yr slip rate for the Bucaramanga-Santa Marta Fault, Colombia

yr slip rate for the Bucaramanga-Santa Marta Fault, Colombia

Accepted Manuscript Magnetic stratigraphy of the Bucaramanga alluvial Fan: Evidence for a ≤ 3 mm/yr slip rate for the Bucaramanga-Santa Marta Fault, C...

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Accepted Manuscript Magnetic stratigraphy of the Bucaramanga alluvial Fan: Evidence for a ≤ 3 mm/yr slip rate for the Bucaramanga-Santa Marta Fault, Colombia Giovanny Jiménez Diaz , Fabio Speranza , Claudio Faccena , German Bayona , Andres Mora PII:

S0895-9811(14)00154-0

DOI:

10.1016/j.jsames.2014.11.001

Reference:

SAMES 1341

To appear in:

Journal of South American Earth Sciences

Received Date: 13 March 2014 Revised Date:

24 October 2014

Accepted Date: 7 November 2014

Please cite this article as: Diaz, G.J., Speranza, F., Faccena, C., Bayona, G., Mora, A., Magnetic stratigraphy of the Bucaramanga alluvial Fan: Evidence for a ≤ 3 mm/yr slip rate for the BucaramangaSanta Marta Fault, Colombia, Journal of South American Earth Sciences (2014), doi: 10.1016/ j.jsames.2014.11.001. This is a PDF file of an unedited manuscript that has been accepted for publication. As a service to our customers we are providing this early version of the manuscript. The manuscript will undergo copyediting, typesetting, and review of the resulting proof before it is published in its final form. Please note that during the production process errors may be discovered which could affect the content, and all legal disclaimers that apply to the journal pertain.

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Magnetic stratigraphy of the Bucaramanga alluvial Fan: Evidence for a ≤ 3

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mm/yr slip rate for the Bucaramanga-Santa Marta Fault, Colombia

3 Giovanny Jiménez Diaz 1, 2, Fabio Speranza 2, Claudio Faccena 1, German

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Bayona 3, Andres Mora 4

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6 1 Università di Roma TRE, Roma, Italy

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2 Istituto Nazionale di Geofisica e Vulcanologia, Roma, Italy

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3 Corporación Geológica ARES, Bogota, Colombia

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4 Instituto Colombiano del Petróleo, Ecopetrol-ICP, Bucaramanga, Colombia

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Abstract

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29 The 550 km long Bucaramanga-Santa Marta Fault is one of the main active tectonic

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features of NW South America. It is a left-lateral strike-slip fault bounding the

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Maracaibo block, and straddling northern Colombia from the Caribbean Sea to the

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Eastern Cordillera. Variable total displacement values (from 40 to 110 km), and

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present-day slip rates (from 0.01 to 10 mm/yr) have been proposed so far for the

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Bucaramanga Fault. Here we report on the paleomagnetic investigation of a Plio-

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Pleistocene (?) continental alluvial fan juxtaposed to the Bucaramanga Fault, and

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horizontally displaced by 2.5 km with respect to its feeding river. Nine (out of

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fourteen) reliable paleomagnetic directions define a succession of six different

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magnetic polarity zones that, lacking additional age constraints, can be correlated

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with several tracks of the Plio-Pleistocene magnetic polarity time scale. If the

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youngest age model is considered, most recent sediments of the fan can be

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reasonably dated at 0.8 Ma (Brunhes-Matuyama chron transition), translating into a

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maximum 3 mm/yr slip rate for the Bucaramanga Fault. Older age models would

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obviously yield smaller slip rates. Our paleomagnetic sites, located at 4-10 km from the fault, do not show significant rotations, implying weak fault coupling and/or ductile upper crust behavior adjacent to the Bucaramanga Fault.

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Keywords: Paleomagnetism, Bucaramanga Fan, Bucaramanga Fault, Slip rate.

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Introduction

52 The NW margin of South America is characterized by a complex pattern of

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mountain ranges (Western, Central, and Eastern Cordillera of Colombia, Fig. 1),

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and by a puzzle of crustal blocks undergoing independent movements (Kellogg et

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al., 1982; Taboada et al., 2000; Trenkamp et al., 2002). The eastward subduction of

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the Nazca Plate beneath South America at a rate of 6 cm/yr is well documented

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(Trenkamp et al., 2002), while the existence of an ESE-ward directed subduction of

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the Caribbean plate is debated (Pindell et al., 1988). A well-developed accretionary

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wedge (Fig. 1) is exposed at the boundary between the Caribbean and South

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American plate (e.g., Flinch et al., 2003).

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The Maracaibo block, the biggest semi-rigid block of the Colombian tectonic

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puzzle, is bounded by three major wrench faults: the dextral Boconó and Oca

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faults, and the sinistral Bucaramanga-Santa Marta Fault (Fig. 1). The relevance,

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age, and displacement rate of these major strike-slip faults have been widely

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discussed in the past (Irving, 1971; Toro, 1990; Ujueta, 2003; Mora and Garcia,

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2006; Lopez et al., 2008), and a consensus on the whole block and fault kinematics

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has not been reached so far.

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1), where it crosses the city of Bucaramanga (ca. 500,000 inhabitants). It can be

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divided along strike into three major zones (Northern, Central and Southern zone),

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where it bounds several distinct geological provinces. The Northern zone, or Santa

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Marta section (Paris, 2000; Ingeominas, 2001a), corresponds to a 140 km long

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The Bucaramanga-Santa Marta Fault system juxtaposes basement rocks to the east and sedimentary Jurassic to Cenozoic rocks to the west. This fault system extends for a distance of 550 km from the Caribbean coast to the Eastern Cordillera (Fig.

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topographic lineament juxtaposing old crystalline rocks of the Santa Marta Massif

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to Neogene deposits of the Lower Magdalena Valley basin (Fig. 1). The 100 km

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long Central zone is covered by alluvial deposits of the Lower Magdalena Valley

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basin (Ariguani graben) and Cesar Valley basin (Mora and García, 2006; Fig.1).

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The Southern zone corresponds to Bucaramanga section (Paris, 2000; Ingeominas,

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2001a), a 310 km long outstanding linear topographic feature separating the

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Santander Massif from the Middle Magdalena Valley basin (Fig. 1). At the city of

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Bucaramanga, the fault clearly left-laterally displaces a 10-15 km wide continental

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alluvial fan of presumable Plio-Pleistocene age, produced by debris carried by the

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Suralá river from the adjacent Santander Massif (Fig. 2). The zone is well known

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for the high seismic activity of the “Bucaramanga nest” (Taboada et al, 2000; Zarifi

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et al, 2007; Fig. 3), but earthquakes are deep (from 100 to 200 km), thus they

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should not be related to the activity of the Bucaramanga Fault.

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In this paper we report on a paleomagnetic investigation of the Bucaramanga Fan to

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constrain its age by magnetic stratigraphy, one of the few viable method to

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dategravel-size alluvial fan deposits. The results allow the documentation of when

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fan displacement occurred, and unravel recent and present-day slip rate of the

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Bucaramanga Fault. The city of Bucaramanga has not been struck by devastating

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Bucaramanga Fault, as GPS data of Trenkamp et al. (2002) might suggest (Fig. 1).

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earthquakes since when historical accounts are available (XVII century AD), thus it is unclear whether we are living an inter-seismic interval preceding a future strong earthquake, or in fact there is no significant present-day activity of the

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Characteristics of the Bucaramanga-Santa Marta Fault

102 Previous work around the City of Bucaramanga has been done in the frame of

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regional and local cartography projects (Ward et al., 1973; Ingeominas, 2001b;

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Diedrix et al., 2009; Fig. 2). In the Santander Massif, which is bounded to the west

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by the Bucaramanga Fault system, Precambrian, Paleozoic, and Mesozoic intrusive

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and metamorphic rocks (schists and gneisses) are exposed. According to Cediel et

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al. (2003), the Bucaramanga-Santa Marta Fault was active during the Precambrian

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Grenville - Orinoco continental collision, and reactivated in the Aptian-Albian

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times. The Bucaramanga Fault bounds a thick deposition of upper Jurassic and

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Cretaceous rocks to the south and west (Kammer and Sanchez, 2006), whereas to

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the north and east the deposition of Jurassic rocks is more condensed and in some

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areas lowermost Cretaceous strata are lacking (Ward et al, 1973).

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Provenance analysis indicates that the Santander Massif and its sedimentary cover

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were uplifted since Paleogene time (Ayala et al, 2012). Paleocene movements may

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be related to other structures in the Cobardes Anticline (Parra et al, 2012, Fig. 1).

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Mora and García (2006) using extensive seismic profile analysis and well data in

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the Central zone, proposed that the Bucaramanga-Santa Marta Fault was

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activity ended after Oligocene, as the Lower Magdalena Valley and Cesar basins

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have been connected without tectonic disturbances.

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responsible for the intense structural deformation that affected pre-Oligocene units, indicating that it was an active boundary between the Lower Magdalena Valley and Cesar basins during the late Eocene-early Oligocene. They also suggested that fault

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Ross et al. (2009) using Apatite fission track analysis (AFTA) of Precambrian to

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Neogene rocks from the Santander Massif and Middle Magdalena Valley proposed

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three paleothermal episodes (interpreted as erosional phases) in the Paleocene (65

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to 60 Ma), Early Miocene (20 to 18 Ma) and Middle Miocene (12 to 9 Ma). This

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evidence provides age clues for the uplift of the Santander Massif with respect to

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the adjacent Magdalena Valley that likely occurred along the Bucaramanga Fault.

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As the Bucaramanga Fault is a recent geomorphological feature, it was likely

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activated in the last phase of deformation of late Miocene age, as suggested by

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AFTA data. Finally, Pindell et al. (1988) proposed that the Bucaramanga – Santa

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Marta fault is the western limit of the Maracaibo Block since Miocene times.

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Reported total displacement values of the Bucaramanga – Santa Marta fault vary

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from 45 to 110 km. Toro (1990) using structural reconstructions proposed for the

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southern fault portion a displacement of 45 km. According to Campbell (1968), the

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total displacement is more than 100 km, relying on a regional scale correlation

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between rocks from the Central Cordillera and the Santa Marta Massif. Other

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authors (Irving, 1971; Tschantz, 1974) proposed 110 km of displacement after the

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analysis of samples drilled in oil wells. Montes et al. (2010) and Bayona et al.

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(2010) considered the Bucaramanga-Santa Marta Fault system as western boundary

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evaluated after regional geology considerations (Rivera, 1989).

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of the Maracaibo block clockwise rotation during the Cenozoic. Reported values for the fault slip rate range between 0.01-0.2 mm/yr, calculated on the basis of geomorphic offset features (Paris, 2000; Ingeominas, 2001a), to 10 mm/yr,

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López et al., (2008) reported the occurrence of Pseudotachylite associated to

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cataclasites in the southern sector of the Bucaramanga Fault, that they interpreted

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as an evidence for paleoseismicity along the fault. Diedrix et al. (2009) using

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paleoseismological investigation and radiocarbon dating of paleosols trenched

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adjacent to the fault proposed eight Holocene seismic events during the last 8300

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years and magnitudes in the order of 6.5-7.0, associated to the Bucaramanga Fault

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activity.

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Ujueta (2003) made an extensive review of the previous works on the Bucaramanga

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Santa Marta Fault available since 1933, and observed that some authors consider

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the Bucaramanga Santa Marta fault as a reverse fault, others as left lateral strike-

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slip fault, while few works propose two different and independent faults.

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Concerning the age of the Bucaramanga Fault activity, a late Mesozoic, Paleocene,

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Eocene or Pliocene-Quaternary age are proposed (Ujueta, 2003). Finally, using

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seismic profiles, he discussed the continuity of the fault Central zone, and proposed

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two different but related faults, with absence of connection between the southern

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and the northern zone.

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The deep seismicity of the Bucaramanga Nest

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No significant shallow crustal seismicity has been recorded along the Santa Marta-

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nests by its high rate of activity in a volume much smaller than the other nests at

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similar intermediate depths (Schneider et al., 1987; Zarifi and Harsco, 2003; Prieto

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et al., 2012). The Bucaramanga nest has been mostly related to tectonic processes

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occurring in the oceanic subducting plates beneath Colombia (Zarifi and Havskov,

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Bucaramanga Fault (Fig. 3), but at depth a remarkable cluster of subcrustal earthquakes in the 100-200 km depth interval is observed in the so-called “Bucaramanga nest”, centered at 7°N 73°W (Fig 3). It differs from other worldwide

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2003). Taboada et al. (2000) proposed that the Bucaramanga Nest is due to the

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interaction between the subducting Nazca and paleo-Caribbean plates, while Zarifi

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et al. (2007) suggested a simultaneous subduction process and collision between

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two subducted slabs. Conversely, Cediel et al. (2003) proposed that the seismic

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activity recorded in the Bucaramanga Nest represents a zone of tectonic detachment

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associated with NW-ward migration of the Maracaibo subplate, while Rivera

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(1989) proposed that there is a relationship between the Bucaramanga Fault and

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Nest.

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The Bucaramanga Fan

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The Bucaramanga Fan is limited to the east by the Santander Massif and the

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Bucaramanga Fault, and to the west by the Suárez Fault (Fig. 2). The Suárez Fault

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is a west-dipping reverse fault with sinistral displacement and Quaternary activity

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(Page, 1986; Paris et al., 2000; Ingeominas, 2001a) that terminates northward

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against the Bucaramanga Fault. In the study area, the Suárez Fault juxtaposes

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Jurassic and Cretaceous strata against the Bucaramanga Fan. Locally, the

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Bucaramanga Fan is folded with vertical to overturned beds by the effect of the

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De Porta (1959) defined the Bucaramanga Fan as a sedimentary deposit of

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Quaternary age with an alluvial fan morphological shape (Fig. 2).

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According to Julivert (1958) The E-W creeks and the shape of the Bucaramanga

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Fan can be related, but the present-day drainage network can't explain the

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Suárez Fault (Ingeominas, 2008).

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Bucaramanga Fan location. Ingeominas (2001b and 2008) suggested that the Suratá

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River is the feeder of the Bucaramanga Fan, although it is presently shifted by 2.5

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km with respect to fan apex. According to Ingeominas (2008) the southern part of

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the Bucaramanga Fan has been more faulted than the northern part, and seems to be

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diachronous. Thus the progressive northward migration of the fan apex has been

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related to the sinistral shear along the Bucaramanga Fault.

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According to Ingeominas (2001b) the thickness of the Bucaramanga Fan increases

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from east to west with an average thickness of 250 m, and from base to the top it

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has been subdivided into, the Organos, Finos, Gravoso, and Limos Rojos member

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(Fig. 2).

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The Organos Member was first defined by Hubach (1952), and according to Bueno

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and Solarte (1994) is a monotonous sequence of conglomerates with intercalations

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of fine sandstones. Conglomerate clasts are 10 - 30 cm in diameter (and in some

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cases more than 1 m) and include gneisses and schists fragments. This member is

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clast supported, contains a clay matrix (Ingeominas, 2001b), and crops out to the

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west of the study area with a maximum thickness of 180 m (Mancera and

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Salamanca, 1994). The Finos Member (Hubach, 1952) is a continuous sub-

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m thick, matrix supported level of gravel-size clasts overlying the Finos Member

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along a net contact. The clasts are on average 15 cm in diameter (cobble size), and

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the matrix includes a mixture of clay- and sand-size fragments. Finally, the

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Gravoso Member transitionally passes upward into the 15 m thick Limos Rojos

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horizontal 15 m thick bed overlying the Organos member along a net discontinuity, and it consists of clays evolving upsection into fine-grained sandstone beds (Ingeominas, 2001b). The Gravoso Member (Vargas and Niño, 1992) is an 8 to 30

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Member (Julivert, 1963); this unit consists of argillaceous sandstones and

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conglomeratic sandstones, interbeded with layers of siltstones. Locally, block

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fragments (meter scale in diameter) of sandstone texture are supported by the red

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silty matrix (Ingeominas, 2001b).

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The Bucaramanga Fan is generally referred to a Plio-Pleistocene age (Ingeominas,

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2001b), although no conclusive age constraints were gathered from the continental

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succession so far.

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Sampling and Methods

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We collected sandy-silty samples for paleomagnetic analysis in fourteen sites (154

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cores, Table 1) from the Bucaramanga Fan, using a petrol-powered portable drill

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cooled by water. Ten sites were gathered in the Organos Member, two in the Finos

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Member, and two in the Gravoso Member (Figure 2 and Table 1). At each site we

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collected 6–12 cores (11 on average), spaced in at least two outcrops in order to try

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to average out secular variation of the geomagnetic field. All samples were oriented

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Cores were prepared into standard cylindrical specimens of 22 mm height, and

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rock magnetic and paleomagnetic measurements were done in the shielded room of

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the paleomagnetic laboratory of the Istituto Nazionale di Geofisica e Vulcanologia

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(Roma, Italy). All samples were thermally demagnetized through 11–12 steps up to

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using a magnetic compass, corrected to account for the local magnetic field declination value at the sampling area (about 7º W) according to NOAA’s National Geophysical Data Center (http://www.ngdc.noaa.gov).

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680°C by a shielded oven, and the natural remanent magnetization (NRM) of the

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specimens was measured after each step with a DC- SQUID cryogenic

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magnetometer (2G Enterprises, USA). Thermal demagnetization data were plotted

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on orthogonal diagrams (Zijderveld, 1967), and the magnetization components

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were isolated by principal component analysis (Kirschvink, 1980). The site-mean

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directions were evaluated by Fisher’s (1953) statistics.

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On a set of selected specimens, magnetic mineralogy analyses were carried out to

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identify and characterize the main magnetic carriers using the thermal

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demagnetization of a three-component isothermal remanent magnetization (IRM)

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imparted on the specimen axes, according to the method of Lowrie (1990). Fields

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of 2.7, 0.6, and 0.12 T were successively imparted on the z, y, and x sample axes

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(respectively) with a pulse magnetizer (Model 660, 2G Enterprises). The

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generalized stratigraphic column of the Bucaramanga Fan was made using field

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data and previous geological maps (Ingeominas, 2001b). The stratigraphic position

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for all sampled sites was calculated using a cross section.

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Results

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samples both the medium coercivity and the hard fractions are demagnetized

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between 600 and 680°C (Fig. 4), pointing to hematite as the main magnetic carrier

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of our samples. In almost all sites, a drop of the medium coercivity and hard

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fraction occurring before 100º shows that a small amount of goethite is also

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Magnetic Mineralogy

The thermal demagnetization of a three-component IRM shows that for most of the

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associated to hematite.

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Paleomagnetism

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cleaning, while the remaining 5 sites showed scattered demagnetization diagrams

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(Figure 5 and Table 1). For most of the sites, a characteristic magnetization

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component (ChRM) was isolated between 550 and 680°C, confirming that hematite

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represents the main magnetic carrier. For about 10% of the samples, a ChRM is

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isolated between 380 and 680°C, suggesting the coexistence of hematite and

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maghaemite (Fig. 5). Mean paleomagnetic directions are reasonably well

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constrained, the α95 values being comprised between 8.4° and 22.4° for all sites but

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one yielding a value of 48.2 (Fig. 6 and Table 1). Three sites are of normal polarity

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(D = 356.1, I = 9.4, K = 136.76 and α95 = 10.6 ) and the other six are of reverse

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polarity (D = 178.2, I =1.8, K = 36.20, and α95 = 11.3 ); the reversal test (according

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to McFadden and McElhinny (1990), is positive of Class “c”.

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The fact that our results yielded reverse polarity directions indicate that the

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Bucaramanga Fan should be older than the Bruhnhes polarity chron (0 to 0.8 Ma)

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direction, except the youngest magnetozone R3, which is corroborated by four

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different site results. As the age of the Bucaramanga Fan is vaguely inferred to be

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Plio-Pleistocene, several different correlations with the global magnetic polarity

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time scale (GPTS, Cande and Kent, 1995) are possible (Fig. 8). If we assign the

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When plotted according to their stratigraphic position, the sites from the Bucaramanga Fan yield a succession of three normal- and three reverse-polarity magnetozones (Fig. 7). Each magnetozone is defined by one paleomagnetic

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youngest possible age to the succession (Fig. 8a), R3 correlates with upper

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Matuyama polarity chron (C1r.1r), and N3, N2, and N1 with the Jaramillo,

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Olduvai, and Gauss chron, respectively. In a slightly older age model (Fig. 8b), R3

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correlates with the mid Matuyama chron (C1r.2r), N3 with Olduvai chron, and N2

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and N1 fall both within the Gauss chron. It is not possible at present to indicate a

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preferred age model using calculated sedimentation rates that vary irregularly

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(considering both age models of Figure 8) between 30 and 300 mm/kyr. In fact in

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this kind of deposits the sedimentation is expected to be highly irregular and

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discontinuous, and the thickness of some magnetozones (such as N3) is poorly

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constrained due to the occurrence of several failed sites located below and above it

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(Fig. 7).

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Discussion and Conclusions

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The slip rate of the southern segment of the Bucaramanga Fault can be in principle

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calculated by dividing its along-fault displacement by the age of the displaced

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rocks. Left-lateral displacement is well known, and equates the 2.5 km distance

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magnetozone succession gathered from the Bucaramanga Fan (Fig. 7).

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from the mouth of the Suralá river to the apex of the Bucaramanga Fan (Ingeominas 2008, Figs. 9 and 10). Conversely, the age of the displaced sediments is not firmly constrained, as several different age models can equally fit the

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However, a maximum possible slip rate can be calculated assigning the youngest

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possible age of the succession, i.e. inferring that magnetozone R3 corresponds to

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the top of the Matuyama polarity chron (Fig. 8a). In this case, a 0.8 Ma age

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(Brunhes-Matuyama boundary, Cande and Kent, 1995) can be reasonably assigned

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to the youngest sediments of the Bucaramanga Fan, by considering that: 1) we did

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not reach the normal-polarity magnetozone above R3, thus the youngest sampled

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sediments (site GJ192) might fall in the lower-medium part of chron C1r.1r, and be

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0.9-1 Ma old; 2) the upper member of the Bucaramanga Fan is the Limos Rojos

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Member, but the youngest paleomagnetic directions were obtained in the

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underlying Gravoso Member; 3) the Limos Rojos Member is only 15 m thick, and

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shares the same fan morphology with the underlying Finos-Gravoso members (Fig.

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2). This suggests that the Limos Rojos Member was rapidly emplaced, and that no

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significant time gap (and displacement of the fan feeding source) occurred with

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respect to the Gravoso Member.

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A 0.8 Ma age of the top of the Bucaramanga Fan translates into a maximum slip

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rate of 3 mm/yr for the Bucaramanga Fault. Obviously, progressively smaller slip

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rates would arise by considering progressively older age models for the

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Bucaramanga Fan. Our slip rate estimate is in rough agreement with conclusions by

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Diedrix et al. (2009), who documented by paleosismology eight main earthquakes

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in the last 8300 years, with 400 to 1300 years recurrence intervals, and estimated

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seismogenic fault is expected to be associated with 7-7.5 M earthquakes (Wells and

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Coppersmith, 1994), slightly greater than Diederix et al. (2009) estimates. We note

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however that older age models for the Bucaramanga Fan would give smaller slip

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rates, thus better agreement with Diederix et al. (2009) calculated values.

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magnitude values of 6.5 to 7.0. Average recurrence interval documented by Diedrix et al. (2009) is 1000 years, which would translate into an accumulated displacement of 3 m, if our 3 mm/yr spreading rate is considered. A 3 m displacement along a

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Considering that the city of Bucaramanga has a documented history of 390 years

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without any catastrophic earthquake occurrence, a 1.2 m displacement could have

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been accumulated since then, if the 3 mm/yr slip rate is considered.

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Sediments of the Bucaramanga Fan have been clearly displaced by left-lateral fault

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shear, thus counterclockwise rotations are expected at fault walls, as already

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observed in several strike-slip fault settings (Sonder et al., 1994; Kimura et al.,

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2011). On the other hand, our sites from the Bucaramanga Fan, located at 4-10 km

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from the fault, do not show significant rotations (Fig. 6).

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Using the power law rheology model (England et al., 1985), in which the relation

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between distance from a fault trace y (km) and vertical-axis relative rotation θ

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(rad.) is expressed as:

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θ=arctan (((4Dsπ √n)/L) exp((−4π √ny)L))

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Ds (km) is the displacement in one side of the fault, L/2 (km) is the length of the

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fault, and n is the stress exponent and describes the average mechanical behavior of

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the lithosphere (Sonder and England, 1986). Clearly, the lack of observed rotations

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may imply that 1) fault locking is extremely weak, whereas fault walls are

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understand this issue, and better constrain the seismic hazard assessment related to

373

the Bucaramanga Fault activity.

369 370

374 375

extremely rigid and undergo minimal internal deformation, and/or 2) the upper crust west of the Bucaramanga Fault has a ductile behavior. Additional geophysical data (e.g. a high-resolution GPS network across fault zone) are needed to fully

16

ACCEPTED MANUSCRIPT 376 377 378

Acknowledgements: Many thanks to Ecopetrol-ICP and the project: “Cronologia de

380

la deformación en las cuencas Subandinas” for funding and supporting the field

381

work. Danilo Seccia (INGV) helped to realize Figure 3. GB acknowledges

382

Colciencias for continuing support ARES. Thanks to Omar Montenegro for

383

logistical and field work. We are grateful to two anonymous referees and to JSAES

384

Editor James Kellogg for providing careful reviews of our work.

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References

387 Ayala-Calvo, C., G. Bayona, A. Cardona, C. Ojeda, O. Montenegro, C. Montes, V.

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Cande, S.C. and D.V. Kent (1995), Revised calibration of the geomagnetic polarity

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Kammer, A., and J. Sanchez (2006), Early Jurassic rift structures associated with

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the Soapaga and Boyacá faults of the Eastern Cordillera, Colombia:

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446

Kellogg. J. N. and W. E. Bonini (1982), Subduction of the Caribbean Plate and

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498

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501

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Sonder. L, J. Jones, C.H. Salyards, S.L and K. M. Murphy (1994), Vertical axis rotation in the Las Vegas Valley shear zone, southern Nevada: paleomagnetic

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512

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516

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523

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525

Vargas, A., G and A. Niño (1992), Patrones de fracturamiento asociados a la Falla

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Bucaramanga. Tesis, Universidad Industrial de Santander, Bucaramanga. Ward, D., Goldsmith, R., Cruz, J., and H. Restrepo (1973), Geología de los

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Cuadrángulos H-12, Bucaramanga y H-13, Pamplona, Departamento de

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Santander, Boletín Geológico Ingeominas 21(1-3), 132 p.

530 531 532

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Wells, D.L and K. J. Coppersmith (1994), New Empirical Relationships among Magnitude, Rupture Length, Rupture Width, Rupture Area, and Surface Displacement. Bulletin of the Seismological Society of America, Vol. 84, No. 4, pp. 974-1002

533

Zijderveld, J. D. A. (1967), A.C. demagnetization of rocks: Analysis of results, in

534

Methods in Palaeomagnetism, edited by D. W. Collinson, K. M. Creer, and S. K.

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Runcorn, pp. 254–286, Elsevier, New York.

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Zarifi, Z., and J. Havskov (2003), Characteristics of dense nests of deep and intermediate-depth seismicity. Adv. Geophys. 46, 237–278. Zarifi, Z., J. Havskov and A. Hanyga (2007), An insight into the Bucaramanga nest Tectonophysics 443, 93–10.

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Figure captions

542 Figure 1. Major tectonic and structural features of the NW margin of South

544

America. Plate velocity vectors with respect to stable South America are from

545

Trenkamp et al. (2002). WC = Western Cordillera, CC = Central Cordillera, EC =

546

Eastern Cordillera, SMF = Santa marta Fault, BF = Bucaramanga Fault.

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547

Figure 2. Geological map of the Bucaramanga Fan (scale 1:25,000, modified from

549

Ingeominas, 2001b) and location of the 14 paleomagnetic sites. See Figure 1 for

550

location.

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Figure 3. Seismicity in NW South American Plate recorded during 2006-2009 by

553

the Red Sismica Nacional de Colombia (RSNC)-Ingeominas.

554

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Figure 4. Thermal demagnetization of a three-component IRM according to the

556

method of Lowrie (1990) for six representative specimens.

557

Figure 5. Orthogonal vector diagrams of typical demagnetization data, in situ

561

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558

EP

555

562

Figure 6. Equal-area projections of the site-mean paleomagnetic directions from the

563

study area. Solid (open) symbols represent projection onto the lower (upper)

564

hemisphere. Open ellipses are the projections of the α95 cones about the mean

565

directions. The star represents the normal polarity geocentric axial dipole (GAD)

559 560

coordinates. Solid and open dots represent projections on the horizontal and vertical planes, respectively. Demagnetization step values are in °C.

25

ACCEPTED MANUSCRIPT 566

field direction (D=0°, I=14°) calculated for the Bucaramanga latitude (7.1° N).

567 Figure 7. Stratigraphic column of the Bucaramanga Fan, and stratigraphic variation

569

of magnetic polarity zones. Magnetic polarity zones are progressively numbered

570

from the section bottom. Uncertain polarity intervals are grey and cross-hatched.

571

The crosses indicate failed sites.

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Figure 8. Stratigraphic distance versus age correlation plots. Magnetic polarity

574

zones are correlated to polarity chrons from the GPTS (Cande and Kent, 1995).

575

Sloping lines are average sediment accumulation rates. Two different possible

576

correlations are shown (see text for explanation).

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577 578

Figure 9. (a) Geomorphological context in the study area, where the Suárez and

579

Bucaramanga faults are located.

580

Bucaramanga Fan apex and the Suratá River. (b) Elevation contours around the

581

area. Three zones are well defined (from E to W), the eastern wall of the

582

Bucaramanga Fault with high topographic expression, the Bucaramanga Fan, and

583

the hanging wall of the Suárez Fault. Finally, three topographic profiles across the

585 586

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EP

AC C

584

A distance of 2.5 km occurs between the

Suratá River, the apex and Bucaramanga Fan are shown. BF = Bucaramanga Fault, SF = Suárez Fault.

587

Figure 10. Scheme showing the displacement of the Bucaramanga Fan apex from its

588

feeding Suratá River along the Bucaramanga Fault.

589

Table 1. Paleomagnetic results

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N/n 10/8 11/6 12/0 12/0 11/9 6/0 12/5 12/0 11/0 12/12 11/8 12/8 12/8 11/5

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Finos Finos Gravoso Organos Organos Organos Gravoso Organos Organos Organos Organos Organos Organos Organos

Geographic coordinates Longitude ºW Latitude ºN 73.132033 7.075063 73.132031 7.075061 73.143939 7.075496 73.168091 7.036684 73.174056 7.049284 73.138192 7.067906 73.132332 7.097189 73.133936 7.090153 73.138862 7.087891 73.138862 7.087891 73.162533 7.088209 73.161192 7.101659 73.165264 7.100704 73.148797 7.066336

EP

Member

AC C

Site GJ186 GJ187 GJ188 GJ189 GJ190 GJ191 GJ192 GJ193 GJ194 GJ195 GJ196 GJ197 GJ198 GJ199

SC

Table 1 Paleomagnetic results from Bucaramanga Fan

D (º) 179.0 176.4 353.5 176.7 188.1 181.5 357.9 356.9 167.9

In Situ I (º) 13.4 9.0 4.0

k 7.75 14.9 9.14

9.2 -19.0 -0.6 7.6 16.7 -1.3

12.61 12.79 11.63 44.45 13.37 3.47

α95 (º) 21.2 17.9 18.0 22.4 12.6 18.5 8.4 15.7 48.2

The geographic coordinates are referred to WGS84 datum. Bedding is sub-horizontal. D and I are in situ declination and inclination; K and α95 are statistical parameters after Fisher (1953).

73º ACCEPTED MANUSCRIPT

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Cretaceous

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Finos and Gravoso Member

Fault Covered Fault or lineament

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Paleomagnetic sites

Figure 2

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79º W

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Figure 5

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Geocentric axial dipole field direction expected at Bucaramanga (Lat 7.13º N) Mean paleomagnetic direction (D = 357.5 I = 2.0 K = 41.63 a 95 = 8.1)

Figure 6

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SYSTEM Stages

0 P LI OC E NE E ar l y Pl i oc e n e Middle Pliocene Za nc l e an

G A U S S

Gelasian

Santern. Emilian Sicilian 1

G I L B E R T

Late Pliocene

P LE I S TOC E N E Early Pleistocene M. Pleistocene

2

BRUNHES

POLARITY CHRONS

Piacenzian 3

Ma

5

M A T U Y A M A

R3

4

1

G A U S S

Santern. Emilian Sicilian

2

3

4

5

G I L B E R T

Gelasian

P LE I S TOC E N E Early Pleistocene M. Pleistocene

60

186 187

M A T U Y A M A

POLARITY CHRONS POLARITY

Jaramillo

Olduvai

Kaena

Mammoth

Cochiti

Nunivak

Sidufjall

Thvera

Jaramillo

Olduvai

Kaena

Mammoth

Cochiti

Nunivak

Sidufjall

Thvera

Figure 8

Polarity Subchrons

Stages

Ma BRUNHES

POLARITY

SYSTEM

Chrono

P LI OC E NE E ar l y Pl i oc e n e Middle Pliocene

80

188 192

40

Chrono

0

Organos Member

80

M AN U

100

180

140

N3

TE D

120

190

200

160

195 191

EP

140

R3

220

SC

180

186 187

160

Organos Member

Limos Rojos Member

188 192

Finos Member

200

Gravoso Member

220

AC C

Finos Member

Gravoso Member

Limos Rojos Member

A

Polarity Subchrons

ACCEPTED MANUSCRIPT

(b)

(a) 73º 9' W

73º 5' W

73º 1' W

RI PT

7º 10' N

2.5 km

C

A` B`

M AN U

SC

7º 8' N

A

AC C

EP

TE D

7º 6' N

Reverse fault Strike-slip fault

B C`

7º 4' N

A 950 m 850 m 750 m 650 m

1050 m

BF

SF B

950 m 850 m 750 m 650 m 1050 m 950 m 850 m 750 m 650 m

Figure 9

A’

1050 m

Apex

B’

BF C

C’

r ve

at

á

Ri

ACCEPTED MANUSCRIPT

Su r

Stage A

Su r

at

TE D

á

Ri

Stage B

M AN U

ve r

SC

D

RI PT

Bucaramanga Fault

D

AC C

EP

2.5 Km

Figure 10

Bucaramanga Fault

ACCEPTED MANUSCRIPT Highlights

Paleomagnetic investigation of a Plio-Pleistocene (?) continental alluvial fan juxtaposed to the Bucaramanga Fault, and horizontally displaced by 2.5 km with respect to its feeding river. Nine reliable paleomagnetic directions define a succession

RI PT

of magnetic polarity zones, correlated with several tracks of the Plio-Pleistocene magnetic polarity time scale. If the youngest age model is considered, most recent sediments of the Bucaramanga Fan can be reasonably dated at 0.8 Ma (BrunhesMatuyama chron transition), translating into a maximum 3 mm/yr slip rate for the

AC C

EP

TE D

M AN U

SC

Bucaramanga Fault.