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1 Revision 1 1 Temporal histories of Cordilleran continental arcs: testing models for 2 magmatic episodicity 3 Moritz Kirsch 1 *, Scott R. Paterson 2 , Florian Wobbe 3 , Ana María Martínez 4 Ardila 4 , Benjamin L. Clausen 4 , and Pablo H. Alasino 5 5 1 Institut für Geologie, Technische Universität Bergakademie Freiberg, Bernhard-von- 6 Cotta-Strasse 2, 09599 Freiberg, Germany 7 2 Department of Earth Sciences, University of Southern California, Los Angeles, CA 8 90089-0740, U.S.A. 9 3 Alfred Wegener Institute, Am Alten Hafen 26, 27568 Bremerhaven, Germany 10 4 Department of Earth and Biological Sciences, Loma Linda University, Griggs Hall, 11 11065 Campus Street, Loma Linda, California 92350, U.S.A 12 5 CRILAR-CONICET, Entre Ríos y Mendoza, Anillaco 5301, La Rioja, Argentina 13 14 * Corresponding author; Phone: +49 (0)3731 1680105; Email: [email protected] 15 freiberg.de 16 Abstract 17 Magmatic activity in continental arcs is known to vary in a non-steady state 18 manner, with the mechanisms driving magmatic activity being a matter of ongoing 19 discussion. Of particular importance is the question of what extent episodic 20 magmatism in continental arcs is governed by external factors (e.g., plate motions) 21 and internal factors (e.g., feedback processes in the upper plate). In order to test 22 existing models for magmatic episodicity, which are mostly based on temporally 23 and spatially limited records, this study uses large datasets of geochronological, 24 geochemical, and plate kinematic data to document the Paleozoic to Mesozoic 25

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Revision 1 1 Temporal histories of Cordilleran continental arcs: testing models for 2 magmatic episodicity 3 Moritz Kirsch1*, Scott R. Paterson2, Florian Wobbe3, Ana María Martínez 4 Ardila4, Benjamin L. Clausen4, and Pablo H. Alasino5 5 1 Institut für Geologie, Technische Universität Bergakademie Freiberg, Bernhard-von-6 Cotta-Strasse 2, 09599 Freiberg, Germany 7 2 Department of Earth Sciences, University of Southern California, Los Angeles, CA 8 90089-0740, U.S.A. 9 3 Alfred Wegener Institute, Am Alten Hafen 26, 27568 Bremerhaven, Germany 10 4 Department of Earth and Biological Sciences, Loma Linda University, Griggs Hall, 11 11065 Campus Street, Loma Linda, California 92350, U.S.A 12 5 CRILAR-CONICET, Entre Ríos y Mendoza, Anillaco 5301, La Rioja, Argentina 13 14 * Corresponding author; Phone: +49 (0)3731 1680105; Email: [email protected] freiberg.de 16

Abstract 17 Magmatic activity in continental arcs is known to vary in a non-steady state 18 manner, with the mechanisms driving magmatic activity being a matter of ongoing 19 discussion. Of particular importance is the question of what extent episodic 20 magmatism in continental arcs is governed by external factors (e.g., plate motions) 21 and internal factors (e.g., feedback processes in the upper plate). In order to test 22 existing models for magmatic episodicity, which are mostly based on temporally 23 and spatially limited records, this study uses large datasets of geochronological, 24 geochemical, and plate kinematic data to document the Paleozoic to Mesozoic 25

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development of the North and South American Cordilleras in eight transects from 26 British Columbia to Patagonia. The temporal distribution of U/Pb bedrock and 27 detrital zircon ages, used as a proxy for timing of magmatic accretion, shows that 28 some minima and maxima of zircon abundance are nearly synchronous for 29 thousands of km along the arc. Some age patterns are characterized by a periodicity 30 of 50–80 Ma, suggesting a cyclic controlling mechanism. Other magmatic lulls or 31 flare-ups find no equivalents in adjacent sectors, indicating that either discrete 32 events or variable lag times may also be important in governing magmatic activity 33 in continental arcs. Magma composition in Mexico, the Peninsular Ranges, and the 34 Sierra Nevada varies episodically and proportionally with the temporal record of 35 arc activity. During flare-up events, there is an increase in Sm/Yb, indicating 36 deeper melting, and a decrease in εNdi, suggesting a higher degree of crustal 37 assimilation. Geochemical scatter also increases during the initiation of flare-up 38 events. Plate kinematic data provide a means of evaluating mantle heat input. The 39 correlation between plate convergence rate and magmatic accretion varies for each 40 sector, suggesting that different flare-ups or lulls likely reflect variable 41 combinations of processes. 42

Keywords: magmatism, continental arc, Cordilleras, geochronology, geochemistry, plate 43 motions, Paleozoic, Mesozoic 44

Introduction 45 Convergent continental margins, where oceanic lithosphere is subducted beneath 46 continental lithosphere, are areas of intense magmatism, and important sites of crustal 47 growth (e.g., Crisp 1984; Rudnick 1995; Tatsumi 2005; Davidson and Arculus 2006). 48 Assessing crustal production rates and understanding the mechanisms controlling 49 magmatic addition in continental arcs are two issues that are of key importance in 50 tectonic studies (e.g., Ducea et al. 2015; Jicha and Jagoutz 2015). The Cordilleran 51 orogenic system of North and South America is particularly well suited for addressing 52 these aspects, as it features a spatially extensive (>15,000 km), nearly continuous 53

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mountain belt that is the expression of subduction of oceanic lithosphere beneath a 54 continental margin. Subduction-related activity in the American Cordilleras was initiated 55 in the Early Paleozoic along some parts of the arc (e.g., Bahlburg and Hervé 1997; 56 Ramos 2009) and is still on-going today, providing an exceptionally long continental 57 magmatic arc record. Based on the relative abundance of igneous rocks with known ages, 58 a non-steady state behavior of magmatic arc activity, characterized by periods of reduced 59 magmatism alternating with magmatic flare-ups, has been documented in several 60 Cordilleran arc segments. These include the Coastal Ranges, British Colombia (e.g., 61 Armstrong 1988; Ducea and Barton 2007; Gehrels et al. 2009), the Cascade Mountains, 62 Washington (Miller et al. 2009), the Sierra Nevada, California (Bateman and Shervais 63 1992; Ducea 2001; DeCelles et al. 2009; Paterson et al. 2014), the Transverse Ranges, 64 California (Barth et al. 1997; 2008), the Salinian arc (Kidder et al. 2003; Ducea et al. 65 2003; Chapman et al. 2014), the Peninsular Ranges Batholith (Premo et al. 2014), the 66 Sierra Madre Occidental and Trans-Mexican Volcanic Belt, Mexico (Ferrari et al. 1999), 67 and the central Andes (Haschke 2002; Haschke et al. 2006; Trumbull et al. 2006). 68 Existing models to explain the non-steady state magmatic activity of continental arcs 69 either invoke (i) external forcing by plate tectonic processes (Pilger 1984; Hughes and 70 Mahood 2008), (ii) intra-arc cyclic processes largely independent of plate motions (Kay 71 and Mahlburg Kay 1993; Ducea and Barton 2007; DeCelles et al. 2009; Lee et al. 2013) 72 or (iii) a crustal modulation of mantle energy input (de Silva and Gosnold 2007; de Silva 73 2008; de Silva et al. 2015). Most of these models are based on a temporally and spatially 74 limited record. In order to test the validity of the proposed models, large datasets are 75 needed. 76

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This paper uses an ever-growing database of U-Pb bedrock and detrital zircon age 77 data between 400 and 80 Ma for the American Cordilleras from British Colombia in the 78 north to Patagonia in the south as a means to evaluate the timing and relative strength of 79 continental arc magmatic activity. As the proposed mechanisms for magmatic arc activity 80 operate over distinct temporal and spatial scales, evaluating the scale of repeated age 81 patterns provides a means to test these proposals. Furthermore, by examining 15,000 km 82 of arc length, we are able to evaluate if the proposed mechanisms invoked for a small 83 segment of an arc are representative for entire arc systems, which exhibit variable 84 basement characteristics and subducting plate parameters. 85

A fundamental question concerns the role of external factors (e.g. plate motions 86 and mantle power) vs. internal factors (e.g. feedback processes in the upper plate) in 87 controlling continental arc magmatic activity. To assess the relative importance of these 88 respective factors, this study evaluates the spatial and temporal pattern of magmatic arc 89 activity as well as the relationship between magmatic accretion rate and (i) plate 90 kinematic parameters such as plate convergence rate that control magma production in 91 the mantle wedge (e.g., Cagnioncle et al. 2007), and (ii) arc magma composition, which 92 is primarily governed by processes during the transfer of magma from the mantle wedge 93 to the upper crust, i.e. it depends on thickness, composition, and state of stress of the 94 upper plate (e.g., Leeman 1983; Mantle and Collins 2008; Chiaradia 2015). 95

Geological setting 96 The North American Cordilleras and the Andes (henceforth collectively referred to as 97 "Cordilleras", "Cordilleran orogen", "Cordilleran arc", or "Cordilleran margin") extend 98 along the western edge of the North and South American continents, respectively, and 99

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together form a long (ca. 15,000 km), nearly continuous belt of magmatic arc 100 assemblages generated by the persistent convergence and interaction between lower 101 oceanic and upper continental plates (Dewey and Bird 1970; e.g., Dickinson 1970; 102 Armstrong 1974). Following the break-up of Rodinia, subduction along the North 103 American Cordilleran margin initiated in the Middle–Late Devonian (Burchfiel and 104 Davis 1972; 1975; Monger and Price 2002; Dickinson 2004; 2009), whereas the western 105 margin of South America preserves a record of almost continuous subduction since the 106 Cambrian, with the inception of the Terra Australis orogen (Rapela et al. 1998a; 1998b; 107 Pankhurst et al. 2000; Ramos and Aleman 2000; Cawood 2005; Chew et al. 2007; Collo 108 et al. 2009). Despite having formed under one geodynamic regime, the Cordilleran 109 orogen is segmented, i.e. features along-strike tectonic, structural, and morphological 110 variations (Sempere et al. 2008; Ramos 2009). For the sake of the analysis in this paper, 111 the Cordilleran margin is divided into eight sectors, from north (British Colombia) to 112 south (Patagonia): (1) the Coast Ranges, (2) the Sierra Nevada, (3) the Peninsular Ranges 113 to Mojave, (4) southeastern Mexico and Central America, (5) the northern Andes, (6) the 114 Peruvian Andes, (7) the south-central Andes, and (8) the southern Andes. In some cases, 115 the boundaries of these sectors coincide with the spatial limits of tectono-magmatic 116 provinces. In other cases the division is arbitrary and simply a matter of choosing sectors 117 large enough to incorporate a statistically meaningful amount of data, and small enough 118 to account for local differences in the geological evolution. In the following sections, the 119 tectonic and magmatic history of the individual Cordilleran arc sectors are briefly 120 summarized. Age compilations and analyses of arc processes presented in this paper are 121 limited to a timeframe between 400 and 80 Ma, hence these summaries focus on the late 122

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Paleozoic and early Mesozoic geological history, with particular emphasis on subduction 123 initiation and evolution. 124 Coast Ranges (55–43° N) 125 The most northern sector is defined as the region between 55 and 43° N and includes 126 magmatic activity in British Columbia, Washington, Oregon, Idaho, and Montana. The 127 pre-Cretaceous geological history of this region includes the accretion of several oceanic 128 arc terranes, such as the Stikinia, Quesnellia, Wrangellia and Triassic Chelan Mountains 129 terrane (Tabor et al. 1989; Miller et al. 1994; Matzel et al. 2004). Subsequent continental 130 arc magmatism in this region is preserved in the ca. 1500 km long Coast Plutonic 131 Complex (e.g., Monger et al. 1982; Tabor et al. 1989), which records continental 132 magmatic arc activity between ca. 170 and ca. 50 Ma with flare-ups at 160–140 Ma, 120–133 78 Ma, and 55–48 Ma (Gehrels et al. 2009). Magmatism was accompanied by crustal 134 extension until the mid-Cretaceous, when the accretion of the Alexander-Wrangellia 135 terrane to the western margin of Laurentia caused local contraction, crustal thickening 136 and thrusting (Gehrels et al. 2009). The Late Cretaceous to Early Tertiary marks a 137 transition to dextral transpressional tectonics in the Coast Mountains sector, attributed to 138 changing plate kinematics, which resulted in a dramatic reduction of magmatic 139 production (Gehrels et al. 2009). During the Late Cretaceous to Early Tertiary, arc 140 magmatism in the Coast Mountains Batholith migrated eastward. From ca. 50 Ma 141 onwards, the temporal and spatial evolution as well as the geochemical characteristics of 142 arc magmatism within the forearc areas from Alaska to Oregon are complex due to the 143 interaction of several spreading ridges and oceanic transforms with the subduction zone 144 (Haeussler et al. 2003; Madsen et al. 2006; du Bray and John 2011). 145

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Sierra Nevada (43–35° N) 146 The Sierra Nevada section of the Cordilleran magmatic arc is located in central and 147 eastern California and western Nevada, USA, between approximately 43° N and 35° N 148 (Barton et al. 1988; Bateman 1992; Van Buer et al. 2009; Van Buer and Miller 2010). 149 After the breakup of Rodinia in the Late Neoproterozoic, this part of the Cordilleran 150 margin remained passive until the middle to late Devonian, when an intraoceanic arc 151 complex formed in the eastern Klamath and northern Sierra terranes (Bradley 2008; 152 Dickinson 2009; Colpron and Nelson 2011). These subduction complexes subsequently 153 collided with the Pacific margin during the the Late Devonian to Early Mississippian 154 Antler orogeny, which involved thrusting the Roberts Mountains Allochthon onto 155 Neoproterozoic to Paleozoic miogeoclinal rocks (Schweickert and Cowan 1975; Stevens 156 and Greene 1999; Gehrels et al. 2000; Chapman et al. 2012). Late Devonian to Early 157 Carboniferous extensional tectonics that gave rise to a marginal ocean basin called the 158 Slide Mountain Ocean Basin (Davis et al. 1978; Nokleberg et al. 2000; Nelson et al. 2006; 159 Saleeby and Dunne 2015). This ocean basin closed in the Middle Permian as a 160 consequence of a subduction zone jump and polarity reversal, which led to the accretion 161 of additional fringing oceanic island arc complexes (e.g., the Golconda Allochthon) onto 162 the Laurentian platform during the Late Permian–Early Triassic Sonoma orogeny (Riley 163 et al. 2000; Dickinson 2009). The Early Triassic marks the inception of a continental 164 magmatic arc along the Sierran sector of the Cordilleran orogen (Barth and Wooden 2006; 165 Paterson et al. 2014). Continued subduction of Pacific lithosphere culminated in the 166 construction of the voluminous Sierra Nevada batholith, which records episodic 167 magmatic activity between ca. 250 and ca. 80 Ma with peaks occurring in Triassic (ca. 168

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230–210 Ma), Middle to Late Jurassic (ca. 180–160 Ma), and mid-Cretaceous (ca. 115–169 85 Ma) time (Stern et al. 1981; Ducea and Barton 2007; Ducea 2011; Paterson et al. 170 2014). Latest Cretaceous pluton crystallization ages become progressively younger 171 towards the east, which has been associated with gradual slab flattening (Chen and Moore 172 1982; Silver and Chappell 1988). The ensuing episode of flat-slab subduction is 173 commonly linked with the Laramide orogeny (Dickinson and Snyder 1978; Miller et al. 174 1992; Saleeby 2003), and eventually led to the cessation of magmatism in the Sierras at 175 ca. 85 Ma (Chen and Moore 1982; Lipman 1992). 176 Peninsular and Transverse Ranges, Mojave, and northern Mexico (35–20° N) 177 This sector extends from the southern limit of the Sierra Nevada at approximately 35° N 178 to about 20° N, and includes the morphotectonic domains of the Peninsular Ranges, 179 Transverse Ranges, Mojave Desert and restored batholithic rocks in Salinia in the US as 180 well as Baja California and the Cordillera Occidental in Mexico. The plutonic record of 181 this region includes overlapping continental arc segments of Permian to Cretaceous age 182 (Barth et al. 2008). Mesozoic (Triassic to Cretaceous) plutonic suites are distributed in 183 this region along three NNW-trending belts (Barth et al. 1997; Kistler et al. 2014). Early 184 to Late Cretaceous magmatism is manifested by the numerous plutons of the ca. 128–86 185 Ma Peninsular Ranges Batholith that records a west to east progression of subduction 186 transitioning from an oceanic to a continental arc setting (Morton et al. 2014; Hildebrand 187 and Whalen 2014b). 188 Southeastern Mexico and Central America (25–15° N) 189 Southeastern Mexico and Central America are composed of several fault-bounded crustal 190

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blocks with different geological histories. These blocks were juxtaposed in the course of 191 Pangea amalgamation and dispersal in the Paleozoic and Mesozoic (Campa and Coney 192 1983; Sedlock et al. 1993; Dickinson and Lawton 2001; Keppie 2004). Processes 193 attributed to the subduction of (Paleo-)Pacific oceanic lithosphere have affected the 194 region at least since the Carboniferous (Proenza et al. 2004; Keppie et al. 2008; 2010; 195 2012; Galaz et al. 2013). Continental arc magmatism was particularly abundant during 196 the Carboniferous–Permian, as suggested by the detrital zircon record and an abundance 197 of Carboniferous–Permian igneous rocks in the Mixteca and Oaxaquia terranes (Torres et 198 al. 1999; Kirsch et al. 2012; Ortega-Obregón et al. 2014) as well as the Chiapas Massif of 199 the Maya block (Schaaf et al. 2002; Weber et al. 2007; Solari et al. 2009). In the Acatlán 200 Complex, which forms the Paleozoic basement of the Mixteca terrane, basin formation 201 and the intrusion of calc-alkaline plutons was associated with local intra-arc extension, 202 interpreted as a result of oblique, east dipping Pacific subduction (Ramos-Arias et al. 203 2008; Keppie et al. 2012; Kirsch et al. 2013). The Middle–Late Triassic history of 204 southeastern Mexico is characterized by subdued magmatic arc activity and local 205 shortening and uplift, which have been attributed to transient flat-slab subduction (Kirsch 206 et al. 2014). Magmatic arc activity was re-established by the Early–Middle Jurassic and 207 continued into the Cretaceous (e.g., Barboza-Gudiño et al. 2004; Campa-Uranda et al. 208 2004; Fastovsky et al. 2005; Barboza-Gudiño et al. 2008; Zavala-Monsiváis et al. 2009; 209 Godínez-Urban et al. 2011; Zavala-Monsiváis et al. 2012). During the Late Triassic to 210 Early Jurassic, peripheral (back-arc?) ocean basins formed at the western margin of 211 continental Mexico (Centeno-García et al. 1993; Martini et al. 2010), accompanied by the 212 deposition of siliciclastic rocks with a passive margin signature (Silva-Romo et al. 2000; 213

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Centeno-García 2005) and the intrusion of mafic rocks with a back-arc geochemical 214 signature (Grajales-Nishimura et al. 1999; Valencia-Moreno et al. 2001; Keppie et al. 215 2006; Helbig et al. 2012a; 2012b). These basins were subsequently closed in the Early 216 Cretaceous, when a Middle Jurassic–Lower Cretaceous arc assemblage known as the 217 Guerrero Composite Terrane accreted to mainland Mexico (Martini et al. 2011; 2013; 218 Palacios-García and Martini 2014). 219 Northern Andes (12° N–5° S) 220 The sector referred to as the Northern Andes comprises the western margin of South 221 America between 12° N and 5° S, i.e. Colombia and Ecuador, and western Venezuela. 222 The southern boundary of this sector coincides with the Huancabanga deflection, which 223 marks a change in strike orientation of the Andean orogen. Due to the paleogeographical 224 location of this region (i.e. proximal to the Ouachita-Marathon suture), the Paleozoic to 225 Mesozoic tectonic and magmatic history of the Northern Andes, recently summarized by 226 Spikings et al. (2014), is to a large part influenced by processes related to Pangea 227 assembly and break-up. The earliest evidence of a continental arc in the northern Andes 228 includes arc-derived Ordovician schists and gneisses in the Eastern Cordillera of Ecuador 229 and the Central Cordillera of Colombia (Litherland et al. 1994; Carmona and Pimentel 230 2002; Chew et al. 2007). Magmatic rocks of age 290–240 Ma occur in the Santa Marta 231 Massif and the Guajira Peninsula, as well as in the Cordillera Central in Colombia 232 (Litherland et al. 1994; Cardona et al. 2010; Villagómez et al. 2011; Laya and Tucker 233 2012; Van der Lelij et al. 2016) and are interpreted to have formed above an east dipping 234 Pacific subduction zone during the final stages of Pangea formation. Based on plate 235 reconstructions (Elías-Herrera and Ortega-Gutiérrez 2002; Weber et al. 2007) and the 236

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occurrence of similarly aged arc-related igneous rocks, the basement terranes of southern 237 Mexico and Central America are interpreted to have formed the conjugate margin to NW 238 South America (Cochrane et al. 2014). Crustal anatectites and juvenile mafic suites with 239 ages of 240–216 Ma may record the oblique rifting of these Mexican terranes from the 240 NW South American margin. The ensuing passive margin stage was superseded by 241 renewed active margin magmatism that initiated diachronously along the North Andean 242 margin between 213 and 185 Ma (Cochrane et al. 2014; Van der Lelij et al. 2016) and 243 continued into the Cretaceous (Villagómez et al. 2011; Boekhout et al. 2012; Reitsma 244 2012; Villagómez and Spikings 2013; Cochrane et al. 2014). A period of back-arc 245 extension marks the period of 145–114 Ma, which led to the emplacement of juvenile 246 igneous rocks in the Cordillera Real, Cordillera Central and the Santander Massif 247 (Litherland et al. 1994; Romeuf et al. 1995; Bustamante et al. 2010; Cochrane et al. 2014; 248 Van der Lelij et al. 2016) and may have resulted in the detachment of continental slivers 249 (Chaucha and Tahamí terranes, Spikings et al. 2014 and references therein). These slivers 250 are inferred to have been accreted back to the margin during a switch to compressional 251 tectonics at ca. 115 Ma (Ruiz et al. 2007; Villagómez et al. 2011). Arc magmatism is 252 scarce between ca. 115 Ma and 100 Ma due to highly oblique convergence between the 253 newly formed Caribbean plate and the South American plate (Pindell and Kennan 2009). 254 The origin of felsic magmatism at 100–75 Ma, e.g. represented by the 95–85 Ma 255 Antioquia batholith (Villagómez et al. 2011; Villagómez and Spikings 2013), is currently 256 debated (Pindell and Kennan 2009; Spikings et al. 2014). Mafic igneous rocks occurring 257 in the Western Cordillera of Ecuador and Colombia that have ages between ca. 100 and 258 85 Ma belong to the Caribbean Large Igneous Province, parts of which amalgamated to 259

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northwestern South America at 75–70 Ma (Spikings et al. 2001; Kerr et al. 2002; Vallejo 260 et al. 2006; Spikings et al. 2010; Villagómez and Spikings 2013). 261 Peruvian Andes (6–18° S) 262 In the Peruvian Andes, located between 6° S (the Huancabamba deflection) and 18° S 263 (the Arica deflection, or Bolivian orocline), continental arc magmatism initiated in the 264 Ordovician as part of the Famatinian orogenic cycle (Mukasa and Henry 1990; Gosen and 265 Prozzi 1998; Pankhurst et al. 2000; Cawood 2005; Vaughan and Pankhurst 2008; 266 Bahlburg et al. 2009). The Silurian and Devonian mark a hiatus in the magmatic arc 267 record (Chew et al. 2007; Bahlburg et al. 2009), possibly due to changing plate 268 kinematics of the detachment of a segment of the Arequipa-Antofalla block, which is a 269 Precambrian basement block that underlies much of the coastal region of southern Peru 270 (Loewy et al. 2004). Magmatic activity resumed in the Early Mississippian (ca. 345 Ma: 271 Chew et al. 2007; Mišković et al. 2009) and was followed by Late Permian to Late 272 Triassic lithospheric thinning, accompanied by metamorphism and deformation, as well 273 as the emplacement of partially migmatized granitoids at 285–223 Ma (Sempere et al. 274 2002; Mišković et al. 2009). Easterly subduction of Pacific lithosphere and associated 275 calc-alkaline magmatism in the Western Peruvian Cordillera was re-established by the 276 Late Triassic (Boekhout et al. 2012; Demouy et al. 2012), but was interrupted by a period 277 of back-arc extension and bimodal igneous activity in the Jurassic (Ramos and Aleman 278 2000; Sempere et al. 2002; Boekhout et al. 2012; Demouy et al. 2012), which is attributed 279 to a global change in plate kinematics (Ramos 2010). The Cretaceous marks the intrusion 280 of the Coastal batholith, a large, linear composite pluton emplaced in the periods 105–101 281 Ma, 91–82 Ma, and 73–62 Ma (Pitcher et al. 1985; Mukasa 1986; Hildebrand and 282

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Whalen 2014a). 283 South-central Andes (18–40° S) 284 The Cordilleran sector defined here as the south-central Andes includes the Andean 285 Range of Bolivia, northern Chile and west-central Argentina from the Arica deflection, at 286 18° S to 40° S. The basement of the south-central Andes is classically interpreted to be 287 composed by a number of parautochthonous and allochthonous crustal fragments, namely 288 the Pampia, Antofalla, Cuyania, and Chilenia terranes, which accreted to the South 289 American margin at various times throughout the Late Neoproterozoic and Early 290 Paleozoic (Ramos 2009 and references therein). However, based on more recent data, the 291 existence of Pampia, Cuyania (or Precordillera), and Chilenia are contentious (Vaughan 292 and Pankhurst 2008; Alasino et al. 2012; Rapela et al. 2016). Evidence for early 293 magmatic activity in the south-central Andes is found in the Famatinian orogen, a 294 continental magmatic arc active between ca. 505 Ma and 420 Ma (Bahlburg et al. 2009). 295 The Devonian is marked by magmatic and tectonic quiescence along the south-central 296 Andean margin (Bahlburg and Hervé 1997; Chew et al. 2007; Bahlburg et al. 2009; 297 Cardona et al. 2009), but locally, such as in the Sierras Pampeanas in NW Argentina, 298 Middle–Late Devonian A-type granitoids occur (Dahlquist et al. 2013). Continental arc 299 magmatism was widespread during the Late Paleozoic to Early Mesozoic, for example 300 represented by the Chilean Frontal Cordillera Batholith that shows magmatic pulses 301 during the Mississippian, Early Permian, Late Permian–Middle Triassic, and Upper 302 Triassic (Hervé et al. 2014; Maksaev et al. 2014). After another gap in arc magmatic 303 activity during the Late Permian to Late Triassic, subduction was re-established and 304 persisted into the present day in what is referred to as the Andean cycle (Ramos and 305

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Aleman 2000; Haschke et al. 2006). During the Jurassic to Early Cretaceous, extensional 306 tectonics characterized the south-central Andean margin, which led to the development of 307 a magmatic arc located along the present-day coastal Cordillera, and a series of back-arc 308 basins to the east (e.g., Oliveros et al. 2012; Rossel et al. 2013). 309 Southern Andes (39–55° S) 310 The southern Andean sector coincides with the tectonic province known as Patagonia, 311 which extends from about 39° S to 55° S. The Paleozoic geological history of Patagonia 312 is not agreed upon in every aspect, but is generally interpreted to have involved the 313 collision of an (para-)autochthonous northern block, and an allochthonous southern block 314 in the Carboniferous (Pankhurst et al. 2006; Ramos 2008; Rapalini et al. 2010; Ramos 315 and Naipauer 2014). Subduction-related magmatic rocks of Early Devonian to 316 Carboniferous age occurring in the North Patagonian Massif are interpreted to reflect the 317 destruction of the ocean basin between these blocks (e.g., Hervé et al. 2013). In the 318 southern block, east-dipping subduction may have commenced at ca. 390 Ma and 319 continued into the Mesozoic (Kato et al. 2008; Chernicoff et al. 2013). Voluminous and 320 regionally extensive Mesozoic to Cenozoic continental magmatic arc activity in the 321 southern Andes is evidenced by the Patagonian batholith that is subdivided into a Late 322 Cretaceous to Late Miocene northern part (Pankhurst et al. 1999), a Late Triassic central 323 part (Rapela and Pankhurst 1992; Zaffarana et al. 2014), and a Late Jurassic to Neogene 324 southern part (Rolando et al. 2002; Hervé et al. 2007). 325

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Methods 326 Age compilations 327 Age spectra between 400 and 80 Ma were constructed on the basis of ~1,300 (bulk) U/Pb 328 crystallization ages of igneous bedrocks, and 15,575 detrital zircon U/Pb ages from 329 published and unpublished sources (see appendix for complete list of references). The 330 compilation contains U-Pb analyses only, because Rb/Sr, K/Ar and 40Ar/39Ar analyses 331 may yield erroneous ages due to daughter isotope loss, low-grade metamorphism and/or 332 hydrothermal activity post-dating volcanic and plutonic rock emplacement, even in young 333 volcanic rocks (e.g., Montecinos et al. 2008). The age compilation combines TIMS 334 (thermal ionization mass spectrometry), LA-ICP-MS (laser ablation inductively coupled 335 plasma mass spectrometer), SHRIMP (sensitive high-resolution ion microprobe), and 336 SIMS (secondary ion mass spectrometry) analyses. Coordinates were extracted for each 337 bedrock and detrital zircon sample to enable the division of age data into predefined 338 sectors along the Cordilleran arc. To constrain data collection and analyses, we focused 339 on age data between 400 Ma and 80 Ma only. These limits are arbitrary, but were chosen 340 because (i) magmatic arc activity started in the Early Paleozoic in many places along the 341 Cordilleran orogen and terminated at around 80 Ma in the Sierran sector, (ii) the number 342 of available Cenozoic igneous and detrital U/Pb ages is inadequate due to the fact that 343 young igneous arcs are commonly dated with the 40Ar/39Ar method and there are less 344 detrital zircon studies of Cenozoic deposits. 345

Each bedrock age represents a multiple or bulk zircon age of analyses from three 346 or more single zircon grains (or domains therein) that were calculated by the original 347 author. This does not apply for the Sierran sector, for which single zircon bedrock ages 348

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have been compiled. The dated rocks summarized as "bedrock ages" comprise chiefly 349 plutonic rocks with a predominantly felsic to intermediate composition and only a few 350 volcanic rocks. 351

Detrital zircon samples of different depositional age were included in the 352 compilation to sample the maximum number of sources exposed at various times in the 353 geological past. The detrital zircons are interpreted to represent magmatic ages. Zircon 354 ages identified to have a metamorphic origin (mostly based on U/Th ratios) by the 355 original investigators are excluded from the compilation. The concordance of each zircon 356 grain was calculated from 206Pb/238U and 207Pb/235U ages to ensure that only concordant 357 grains, i.e. with < 10 % normal and < 5 % reverse discordance, were included in the age 358 compilation. 359

For igneous and detrital zircon data, respectively, age data (Fig. 1) are plotted as (i) 360 histograms with a 10 m.y. bin width, and (ii) kernel density estimates (KDEs; Vermeesch 361 2012), which are overlain on the histograms. The histograms allow visual evaluation of 362 the number of samples forming age peaks and enable inter-sample comparison, but are 363 constructed using a constant bin size, which may not be appropriate for zircon age 364 distributions, which are neither smooth nor unimodal (e.g., Vermeesch 2012). The 365 calculated KDEs, on the other hand, are based on adaptive kernel density estimation, in 366 which the bandwidth is varied according to the local density. As a smooth and continuous 367 alternative to the discrete and discontinuous histogram, KDEs facilitate the automatic 368 extraction of peaks and other time series parameters and allows normalization and thus 369 the combination of bedrock and detrital zircon age data. KDEs were chosen as a 370 statistical technique to visualize age populations rather than probability density plots 371

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(PDPs) because KDEs are considered statistically more robust than the more commonly 372 used PDP, especially when data quantity and/or precision is high (Vermeesch 2012). 373 Furthermore, because the kernel density estimate does not take into account analytical 374 uncertainties, the different levels of precision of the compiled TIMS, LA-ICP-MS, 375 SHRIMP, and SIMS age data have no effect on the shape of the KDEs. KDE calculation 376 was accomplished using an open-source Java application developed by Peter Vermeesch 377 (Density Plotter, http://www.ucl.ac.uk/~ucfbpve/densityplotter/). Composite KDE 378 functions, in which bedrock and detrital age spectra are combined by summing the 379 respective normalized KDE values for each age interval, are plotted in a space-contour 380 plot (Fig. 2a) to visualize along-arc variation in magmatic activity. Using Gauss fitting, 381 statistical parameters such as peak location, height, prominence, width, and skewness 382 were calculated from these composite KDE functions. Furthermore, a time-series spectral 383 analysis was performed using the Lomb-Scargle method (Lomb 1976; Scargle 1982) to 384 establish whether or not the zircon age spectra exhibit cyclic behavior. The term "cyclic" 385 in this paper is used synonymously with "periodic", and is defined as a repetition of an 386 event or a sequence of events at regular time intervals. The terms "episode" and 387 "episodic", on the other hand, refer to unique or randomly repeated events. The Lomb-388 Scargle method is based on a fast Fourier transform, in which the individual composite 389 KDE functions (containing both bedrock and detrital zircon ages from each Cordilleran 390 sector) are decomposed into a combination of sinusoids of different frequencies, 391 amplitudes, and phases. Magnitudes in the resulting Lomb-Scargle periodogram (Fig. 2b) 392 represent the contribution of a frequency or period to the original time series. A periodic 393 event or cycle in the data will create a distinct spike in the periodogram. Frequencies or 394

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periods with a high spectral magnitude can be attributed to a periodic event, but only if 395 the sampling interval supports at least 3 periods of that frequency (e.g., Telgársky 2013). 396 Hence, only periods up to 100 m.y. are considered. 397 Geochemical data 398 In order to investigate how changes in geochemical composition of arc-related igneous 399 rocks correlate with magmatic arc activity, geochemical data are currently being 400 compiled by the authors for all eight arc domains. In this paper, the three datasets from 401 the (i) Sierra Nevada, (ii) Peninsular Ranges, Transverse Ranges, Mojave, and northern 402 Mexico, and (iii) southeastern Mexico and Central America are presented. Flare-up 403 events, identified on composite KDE functions of the individual arc sector by visual 404 gauging of peak distribution, width, and height, were used as a reference for description 405 of trends in geochemical data. The geochemical proxies include SiO2 to evaluate extent 406 of differentiation, εNdi and 87Sr/86Sri to assess the relative roles of crustal and mantle 407 components in arc magmas (e.g., DePaolo and Wasserburg 1979; DePaolo 1981a), and 408 Sr/Y and (Sm/Yb)n (normalized to chrondrite values) for a measure of magma source 409 depth and crustal thickness (e.g., Gromet and Silver 1987; Mamani et al. 2010; Chapman 410 et al. 2015; Chiaradia 2015; Profeta et al. 2015). Due to the scarcity of available 411 geochemical data with U/Pb zircon ages in the Peninsular Ranges and the southern 412 Mexican sector, U-Pb-zircon constrained data were supplemented by geochemical data 413 with ages constrained by other means in these sectors, including 40Ar/39Ar, K/Ar, Rb-Sr, 414 and Sm-Nd geochronology, and ages estimated using (bio-)stratigraphic evidence. Apart 415 from the data points, median values ± one standard deviation were plotted for a moving 416 10 m.y. average to allow a better evaluation of trends and degree of scatter (Fig. 3). In the 417

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case of Sr/Y and (Sm/Yb)n, only rocks with < 70 wt.% SiO2 are plotted to exclude the 418 effect of plagioclase fractionation, affecting Sr/Y, and to exclude garnet bearing granites 419 (e.g., Zhang et al. 2012), affecting both Sr/Y and (Sm/Yb)n. 420 Kinematic data 421 In order to investigate the relationship between continental magmatic arc activity and 422 plate kinematics, rates of (i) trench-orthogonal convergence and (ii) trench-parallel 423 displacement between subducting oceanic and upper continental plates, as well as (iii) 424 slab age were compared. 425

We obtained relative plate motion from a recent plate kinematic model for the 426 interval of 200–0 Ma (Shephard et al. 2013) by using the Python script convergence.py 427 written by Nathaniel Butterworth, EarthByte Group, School of Geosciences, University 428 of Sydney, and based on the pyGPlates application programming interface for GPlates1 429 (Boyden et al. 2011). The relative movement of the upper plate was sampled at 24 430 selected locations (three per arc domain) in the vicinity of the subduction zone vertices in 431 1 m.y. intervals using GMT2. To account for changes in plate motion rate within 432 individual arc domains, these three sets of plate motion values per arc domain were used 433 to calculate and plot average values together with minimum and maximum values (Fig. 3, 434 4). The slab age, i.e., the age of the plate entering the trench, was extracted for 200–0 Ma 435 in 5 m.y. intervals from paleo-age grids used by Seton et al. (2012) and released in Müller 436 et al. (2013) by applying the same procedure as described above. 437

To statistically evaluate the link kinematic parameters and magmatic activity, the 438 1 http://www.gplates.org/

2 http://gmt.soest.hawaii.edu/

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Pearson product moment correlation coefficient, which reflects the extent of a linear 439 relationship, was calculated for each parameter pair after reducing the variables to evenly 440 spaced values (Fig. 5). Age spectra for arc sectors D–H were extended to 50 Ma to allow 441 for a more rigorous evaluation of patterns. 442

Results 443 Age compilation 444 The number of age data for each Cordilleran arc sector varies between a minimum of 112 445 (SE Mexico and Central America) to a maximum of 257 multiple zircon bedrock ages 446 (Peruvian Andes) or 1678 single zircon bedrock ages (Sierra Nevada), and between 757 447 (Peruvian Andes) and 5869 (Sierra Nevada) detrital zircon ages. Detrital zircon age 448 spectra are complex, exhibiting many peaks (from 10 in the Sierra Nevada to 29 in the 449 Northern Andes), whereas the igneous spectra are characterized by fewer peaks (from 3 450 in the Sierra Nevada to 11 in SE Mexico and Central America) of comparatively larger 451 wavelength. KDEs based on bedrock and detrital zircon ages, generally show a similar 452 distribution of peaks, but these peaks may have different relative amplitudes (Fig. 1). In a 453 few cases, maxima in the bedrock age data coincide with minima in the detrital zircon 454 data and vice versa (e.g., at ca. 130 Ma and 275 Ma in F, and at ca. 150 Ma in H), which 455 may be an artifact of relatively low data density in these sectors. The Pearson product 456 moment correlation coefficient, evaluating the similarity between bedrock and detrital 457 age KDE functions, ranges between 0.14 (Peruvian Andes) and 0.87 (Coast Ranges). 458 Correlation coefficients show a bimodal distribution—high values (0.62–0.87) 459 correspond to the North American sectors, whereas the Andean sectors are characterized 460

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by low values (0.14–0.42). 461 The spatial and temporal distribution of maxima and minima of composite KDEs 462

along the Cordilleran arc, displayed in the color contour plot of figure 2a, shows bull’s-463 eye-features reflecting high-amplitude variations of zircon age populations of limited 464 spatial and temporal extent (e.g., ca. 130 Ma minimum in B-C; 134 Ma maximum in D; 465 200 Ma maximum in E). The figure also shows subtle, along-arc striking linear features 466 of variable length, such as a 105–90 Ma band of high values along A-B-C, a 280–265 Ma 467 band of high values along D-E-F-G-H, and a 175–165 Ma band of high values and 220–468 210 Ma band of low values along the entire Cordilleran orogen. The Lomb-Scargle 469 periodogram (Fig. 2b) shows relatively high power values at periods of ca. 60–90 m.y. 470 across most of the Cordilleran orogen. In the Coast Ranges, the Peninsular Ranges and 471 the Peruvian Andes, a periodic signal of 80–85 m.y. is particularly pronounced, and 472 periods of ca. 62–68 m.y. have the highest magnitudes in the Sierra Nevada, the South-473 central and Southern Andes. Smaller, ca. 44–46 m.y. periods are identified in the Coast 474 Ranges, the southeastern Mexican sector and the northern Andes. Other, subordinate, 475 peaks occur at periods of ca. 31 m.y. (Sierra Nevada), 52 m.y. (Peninsular Ranges), 39 476 m.y. (southeastern Mexico), and 36 m.y. (Northern Andes). Other statistical parameters 477 derived from the composite KDE time series show a high variability, but with increasing 478 age peak height and prominence decreases, and peak width normalized to peak height 479 increases for most of the datasets, as a result of a decrease in analytical precision with 480 increasing age inherent to the geochronological datasets. Peak symmetry also varies 481 within any given arc sector, but is predominantly positively skewed (i.e., has a longer 482 right tail) in the Sierra Nevada, and negatively skewed in the Peninsular Ranges sector. 483

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Geochemical data 484 Sierra Nevada (sector B). For Cordilleran sector B (Fig. 3a), flare-up events (F) occur 485 during the Triassic at ca. 234–213 Ma (FT), during the Jurassic, at ca. 170–150 Ma (FJ), 486 and during the Cretaceous, at ca. 103–88 Ma (FC). These flare-up events are separated by 487 periods of low zircon production, i.e. magmatic lulls. Overall, the number of available 488 age-constrained geochemical data in the Sierra Nevada sector is high, ranging between 489 392 samples (εNdi) to 3808 samples (SiO2). The following trends can be observed (Fig. 490 3a): SiO2 exhibits higher median values during FT than during lulls prior and following 491 FT. From ca. 180 Ma to 90 Ma, median SiO2 values fluctuate between 60 and 70 wt.%, 492 independent of age relative to a flare-up or lull. SiO2 increases further from ca. 90 Ma to 493 the end of the observation period. εNdi exhibits similar median values of ca. -3 during FT 494 and FJ. Between these two flare-up events, there is a data gap. Subsequent to FJ, εNdi 495 increases to median values of up to +5, and then decreases back to values around -5 496 during FC, and keeps decreasing after FC. Approximately the inverse trend of that for εNdi 497 is observed for 87Sr/86Sri, i.e., relatively high values during flare-ups, and low values 498 during lulls. 87Sr/86Sri data density and scatter are generally lower during lulls than during 499 flare-ups. There is an increase in 87Sr/86Sri above average values during the last 10 m.y. of 500 the observation period. Sr/Y and (Sm/Yb)n show almost identical patterns, with highly 501 variable values during flare-ups, but with lower median values than during lulls. At the 502 end of FC to 80 Ma, both proxies increase to median values above average. 503 Peninsular Ranges, Transverse Ranges, Mojave, and northern Mexico (sector C). 504 The number of compiled age-constrained geochemical data in Cordilleran sector D ranges 505

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between 221 samples (εNdi) and 1522 (SiO2). Flare-up events are recognized within the 506 following approximate limits (Fig. 3b): (FPT) 260–237 Ma, (FJ) 175–160 Ma, (FC1) 110–507 94 Ma, and (FC2) 86–80 Ma. Median SiO2 values are lower during FPT and FJ than during 508 periods following these respective flare-up events. From about 120 Ma onwards, SiO2 509 fluctuates only slightly around a median value of ca. 67 wt.%. In terms of εNdi, data 510 density is low for ages up to 180 Ma, but εNdi seems to decrease from a median of ca. +5 511 during FPT to a median of ca. -7 in the following lull. Median values form a "plateau" 512 between ages of 180 and 140 Ma. Halfway through the lull between FJ and FC1, εNdi 513 increases, before decreasing steadily through FC1 and FC2 until the end of the observation 514 period. There is little 87Sr/86Sri data for the time up to ca. 130 Ma, but median 87Sr/86Sri 515 values are relatively high at the end of FPT and shortly prior to FJ. Following FJ, median 516 87Sr/86Sri increases from values around 0.705, to about 0.713 halfway through the 517 following lull, before it drops back to 0.705 at the beginning of FC1, and then increases 518 steadily until 80 Ma. Thus, from ca. 130 Ma onward, the 87Sr/86Sri signal is 519 approximately inverse to the εNdi signal. Data density is low for Sr/Y in the time prior to 520 180 Ma. Median Sr/Y values either decrease (FPT, FJ, FC2) or increase (FC1) during flare-521 up events. Short-lived excursions of median Sr/Y values towards higher values are 522 observed during magmatic lulls. The peak at ca. 220 Ma up to median Sr/Y values of ca. 523 100 is particularly pronounced. (Sm/Yb)n shows a similar trend as Sr/Y, with a decrease 524 (FPT, FJ, FC2) or increase (FC1) in median values through flare-up events, and short-lived 525 excursions to higher values during lulls. The peak in (Sm/Yb)n during FJ is only based on 526 four values. Data scatter is high during FC1 and the following lull. 527 SE Mexico and Central America (sector D). The oldest flare-up event that can be 528

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identified in the Cordilleran arc sector D (Fig. 3c) is a Carboniferous, ca. 312–302 Ma 529 event (FCA), which is followed by a Permian, ca. 272–250 Ma event (FP), a Jurassic, ca. 530 177–155 Ma event (FJ) and two Cretaceous events at ca. 141–128 Ma (FC1) and 102–94 531 Ma (FC2), respectively. Within an observation period of 400–80 Ma, the amount of age-532 constrained geochemical data for southeastern Mexico is only a fraction of that available 533 for sector B and C, i.e., ranges between only 67 samples (87Sr/86Sri) to 274 samples 534 (SiO2). Despite overall low data density and occasional data gaps, the following trends 535 are discernable: SiO2 increases more or less steadily from values around 50 wt.% to 536 values of 70 wt.% that are reached shortly after the end of FP. The Triassic lull marks a 537 drop in SiO2 values, before peaking again during FJ. This pattern, of low SiO2 during lulls, 538 and high SiO2 during flare-up events, is maintained throughout the next two sets of flare-539 ups and lulls. During FC2, SiO2 remains low, but increases towards the end of the 540 observation period. Initial εNd values decrease up to FP and then oscillate two times 541 between median values of ca. +7 and -2 prior to FJ. Data density is low in the following 542 period, but the lull between FC1 and FC2 seems to be dominated by high εNdi, whereas the 543 subsequent flare-up event is accompanied by a decrease in εNdi values. There is little 544 87Sr/86Sri data in the period prior to ca. 230 Ma, but the data suggest that there is an 545 increase in 87Sr/86Sri values in the period leading up to FP. During the Triassic lull, 546 87Sr/86Sri fluctuates inversely to the εNdi pattern, reaching extremely high median values 547 at the beginning of FJ. Data is absent during the following lull. The lull between FC1 and 548 FC2 marks an increase in 87Sr/86Sri from low to moderately high values. Both Sr/Y and 549 (Sm/Yb)n patterns are similarly displaying an increase up toward FP, a fluctuation about 550 low values through most of the Mesozoic (with intermittent data gaps), and finally an 551

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increase in the period leading up to FC2. 552 Kinematic data 553 Trench-orthogonal convergence rates vary in a non-steady state manner. Rates are 554 predominantly positive for all Cordilleran arc sectors (Fig. 4), i.e., associated with 555 advancing slabs, but small negative values are present during the intervals 200–160 Ma in 556 sector A, 140–130 Ma in sector E, 140–110 Ma in sector F, 98–58 Ma in sector G, and 557 120–50 Ma in sector H indicating minor episodes of slab retreat. The variation of 558 orthogonal convergence rates within an individual arc sector is usually < 50 mm/a. 559 Higher variation is exhibited by (i) sector A at 160–140 Ma due to the accretion of the 560 Wrangellia Superterrane and associated closure of the Cache Creek Ocean (Shephard et 561 al. 2013), (ii) sector D at 120–110 Ma and 72–65 Ma as a result of changes in the position 562 of the trench leading to a ca. 2000 km offset of the points from the active subduction 563 trench, and (iii) sector E at 200–185 Ma that is due to a combination of the geometry of 564 the subduction zone of the northern Andean sector and highly oblique (sinistral) 565 convergence, leading to positive convergence in the north, and negative convergence in 566 the southern part. The Pearson product moment correlation coefficient (r), providing a 567 statistical means of evaluating the likeness of the composite zircon age spectra and 568 trench-orthogonal plate convergence velocities, shows values between -0.38 (sector D) to 569 0.62 (sector G) (Fig. 5). 570

Trench-parallel displacement rates fluctuate between positive (right-lateral) and 571 negative (left-lateral) values in most arc sectors (Fig. 4). Sectors B and C predominantly 572 exhibit right-lateral tectonics throughout the observation period, whereas mainly left-573 lateral movement is observed in the northern Andean domain. The variation of lateral 574

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displacement within an individual arc sector is generally < 80 mm/a. Larger variations are 575 observed in certain intervals due to points getting caught on the other side of trenches as a 576 result of changes in the shape and position of the subduction zones as defined in the plate 577 models. Composite zircon age spectra and trench-parallel displacement rates exhibit r 578 values between -0.24 and 0.52 (Fig. 5). 579

Slab age data exhibit large wavelength fluctuations that are poorly correlated with 580 the composite KDE age spectra (r = -0.53–0.54). Up to 50 m.y. variations of slab ages 581 within individual arc sectors can be explained by the different temporal resolution of the 582 kinematic data sets (1 m.y. for plate polygon data, 5 m.y. for age grids). Larger variations 583 occur in certain intervals of sectors B, F, and H as a result of two different oceanic plates 584 subducting beneath the same arc domain, i.e. Farallon–Kula in B, Farallon–585 Phoenix/Chasca in F, and Antarctica–Phoenix in H. 586 Limits, biases, uncertainties, and artifacts 587 Age compilations. Preservation bias: The underlying premise of this study is that the 588 observed distributions of U-Pb ages reflect relative changes in the vigor of subduction-589 related magmatic activity in the Cordilleran arc. However, rather than measuring 590 additions of new crustal material, peaks in zircon age spectra have been argued to reflect 591 times of reduced destruction by subduction erosion (Condie et al. 2009; Hawkesworth et 592 al. 2009; Belousova et al. 2010; Hawkesworth et al. 2010; Condie et al. 2011; Cawood et 593 al. 2012; Hawkesworth et al. 2013). We use a combination of bedrock ages and detrital 594 zircon ages (from samples with different depositional age) to compensate for the 595 fragmentary preservation record of arc magmatism. Hence, although the igneous suite of 596 a certain age may no longer be preserved in situ due to recycling processes occurring at 597

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subduction zones, such as subduction erosion (Clift and Vannucchi 2004; Hawkesworth 598 et al. 2009; Scholl and Huene 2009), detrital zircons from sediments in arc-flanking 599 basins may provide a record of the magmatic activity represented by the obliterated crust. 600 Intrinsic factors, such as erodibility and zircon abundance of the source rock, as well as 601 extrinsic factors, such as erosion (climate, relief, etc.) and transport processes (wind and 602 drainage patterns, distance of source to sink, etc.) determine to what degree an igneous 603 source is represented in the detrital zircon record (Cawood et al. 2012). These factors and 604 the issue of preservation likely bias the observed abundance relative to the true 605 abundance in the source area. Hence, the age spectra cannot be used to quantitatively 606 evaluate the mass balance of igneous rocks, but can only be used as a general, qualitative 607 indicator of magmatic arc activity. 608 Sampling bias: Igneous rocks that are only exposed in remote or logistically challenging 609 areas will be under-represented in the bedrock age spectrum, whereas intense sampling of 610 igneous rocks from small geographic areas can bias the relative significance of a peak in 611 the age spectrum. Furthermore, arc-parallel drainage systems or wind trajectories may 612 potentially introduce zircons from adjacent sectors, yielding extraneous peaks in the 613 detrital zircon spectra of a certain arc domain. Trench-parallel displacements of crustal 614 blocks along strike-slip faults may be another way of introducing external material to any 615 given arc sector. Since the boundaries of the eight arc domains are based on present day 616 geographic location, trench-parallel displacements of crustal fragments, either during or 617 subsequent to the 400–80 Ma observation period, such as those documented in southern 618 California (Luyendyk et al. 1980; Jackson and Molnar 1990; Nicholson et al. 1994), 619 southern Mexico (e.g., Dickinson and Lawton 2001; Elías-Herrera and Ortega-Gutiérrez 620

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2002; Pindell et al. 2012), the south-central Andes (Brown 1993; Taylor et al. 1998), and 621 the southern Andes (Cembrano et al. 2002; Rosenau et al. 2006), may distort age spectra 622 of these or adjacent arc domains. Considering that along-arc translations of the mentioned 623 crustal blocks are usually in the range of a few hundred kilometers at the most, and that 624 the geographic limits of individual arc domains mostly coincide with tectonic boundaries, 625 the effects on age spectra imposed by lateral displacements of crustal fragments should be 626 relatively minor. 627 Tectonic setting bias: Our study is concerned with continental arc magmatism, so we 628 want to compare rocks from the same tectonic setting. The compiled zircon ages, both 629 igneous and detrital, are believed to represent magmatic ages, as zircon ages identified as 630 metamorphic ages by the original investigators, have been excluded. However, apart from 631 being produced in continental arc magmas, igneous zircon can also be generated due to 632 continental collision, or rifting (e.g., Hawkesworth et al. 2009). Collisional processes 633 associated with plate reorganizations during Pangea assembly particularly influence the 634 Northern and Peruvian Andean sectors at 300–230 Ma (Mišković et al. 2009; Spikings et 635 al. 2014), whereas notable episodes of extensional tectonics are documented in sector D 636 at 215–185 (Centeno-García et al. 1993; Martini et al. 2010), in sector E at 240–216 Ma 637 (Spikings et al. 2014), in sector F in the Permo-Triassic (Sempere et al. 2002; Mišković et 638 al. 2009) and Jurassic (Ramos 2010), and in sector G at 200–140 Ma. However, magma 639 volumes generated as a result of continental collision are typically low, and igneous rocks 640 associated with extensional tectonics are predominantly mafic (Storey 1995), and are thus 641 not expected to yield large amounts of zircon (Cawood et al. 2012). Island arcs, which 642 after their formation have collided with the continental margin, potentially represent 643

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additional sources of magmatic zircon, and can lead to spurious peaks in the zircon age 644 spectra. Oceanic terranes and island arcs with ages between 400 and 80 Ma are 645 documented in (i) the Coast Ranges, i.e. the Triassic Chelan Mountains terrane (Tabor et 646 al. 1989; Matzel et al. 2008), (ii) the Sierra Nevada, i.e. Early Paleozoic and Jurassic 647 intraoceanic arc complexes in the eastern Klamath and northern Sierra terranes (Colpron 648 and Nelson 2009; Dickinson 2009; Colpron and Nelson 2011) and the Late Paleozoic 649 Golconda Allochthon (Riley et al. 2000), (iii) northern Mexico, i.e. the Early Cretaceous 650 Alisitos arc terrane (Busby 2004), and (iv) southeastern Mexico, i.e. the Middle Jurassic–651 Lower Cretaceous Guerrero Composite Terrane (Martini et al. 2011; 2013; Palacios-652 García and Martini 2014). Accumulating evidence indicates that both the Alisitos and the 653 Guerrero Composite Terrane are not far-travelled island arc terranes, but peripheral arc 654 systems that formed due to subduction-related extension at the Mexican continental 655 margin (Busby 2004; Centeno-García et al. 2011 and references therein). In that sense, 656 magmatism relating to these respective terranes is not exotic with respect to the 657 continental arc to which these terranes subsequently accreted, but a result of "accordion" 658 tectonics characteristic of convergent continental margins (e.g., Collins 2002). However, 659 the Alisitos and Guerrero fringing arc terranes are not underlain by continental crust, but 660 by transitional to oceanic crust (Busby 2004; Centeno-García et al. 2011). Hence, 661 compositional data derived from these domains have to be interpreted with care, as there 662 can be a bias towards more juvenile compositions. The contribution of Devonian-aged 663 island arc-derived zircons in the Sierra Nevada arc domain seems to be only minor, as 664 apparent from the age compilation (Fig. 1). 665

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Methodological bias: Plutons in continental arcs are often assembled incrementally (e.g., 666 Barboni et al. 2013; Klemetti and Clynne 2014). The longevity of silicic magmatic 667 systems can lead to complex growth of zircon, which may impart a positive age bias. 668 Furthermore, age analyses acquired by techniques in which zircons are not treated by 669 chemical abrasion may be affected by lead loss (e.g., Crowley et al. 2015; Schaltegger et 670 al. 2015), possibly imparting a negative age bias. For the compilation of bedrock ages, 671 which are multi-zircon ages (except for Sierra Nevada bedrock ages) we blindly accept 672 the interpretation of the original authors that these represent the true crystallization age of 673 the igneous rock. For detrital zircon data, the statistical adequacy, i.e., to what degree the 674 observed age abundance matches the corresponding abundance in the sediment, is 675 influenced by the number of grains analyzed and by the sample preparation procedure. 676 An artificial bias introduced during sample preparation and an insufficient number of 677 zircon grains analyzed per sample may cause certain age populations to go undetected, or 678 result in spurious peaks in the age spectra (e.g., Dodson et al. 1988; Sircombe 2000; 679 Vermeesch 2004; Andersen 2005). As with the bedrock data, we have compiled detrital 680 zircon data with no regard for the statistical robustness of the individual datasets, thus 681 accepting the methodological choices made by the original investigators. An additional 682 factor that may influence the distribution of peaks in the age spectra concerns the 683 representation of age frequency data. For histograms of this study, a constant bin size of 684 10 Ma, which corresponds to the average value of "ideal" bin widths as calculated for 685 every dataset using Sturge’s or Rice’s rule, was chosen to allow a comparison between 686 datasets. However, because zircon age distributions are neither smooth nor unimodal, 687 choosing a constant band- or bin-width to visualize age frequency data may not be 688

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appropriate (e.g., Vermeesch 2012). Hence, in addition to histograms, kernel density 689 estimates (KDEs) are used for statistical analyses of the age data. For the calculation of 690 KDEs, bandwidths are varied according to local density, i.e., where data density is low, a 691 large bandwidth is used resulting in a smoothed distribution, and in parts with abundant 692 data, a narrower bandwidth is used providing a higher resolution (Vermeesch 2012). The 693 resulting KDEs of the detrital zircon datasets, each based on 757 data points and more, 694 locally exhibit frequency variations on the order of ca. 3–5 Ma, whereas generally low 695 data density in bedrock data results in relatively large-scale temporal variations in the 696 KDE at a resolution of ca. 20–40 Ma. Hence, the temporal resolution of bedrock data 697 only allows the identification of large-scale temporal variations in arc-magmatism. 698 Geochemical data. Preservation bias: Geochemical data may be biased by the ages of the 699 material preserved and sampled, so they underlie the same biases and uncertainties that 700 apply for the age compilations. 701 Sampling bias: The Alisitos and Guerrero fringing arc terranes of Triassic to Jurassic age, 702 which cover a substantial area in arc domains C and D, respectively, are not underlain by 703 continental crust, but by transitional to oceanic crust (Busby 2004; Centeno-García et al. 704 2011), which causes a bias towards more juvenile compositions in this age interval. 705 Hence, caution should be used in interpretations concerning crustal vs. mantle 706 components in arc magmas as well as estimates of crustal thickness. Slab window 707 formation, slab tearing or cracking, and slab detachment may cause upwelling of hotter 708 asthenospheric mantle and associated adakite-type igneous activity in certain arc 709 segments (e.g., Yogodzinski et al. 2001). Compositional data may furthermore be 710

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affected by inboard or outboard migration of the continental arc due to changes in the 711 angle of the subducting slab, episodes of subduction erosion, or accretion of terranes. 712 Spatial migration of the arc may shift the focus of magmatism to areas where the crust 713 exhibits differing thermal or compositional properties, potentially introducing artifacts 714 into the compositional data. The location of continental arcs may be traced by the 715 distribution of currently exposed igneous rocks, and to a lesser degree by the distribution 716 of detrital zircon populations. In southeastern Mexico and Central America, for example, 717 the Carboniferous–Permian arc seems to spatially coincide with the Jurassic (Nazas) arc, 718 whereas the Cretaceous arc is located further outboard, due to the accretion of the 719 Guerrero Composite Terrane in the Early Cretaceous (Fig. 6). 720 Tectonic setting bias: In this paper, we intend to compare the compositions of igneous 721 rocks that are a product of continental arc magmatism only. Whereas excluding data 722 associated with other tectonic settings is difficult for zircon age data, compositional data 723 can be filtered using suitable proxies and threshold values. For instance, according to 724 Pearce et al. (1984), Yb+Ta values allow an effective separation of igneous rocks of 725 volcanic arcs (Yb+Ta < 6) from those of within plate settings and ocean ridges (Yb+Ta > 726 6). However, applying this constraint to major element and isotopic data results in a 727 reduction in the number of samples by up to 80 % (e.g., SiO2 values in the Sierra Nevada 728 sector), caused not by a within-plate signature of the samples, but predominantly due to 729 the fact that major element and isotopic data are rarely accompanied by Yb and Ta values. 730 Overall, the Yb+Ta filter yields negligible changes in the general pattern of the 731 compositional data. Hence, in figure 3, the complete and unfiltered datasets are presented. 732

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Methodological bias: Mafic rocks are notoriously difficult to date by U-Pb zircon 733 methods, hence, mafic rocks may be underrepresented in the geochemical dataset. 734 However, U-Pb-zircon constrained data were supplemented by geochemical data with 735 ages constrained by other means, including 40Ar/39Ar, K/Ar, Rb-Sr, and Sm-Nd 736 geochronology, and ages estimated using (bio-)stratigraphic evidence. These dating 737 techniques should not be greatly affected by magma chemistry. A problem with 40Ar/39Ar, 738 K/Ar, Rb-Sr, and Sm-Nd geochronology, however, is an increased risk of daughter 739 isotope loss brought about by low-grade metamorphism and/or hydrothermal activity 740 post-dating volcanic and plutonic rock emplacement. This may result in erroneous ages, 741 i.e. affect the position of data points along the x(time)-axis, and in the case of Nd and Sr 742 isotopic data, also along the y-axis, as ages are used to calculate the initial Nd and Sr 743 compositions. Plotting median values ± one standard deviation for a moving 10 m.y. 744 average allows for a fast evaluation of trends and degree of scatter. However, the median 745 and standard deviation of the compositional data are strongly influenced by the size of 746 bins. A bin size of 10 m.y. has been chosen for all geochemical proxies of this study 747 (independent of sample size, to allow comparison between datasets), as this seems 748 appropriate for an analysis on this temporal scale, but this precludes the recognition of 749 smaller-scale compositional variations. 750 Uncertainties concerning magma source: Continental arc magmas reflect variable 751 contributions from mantle, crustal and subducted reservoirs (e.g., Hildreth and Moorbath 752 1988; Hawkesworth et al. 1993; Jones et al. 2015). In this paper the geochemical proxies 753 Sr/Y and Sm/Yb are in this paper primarily used to estimate magma source depth and 754 crustal thickness (e.g., Mamani et al. 2010; Chapman et al. 2015; Chiaradia 2015; Profeta 755

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et al. 2015). Magmas of thicker arcs evolve at deeper average levels, stabilizing 756 amphibole ± garnet at the expense of plagioclase in the mineral assemblage of residual 757 magmas and partial melts (e.g., Kay 1978; Defant and Drummond 1990; Mahlburg Kay 758 and Mpodozis 2001). Given the marked affinity of Yb for garnet, Y for garnet and 759 amphibole, and Sr for plagioclase, higher Sr/Y and Sm/Yb values arguably indicate 760 amphibole and garnet-dominated melts sources (either lower crustal residue or deep 761 mantle), and thus, a thicker crust. However, there are several additional processes that can 762 have an impact on the Sr/Y ratio, such as (i) a contribution of slab melts (e.g., Defant and 763 Kepezhinskas 2001; König et al. 2006; Chiaradia 2015), (ii) plagioclase fractionation, 764 and (iii) crustal anatexis producing garnet-bearing granites (e.g., Zhang et al. 2012). 765 While adakitic rocks derived from slab melts are relatively rare in continental arcs, only 766 rocks with < 70 wt.% SiO2 are plotted for Sr/Y and (Sm/Yb)n to exclude the effect of 767 plagioclase fractionation, and to exclude highly felsic garnet-bearing granites. 768 Kinematic data. Our analysis implicitly accepts the respective plate motion models and 769 the geodynamic concepts upon which these are based. However, due to the progressive 770 destruction of oceanic lithosphere by subduction, uncertainties associated with 771 paleogeographic reconstructions increase with age. For example, the link between South 772 America and the subducting Farallon Plate must be determined indirectly by a series of 773 intermediate rotations, called plate circuits, because subduction has consumed most of 774 Panthalassa's oceanic plates (e.g., Seton et al. 2012). The Farallon-South America plate 775 circuit involves five "hops" via the Farallon, Pacific, West and East Antarctic, African, 776 and finally, South American Plates. The link through the Pacific Plate is only possible for 777 times since the Late Cretaceous, when seafloor spreading between the Pacific and West 778

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Antarctic Plates was established (e.g., Eagles et al. 2004; Wobbe et al. 2012). For the 779 time prior to the Late Cretaceous, a hotspot reference system must be used for the Pacific 780 Plate (Seton et al. 2012). The Early Cretaceous separation of Patagonia from Africa 781 involved substantial intracontinental extension, which led to misfits in the South Atlantic 782 plate reconstruction. Several models have been proposed to minimize uncertainties in the 783 block rotation between Patagonia and South America (e.g., Eagles 2007; Torsvik et al. 784 2009; Heine et al. 2013), but they show large discrepancies. Similar problems exist for 785 other portions of the Cordilleran margin. Plate kinematic parameters used in this paper 786 must thus be considered with care and applied to first-order processes only. 787

Discussion 788 Testing of models 789 There are two schools of thought on what governs the episodic behavior of arc systems. 790 One set of models invokes events outside the arc, such as plate reconfigurations and 791 changes in mantle flow and/or magma production as the ultimate driver of magmatic 792 activity in arcs (e.g., Armstrong 1988; Hughes and Mahood 2008; Zellmer 2008; de Silva 793 et al. 2015), whereas another set of models is based on arc-internal feedback processes 794 involving magmatic/tectonic crustal thickening, crustal melting, and delamination 795 (Karlstrom et al. 1993; Ducea 2001; DeCelles et al. 2009; Karlstrom et al. 2014; Chin et 796 al. 2015; DeCelles et al. 2015; Cao et al. 2016). These sets of models predict differences 797 in terms of the spatial distribution and the temporal scale of magmatic activity as well as 798 the relationship between magmatic activity and magma composition, and kinematic 799 parameters, respectively. More specifically, if arc systems were externally controlled, i.e. 800

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governed by parameters of the down-going plate, such as convergence rate, age, and 801 subduction angle, flare-ups and lulls in magmatic activity would likely be widely 802 distributed along the arc and occur as distinct (random) events that may coincide with 803 periods of global plate reorganization. In contrast, models invoking an internal forcing 804 should be independent of plate parameters, and are often characterized by cyclic behavior, 805 i.e. events recurring at regular intervals. Flare-ups and lulls would also be spatially 806 limited, because, depending on the crustal architecture of the arc sector, different parts 807 may be at different stages in the cycle at any given time. Furthermore, arc-internal 808 processes, such as crustal thickening, delamination, etc., predict changes in arc chemistry 809 that should correspond to variations in magmatic activity, whereas no such correlation is 810 expected in the case of an external forcing. These criteria are discussed in the following 811 sections. 812 Spatial and temporal pattern. The distribution of U/Pb bedrock and detrital zircon ages, 813 used as a proxy for the timing of magmatic accretion, shows a great variability in the 814 spatial scales of Cordilleran magmatic arc activity (Fig. 2). Some minima and maxima are 815 nearly synchronous for thousands of km along the arc. Other peaks and troughs, although 816 the period may be the same, are “shifted” by up to 30 m.y. from one sector to the next 817 (e.g. Permo-Triassic flare-up and lull in sector B and C). On one hand, these features 818 suggest an external, i.e. plate tectonic influence on Cordilleran arc magmatism; on the 819 other, they highlight the importance of internal feedback processes operating 820 independently in different sectors due to distinct crustal properties. 821

Previous studies in Cordilleran magmatic arcs suggest that flare-up events occur 822 with a periodicity of 25–45 m.y. in the Central Andes (Haschke et al. 2006), and 20–50 823

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m.y. in different parts of the North American Cordilleras (Barton 1996; Ducea 2001; 824 Gehrels et al. 2009; Mahoney et al. 2009; Paterson et al. 2011; Barth et al. 2013; 825 DeCelles et al. 2015). Our analysis shows that while periods between 20 and 50 m.y. are 826 present in the dataset, a period of ca. 60 to 80 m.y. is more prominent in the Cordilleran 827 orogen, although the relative magnitude of this periodicity is highly variable for different 828 sectors. In models advocating internal feedback processes in the upper plate as a control 829 of arc magmatism, the periodicity signal is often attributed to a cyclic development and 830 subsequent removal of a crustal arc root (e.g., Ducea 2001; DeCelles et al. 2009; 831 Karlstrom et al. 2014; Chin et al. 2015; DeCelles et al. 2015). According to a recent 832 numerical model (Lee and Anderson 2015), which does not factor in tectonics or erosion, 833 these processes have a period of 10–30 million years. The presence or absence of a 834 periodic component in itself may be diagnostic of either an internal or an external control 835 on arc magmatism, respectively. Although supercontinent formation, too, has been 836 suggested to be cyclic (Nance et al. 2014 and references therein), it exhibits a period of 837 250–320 m.y. and hence it is not directly apparent in the lifetime of Cordilleran arcs. 838 However, processes associated with the fragmentation and assembly of supercontinents 839 may register as distinct events in the record of magmatic activity that may be 840 superimposed on any cyclicity, or even cause cycles to become interrupted or (re-) 841 initiated. The observed variability in period and magnitude are likely a consequence of a 842 superposition of different processes, both cyclic and random. 843 Relationship with magma chemistry. Annen et al. (2006) state that although melt 844 production in the lower crust strongly depends on emplacement rate of mantle-derived 845 basalt, crustal melting is limited by the availability of fertile crust that can be partially 846

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melted. In the model by DeCelles et al. (2009; 2015) the availability of fertile crustal 847 material is the driving force of magmatic episodicity. According to this model, periods of 848 high arc magma production in the continental arc are fueled by underthrusting of forearc 849 and/or retroarc lithosphere, which may also be brought about by slab shallowing 850 (Chapman et al. 2013) or increased plate convergence (DeCelles et al. 2015). Hence, the 851 correlation between convergence rates and continental arc magmatism apparent in our 852 data can also be interpreted to reflect a relationship between convergence rates and the 853 rate at which melt-fertile continental lithosphere is fed into the zone of high heat flux and 854 melting (DeCelles et al. 2015). In terms of arc magma geochemistry, this crustal 855 thickening model predicts SiO2, 87Sr/86Sri, Sr/Y, (Sm/Yb)n to be proportional, and εNdi 856 inversely proportional to arc magma production (DeCelles et al. 2009). The presented 857 geochemical data in this paper generally shows a good correlation between geochemistry 858 and arc magma production, but with notable limitations: (i) In the Sierra Nevada, the 859 expected increase in 87Sr/86Sri, Sr/Y, (Sm/Yb)n during flare-ups is not as pronounced for 860 the Triassic and Jurassic flare-up event as for the Cretaceous event. Accordingly, 861 numerical modeling (Cao et al. 2016) suggests that crustal thickening was not as 862 pronounced for the pre-Cretaceous flare-up events. Furthermore, the Early Cretaceous 863 marks a period of high variation in Sr/Y and (Sm/Yb)n ratios that finds no expression in 864 the age spectrum. (ii) The Peninsular Ranges and northern Mexico sector shows an anti-865 correlation between SiO2 and zircon age density estimates for the time prior to ca. 130 866 Ma. Moreover, there are short periods of elevated Sr/Y and (Sm/Yb)n ratios during 867 magmatic lulls. (iii) Southeastern Mexico and Central America exhibit relatively low 868 SiO2, high εNdi, and low (Sm/Yb)n during the Carboniferous flare-up event. In addition, 869

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the Triassic lull is characterized by low εNdi and high 87Sr/86Sri. 870 These observations suggest that not every flare-up event is associated with thick 871

crust, and not every lull is associated with thin crust, so other factors apart from a 872 periodic modulation of crustal thickness may be important in governing the rates of 873 magma production in continental arcs. Even if age and geochemical patterns show the 874 correlation predicted by crustal thickening and ensuing delamination of arc roots, these 875 mechanisms may not be the only explanation. Instead, an increase in SiO2, 87Sr/86Sri, 876 Sr/Y, (Sm/Yb)n, and a decrease in εNdi may reflect a migration of the arc through crust 877 with different properties. In the Peninsular Ranges Batholith, where the Cretaceous flare-878 up event is marked by a west–east progression from an oceanic arc to a continental arc 879 setting (e.g., Morton et al. 2014), overall chemical changes within this corridor (Fig. 3b) 880 are likely the result of an associated increased proportion of assimilated continental 881 material. Hence, the flare-up event may not have been triggered by crustal thickening, but 882 by an increase in mantle input (Paterson et al. 2016). 883 Relationship with plate parameters. The source region for arc magmas is located in the 884 mantle beneath the arc, where melts are generated as a result of fluid release from the 885 subducted slab (e.g., Gill 1981; Arculus 1994; Tatsumi and Eggins 1995) and mantle 886 decompression caused by subduction-induced corner-flow (e.g., Elkins Tanton et al. 2001; 887 England and Katz 2010). Next to lithospheric thickness of the overriding plate, which 888 may determine the length of the melting column in the mantle wedge (e.g., England et al. 889 2004; Karlstrom et al. 2014; Chin et al. 2015), subduction parameters such as 890 convergence rate or slab age have also been proposed to influence the wedge thermal 891 structure and extent of melting beneath arcs (Peacock 1990; Iwamori 1998; Hebert et al. 892

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2009; England and Katz 2010; Turner and Langmuir 2015a; 2015b). Higher convergence 893 rates have been shown to (i) lead to more vigorous hydration of the mantle wedge causing 894 increased melting (e.g., Cagnioncle et al. 2007; Plank et al. 2009) and/or (ii) increase the 895 flux of hot mantle into the wedge corner, raising the temperature and causing increased 896 melt formation beneath the arc (England and Wilkins 2004; England and Katz 2010; 897 Turner and Langmuir 2015a; 2015b). In terms of the age of the ocean floor, two 898 competing processes may invoke magma formation in the mantle: fluid fluxing 899 (proportional to age; e.g., Leeman 1996; Hebert et al. 2009) and thermal gradient 900 (inversely proportional with age; e.g., England et al. 2004). 901

Igneous rocks with mafic–ultramafic composition that are in equilibrium with the 902 mantle wedge are scarce in exposed portions of continental arcs due to density filtering 903 and internal modification processes of ascending magmas in the continental crust, mainly 904 by a combination of fractional crystallization of primary magmas, and partial melting 905 and/or assimilation of crustal material (DePaolo 1981b; Hildreth and Moorbath 1988; 906 Tatsumi and Stern 2006). The majority of models for the generation of intermediate melts 907 characteristic of continental arcs invokes processes occurring at lower crustal depth, such 908 as underplating, or the intrusion of mafic magma in the form of sills and/or dykes 909 (Huppert and Sparks 1988; Bergantz 1989; Petford and Gallagher 2001; Annen and 910 Sparks 2002; Jackson et al. 2003; Annen et al. 2006; Otamendi et al. 2009; Jagoutz 2010; 911 Otamendi et al. 2012). The extent to which magma production in the mantle influences 912 the rate at which magmas migrate to upper crustal levels is an issue of much controversy 913 (e.g., de Silva et al. 2015). Numerical models show that, to a first order, a higher basalt 914 emplacement rate into the lower crust leads to an increase in the production of residual 915

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melts (due to crystallization of basalt) and partial melts (Bergantz 1989; Barboza et al. 916 1999; Barboza and Bergantz 2000; Dufek and Bergantz 2005; Annen et al. 2006), 917 although it is known that magma transfer rates through the crust are also dependent on 918 other second order factors, such as the initial geotherm as well as crustal thickness, stress 919 state, density, and composition (e.g., Lima et al. 2012; Chaussard and Amelung 2014). 920

If convergence rates and plate ages governed melt production in the mantle wedge, 921 and if the magma transferred to the middle and upper crust was proportional to the 922 magma advected from the mantle wedge (e.g., Zellmer and Annen 2008), there should be 923 a correlation between plate parameters and magmatic arc activity. Although some studies 924 (e.g., Armstrong 1988; Hughes and Mahood 2008; Zellmer 2008) provide evidence of 925 such a correlation, others (e.g., Ducea 2001; DeCelles et al. 2009; 2015; Cao et al. 2016) 926 have negated such a link, because flare-up events in some parts of the Cordillera are 927 seemingly out of sync with peaks in convergence rates. However, the latter studies are 928 based on spatially and temporally limited geochronological and plate motion data (e.g., 929 Engebretson et al. 1985; Pardo Casas and Molnar 1987; Somoza 1998; Sdrolias and 930 Müller 2006). Our compilation of geochronological data and plate parameters extracted 931 from a modern global plate motion model (Seton et al. 2012) that extends back to 200 Ma 932 allows us to re-evaluate the strength of this relationship on a broader scale. The data show 933 that the degree of correlation between orthogonal convergence rates and age spectra is 934 generally poor, but highly variable from one Cordilleran arc sector to the next. However, 935 if variable lag times (up to 10 m.y.) are introduced to account for an incubation period or 936 thermal lag as the system adapts to a new configuration between magmatic episodes (e.g., 937 Annen et al. 2006; de Silva et al. 2006; Mamani et al. 2010; Paterson and Ducea 2015), it 938

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leads to a notable increase (up to 2.0 times) in the correlation coefficient for several 939 sectors, resulting in a moderate (0.3 < r < 0.5) to high (0.5 < r < 1.0) degree of correlation 940 for all sectors but the southeastern Mexican (Fig. 7). For pre-Jurassic times, no plate 941 parameters can be extracted due to the lack of a reliable plate model, but certain maxima 942 and minima in the along-arc age correlation chart (Fig. 2) coincide with known tectonic 943 events along the Pacific margin of Pangea, such as (i) the onset of the Pan-Pacific 944 Gondwanide Orogeny at ca. 300 Ma (e.g., Cawood 2005; Cawood and Buchan 2007), (ii) 945 the closure of the Panthalassan Gondwana suture at ca. 250 Ma (Scotese 1997; Cocks and 946 Torsvik 2002; Stampfli and Borel 2002; Murphy and Nance 2008), and (iii) the opening 947 of the central Atlantic and dispersal of Gondwana at ca. 200 Ma (Nance et al. 2012; Seton 948 et al. 2012; Keppie 2015). These events are associated with global plate kinematic 949 reorganization, affecting the direction and speed of plate convergence along the 950 Cordilleran orogen. A major plate reorganization event also occurred at ca. 100 Ma 951 (Matthews et al. 2012), which may have triggered the Cretaceous flare-up events in the 952 Northern Cordilleran sectors (Fig. 2). Together, these data suggest that a possible link 953 between arc-external events and magmatic episodicity should be re-evaluated and once 954 again explored as larger and more precise geochronological and plate kinematic datasets 955 become available. 956 Future research 957 The geochronological, geochemical, and plate kinematic database that form the 958 foundation of this study are a work in progress. Increasing the sample size as more data 959 become available, adding more geochemical/isotopic proxies, and amplifying the 960 temporal and spatial range will allow more rigorous interpretations of these large datasets 961

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in terms of characterizing episodic arc magmatism and testing model predictions. To 962 minimize the sampling bias, time dependent magma addition rates need to be determined 963 from retro-deformed surface areas of magmatic rocks and geobarometric data (Matzel et 964 al. 2006; Paterson et al. 2011; Memeti et al. 2014; Paterson and Ducea 2015). 965 Lithospheric stress state is a crucial parameter in models of arc magmatism (e.g., 966 DeCelles et al. 2009; 2015) and a controlling factor for magma ascent; hence establishing 967 structural databases is essential in order to estimate rates of tectonic shortening. Another 968 critical aspect concerns the temporal record of island arc magmatism. Lacking the density 969 filter of thick continental crust, oceanic arcs can provide a simpler, more direct way of 970 studying cause and effect, so obtaining large temporal records for island arcs would be 971 desirable. However, this is a difficult task, because island arcs are often short-lived, 972 usually poorly preserved, and predominantly mafic, the latter of which makes them 973 harder to date by zircon geochronology. Preliminary age records from the Talkeetna, 974 Aleutian, and Kohistan island arcs (Paterson and Ducea 2015), however, show a certain 975 degree of episodicity, suggesting that plate parameters and the availability of mantle 976 melts play a big part in governing arc magmatism, irrespective of the thickness and 977 composition of the upper plate. Oceanic arcs can also be used to estimate the background 978 magma production rate of continental arcs. Recent studies have shown that magma 979 production rates in intraoceanic arcs are comparable to the volumes of magma produced 980 during flare-ups in continental arcs (Jicha and Jagoutz 2015). This means that instead of 981 finding a process to explain increased magma production during flare-ups, a mechanism 982 is needed to temporarily suppress magma production in continental arcs, such as flat slab 983 subduction (e.g., McGeary et al. 1985; Gutscher et al. 2000; Stern 2004). 984

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Implications 985 We examine large geochronological, geochemical and kinematic data sets for the 986 Cordilleran orogen as a means to test existing models for episodic magmatism in 987 continental arcs. Bedrock and detrital U-Pb zircon age distributions, which have been 988 shown to be qualitative indicators of magmatic activity within the arc, show a clear non-989 steady state pattern of variable temporal and spatial scales. Whereas most flare-up events 990 are discrete in time and space, some are synchronous for many thousand kilometers along 991 arc-strike, and a moderate periodicity between 60 and 80 million years is apparent in 992 certain portions of the Cordilleran orogen. Covariations between arc magma chemistry 993 and magmatic arc activity suggest crustal thickening during flare-up events, but arc 994 migration poses a challenge, as it can produce similar geochemical patterns. Kinematic 995 data based on recent global plate reconstructions provide a means of evaluating mantle 996 heat input. The correlation between orthogonal convergence rate and Cordilleran arc 997 activity as well as the coincidence between certain flare-up events and lulls with global 998 events of plate tectonic reorganization demonstrates that an external control of 999 continental arc magmatism should be reevaluated. Our results suggest that the driving 1000 mechanisms for flare- ups/lulls vary along this Mesozoic arc and that second order effects 1001 vary between flare-ups and arc segments. 1002

Acknowledgements 1003 We thank George Bergantz and Alan Chapman for their constructive reviews, and David London 1004 for his role as Associate Editor. Kirsch is grateful to Nathaniel Butterworth for the convergence 1005 python script and to Maria Helbig and Uwe Kroner for helpful discussions. Paterson 1006 acknowledges support from NSF grants EAR-1019636, EAR-0537892 and EAR-0073943 and 1007 USGS EDMAP grants G13AC00120 and 03HQA0038. We thank Mark Pecha, and other lab 1008

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Zaffarana, C., Tommasi, A., Vauchez, A., and Gregoire, M. (2014) Microstructures and 1939 seismic properties of south Patagonian mantle xenoliths (Gobernador Gregores and 1940 Pali Aike). Tectonophysics, 621, 175–197. 1941

Zavala-Monsiváis, A., Barboza-Gudiño, J.R., Valencia, V.A., Rodríguez-Hernández, 1942 S.E., and García-Arreola, M.E. (2009) Las sucesiónes volcánicas pre-Cretácicas en el 1943 noreste de México. GEOS Unión Geofísica Mexicana, 29, 53. 1944

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Zellmer, G.F. (2008) Some first-order observations on magma transfer from mantle 1949 wedge to upper crust at volcanic arcs. In C. Annen and G.F. Zellmer, Eds., Dynamics 1950 of Crustal Magma Transfer, Storage and Differentiation. Geological Society, London, 1951 Special Publication 304, pp. 15–31. 1952

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A-type granite intrusion in the East Qinling Orogen, central China: Petrological, 1957 mineralogical and geochemical constraints. Geoscience Frontiers, 3, 635–646. 1958

Figure captions 1959 Figure 1. Igneous and detrital zircon U-Pb age spectra providing a temporal record of 1960 Cordilleran arc magmatism between 400 and 80 Ma. Individual diagrams include TIMS, 1961 LA-ICP-MS, SHRIMP, and SIMS age data presented as histograms with a 10 m.y. bin 1962 width and adaptive KDE functions (see text for details). For bedrock ages (BA), the 1963 number of analyses (n) given in each plot represents the number of crystallization ages, 1964 which are composite ages calculated from three or more single zircons. Exception: 1965 igneous ages from the Sierra Nevada represent single zircon ages. In detrital zircon 1966 spectra (DZ), n refers to ages of single zircon grains (or a domain therein). On the right 1967 hand side, a map shows the extent of defined arc sectors and sample locations. Geological 1968 map data from Bouysse et al. (2010). Abbreviations in the age plots are as follows: PR—1969 Peninsular Ranges, TR—Transverse Ranges, Moj—Mojave Desert, N Mex—Northern 1970 Mexico, SE Mexico—Southeastern Mexico. See DR-1 for data sources. 1971 Figure 2. (a) Color contour plot of composite KDE functions, highlighting the spatial and 1972 temporal distribution of age populations (i.e., magmatic arc activity) along the 1973 Cordilleran arc. Labels of y-axis indicate the latitudinal centers of each Cordilleran arc 1974 sector along an along-arc profile. Letters A–H refer to the following arc sectors from 1975 north to south: A—Coast Ranges, B—Sierra Nevada, C—Peninsular and Transverse 1976 Ranges, Mojave, and northern Mexico, D—Southeastern Mexico and Central America, 1977 E—Northern Andes, F—Peruvian Andes, G—South-Central Andes, H—Southern Andes. 1978 (b) Color contour plot showing results of a Fast Fourier Transform (FFT) based time 1979

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series analysis to evaluate periods of dominant frequencies in Cordilleran arc age data. 1980 Figure 3. Comparison of geochronological (panel 1), geochemical (panels 2–6), and 1981 kinematic data (panels 7–9) for arc-related igneous rocks in the sectors of (a) the Sierra 1982 Nevada, (b) the Peninsular and Transverse Ranges, Mojave, and northern Mexico, and (c) 1983 southeastern Mexico and Central America. Diagonally hatched bands mark magmatic 1984 flare-up events, visually delineated on the basis of peaks in the age spectra. For 1985 geochemical data, individual data points are plotted (dots), along with median values ± 1986 1σ (circles and grey bars) for a moving 10 m.y. average. For kinematic data, black dots 1987 are average values and grey envelopes represent minimum–maximum ranges from a set 1988 of three values extracted per arc domain. Note differing age range in (c). Abbreviations: 1989 BA—bedrock ages, DZ—detrital zircons, OConv.—orthogonal convergence rate, 1990 PDispl.—parallel displacement rate. For data sources see DR-1. 1991 Figure 4. Compilation of kinematic data for the Cordilleran orogen for the time between 1992 200 and 50 Ma. Letters A–H refer to the following arc sectors from north to south: A—1993 Coast Ranges, B—Sierra Nevada, C—Peninsular and Transverse Ranges, Mojave, and 1994 northern Mexico, D—Southeastern Mexico and Central America, E—Northern Andes, 1995 F—Peruvian Andes, G—South-Central Andes, H—Southern Andes. Each diagram 1996 contains (1) kernel density estimates of combined bedrock and detrital zircon age data, (2) 1997 trench-orthogonal convergence rates and (3) trench-parallel displacement rates between 1998 down-going oceanic and upper continental plates, and (4) slab age. Black dots in 2–4 are 1999 average values and grey envelopes represent minimum–maximum ranges from a set of 2000 three values extracted per arc domain. 2001

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Figure 5. Covariance matrix showing Pearson correlation coefficients for parameters of 2002 magmatism and plate kinematics. Letters A–H refer to the following arc sectors from 2003 north to south: A—Coast Ranges, B—Sierra Nevada, C—Peninsular and Transverse 2004 Ranges, Mojave, and northern Mexico, D—Southeastern Mexico and Central America, 2005 E—Northern Andes, F—Peruvian Andes, G—South-Central Andes, H—Southern Andes. 2006 Red is strong positive correlation; blue is strong negative correlation. 2007 Figure 6. Tectonic map showing the principal geologic features of southeastern Mexico 2008 and Central America (J. D. Keppie 2004; Dowe et al. 2005; Helbig et al. 2012b). Colored 2009 squares indicate the location and age of igneous rocks. Pie-charts show detrital zircon age 2010 populations between 400 and 80 Ma. 2011 Figure 7. Effect of lag time on Pearson correlation coefficients between age composite 2012 and orthogonal convergence rate. Letters A–H refer to the following arc sectors from 2013 north to south: A—Coast Ranges, B—Sierra Nevada, C—Peninsular and Transverse 2014 Ranges, Mojave, and northern Mexico, D—Southeastern Mexico and Central America, 2015 E—Northern Andes, F—Peruvian Andes, G—South-Central Andes, H—Southern Andes. 2016 Arc sectors represented by bold lines show an increase in correlation coefficients with 2017 variable lag times. 2018

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A

C

B

D

E

F

G

H

Bedrock ages (BA)Detrital zircon samples (DZ)

A

B

C

D

E

F

G

H

Cenozoic

Mesozoic

Upper Paleozoic

Lower Paleozoic

Neoproterozoic

Mesoproterozoic

Paleoproterozoic

Archean

Plio-Quaternary

Miocene

Oligocene

Eocene

Paleocene

Upper Cretaceous

Lower Cretaceous

Upper Jurassic

Middle Jurassic

Onshore Offshore

Extrusive rocks

Endogenous rocks

LEGEND

Figure 1

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a

b

Period (m.y.)20 30 40 50 60 70 80 90 100

Nor

mal

ized

dis

tanc

e al

ong

arc

H

G

F

E

D

C

B

A

10

20

30

40

50

60

70

80

Nor

mal

ized

Lom

b-S

carg

le p

ower

(%

)

Age (Ma)100 150 200 250 300 350 400

Nor

mal

ized

dis

tanc

e al

ong

arc

H

G

F

E

D

C

B

A

Nor

mal

ized

Ker

nel D

ensi

ty E

stim

ate

(%)

10

20

30

40

50

60

70

80

90

Figure 2

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0

50

100–100

0

100

200

0

100

200

Age (Ma)100 150 200 250 300

(Sm

/Yb)

nS

r/Y

87S

r/86

Sr i

iS

iO2(w

t.%)

Zirc

on a

ges

(Ma)

(mm

/a)

OC

onv.

rat

e(m

m/a

)

convergence

Sierra Nevada (43–35° N)

BA, nDZ, n = 5869

FC

FJFT

100 150 200 250 300

n = 3805

n = 392

n = 914

n = 1686

n = 637

2

4

60

50

100

0.705

0.710

0.715

10

0

10

50

60

70

0

50

100

0

100

200

0

100

200

Age (Ma)100 150 200 250 300

100 150 200 250 300

(Sm

/Yb)

nS

r/Y

87S

r/86

Sr i

iS

iO2(w

t.%)

Zirc

on a

ges

(Ma)

(mm

/a)

OC

onv.

rat

e(m

m/a

)

Peninsular and Transverse Ranges, Mojave, and northern Mexico (35–20° N)

BA, n = 208 DZ, n = 2846

FC2 FC1 FJ FPT

n = 1522

n = 221

n = 464

n = 845

n = 384

0

2

4

60

20

40

60

80

0.705

0.710

0.715

10

0

1055

60

65

70

75

0

20

40

60

80–200

–100

0

100–50

0

50

100

150

Age (Ma)100 150 200 250 300 350 400

(Sm

/Yb)

nS

r/Y

87S

r/86

Sr i

iS

iO2(w

t.%)

Zirc

on a

ges

(Ma)

(mm

/a)

OC

onv.

rat

e(m

m/a

)

Southeastern Mexico and Central America (25–15° N)

convergence

BA, n = 112DZ, n = 4553

FC2

FC1

FJ FCAFP

100 150 200 250 300 350 400

n = 274

n = 164

n = 67

n = 215

n = 207

0

2

4

0

20

40

60

0.703

0.704

0.705

0.706

0.7075

0

5

10

50

60

70

80

a b c

SiO2 < 70 wt.%

SiO2 < 70 wt.%

SiO2 < 70 wt.% SiO2 < 70 wt.%

SiO2 < 70 wt.%SiO2 < 70 wt.%

Figure 3

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A KDE composite

OConv. (mm/a)

PDispl. (mm/a)

Slab age (Ma)

0

50

100

0100

0

100

200

B KDE composite

OConv. (mm/a)

PDispl. (mm/a)

Slab age (Ma)

0

50

1000

100200

0

100

200

C KDE composite

OConv. (mm/a)

PDispl. (mm/a)

Slab age (Ma)

0

50

100100

0100200

0

100

200

D KDE composite

OConv. (mm/a)

PDispl. (mm/a)

Slab age (Ma)

0

50

200

100

0

100

0

100

60 80 100 120 140 160 180 200 220 240 60 80 100 120 140 160 180 200 220 240

E KDE composite

OConv. (mm/a)

PDispl. (mm/a)

Slab age (Ma)

0

50

100

100

0

0

100

G KDE composite

OConv. (mm/a)

PDispl. (mm/a)

Slab age (Ma)

0

50

100100

0

100

0

100

H KDE composite

OConv. (mm/a)

PDispl. (mm/a)

Slab age (Ma)

0

100

200100

0100200

0

100

200

F KDE composite

OConv. (mm/a)

PDispl. (mm/a)

Slab age (Ma)

25

50

75

100

0

100

0

100

Age (Ma) Age (Ma)

60 80 100 120 140 160 180 200 220 240 60 80 100 120 140 160 180 200 220 240

right-lateral

left-lateral

convergence

divergence

right-lateral

left-lateral

right-lateral

left-lateral

convergence

divergence

right-lateral

left-lateral

convergence

divergence

right-lateral

left-lateral

convergence

divergence

right-lateral

left-lateral

convergence

divergence

right-lateral

left-lateral

convergence

divergence

right-lateral

left-lateral

convergence

divergence

Figure 4

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Agecomposite

Bedrockages

Detritalzircon ages

Trench-orthogo-nal convergence

Trench-parallel displacement

Slab age

Age

com

posi

te

Bed

rock

ages

Det

rital

zirc

on a

ges

Tren

ch-o

rtho

gona

l co

nver

genc

e

Tren

ch-p

aral

lel

disp

lace

men

t

Sla

b ag

e

Age

com

posi

te

Bed

rock

ages

Det

rital

zirc

on a

ges

Tren

ch-o

rtho

gona

l co

nver

genc

e

Tren

ch-p

aral

lel

disp

lace

men

t

Sla

b ag

e

A

Agecomposite

Bedrockages

Detritalzircon ages

Trench-orthogo-nal convergence

Trench-parallel displacement

Slab age

E F

G H

B

C DAge

composite

Bedrockages

Detritalzircon ages

Trench-orthogo-nal convergence

Trench-parallel displacement

Slab age

Agecomposite

Bedrockages

Detritalzircon ages

Trench-orthogo-nal convergence

Trench-parallel displacement

Slab age

-1 -0.6 -0.2 0.2 0.6 1

Pearson correlation coefficient

Figure 5

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Sierra

Ma

dre

Orie

nta

l

Sie

rraM

adre

Occidental

Gulf o

f

Mexico Maya

(MiddleAmerica)

Chortís(Middle America)

Yucatánplatform

Cayman troughXolapa complex

P a c i f i cO c e a n

Ch iapas

massi f

Laramidefront

Central

Parral

Tahué

Cretaceous

Jurassic

Triassic

Permian

Carboniferous

Devonian

Detrital zirconpopulationsLocation ofigneous rocks

Symbol colors:

N0 200100 km

Juárez

Oaxaquia

Oaxaquia

Mixteca

Trans-MexicanVolcanic Belt

GuerreroCompositeTerrane

1:8,000,000Datum: WGS84

Projection: World Mercator

90° W95° W100° W105° W

25°N

20°N

15°N

Figure 6

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Figure 7

A (55–43° N)B (43–32° N)C (35–20° N)D (25–15° N)E (12° N–5° S)F (6–18° S)G (18–40° S)H (39–55° S)

0

0.2

0.4

0.6

0.8

Lag time (Ma)

0 2 4 6 8 10