – – – – – – – – 1.505 – 1.503 – – – – – – – – – – – – – – – 1.506 – – – – 14 – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – 37 – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – 49 – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – Latitude Longitude Opal Relative % from XRD % Relative % from Smectite Zeolite Smectite Sand Silt Clay (wt%) Clay Quartz Plagio- Calcite Calcite XRD (<2 mm) % peak† 060 (%) (%) (%) clase from Smectite Illite Kaolinite expanpeak, TIC dibility d-value –, No data; TIC, total inorganic carbon; Tr, trace (<1%); XRD, X-ray diffraction. Y, there is a peak ~10∞ 2q in the <2 mm XRD data, likely indicating the presence of zeolite; N, no peak. ‡ Hemipelagic mud = dark olive gray hemipelagic mud. MV0209 MV0209 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 Cruise Sample ID Core Interval (cm) Olive brown clay Hemipelagic mud Hemipelagic mud Calcareous ooze Mixed sediment Calcareous ooze Calcareous ooze Hemipelagic mud Mixed sediment Hemipelagic mud Hemipelagic mud Hemipelagic mud Hemipelagic mud Hemipelagic mud Hemipelagic mud Hemipelagic mud Hemipelagic mud Hemipelagic mud Hemipelagic mud Hemipelagic mud Hemipelagic mud Hemipelagic mud Hemipelagic mud Hemipelagic mud Hemipelagic mud Mixed sediment Olive brown clay Hemipelagic mud Mixed sediment Olive brown clay Olive brown clay Calcareous ooze Mixed sediment Sediment type‡ Costa Rica sediment: Fluid partitioning 441 28GC 30–32 33GC 24–26 34GC 187–188 34GC 210–212 35GC 230–232 36PC 54–55 36PC 163–165 37PC 135–137 38PC 28–30 39PC 20–22 40GC 125–127 42GC 5–6 43GC 30–32 1040C Sec 2R-4 (115–150 cm) 1040C Sec 20R-5 (115–150 cm) 1040C Sec 24R-1 (120–150 cm) 1040C Sec 36R-3 (135–150 cm) EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 EW0104 ODP Leg 170 ODP Leg 170 ODP Leg 170 ODP Leg 170 54/2 – 4 1 -86.1789 -86.1789 9.6616 – 2 4 -86.1789 9.6616 – 1 -86.1789 9.6616 9.6616 1 – – – 11 – 4 – 6 8 – – 5 2 -85.7779 -86.2304 -86.2503 -86.2503 -86.3117 -86.6826 -86.6826 -86.6852 -86.5689 -86.5692 -86.9098 -86.9048 -86.9141 -86.1789 8.5804 9.2685 9.2501 9.2501 9.2259 8.9375 8.9375 8.9409 9.6765 9.6762 9.1351 9.1254 9.1357 9.6616 80 80 tr 70 81 64 75 77 55 71 67 86 75 71 75 – 73 69 78 4 tr 4 4 4 3 3 3 Tr 5 7 2 4 4 3 – 3 4 5 16 8 4 26 15 25 22 20 45 24 26 12 21 25 22 – 24 27 17 Tr 12 92 Tr Tr 8 Tr Tr Tr Tr Tr Tr Tr Tr Tr – Tr Tr Tr – 15.3 – – – 6.5 – – – – – – 4.1 – – – – – – † – – – – – 91 94 97 100 – 86 – 75 89 91 91 81 94 – – – – – – 2 0 0 0 – 3 – 0 1 0 0 2 1 – – – – – – 7 6 3 0 – 11 – 25 10 9 9 17 5 – – – – – – 66 66 52 53 – 61 – 60 58 58 63 61 65 – – – – – – Y Y N N – Y – Y Y Y Y N Y – – – – – – 1.504 1.503 – – – – – – – – – – 1.503 – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – – Latitude Longitude Opal Relative % from XRD % Relative % from Smectite Zeolite Smectite Sand Silt Clay (wt%) Clay Quartz Plagio- Calcite Calcite XRD (<2 mm) % peak† 060 (%) (%) (%) clase from Smectite Illite Kaolinite expanpeak, TIC dibility d-value –, No data; TIC, total inorganic carbon; Tr, trace (<1%); XRD, X-ray diffraction. Y, there is a peak ~10∞ 2q in the <2 mm XRD data, likely indicating the presence of zeolite; N, no peak. ‡ Hemipelagic mud = dark olive gray hemipelagic mud. CR Trench ODP 1040C Sec 51R-4 Leg 170 (103–107 cm) Sample ID Core Interval (cm) Cruise Table 2 Continued Diatomite (underthrust) Siliceous nannofossil chalk (underthrust) Calcareous diatomite (underthrust) Hemipelagic mud Claystone (prism) Olive brown clay Olive brown clay Hemipelagic mud Altered ash Hemipelagic mud Olive brown clay Olive brown clay Hemipelagic mud Hemipelagic mud Hemipelagic mud Hemipelagic mud Olive brown clay Olive brown clay Claystone (prism) Sediment type‡ 442 G. A. Spinelli and M. B. Underwood Costa Rica sediment: Fluid partitioning 443 Table 3 Weight percentage of hydrous phases in sediment Opal (wt%) Smectite (approximate wt%) Expandability of smectite (%) 10 5 2 60 64 <1 59 62 No data Dark olive gray hemipelagic mud Olive brown clay Calcareous ooze analysis closely approximate the absolute weight percentages). To estimate absolute values of total clay (wt%), we used the wt% opal and the relative abundance of total clay minerals determined by XRD: Relative % calcite (from XRD and opal) 50 40 30 Total clay (wt%) ª [1 - (opal wt%/100)] · relative abundance clay (%) y = 1.40x – 4.53 r2 = 0.91 We then solved for wt% smectite using the value for total clay and the relative abundance of smectite in the <2 mm size fraction: 20 10 Smectite (wt%) ª (clay wt%/100) · relative abundance smectite (%) 0 0 10 20 30 40 (1) 50 % Calcite (from total inorganic carbon) Fig. 8 Relative percent calcite from X-ray diffraction (XRD) analysis for 18 hemipelagic sediment samples (dark olive gray hemipelagic mud and olive brown clay) as a function of the absolute percent calcite calculated from determination of the total inorganic carbon content of the sediment samples. The raw relative percentages of calcite () are corrected () for the opal content of the sediment samples. For samples with <20% calclite, the corrected relative percentages closely approximate the absolute percentages of calcite. we also corrected for the amount of salt in the bulk powders (precipitated during freeze-drying), but that would require a parallel program of systematic physical properties measurements (e.g. water content, grain density, porosity). The XRD analysis slightly underestimates the wt% calcite for samples with very low calcite content, suggesting that approximately 2–5 wt% calcite may be the practical detection limit for the analysis. The relative wt% calcite closely matches the absolute wt% for hemipelagic and mixed-sediment samples with moderate calcite content (~5–15%). For mixed-sediment samples with >15 wt% calcite, the XRD analysis overestimates the fraction of calcite present. The hydrous phases are dominantly contained within the hemipelagic sediment (in which there is much less than 15 wt% calcite, and the relative weight percentages determined by XRD (2) Limitations of this approach include the possibility of clay mineral partitioning as a function of grain size and incorporation of non-clay minerals (e.g. quartz, zeolite) into the clay-sized fraction. Our XRD results, however, show only traces of clay-sized quartz and zeolite, and the amount of smectite should increase in progressively finer size fractions. On average, hemipelagic mud from the Costa Rica study area contains approximately 60% smectite by weight. Smectite in pelagic chalk can not be determined precisely due to the low clay content, but it must be less than 1% (i.e. the relative percent of total clay in the pelagic sediment). CHARACTERISTICS OF SMECTITE The expandability of smectite averages 59% and ranges from 48 to 70% (Table 3). These results indicate that the expandable clay is detrital in origin, rather than a product of authigenic alteration of volcanic ash, and it probably includes crystallites of illite in a disordered mixed-layer structure. Accordingly, when making calculations of water volume within the interlayer site of smectite, we assumed an intermediate state of hydration with two layers of water. This hydration state corresponds to approximately 20% water by weight and approximately 40% water by volume. Analyses of 13 powders revealed broad smectite (060) peaks centered near d = 1.503 Å (Fig. 9). This result indicates the smectite is mostly dioctahedral (Brown & Brindley 1980; Moore & Reynolds 1997). 444 G. A. Spinelli and M. B. Underwood Table 4 Volume of water (m3) per m3 of sediment entering subduction zone Hemipelagic mud Calcareous ooze Weighted average for entire sediment column % of total water 200 quartz d = 1.82 A quartz d = 1.542 A Counts 160 smectite 060 120 80 40 trioctahedral 0 48 50 52 54 56 dioctahedral 58 60 62 ˚2q Fig. 9 Example of X-ray diffraction (XRD) analysis of randomly oriented <2 mm grain size fraction (E43gc 30–32 cm). The diffractogram is aligned to the prominent quartz peaks at d-spacings of 1.82 and 1.542 Å. The smectite 060 peak is close to the typical range (bold lines) for dioctahedral smectite, suggesting it is detrital in origin. Dioctahedral members of the smectite group (montmorillonite, Al-rich beidellite) typically form through pedogenesis of diverse protoliths under a wide range of environmental conditions (e.g. Fagel et al. 2001), although pure bentonite layers also form through submarine alteration of silicic volcanic ash (Hodder et al. 1990; Naish et al. 1993). In contrast, trioctahedral varieties (saponite) and Ferich dioctahedral end-members (non-tronite) originate through meteoric weathering and hydrothermal alteration of basalt (e.g. McMurtry et al. 1982; Parra et al. 1986; Güven 1988; Chamley 1989). Most of the dioctahedral clay that was deposited offshore Costa Rica probably formed through tropical weathering of volcanic and sedimentary rocks in Central America. DISCUSSION FLUID PARTITIONING Sediment-hosted fluids on the incoming Cocos Plate are partitioned between a basal pelagic section and an overlying hemipelagic section. Within Pore space Opal Smectite 0.752 0.700 0.727 96.2% 0.0051 0.0015 0.0029 0.4% 0.0653 0.0016 0.0258 3.4% each of those sections, fluid is partitioned between sediment pores and hydrous minerals. We estimate sediment porosity using data from ODP Site 1039. The average porosity of hemipelagic samples from Site 1039 is 75%; the average porosity of pelagic samples is 70% (Kimura et al. 1997). Porosity averages 73% over the entire sediment column. The thicknesses of hemipelagic and pelagic intervals cored at Site 1039 (152 and 225 m) are similar to the medians derived from seismic data (135 and 213 m). The pelagic section, on average, is approximately 2% opal by weight and <1% smectite by weight. The hemipelagic section is approximately 10% opal by weight and 60% smectite by weight. We convert the weight percentages of opal and smectite to volume percentages based on their densities (ropal ª 2.47 g/cm3; rsmectite ª 2.02 g/cm3), then calculate the volume of water in opal within a typical 1 m3 of sediment by: Volume water in opal ª (1 - [n/100]) · vol% opal · vol% water in opal (3) where n is porosity, and the vol% of water in opal is 23% (equivalent to 11% water by weight). A similar approach is used to determine the volume of water in smectite within a typical 1 m3 of sediment: Volume water in smectite ª (1 - [n/100]) · vol% smectite · vol% water in smectite (4) where the vol% of water in smectite is 40% (equivalent to 20% water by weight, or two layers of interlayer water). As initially deposited, the pelagic and hemipelagic sediments contain more than 70% water by volume. Distributed over the entire sediment column, 96% of that water is within pore spaces, 3.6% is in smectite and 0.4% is in opal (Table 4). Once subduction begins, rapid loading consolidates sediment within the first ~5 km from the trench (Shipley et al. 1990; Kimura et al. 1997; McIntosh & Sen 2000; Saffer et al. 2000; Saito & Goldberg 2001). The hemipelagic sediment section Costa Rica sediment: Fluid partitioning 445 Average porosity (%) (a) 80 n = –1.34 ln(x) + 64.9 r2 = 0.76 70 60 50 0 1 2 3 4 5 Distance into subduction zone (km) Average porosity (%) (b) 80 70 n = 65.1 e–0.055x r2 = 0.71 60 50 0 1 2 3 4 5 Distance into subduction zone (km) Fig. 10 Average porosity of underthrust sediment around Ocean Drilling program (ODP) Sites 1039, 1040 and 1043, based on index properties measurements (Kimura et al. 1997), laboratory consolidation tests (Saffer et al. 2000), variations in layer thickness (Saito & Goldberg 2001) or reflection seismic experiments (Shipley et al. 1990; McIntosh & Sen 2000). The hemipelagic section (a) of the sediment column compacts and looses a large fraction of its porosity in the first kilometer beyond the Middle America Trench, after which the rate of porosity loss decreases. The pelagic section (b) compacts less than the hemipelagic section in the first few kilometers of the subduction zone. , Kimura et al. (1997); +, McIntosh and Sen (2000); ¥, Saffer et al. (2000); , Saito and Goldberg (2001); , Shipley et al. (1990). loses a substantial fraction of its porosity (down to ~65–60%) within the first kilometer of the subduction, but the rate of consolidation decreases over the next 4 km. Porosity loss in the pelagic section is more gradual and uniform (Fig. 10). Low permeability within the clay-rich sediment inhibits drainage of the pore water. Consequently, on the Costa Rica margin, underthrust sediment in the shallow portion of the subduction zone is underconsolidated due to sustained pore-fluid pressures above hydrostatic (Saffer et al. 2000). The amount of additional porosity loss is poorly constrained beyond the coverage of reflection seismic data (i.e. farther than ~5 km into the subduction zone), but some insights can be gained from the numerical modeling of fluid by Saffer and Bekins (1998), who suggested that the underthrust sediment in Nankai Trough reached a normally consolidated state by ~30 km into the subduction zone. If the underthrust sediment on the Costa Rica margin follows a similar response (normally consolidated 30 km from the subduction front), then we can identify a reference point for comparison. The point’s depth below seafloor depends upon the margin’s subduction geometry. The slope of the margin wedge off Nicoya is approximately 5.4∞; the decollement dips approximately 6∞ for the first 30 km, then increases to approximately 13∞ (Christeson et al. 1999). Thus, the wedge is approximately 6 km thick 30 km landward of the trench. A global compilation of porosity versus depth (Bray & Karig 1985) can be used to estimate corresponding porosity values of approximately 5–15%. If those estimates are correct, then the switchover in fluid budget from mostly porehosted water to mostly mineral-hosted water occurs before strata reach 30 km into the Costa Rica subduction zone (Fig. 11). SEDIMENT DEHYDRATION Release of water from the mineral structures of opal and smectite is controlled by reaction kinetics (Ernst & Calvert 1969; Pytte & Reynolds 1988; Huang et al. 1993). Opal dehydration goes to completion between temperatures of approximately 50 and 100∞C (Murata et al. 1977; Behl & Garrison 1994). In typical sedimentary basins, most progress of the smectite-to-illite reaction (with two pulses of smectite dewatering) occurs between 60 and 140∞C (Perry & Hower 1970, 1972; Freed & Peacor 1989). Geochemical analyses of fluids collected from the frontal decollement (Kimura et al. 1997) indicate that key reactions occurred at temperatures of at least 80–120∞C but less than 150∞C (Chan & Kastner 2000; Silver et al. 2000). This inferred window overlaps the temperatures for both opal and smectite dehydration. In situ temperature at the frontal decollement (Site 1040) is <5∞C (Kimura et al. 1997), suggesting a deeper source for the fluids. Thermal models for the Nicoya subduction zone yield temperature predictions of 100∞C at horizontal distances 40–75 km into the subduction zone and 160∞C once strata reach 60–100 km into the subduction zone (Harris & Wang 2002); the upper 446 G. A. Spinelli and M. B. Underwood Depth (km) (a) 0 Plate interface 10 20 Earthquakes 30 40 CNS (warm) EPR (cool) 20 0 40 60 80 100 Distance into subduction zone (km) (b) 0 20 40 ? 0.6 60 cool 0.8 warm 0.4 ? Proportion of water in smectite+opal 1 0.2 0 Increased fluid pressure during diagenetic dewatering 80 100 Smectite and opal reactions completed (cool case) Dissipating fluid pressure; increasing effective stress and lower limits of the modeling solution depend on the inferred thermal state of the incoming crust. On the basis of those numerical simulations, we suggest that opal and smectite dewater in discrete pulses after porosity drops below approximately 15% and the rate of compaction slows. Zones of elevated fluid pressures along the plate boundary fault should coincide with compartments of diagenetic fluid release (e.g. Saffer & Bekins 1998), thereby decreasing effective stress in a patchy 3-D pattern. Heat flow also varies alongstrike, with higher values (average ~105 mW/m2) on CNS crust in the southeast and lower values (average ~20 mW/m2) on EPR crust in the northwest. There are also local zones of high heat flow on EPR crust caused by hydrothermal circulation. This variation in heat flow likely leads to an alongstrike difference in the distance into the subduction zone at which much of the diagenetic dewatering reaction progress occurs. IMPLICATIONS FOR OTHER CIRCUM-PACIFIC SUBDUCTION ZONES The volumetric contribution and spatial distribution of diagenetic fluid sources along a subduction thrust depend on the composition and temperature path of subducted and accreted sediment, Fig. 11 Earthquake locations (a) from Newman et al. (2002) and proportion of water contained in hydrous minerals within sediments subducted offshore Costa Rica (b). The volume of water in the hydrous mineral phases (relative to pore space) increases with distance into the subduction zone as porosity decreases. The gray polygon indicates the range of potential fluid partitioning scenarios based on a range of sediment porosities from Bray and Karig (1985). Beyond 20–30 km into the subduction zone, most of the water in the sediment is contained in hydrous minerals. The location in the subduction zone at which water is released from the hydrous minerals is a function of reaction kinetics; fluid will be released closer to the trench in a warm subduction zone than in a cool one. Shallow earthquakes occur closer to the trench in the warm portion of the subduction zone than in the cool section (a). The up-dip limit of seismicity may be related to increased effective stress as fluid pressures from diagenetic dewatering reactions dissipate. CNS, Cocos–Nazca Spreading Center; EPR, East Pacific Rise. which can vary both between and within subduction zones. To place Costa Rica within a broader context of circum-Pacific subduction zones, we compare results from Nankai Trough, the Japan Trench, the Aleutian Trench and Cascadia. The Nankai Trough is characterized by sediment with low opal content, highly variable smectite content, and highly variable heat flow. Diatoms and radiolarians are rare in the upper and lower Shikoku Basin sections, but are more abundant in the trench-wedge facies (Shipboard Scientific Party 1975, 1986, 2001). The content of biogenic silica is less than 1 wt%. The smectite content of sediment along the central (Muroto) transect is modest because of presubduction diagenesis, generally <25% of the bulk sediment by weight (Underwood et al. 1993; Steurer & Underwood 2003a). Seafloor heat flow near the trench on the Muroto transect is high, approximately 130– 180 mW/m2 (Hyndman et al. 1995; Shipboard Scientific Party 2001). Along the western (Ashizuri) transect, smectite is much more abundant in the lower Shikoku Basin strata, typically 30–50% of the bulk sediment by weight (Steurer & Underwood 2003a; Underwood et al. 2003), and heat flow is substantially lower, approximately 63 mW/m2 (Kinoshita & Yamano 1986; Shipboard Scientific Party 1986). Costa Rica sediment: Fluid partitioning 447 The sediment inputs to the Japan Trench have moderate to high opal and smectite contents. Seafloor heat flow is low, approximately 25–65 mW/m2 (Burch & Langseth 1981), because the subducting Pacific Plate is relatively old. Sediment from Site 436 (outer rise off the Japan Trench) is consistently 5–20% opal (Mann & Muller 1980; Shipboard Scientific Party 1980) and smectite composes approximately 30–50% of the clay minerals (Mann & Muller 1980). The Aleutian Trench is characterized by high opal content and spatially variable smectite content. Heat flow is not well constrained in the North Pacific, but it is likely moderate to low because of the age of subducting lithosphere. Heat flow at Site 183 (off the Alaska Peninsula) is estimated at 25 mW/m2 (Erikson 1973). On the basis of lithospheric cooling models, ages of 50– 70 Ma (Muller et al. 1997) correspond to heat flow of 70–60 mW/m2 (e.g. Parsons & Sclater 1977; Harris & Chapman in press). The area seaward of the Aleutian Trench is within a zone of high diatom productivity (Kastner 1981). Therefore, those sediments have high opal contents (Shipboard Scientific Party 1973a, 1973b, 1993; Rea & Ruff 1996). The percentage of smectite in the <2 mm fraction steadily increases westward from 10–20% in the Gulf of Alaska to 30–40% in the central Aleutian Trench (Hathon & Underwood 1991). Sediment approaching the Cascadia subduction zone has low opal content and spatially variable smectite content; heat flow and sediment thickness are unusually high. At two sites in the Cascadia Basin, opal accounts for approximately 5% of the late Quaternary sediment (Heath et al. 1976). Off southern Washington and northern Oregon, 30– 50% of the <2 mm fraction is smectite, but values drop to 20–30% off southern Oregon and northern California (Karlin 1980; Underwood 2002). Heat flow near the trench off Oregon ranges from approximately 55 to 150 mW/m2 (Korgen et al. 1971; Moran & Lister 1987). Heat flow at Site 888 (off British Columbia) is 80 mW/m2 (Shipboard Scientific Party 1994); similar to the southern Cascadia subduction zone, seafloor heat flow on the incoming plate near the trench off British Columbia ranges from approximately 50 to 150 mW/m2 (Davis et al. 1990). Subduction zones with relatively large inputs of opal and/or smectite (Costa Rica, Aleutians, Japan Trench, southwestern Nankai Trough) have large diagenetic fluid sources along the plate interface. Where opal content is higher (Aleutians, Japan Trench) dehydration will start closer to the trench (at lower temperatures) than in subduction zones where smectite content is higher. High heat flow (southeastern Costa Rica, Cascadia, central Nankai Trough) will push the diagenetic fluid sources closer to the trench. Where large fractions of the incoming sediment are subducted (Costa Rica, Japan Trench) rather than accreted, diagenetic fluid sources will be concentrated along or beneath the decollement, not distributed throughout the prism. CONCLUSIONS The hemipelagic sediment subducting beneath the Nicoya Peninsula, Costa Rica, has moderate opal content and high smectite content (relative to other subduction zones and in absolute terms). These hydrous minerals convey a large volume of water into the subduction zone. As kinetically controlled diagenetic reactions proceed rapidly at high temperature (10 s of km into the subduction zone), that water is released. Hydrous minerals contain most of the fluid within subducted sediment beyond approximately 20 km into the subduction zone (Fig. 11). Therefore, within loci of diagenetic dewatering reactions, the volume of fluid released from the opal-to-quartz and smectite-to-illite transitions is larger than sediment compaction sources. Once opal and smectite dehydration are exhausted, elevated fluid pressures should dissipate. The down-dip increase of effective stress might, in turn, affect the up-dip limit of seismicity. Along-strike variations in sediment composition, the thermal state of crust approaching the trench, and the stratigraphic position of the decollement lead to spatial variability in diagenetic fluid sources (and therefore fluid pressure and effective stress along the plate interface). On the Costa Rica margin, sediment composition is uniform but there is a large, abrupt change in seafloor heat flow along-strike. This thermal variability probably controls the loci where large amounts of subducted smectite and opal release their bound water (Spinelli & Saffer 2004). In the Cascadia and Aleutian subduction zones, along-strike variations in smectite content modulate diagenetic fluid sources. In the Nankai Trough, sediment composition and heat flow both vary along-strike. Thus, each subduction system displays a unique combination of thermal and compositional inputs that change in 3-D. The influence of those subduction 448 G. A. Spinelli and M. B. Underwood inputs on fluid pressure and effective stress along the deeper plate boundaries needs to be evaluated on a case-by-case basis. ACKNOWLEDGEMENTS This work was supported by NSF MARGINS grants OCE-0304946 and OCE-02106921 and the University of Missouri Research Council. We thank the captains and crew of the R/V Maurice Ewing and R/V Melville for their assistance during the TicoFlux I and II expeditions (funded by NSF grants OCE-0001892, OCE-0001944, OCE0001941 and OCE-0002031). This research also used samples provided by the Ocean Drilling Program, sponsored by the US National Science Foundation and participating countries under management of Joint Oceanographic Institutions Inc. E. Silver, P. Costa, and H. DeShon (University of California at Santa Cruz) acquired and processed the reflection seismic data. Y. Chan (University of Minnesota–Duluth Large Lakes Observatory) provided advice on opal analysis. N. Basu, S. Udas, K. Hoke, J. Dartt and A. Bidesi assisted in the lab. We thank Yujiro Ogawa and Tetsuro Hirono for helpful reviews of the manuscript. REFERENCES ATHY L. F. 1930. Density, porosity, and compaction of sedimentary rocks. Bulletin of the American Association of Petroleum Geologists 14, 1–24. BAHR D. B., HUTTON E. W. H., SYVITSKI J. P. M. & PRATSON L. F. 2001. Exponential approximations to compacted sediment porosity profiles. Computers and Geosciences 27, 691–700. BARCKHAUSEN U., RANERO C. R., VON HUENE R., CANDE S. C. & ROESER H. A. 2001. Revised tectonic boundaries in the Cocos Plate off Costa Rica: Implications for the segmentation of the convergent margin and for plate tectonic models. Journal of Geophysical Research 106, 19 207–220. BEHL R. J. & GARRISON R. E. 1994. The origin of chert in the Monterey Formation of California (USA). In Proceedings of the 29th International Geology Congress, Part C; 24 Aug-3 Sep 1992; Kyoto, Japan; pp. 101–32. VSP International Science Publishers, Zeist, the Netherlands. BEKINS B. A. & DREISS S. J. 1992. A simplified analysis of parameters controlling dewatering in accretionary prisms. Earth and Planetary Science Letters 109, 275–87. BIRD P. 1984. Hydration-phase diagrams and friction of montmorillonite under laboratory and geologic conditions, with implications for shale compaction, slope stability, and strength of fault gouge. Tectonophysics 107, 235–60. BISCAYE P. E. 1965. Mineralogy and sedimentation of recent deep-sea clay in the Atlantic Ocean and adjacent seas and oceans. Geological Society of America Bulletin 76, 803–32. BOLES J. R. & FRANKS S. G. 1979. Clay diagenesis in Wilcox sandstones of southwest Texas: Implications of smectite diagenesis on sandstone cementation. Journal of Sedimentary Petrology 49, 55–70. BRAY C. J. & KARIG D. E. 1985. Porosity of sediments in accretionary prisms and some implications for dewatering processes. Journal of Geophysical Research 90, 768–78. BROWN G. & BRINDLEY G. W. 1980. X-ray diffraction procedures for clay mineral identification. In Brindley G. W. & Brown G. (eds.) Crystal Structures of Clay Minerals and their X-Ray Identification, pp. 305–59, Mineral Society Monograph 5. Mineralogical Society (Great Britain), London. BRUCE C. H. 1984. Smectite dehydration—Its relation to structural development and hydrocarbon accumulation in northern Gulf of Mexico basin. American Association of Petroleum Geologists Bulletin 68, 673–83. BURCH T. K. & LANGSETH M. G. 1981. Heat-flow determination in three DSDP boreholes near the Japan Trench. Journal of Geophysical Research 86, 9411– 419. BYERLEE J. D. 1990. Friction, overpressure and fault normal compression. Geophysical Research Letters 17, 2109–112. BYERLEE J. D. 1993. Model for episodic flow of highpressure water in fault zones before earthquakes. Geology 21, 303–306. CHAMLEY H. 1989. Clay Sedimentology. SpringerVerlag, Berlin. CHAN L.-H. & KASTNER M. 2000. Lithium isotopic compositions of pore fluids and sediments in the Costa Rica subduction zone; implications for fluid processes and sediment contribution to the arc volcanoes. Earth and Planetary Science Letters 183, 275–90. CHRISTESON G. L., MCINTOSH K. D., SHIPLEY T. H., FLUEH E. R. & GOEDDE H. 1999. Structure of the Costa Rica convergent margin, offshore Nicoya Peninsula. Journal of Geophysical Research 104, 25 443– 68. COLTEN-BRADLEY V. A. 1987. Role of pressure in smectite dehydration—Effects on geopressure and smectite-to-illite transformation. American Association of Petroleum Geologists Bulletin 71, 1414–27. DAVIS E. E., HYNDMAN R. D. & VILLINGER H. 1990. Rates of fluid expulsion across the northern Cascadia accretionary prism: Constraints from new heat flow Costa Rica sediment: Fluid partitioning 449 and multichannel seismic reflection data. Journal of Geophysical Research 95, 8869–89. DEMASTER D. J. 1981. The supply and accumulation of silica in the marine environment. Geochimica et Cosmochimica Acta 45, 1715–32. DEMETS D. C. 2001. A new estimate for present-day Cocos-Caribbean plate motion: Implications for slip along the Central American volcanic arc. Geophysical Research Letters 28, 4043–6. DENG X. & UNDERWOOD M. B. 2001. Abundance of smectite and the location of the plate boundary fault, Barbados accretionary prism. Geological Society of America Bulletin 113, 495–507. DREVER J. J. 1973. The preparation of oriented clay mineral specimens for X-ray diffraction analysis by the filter-membrane technique. American Mineralogist 58, 553–4. ERNST W. G. & CALVERT S. E. 1969. An experimental study of the recrystallization of porcelanite and its bearing on the origin of some bedded cherts. American Journal of Science 267A, 114–33. ERIKSON A. 1973. Initial report on downhole temperature and shipboard thermal conductivity measurements, Leg 19. Initial Reports of the Deep Sea Drilling Project 19, 643–56. FAGEL N., ROBERT C., PREDA M. & THOREZ J. 2001. Smectite composition as a tracer of deep circulation: the case of the Northern North Atlantic. Marine Geology 172, 309–30. FISHER A. T., STEIN C. A., HARRIS R. N. et al. 2003. Abrupt thermal transition reveals hydrothermal boundary and role of seamounts within the Cocos Plate. Geophysical Research Letters 30, 1550 (doi: 10.1029/2002GL016766). FISHER A. T. & UNDERWOOD M. B. 1995. Calibration of an X-ray diffraction method to determine relative mineral abundances in bulk powders using matrix singular value decomposition: a test from the Barbados accretionary complex. Proceedings of the Ocean Drilling Program, Initial Reports 156, 29–37. FREED R. L. & PEACOR D. R. 1989. Variability in temperature of the smectite/illite reaction in Gulf Coast sediments. Clay Minerals 24, 171–80. FRIEDMANN P. K., WHEAT C. G., UNDERWOOD M. B. et al. 2001. Evidence for hydrothermal circulation and alteration on 20–25 Ma crust in the Middle American Trench. EOS Transactions (AGU Fall Meeting Suppl.) 82, Abstract T22C-0922. GRASSHOFF K., EHRHARDT M. & KREMLING K. 1983. Methods of Seawater Analysis. Verlag Chemie, Weinheim. GÜVEN N. 1988. Smectites. In Bailey S. W. (ed.) Hydrous Phyllosilicates, Reviews in Mineralogy 19, pp. 497–559. Mineral Society of America, Washington, DC. HARRIS R. N. & CHAPMAN D. S. in press. Deep-seated oceanic heat flow, heat deficits, and hydrothermal circulation. In Davis E. E. & Elderfield H. (eds.) Hydrogeology of the Oceanic Lithosphere. Cambridge University Press. HARRIS R. N. & WANG K. 2002. A thermal model of the Middle America Trench at the Nicoya Peninsula, Costa Rica. Geophysical Research Letters doi: 10.1029/2002GL015406. HATHON E. G. & UNDERWOOD M. B. 1991. Clay mineralogy and chemistry as indicators of hemipelagic sediment dispersal south of the Aleutian arc. Marine Geology 97, 145–66. HEATH G. R., MOORE T. C. Jr & DAUPHIN J. P. 1976. Late Quaternary accumulation rates of opal, quartz, organic carbon, and calcium carbonate in the Cascadia Basin area, northeast Pacific. Geological Society of America Memoir 145, 393–409. HODDER A. P. W., GREEN B. E. & LOWE D. J. 1990. A two-stage model for the formation of clay minerals from tephra-derived volcanic glass. Clay Minerals 25, 313–27. HOLBROOK P. 2002. The primary controls over sediment compaction. Pressure Regimes in Sedimentary Basins and their Prediction, AAPG Memoir 76, 21– 32. HOWER J., ESLINGER E. V., HOWER M. E. & PERRY E. A. 1976. Mechanism of burial and metamorphism of argillaceous sediment: 1. Mineralogical and chemical evidence. Geological Society of America Bulletin 87, 725–37. HUANG W.-L., LONGO J. M. & PEVEAR D. R. 1993. An experimentally derived kinetic model for smectite-toillite conversion and its use as a geothermometer. Clays and Clay Minerals 41, 162–77. HYNDMAN R. D., WANG K. & YAMANO M. 1995. Thermal constraints on the seismogenic portion of the southwestern Japan subduction thrust. Journal of Geophysical Research 100, 15 373–92. HYNDMAN R. D., YAMANO M. & OLESKEVICH D. A. 1997. The seismogenic zone of subduction thrust faults. The Island Arc 6, 244–60. KARLIN R. 1980. Sediment sources and clay mineral distributions off the Oregon coast. Journal of Sedimentary Petrology 50, 543–59. KASTNER M. 1981. Authigenic silicates in deep-sea sediments: Formation and diagenesis. In Emiliani C. (ed.) The Sea, Vol. 7, pp. 915–80. Wiley Interscience, New York. KASTNER M., ELDERFIELD H. & MARTIN J. B. 1991. Fluids in convergent margins: what do we know about their composition, origin, role in diagenesis and importance for oceanic chemical fluxes? Philosophical Transactions of the Royal Society of London A 335, 243–59. KIMURA G., SILVER E., BLUM P. et al. 1997. Proceedings of the Ocean Drilling Program, Initial Reports 170. Ocean Drilling Program, College Station, TX. KINOSHITA H. & YAMANO M. 1986. The heat flow anomaly in the Nankai Trough area. Initial Reports of the Deep Sea Drilling Project 87, 737–43. 450 G. A. Spinelli and M. B. Underwood KORGEN B. J., BODVARSSON G. & MESECAR R. S. 1971. Heat flow through the floor of Cascadia Basin. Journal of Geophysical Research 76, 4758–74. LANGSETH M. G. & MOORE J. C. 1990. Introduction to special section on the role of fluids in sediment accretion, deformation, diagenesis, and metamorphism in subduction zones. Journal of Geophysical Research 95, 8737–41. MAGEE M. E. & ZOBACK M. D. 1993. Evidence for a weak interplate thrust fault along the northern Japan subduction zone and implications for the mechanics of thrust faulting and fluid expulsion. Geology 21, 809–12. MANN U. & MULLER G. 1980. Composition of sediments of the Japan Trench transect, Legs 56 and 57, Deep Sea Drilling Project. Initial Reports of the Deep Sea Drilling Project 56–57, 939–77. MCINTOSH K. D. & SEN M. K. 2000. Geophysical evidence for dewatering and deformation processes in the ODP Leg 170 area offshore Costa Rica. Earth and Planetary Science Letters 178, 125–38. MCMURTRY G. M., WANG C.-H. & YEH H.-W. 1982. Chemical and isotopic investigations into the origin of clay minerals from the Galapagos hydrothermal mounds field. Geochimica et Cosmochimica Acta 47, 475–89. MOORE D. & REYNOLDS R. C. 1997. X-Ray Diffraction and the Identification and Analysis of Clay Minerals. Oxford University Press, Oxford. MOORE J. C. & SAFFER D. 2001. Updip limit of the seismogenic zone beneath the accretionary prism of southwest Japan: An effect of diagenetic to lowgrade metamorphic processes and increasing effective stress. Geology 29, 183–6. MOORE J. C. & VROLIJK P. 1992. Fluids in accretionary prisms. Reviews of Geophysics 30, 113–35. MORAN J. E. & LISTER C. R. B. 1987. Heat flow across Cascadia Basin near 47∞N, 128∞W. Journal of Geophysical Research 92, 11 416–32. MULLER R. D., ROEST W. R., ROYER J. Y., GAHAGAN L. M. & SCLATER J. G. 1997. Digital isochrons of the world’s ocean floor. Journal of Geophysical Research 102, 3211–14. MURATA K. J., FRIEDMAN I. & GLEASON J. D. 1977. Oxygen isotope relations between diagenetic silica minerals in Monterey Shale, Temblor Range, California. American Journal of Science 277, 259–72. NAISH T. R., NELSON C. S. & HODDER A. P. W. 1993. Evolution of Holocene sedimentary bentonite in a shallow-marine embayment, Firth of Thames, New Zealand. Marine Geology 109, 267–78. NEWMAN A. V., SCHWARTZ S. Y., GONZALEZ V., DESHON H. R., PROTTI J. M. & DORMAN L. M. 2002. Along-strike variability in the seismogenic zone below Nicoya Peninsula, Costa Rica. Geophysical Research Letters 29, 1977–81. PARRA M., PONS J. C. & FERRAGNE A. 1986. Two potential sources for Holocene clay sedimentation in the Caribbean Basin: The Lesser Antillies Arc and the South American continent. Marine Geology 72, 287– 304. PARSONS B. & SCLATER J. G. 1977. An analysis of the variation of ocean floor bathymetry and heat flow with age. Journal of Geophysical Research 82, 803–29. PEACOCK S. M. 1990. Fluid processes in subduction zones. Science 248, 329–37. PERRY E. & HOWER J. 1970. Burial diagenesis in Gulf Coast pelitic sediments. Clays and Clay Minerals 18, 165–77. PERRY E. & HOWER J. 1972. Late-stage dehydration in deeply buried pelitic sediments. American Association of Petroleum Geologists Bulletin 56, 2013– 21. POWERS M. C. 1967. Fluid-release mechanisms in compacting marine mudrocks and their importance in oil exploration. American Association of Petroleum Geologists Bulletin 51, 1240–54. PYTTE A. M. & REYNOLDS R. C. 1988. The thermal transformation of smectite to illite. In Naeser N. D. & McCulloh T. M. (eds.) Thermal Histories of Sedimentary Basins, pp. 133–40. Springer-Verlag, New York. RAYMOND S. 1983. Burial history and diagenetic reaction kinetics. American Association of Petroleum Geologists Bulletin 67, 684–91. REA D. K. & RUFF L. J. 1996. Composition and mass flux of sediment entering the world’s subduction zones: Implications for global sediment budgets, great earthquakes, and volcanism. Earth and Planetary Science Letters 140, 1–12. RETTKE R. C. 1981. Probable burial, diagenetic, and provenance effects on Dakota Group clay mineralogy, Denver Basin. Journal of Sedimentary Petrology 51, 541–51. SAFFER D. M. & BEKINS B. A. 1998. Episodic fluid flow in the Nankai accretionary complex: Timescale, geochemistry, flow rates, and fluid budget. Journal of Geophysical Research 103, 30 351–70. SAFFER D. M. & SCREATON E. J. 2003. Fluid flow at the toe of convergent margins: interpretation of sharp pore-water geochemical gradients. Earth and Planetary Science Letters 213, 261–70. SAFFER D. M., SILVER E. A., FISHER A. T., TOBIN H. & MORAN K. 2000. Inferred pore pressures at the Costa Rica subduction zone: implications for dewatering processes. Earth and Planetary Science Letters 177, 193–207. SAITO S. & GOLDBERG D. 2001. Compaction and dewatering processes of the oceanic sediments in the Costa Rica and Barbados subduction zones: estimates from in situ physical properties measurements. Earth and Planetary Science Letters 191, 283–93. SCHLÜTER M. & RICKERT D. 1998. Effect of pH on the measurement of biogenic silica. Marine Chemistry 63, 81–92. SCREATON E., SAFFER D. M., HENRY P., HUNZE S. et al. 2002. Porosity loss within the underthrust sed- Costa Rica sediment: Fluid partitioning 451 iments of the Nankai accretionary complex: Implications for overpressures. Geology 30, 19–22. SHIPBOARD SCIENTIFIC PARTY. 1973a. Site 178. Initial Reports of the Deep Sea Drilling Project 18, 287–376. SHIPBOARD SCIENTIFIC PARTY. 1973b. Site 183. Initial Reports of the Deep Sea Drilling Project 19, 19–91. SHIPBOARD SCIENTIFIC PARTY. 1975. Site 297. Initial Reports of the Deep Sea Drilling Project 31, 275–316. SHIPBOARD SCIENTIFIC PARTY. 1980. Site 436: Japan Trench outer rise, Leg 56. Initial Reports of the Deep Sea Drilling Project 56–57, 399–446. SHIPBOARD SCIENTIFIC PARTY. 1986. Site 582. Initial Reports of the Deep Sea Drilling Project 87, 35–122. SHIPBOARD SCIENTIFIC PARTY. 1993. Site 884. Proceedings of the Ocean Drilling Program, Initial Reports 145, 209–302. SHIPBOARD SCIENTIFIC PARTY. 1994. Site 888. Proceedings of the Ocean Drilling Program, Initial Reports 146, 55–125. SHIPBOARD SCIENTIFIC PARTY. 2001. Site 1173. In Moore G. F., Taira A., Klaus A. et al. Proceedings of the Ocean Drilling Program, Initial Reports 190 [online]. Available from: http://www-odp.tamu.edu/ publications/190_IR/chap_04/chap_04.htm. SHIPLEY T. H., STOFFA P. L. & DEAN D. F. 1990. Underthrust sediments, fluid migration paths, and mud volcanoes associated with the accretionary wedge off Costa Rica: Middle America Trench. Journal of Geophysical Research 95, 8743–52. SIBSON R. H. 1981. Controls on low-stress hydrofracture dilatancy in thrust, wrench and normal fault terrains. Nature 289, 665–7. SILVER E., KASTNER M., FISHER A., MORRIS J., MCINTOSH K. & SAFFER D. 2000. Fluid flow paths in the Middle America Trench and Costa Rica margin. Geology 28, 679–82. SPINELLI G. A. & SAFFER D. M. 2004. Along-strike variations in underthrust sediment dewatering on the Nicoya margin, Costa Rica related to the updip limit of seismicity. Geophysical Research Letters 31, L04613 (doi: 10.1029/2003GL018863). STEIN C. & STEIN S. 1994. Constraints on hydrothermal heat flux through the oceanic lithosphere from global heat flow. Journal of Geophysical Research 99, 3081– 95. STEURER J. F. & UNDERWOOD M. B. 2003a. Clay mineralogy of mudstones from the Nankai Trough reference Sites 1173 and 1177 and frontal accretionary prism Site 1174. In Mikada H., Moore G. F., Taira A., Becker K., Moore J. C. & Klaus A. (eds.) Proceedings of the Ocean Drilling Program, Scientific Results 190/196 [online]. Available from: http://wwwodp.tamu.edu/publications/190196SR/211/211.htm. STEURER J. F. & UNDERWOOD M. B. 2003b. Data Report: The relation between physical properties and grain-size variations in hemipelagic sediments from Nankai Trough. In Mikada H., Moore G. F., Taira A., Becker K., Moore J. C. & Klaus A. (eds.) Proceedings of the Ocean Drilling Program, Scientific Results 190/196 [online]. Available from: http://www-odp.tamu.edu/publications/190196SR/ 210/210.htm. SWARBRICK R. E., OSBORNE M. J. & YARDLEY G. S. 2002. Comparison of overpressure magnitude resulting from the main generating mechanisms. In Huffman A. R. & Bowers G. L. (eds.) Pressure Regimes in Sedimentary Basins and their Prediction, AAPG Memoir 76, 1–12. TRASK P. D. 1931. Compaction of sediments. Bulletin of the American Association of Petroleum Geologists 15, 271–6. TRIBBLE J. S. 1990. Clay diagenesis in the Barbados accretionary complex; potential impact of hydrology and subduction dynamics. Proceedings of the Ocean Drilling Program, Scientific Results 110, 97–110. UNDERWOOD M. B. 2002. Strike-parallel variations in clay minerals and fault vergence in the Cascadia subduction zone. Geology 30, 155–8. UNDERWOOD M. B. & PICKERING K. T. 1996. Claymineral provenance, sediment dispersal patterns, and mudrock diagenesis in the Nankai accretionary prism, Southwest Japan. Clays and Clay Minerals 44, 339–56. UNDERWOOD M. B., PICKERING K. T., GIESKES J. M., KASTNER M. & ORR R. 1993. Sediment geochemistry, clay mineralogy, and diagenesis: a synthesis of data from Leg 131, Nankai Trough. Proceedings of the Ocean Drilling Program, Scientific Results 131, 343–63. UNDERWOOD M. B., BASU N., STEURER J. & UDAS S. 2003. Data Report: Normalization factors for semiquantitative X-ray diffraction analysis, with application to DSDP Site 297, Shikoku Basin. In Mikada H., Moore G. F., Taira A., Becker K., Moore J. C. & Klaus A. (eds.) Proceedings of the Ocean Drilling Program, Scientific Results 190/196 [online]. Available from: http://www-odp.tamu.edu/publications/ 190196SR/203/203.htm. UNSWORTH M. J., MALIN P. E., EGBERT G. D. & BOOKER J. R. 1997. Internal structure of the San Andreas Fault at Parkfield, California. Geology 25, 359–62. VROLIJK P. 1990. On the mechanical role of smectite in subduction zones. Geology 18, 703–707.
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