Lateral movement of lithospheric fragments along strike-slip faults in response to collision (escape tectonics) has characterized convergent settings since the onset of plate tectonics and is a mechanism for the formation of new plates. The Anatolian plate was created by the sequential connection of strike-slip faults following ≥10 m.y. of distributed deformation that ultimately localized into plate-bounding faults. Thermochronology data and seismic images of lithosphere structure near the East Anatolian fault zone (EAFZ) provide insights into the development of the new plate and escape system. Low-temperature thermochronology ages of rocks in and near the EAFZ are significantly younger than in other fault zones in the region, e.g., apatite (U-Th)/He: 11–1 Ma versus 27–13 Ma. Young apatite (U-Th)/He ages and thermal history modeling record thermal resetting along the EAFZ over the past ~5 m.y. and are interpreted to indicate thermal activity triggered by strike-slip faulting in the EAFZ as it formed as a through-going, lithosphere-scale structure. The mechanism for EAFZ formation may be discerned from S-wave velocity images from the Continental Dynamics–Central Anatolian Tectonics (CD-CAT) seismic experiment. These images indicate that thin but strong Arabian lithospheric mantle extends ~50–150 km north beneath Anatolian crust and would have been located near the present surficial location of the Bitlis-Zagros suture zone (co-located with the EAFZ in our study area) at ca. 5 Ma. Underthrusting of strong Arabian lithosphere facilitated localization of the EAFZ and thus was a fundamental control on the formation of the Anatolian plate and escape system.

The formation of a new tectonic plate occurs when lithospheric weak zones localize deformation (Tackley, 2000) and connect to create a block of fault-bounded lithosphere that moves in a direction distinct from that of the ancestral plate. Plate formation by this mechanism has likely occurred since the inception of plate tectonics, although this process can be documented only in opportune cases, such as the Anatolian plate. In this study, we show how and when the Anatolian plate was created from the Eurasian plate.

One mode of plate formation is associated with escape tectonics, a strike-slip–dominated regime of large-scale transport of lithosphere obliquely away from a convergent zone, as is occurring today in Anatolia, SE Asia and other regions related to India-Asia collision, the western Pacific, and the Caribbean (Burke and Şengör, 1986). The relative importance of push (collision) and pull (retreating subduction) in driving escape has long been debated (Tapponnier et al., 1982; Faccenna et al., 2013).

The Anatolian plate developed under near-ideal conditions for escape owing to components of push (Arabia-Eurasia collision) and pull (Aegean slab pull), assisted by favorably oriented lithospheric weak zones and rheological boundaries (Black Sea region lithosphere; Molnar and Dayem, 2010). Nevertheless, the development of the escape system was protracted: It took ≥10 m.y. after early to mid-Miocene Arabia-Anatolia collision (i.e., so-called “hard collision”) for the East Anatolian fault zone (EAFZ) to form as a through-going fault. We evaluate the timing and contributing factors in the development of escape tectonics, with a focus on the EAFZ because its formation completed the escape system and created the Anatolian plate.

Anatolia was assembled by numerous subduction and collision events. Late Mesozoic–early Paleogene metamorphism, magmatism, and deformation were followed by extension in the west, collision in the east, slab tearing/break-off below central and eastern Anatolia, extension-driven exhumation of midcrustal rocks, episodic and voluminous volcanism, and uplift of a plateau and mountain ranges (Schildgen et al., 2014; Okay et al., 2020).

Arabia-Eurasia convergence was a driver of the escape system. Collision resulted in widespread deformation, with effects as far west as the Central Anatolian fault zone (Fig. 1A; Umhoefer et al., 2020). Low-temperature thermochronology from the Bitlis-Zagros suture zone (BZSZ) and the timing of Miocene marine carbonate sedimentation indicate complete closure of a marine basin by ca. 20 Ma (Okay et al., 2010; Cavazza et al., 2018).

Evidence from faults and other deformation features across central/eastern Anatolia indicates a transition from approximately N-S regional transpression to N-S compression accommodated by approximately E-W extension from ca. 25 to 5 Ma (Kaymakçı et al., 2010; Umhoefer et al., 2020). A subducted slab below Anatolia experienced tearing and break-off at ca. 13–11 Ma, corresponding to volcanism in central and eastern Anatolia and uplift of the Tauride Mountains (e.g., Meijers et al., 2018).

The boundaries of the Anatolian plate are the conjugate North and East Anatolian fault zones and a megathrust accommodating subduction of African lithosphere in the west and south (Fig. 1A). The timing of faulting has been determined by a variety of methods, including dating volcanic rocks in fault zones. The >1200-km-long dextral North Anatolian fault zone (NAFZ) formed by ca. 15–11 Ma in the east and propagated to the west (Şengör et al., 2005). There have been fewer studies of the ~700-km-long EAFZ. A wide range of ages has been proposed, but most estimates are Pliocene (McKenzie, 1976; Muehlberger and Gordon, 1987; Rojay et al., 2001; Cosca et al., 2021). The EAFZ exhibits transpression and transtension segments in a dominantly sinistral strike-slip system (Duman and Emre, 2013).

To evaluate the age of the EAFZ, formation of the Anatolian plate, and inception of escape tectonics, we obtained low-temperature thermochronology data from metamorphic and intrusive rocks in and near the EAFZ and other major faults, and we evaluated these data in the context of seismic images that illuminate lithosphere structure.


We present apatite fission-track (AFT) ages from 14 samples and 109 apatite and 12 zircon single-grain (U-Th)/He (AHe and ZHe) ages from 23 and 4 samples, respectively, including 21 samples from a NW-SE traverse of Late Cretaceous metamorphic rocks of the Pütürge massif across the EAFZ near where the Euphrates River is displaced by the fault (Figs. 1B and 2; for methods and full data set, see Supplemental Material1 and Tables S2–S5). These thermochronometers record cooling <~200–160 °C (ZHe), ~120–100 °C (AFT), and ~70–50 °C (AHe) for cooling rates of 1–10 °C/m.y.

AFT ages near the EAFZ are between 22 and 11 Ma (Figs. 1B and 2; Tables S2–S3). In the near-Euphrates traverse, AFT ages (ca. 16–10 Ma) are similar over ~1400 m in elevation change, consistent with rapid mid-Miocene cooling. This matches the time of rapid cooling reported in thermochronologic studies along the BZSZ to the east (Okay et al., 2010; Cavazza et al., 2018), interpreted as recording increased exhumation rates related to mid-Miocene hard collision.

AHe data show significant intrasample age dispersion with no correlation of age versus U and Th concentration and/or grain size. In the absence of such correlations, age dispersion in rapidly cooled samples is most likely caused by excess He such that the AHe grain age of the youngest sample represents the time of fast cooling (He et al., 2021; Tables S2 and S4). In our study, the youngest AHe grain ages mostly range from 15 to 5 Ma, with very young ages (<3 Ma) only in the EAFZ.

Single-grain ZHe ages from the near-Euphrates traverse are between 35 and 14 Ma (Fig. 2; Tables S2 and S5). ZHe ages SE of the EAFZ are younger (26–14 Ma) than those on the NW side (35–25 Ma), with the latter being slightly younger than ca. 39–36 Ma ZHe ages reported by Cavazza et al. (2018) ~10 km SW of the traverse (Fig. 1B).

Thermal History Modeling

We conducted inverse thermal history modeling (QTQt) on samples with age data from multiple thermochronometers, including multisample modeling from three traverses over a range of elevations (Figs. 3A3C; Supplemental Material S1 and Figs. S6–S9). Nearly all modeling results support rapid cooling through the AFT partial annealing zone ca. 18–12 Ma, as previously reported along the BZSZ to the east (Okay et al., 2010; Cavazza et al., 2018). To predict the very young AHe ages from the EAFZ traverse, the modeling results favor a period of short-lived reheating followed by rapid cooling to surface temperatures over the past ~5–4 m.y. confined to the EAFZ. Modeling results from other parts of the Pütürge massif and Mount Berit to the west of the EAFZ (Figs. 3B3C) show only steady Pliocene to Pleistocene cooling.

The crust and upper-mantle structure in and near the EAFZ is revealed by S-wave velocities derived from joint inversion of P-wave receiver functions and Rayleigh wave dispersion data (Abgarmi et al., 2017; Delph et al., 2017). Results show that the western half of the EAFZ cuts through a region underlain by fast S-wave velocities (~4.4–4.6 km/s; Figs. 1B and 4). These velocities are more consistent with Arabian plate lithospheric mantle (~4.5 km/s) than velocities of Anatolian lithospheric mantle (~4.2 km/s), despite lying ~50–150 km N of the surface expression of the BZSZ (Figs. 1B and 4; Fig. S10), and they show clear continuity with the Arabian upper-mantle structure. Therefore, we interpret these fast upper-mantle seismic velocities to represent rigid lithospheric mantle underthrusting the slow (and therefore weak and/or thin-to-negligible) lithospheric mantle of the Anatolian plate. Indeed, geochemical evidence from basalts in the Anatolian plate indicates that a thin lithospheric mantle has existed below Anatolia since at least the mid-Miocene (Reid et al., 2019). The patterns of lithospheric mantle velocity structure today may reflect variations in the precollision geometry and structure of the northern Arabian margin.

Prior to the inception of the full escape system with the formation of the NAFZ and EAFZ, a broad region of Anatolia was deformed in response to Arabia-Eurasia collision (Albino et al., 2014; Darin et al., 2018; Umhoefer et al., 2020), initially in compression and later (by early Miocene) mostly under transtension (Kaymakçı et al., 2010). This phase of widespread distributed deformation driven by collision (“proto-escape”) was protracted (ca. 23–5 Ma).

There was a major change in fault activity in many regions of the Arabia-Eurasia collision zone ca. 5 Ma (e.g., Allen et al., 2004). In addition, eastern Mediterranean marine basin sediments record a transition from thrusting to major subsidence at 5 Ma (Burton-Ferguson et al., 2005) related to a shift from contraction to transtension that is recorded up to the western border of submarine Arabian continental crust (Fig. 1A). The SE Anatolian plate boundary was dominated by strike-slip tectonics after ca. 5 Ma, when we propose that the EAFZ became a through-going structure linking the NAFZ and the Dead Sea fault zone (Fig. 1A). Rapid cooling following increased heat flow at ca. 5 Ma in the EAFZ is recorded by apatite He ages, coeval with the onset of basaltic volcanism (5–2.6 Ma) near the current location of the Anatolia-Arabia-Africa triple junction (Cosca et al., 2021; site of the 2023 M = 7.8 earthquake) and major rapid rearrangement of drainage systems within the uplifted Central Anatolian Plateau (Brocard et al., 2021), indicating that the transition to a strike-slip–dominated system was a regional phenomenon.

We interpret the young ages in and near the EAFZ to record heating driven by infiltration of hot fluids in fractured rock, as indicated by hot springs and travertine deposits (Duman and Emre, 2013). The geochemistry of thermal fluids in the EAFZ has a mantle signature, providing evidence for their deep-seated origin, even in fault segments not associated with magmatic activity (Italiano et al., 2013). The near-Euphrates traverse crosses a deep valley carved into fractured schist; the combination of focused erosion and fault-related infiltration of thermal fluids at temperatures high enough to reset apatite thermochronometers could explain the young ages in/near the EAFZ. Resetting of AHe and AFT ages by fault-related fluids has been documented in both strike-slip and normal faults (e.g., Wölfler et al., 2010).

The restriction of young ages to the vicinity of the EAFZ indicates its significance as a major structure starting ca. 5 Ma, which is >10–35 m.y. after the much-debated timing of Arabia-Eurasia collision. It is also long after the start of major extension in the Aegean (ca. 45 Ma), 10 m.y. after a significant increase in the rate of extension in the Aegean (ca. 15 Ma; Thomson et al., 1998), and at least 6–8 m.y. after tearing and break-off of the subducting slab below Anatolia (Reid et al., 2019).

Today, the inferred Arabia plate lithospheric mantle extends 100 ± 50 km north of the BZSZ under Anatolian crust (Figs. 1B and 4; Fig. S10). If we assume that this lithosphere was underthrust at a rate similar to modern convergence rates (~18 mm/yr), then the boundary was ~90 km south of its current location at 5 Ma, i.e., ~10 ± 50 km north of the suture. This significant rheological boundary at the margin of underthrust Arabian mantle likely facilitated localization of the EAFZ.

Anatolia is ideal for evaluating how and over what time scale strike-slip faults become boundaries of a new plate. Lithosphere-scale strike-slip faults develop in orthogonal and oblique convergence but in most cases do not become plate-bounding structures. The development of an escape system, and therefore the creation of a plate such as Anatolia, requires a combination of collision and slab pull, with the latter related in part to mantle flow and slab dynamics, including tearing and fragmentation such as are observed in central Anatolia (e.g., Faccenna et al., 2014). The Ailao Shan–Red River shear zone in SE Asia may be analogous to the Anatolian escape structures in that it is an intracontinental fault zone at the edge of an orogenic plateau, connecting a convergence zone with extension in a marine basin (Leloup et al., 2001).

The Anatolian region had many factors facilitating the development of tectonic escape: high-angle indentation by Arabia, rheologically strong regions to the north and south, preexisting weak zones in favorable orientation relative to convergence, and ongoing extension in the west. Rheological boundaries controlled the locations of both major, ultimately plate-bounding, strike-slip faults. In the case of the EAFZ, the rheological boundary is between the Eurasian plate and the underthrusting strong Arabia plate lithospheric mantle, culminating in creation of the Anatolian plate at ca. 5 Ma.

1Supplemental Material. S1: Description of thermochronology methods and associated references. Tables S2–S5. S6-8: Maximum Mode thermal history. S6-9: Summary of graphical QTQt inverse thermal modeling plots. Figures S6–S10. Please visit to access the supplemental material, and contact with any questions.

This research was funded by National Science Foundation grants “Continental Dynamics: Central Anatolian Tectonics” (CD-CAT) to Whitney and Teyssier (EAR-1109762); to Umhoefer (EAR-1109826); and to Thomson and Beck (EAR-1109336). Samples were collected by C. Lefebvre and analyzed with the assistance of P. Reiners. We thank U.S. Geological Survey reviewers N. Griffis and C. Sturrock and journal reviewers W. Cavazza, T. Schildgen, and two anonymous reviewers. Any use of trade, firm, or product names is for descriptive purposes only and does not imply endorsement by the U.S. government.

Gold Open Access: This paper is published under the terms of the CC-BY license.