Dynamics of a large, restless, rhyolitic magma system at Laguna del Maule, southern Andes, Chile

Explosive eruptions of large-volume rhyolitic magma systems are common in the geologic record and pose a major potential threat to society. Unlike other natural hazards, such as earthquakes and tsunamis, a large rhyolitic volcano may provide warning signs long before a caldera-forming eruption occurs. Yet, these signs—and what they imply about magma-crust dynamics—are not well known. This is because we have learned how these systems form, grow, and erupt mainly from the study of ash flow tuffs deposited tens to hundreds of thousands of years ago or more, or from the geophysical imaging of the unerupted portions of the reservoirs beneath the associated calderas. The Laguna del Maule Volcanic Field, Chile, includes an unusually large and recent concentration of silicic eruptions. Since 2007, the crust there has been inflating at an astonishing rate of at least 25 cm/yr. This unique opportunity to investigate the dynamics of a large rhyolitic system while magma migration, reservoir growth, and crustal deformation are actively under way is stimulating a new international collaboration. Findings thus far lead to the hypothesis that the silicic vents have tapped an extensive layer of crystal-poor, rhyolitic melt that began to form atop a magmatic mush zone that was established by ca. 20 ka with a renewed phase of rhyolite eruptions during the Holocene. Modeling of surface deformation, magnetotelluric data, and gravity changes suggest that magma is currently intruding at a depth of ~5 km. The next phase of this investigation seeks to enlarge the sets of geophysical and geochemical data and to use these observations in numerical models of system dynamics. INTRODUCTION Caldera-scale rhyolitic volcanoes can rapidly deposit hundreds of cubic kilometers of ash over several million square kilometers, threatening people and agriculture at the scale of an entire continent (Sparks et al., 2005; Lowenstern et al., 2006; Self, 2006). Sooner or later, Earth will experience another eruption of this magnitude (Lowenstern et al., 2006; Self and Blake, 2008); consequently, there is a need to gather comprehensive information and create multi-scale models that realistically capture the dynamics leading to these destructive events. Most of our current understanding of this type of volcanic system has been gleaned from the study of eruptive products long after the catastrophic eruption, including voluminous ash flow deposits, such as the Bishop, Bandelier, Huckleberry Ridge, and Oruanui Tuffs (Lowenstern et al., 2006; Hildreth and Wilson, 2007; Bachmann and Bergantz, 2008; Wilson, 2008). The most recent rhyolitic “super-eruption” produced the Oruanui Tuff 26,500 years ago in New Zealand. Even in this relatively recent case, the geologic evidence has been partly obliterated by caldera-collapse, erosion, and burial (Wilson et al., 2005). Moreover, probing the present-day structures beneath a number of calderas using seismic tomography (e.g., Romero et al., 1993; Steck et al., 1998; Farrell et al., 2014) or other geophysical measures (e.g., Lowenstern et al., 2006; Battaglia et al., 2003; Tizzani et al., 2009) has not detected eruptible domains of crystal-poor melt in the shallow crust, nor has it captured the dynamics that preceded these large eruptions. This paper focuses on the Laguna del Maule Volcanic Field, Chile, a large, potentially hazardous, rhyolitic magmatic system, where an alarming rate of surface uplift for the past seven years and concentrated swarms of shallow earthquakes prompted Observatorio Volcanologico de los Andes del Sur (OVDAS) to declare in March 2013 a yellow alert, signaling a potential eruption within months or years. Straddling the Andean range crest at 36° S (Fig. 1A), this volcanic field features: (1) 13 km of rhyolite that erupted both explosively and effusively during the past 20 k.y.; (2) a zone of low electrical resistivity in the shallow crust below the deforming area; (3) widespread elevated CO 2 concentrations; and (4) a negative (~10 mGal) Bouguer anomaly and preliminary evidence for a positive dynamic gravity signal indicating mass addition. The underlying magma system has been sampled by eruptions numerous times since its apparent inception in the late Pleistocene, including a dozen crystal-poor, glassy rhyolitic lavas during the Holocene. Linking the assembly and evolution of this

[1]  J. Farrell,et al.  Tomography from 26 years of seismicity revealing that the spatial extent of the Yellowstone crustal magma reservoir extends well beyond the Yellowstone caldera , 2014 .

[2]  Kurt L. Feigl,et al.  Rapid uplift in Laguna del Maule volcanic field of the Andean Southern Volcanic zone (Chile) 2007–2012 , 2014 .

[3]  K. Feigl,et al.  Unrest within a large rhyolitic magma system at Laguna del Maule volcanic field (Chile) from 2007 through 2013: geodetic measurements and numerical models , 2013 .

[4]  D. Günther,et al.  Tracking the evolution of large-volume silicic magma reservoirs from assembly to supereruption , 2013 .

[5]  Antonio G. Camacho,et al.  Diapiric ascent of silicic magma beneath the Bolivian Altiplano , 2013 .

[6]  Matthew E. Pritchard,et al.  Decadal volcanic deformation in the Central Andes Volcanic Zone revealed by InSAR time series , 2013 .

[7]  Paul Lundgren,et al.  Source model of deformation at Lazufre volcanic center, central Andes, constrained by InSAR time series , 2013 .

[8]  M. Unsworth,et al.  Mapping the Distribution of Fluids in the Crust and Lithospheric Mantle Utilizing Geophysical Methods , 2013 .

[9]  Demitris Paradissis,et al.  Evolution of Santorini Volcano dominated by episodic and rapid fluxes of melt from depth , 2012 .

[10]  Fanis Moschas,et al.  Recent geodetic unrest at Santorini Caldera, Greece , 2012 .

[11]  A. Pommier,et al.  "SIGMELTS": A web portal for electrical conductivity calculations in geosciences , 2010, Comput. Geosci..

[12]  Jamie Farrell,et al.  An extraordinary episode of Yellowstone caldera uplift, 2004–2010, from GPS and InSAR observations , 2010 .

[13]  Matthew E. Pritchard,et al.  Duration, magnitude, and frequency of subaerial volcano deformation events: New results from Latin America using InSAR and a global synthesis , 2010 .

[14]  W. Hildreth,et al.  Laguna del Maule Volcanic Field: Eruptive history of a Quaternary basalt-to-rhyolite distributed volcanic field on the Andean rangecrest in central Chile , 2010 .

[15]  Paolo Berardino,et al.  Uplift and magma intrusion at Long Valley caldera from InSAR and gravity measurements , 2009 .

[16]  O. Bachmann,et al.  Rhyolites and their Source Mushes across Tectonic Settings , 2008 .

[17]  Mark S. Ghiorso,et al.  Thermodynamics of Rhombohedral Oxide Solid Solutions and a Revision of the FE-TI Two-Oxide Geothermometer and Oxygen-Barometer , 2008, American Journal of Science.

[18]  C. Wilson Supereruptions and Supervolcanoes: Processes and Products , 2008 .

[19]  P. Renne,et al.  Implications of pre-eruptive magmatic histories of zircons for U–Pb geochronology of silicic extrusions , 2008 .

[20]  M. Reid How Long Does It Take to Supersize an Eruption , 2008 .

[21]  S. Self,et al.  Consequences of Explosive Supereruptions , 2008 .

[22]  K. Cooper,et al.  Uranium-series Crystal Ages , 2008 .

[23]  E. Watson,et al.  New thermodynamic models and revised calibrations for the Ti-in-zircon and Zr-in-rutile thermometers , 2007 .

[24]  Colin J. N. Wilson,et al.  Compositional Zoning of the Bishop Tuff , 2007 .

[25]  J. Lowenstern,et al.  Monitoring super-volcanoes: geophysical and geochemical signals at Yellowstone and other large caldera systems , 2006, Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences.

[26]  S. Self The effects and consequences of very large explosive volcanic eruptions , 2006, Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences.

[27]  D. Vokrouhlický,et al.  Seismic Triggering of Eruptions in the Far Field : Volcanoes and Geysers , 2006 .

[28]  Michael Manga,et al.  Seismic triggering of eruptions in the far field , 2006 .

[29]  Yongwimon Lenbury,et al.  Three-dimensional magnetotelluric inversion : data-space method , 2005 .

[30]  C. Oppenheimer,et al.  Super-eruptions: global effects and future threats , 2005 .

[31]  J. Lowenstern,et al.  Magma Generation at a Large, Hyperactive Silicic Volcano (Taupo, New Zealand) Revealed by U–Th and U–Pb Systematics in Zircons , 2005 .

[32]  W. Hildreth Volcanological perspectives on Long Valley, Mammoth Mountain, and Mono Craters: several contiguous but discrete systems , 2004 .

[33]  D. DePaolo,et al.  A model for the origin of large silicic magma chambers: precursors of caldera-forming eruptions , 2003 .

[34]  P. Segall,et al.  Constraining the nature of the source using geodetic and microgravity data , 2003 .

[35]  C. Thurber,et al.  Crust and upper mantle P wave velocity structure beneath Valles caldera, New Mexico: Results from the Jemez teleseismic tomography experiment , 1998 .

[36]  A. Michelini,et al.  Velocity structure of the Long Valley caldera from the inversion of local earthquake P and S travel times , 1993 .