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Triggering of volcanic degassing by large earthquakes

Dulcinea M. Avouris1,2, Simon A. Carn1, and Gregory P. Waite1 1Department of Geological and Mining Engineering and Sciences, Michigan Technological University, Houghton, Michigan 49931, USA 2Department of Geology, Kent State University, Kent, Ohio 44242, USA

ABSTRACT target volcanoes, covering a variety of eruption

Statistical analysis of temporal relationships between large earthquakes (Mw ≥ 7) and styles in diverse arc settings, from those with SO2 volcanic eruptions suggests that seismic waves may trigger eruptions over great (>1000 km) emissions detectable by OMI (e.g., Carn et al., distances from the epicenter, but a robust relationship between volcanic and teleseismic activity 2017): Ambrym and (); Bagana, remains elusive. Here we investigate the relationship between dynamic stresses propagated Rabaul, and Ulawun (Papua New Guinea);

by surface waves and a volcanic response, manifested by changes in sulfur dioxide (SO2) Fuego and Pacaya (Guatemala); Merapi, Semeru, emissions measured by the spaceborne Ozone Monitoring Instrument (OMI). Surface wave and Bromo (Indonesia); Turrialba (Costa Rica); amplitudes for a catalog of 69 earthquakes in A.D. 2004–2010 are modeled at 12 persistently and Villarrica (Chile) (Table DR1 in the GSA degassing volcanoes detected by the OMI. The volcanic response is assessed by examining Data Repository1). These volcanoes were all in

daily OMI SO2 measurements in 28 day windows centered on earthquakes meeting a vari- an open-vent state in 2004–2010 (i.e., with a able peak dynamic stress threshold. A positive volcanic response is identified if the average -atmosphere interface at or close to the

post-earthquake SO2 mass was at least 20% larger than the pre-earthquake SO2 mass. We surface), and therefore may be more sensitive to find two distinct volcanic responses, correlating strongly with eruption style. Open-vent, small earthquake-induced pressure changes. The basaltic volcanoes exhibit a positive response to earthquake-generated dynamic stress (i.e., eruptive styles represented range from active

the earthquake triggers increased SO2 discharge), and andesitic volcanoes exhibit a negative lakes (e.g., Ambrym, Villarrica) to open- response. We suggest that the former is consistent with disruption or mobilization of bubbles, vent degassing (e.g., Turrialba, Ulawun) to lava or magma sloshing, in low-viscosity , whereas the latter observation may reflect more dome growth (e.g., Merapi, Semeru, Bagana). dominant controls on degassing in viscous magmas or a post-earthquake reduction in perme- For each target, we created a time series of

ability. Overall this analysis suggests that the potential effects of large earthquakes should daily SO2 loading measured by OMI between be taken into account when interpreting trends in volcanic gas emissions. 1 October 2004 and 30 September 2010 (e.g., Fig. 1). Volcanic plume altitude affects the OMI

INTRODUCTION surface wave propagation from M7 and greater SO2 retrievals (Yang et al., 2007), and so OMSO2 The potential for triggering of volcanic activ- earthquakes in 2004–2010 to a selection of tar- products are provided for several assumed alti-

ity by large earthquakes has been pondered for get volcanoes with sulfur dioxide (SO2) emis- tudes (Carn et al., 2013), including lower tropo- centuries: Pliny the Elder addressed the topic in sions measurable by satellite remote sensing. sphere (~3 km altitude) and mid-troposphere (~8 A.D. 77–79 (Holland, 1601). Volcanic responses Surface wave modeling and the associated peak km). For plumes with a designated altitude in the to earthquakes are difficult to quantify in a robust dynamic stress (PDS) calculations provide a Smithsonian Institution volcanic activity reports manner, however, largely because only a small robust method for identifying the earthquakes (Global Volcanism Program; Venzke, 2013), the proportion of global volcanoes are adequately most likely to trigger a change in volcanic activ- OMSO2 product closest to the reported altitude

monitored. Despite this, there is mounting evi- ity. SO2 is the optimal indicator of volcanic was used. In all other cases the lower troposphere

dence for earthquake-triggered volcanic activity degassing because it is easily distinguishable SO2 product was used, assuming that passively

on various time scales (e.g., Linde and Sacks, against the atmospheric background; for this degassed SO2 would rise no higher than 3–4

1998; Brodsky et al., 1998; Manga and Brodsky, reason it is the most commonly measured volca- km at the target volcanoes. Daily SO2 loading 2006; Cigolini et al., 2007; Harris and Ripepe, nic gas, and thus it is also crucial to understand was calculated for each target in a 2° × 2007; Walter and Amelung, 2007; Walter et al., processes that modulate its emission. We use 2° region centered on the vent. Where the 2° ×

2007; Watt et al., 2009; De la Cruz-Reyna et al., daily measurements of volcanic SO2 emissions 2° regions for 2 or more volcanoes overlapped, 2010; Delle Donne et al., 2010). Some of these from the Ozone Monitoring Instrument (OMI) a larger box was established with boundaries studies have been catalyzed by decade-scale sat- on the NASA Aura satellite (Carn et al., 2013) 1° from the edges of the volcano cluster. This ellite remote sensing observations of volcanic that provide a consistent measure of volcanic resulted in the clustering of Ambrym and Gaua activity (e.g., Delle Donne et al., 2010). Quan- degassing to compare with calculated PDS. The (Fig. 1), Rabaul and Ulawun, Fuego and Pacaya; titative measurements of changes in both the availability of daily satellite measurements of and Merapi, Semeru, and Bromo; in these cases

earthquake-generated state of stress and volcanic volcanic SO2 emissions permits such an analysis multiple sources of SO2 degassing were consid- activity (including ground deformation, heat flux, on a large scale for the first time. ered as a single source. However, recent work and degassing) may provide greater insight into (Carn et al., 2017) indicates that the dominant

the triggering mechanism as well as the types of DATA AND METHODS SO2 sources in these regions are Ambrym,

volcanoes that may be susceptible to triggering. To quantify daily volcanic SO2 emissions, we Rabaul, Fuego, and Semeru-Bromo (emissions

However, to date there has been no analysis of use the operational OMI SO2 product derived from the latter are essentially indistinguishable in the volcanic response to earthquakes based on using the linear fit algorithm (Level 2 OMSO2 direct observations of volcanic degassing. data product; Yang et al., 2007), obtained from 1 GSA Data Repository item 2017230, additional results, Tables DR1–DR9, and Figures DR1and Here we assess the links between volcanic the NASA Goddard Earth Sciences Data and DR2, is available online at http://www.geosociety​.org​ degassing and dynamic (not static) stresses Information Services Center (DISC; http://disc. /datarepository​/2017/ or on request from editing@ propagated by large earthquakes by modeling sci.gsfc.nasa.gov/). We selected the following geosociety.org.

GEOLOGY, August 2017; v. 45; no. 8; p. 715–718 | Data Repository item 2017230 | doi:10.1130/G39074.1 | Published online 19 May 2017 ©GEOLOGY 2017 The Authors.| Volume Gold 45 |Open Number Access: 8 | www.gsapubs.orgThis paper is published under the terms of the CC-BY license. 715

Downloaded from http://pubs.geoscienceworld.org/gsa/geology/article-pdf/45/8/715/2315612/715.pdf by guest on 26 September 2021 5 more sophisticated modeling would significantly In order to compare the occurrence of posi- improve the discrepancy between the synthetic tive response to an earthquake to coinciden- 4 and real seismograms. tal occurrence of elevated SO2 emissions, we Synthetic seismograms were computed for repeated the same windowing analysis for each 3 M7.1 Vanuat u M8.1 Solomon Is eruption each earthquake in our catalog, using the tar- day of the study period. This revealed any nota- get volcano locations as receiver positions. We ble deviation in occurrence of response to an 2 mass [kilotons ]

2 used the synthetic seismograms to estimate the earthquake from that expected from random

SO PDS with the simplified shear-wave method of coincidence. We also further examined the varia- 1 Velasco et al. (2004): tion in SO2 response of two volcano clusters (Ambrym-Gaua and Merapi-Semeru-Bromo) by 0 PDS = vµβ/ , (1) stacking the SO emissions in a 31 day window 01/02 15/02 01/03 15/03 01/04 15/04 01/05 15/05 01/06 2 Date in 2007 (DD/MM) centered on each qualifying earthquake gener- Figure 1. Example of pre-earthquake and where v is ground velocity, µ is rigidity, and β ating PDS > 5 kPa. This provides a visualiza-

post-earthquake window analysis using a is shear wave velocity. We used average crustal tion of SO2 degassing patterns before and after time series of daily spaceborne Ozone Moni- values of 3.3 × 1010 Pa for µ and 3.5 km/s for each earthquake and reveals how degassing re- toring Instrument SO measurements (black 2 β (Velasco et al., 2004). Rather than calculate equilibrates after an earthquake. bars) at Ambrym-Gaua (Vanuatu), from 1 February to 1 June 2007. Two major regional separate PDS for Rayleigh and Love waves, the three components of each synthetic seismogram RESULTS AND DISCUSSION earthquakes occurred in this period: a Mw 7. 1 event in Vanuatu on 25 March and an Mw 8.1 were combined into a single velocity vector, PDS values calculated using modeled seis- event in the Solomon Islands (~1500 km from from which peak velocity was derived for the mograms contain more useful information than Ambrym) on 1 April (blue lines). The gray shad- time period spanning the arrivals of 40 s to 15 s moment magnitude because the effects of focal ing indicates the 14 day pre-earthquake and post-earthquake time windows in which daily period waves. Clearly our method does not prop- mechanism and distance are included. For exam-

SO2 loadings were averaged for the Mw 8.1 erly account for Rayleigh wave PDS, but serves ple, there are instances where the PDS generated Solomon Islands earthquake; horizontal red as a quantitative proxy for total surface wave PDS. by a smaller earthquake is higher for specific lines indicate the corresponding average SO 2 The OMI-derived SO mass was averaged volcanoes than the PDS generated by a larger loadings in the two windows, showing higher 2 in two 14 day windows, one preceding and one earthquake (e.g., Fig. DR1). Notably, an Mw SO2 after the earthquake. We also note that Lopevi (south of Ambrym) erupted on 20 April following each earthquake, including the day of 7.3 event generated a higher PDS than all other

2007. Lopevi was not included in our analysis, the event (e.g., Fig. 1). For each earthquake, the earthquakes up to Mw 8.0 (Fig. DR1). Full results but its eruption soon after two large regional ratio of post-earthquake average SO mass to of the 14 day SO data window analysis for each earthquakes is an interesting coincidence. 2 2 pre-earthquake average SO2 mass was calculated. target volcano or volcano cluster are reported in The relationship between earthquake occurrence Tables DR3–DR9, and summarized in Figure 2.

satellite data), respectively. The daily SO2 mass and SO2 mass ratio was evaluated with variable There are at least two challenges to assess- was smoothed using a 1 week moving average thresholds of 1.2–2.0 (Tables DR3–DR9). The ing the volcanic degassing response to earth-

to mitigate the impact of daily variations in OMI inverse of each SO2 mass ratio was also calcu- quakes with our method: the frequency of major viewing geometry (e.g., Flower et al., 2016), and lated, to investigate if the PDS changes caused earthquakes at shallow depths is relatively low,

OMI ultraviolet reflectivity data were also used a decrease in volcanic degassing (i.e., a negative and we expect any SO2 degassing response to

to screen excessively cloudy SO2 observations. response). These calculations were repeated for be modest and so not always detectable from Our earthquake catalog (69 events) was PDS from 5 to 100 kPa, to investigate the effect space. However, considering our target volca- derived from the U.S. Geological Survey global of different levels of dynamic stress. To mini- noes as an ensemble, two robust results emerge catalog (https://earthquake.usgs.gov/earthquakes​ ​ mize the influence of meteorological clouds on (Fig. 2): open-vent basaltic volcanoes show a

/search/), and includes all moment magnitude the SO2 data, we rejected days with a scene aver- clear occurrence of elevated SO2 output follow-

(Mw) ≥ 7 earthquakes at depths of ≤35 km age reflectivity value >35%; in addition, if fewer ing earthquakes that generated high PDS (posi- between 1 January 2004 and 30 September 2010 than 8 days in either window met the reflectivity tive response; e.g., Ambrym, Villarrica), and (Table DR2 in the GSA Data Repository). In criterion, the earthquake was rejected. volcanoes undergoing cyclic activity that may

addition, all Mw ≥ 8 events during the period are included, regardless of depth. We use Com- puter Programs in Seismology (CPS; Herrmann, Figure 2. Volcano response to earthquake peak dynamic 2013) to model surface wave amplitudes. CPS Merapi-Semeru-Bromo (7) stress (PDS) at the 1.2 SO2 produces synthetic seismograms based on a mass ratio level, indicating the percentage of positive layered Earth velocity model (ak135-F, http:// Fuego-Pacaya (5) ds.iris.edu/ds/products/emc-ak135-f/), the focal or negative response to earthquake PDS at 5 kPa mechanism, depth, and Mw of the earthquake, and 25 kPa threshold levels. Bagana (8) and incorporates the distance and azimuth of the The number of earthquakes target from the epicenter. To validate our syn- above the PDS threshold at each volcano is given thetic waveform data set, we compared a subset Villarrica (4) of synthetic seismograms to real data at a variety in parentheses (Tables DR3–DR [see footnote 1]). of azimuths and distances. We found that surface 5 kPa PDS Ambrym-Gaua (16) We observe a clear depen- wave amplitudes in the synthetic seismograms 25 kPa PDS dence of response on were typically within a factor of 2–3 of the real eruptive style: volcanoes data, consistent with other studies (e.g., van der Turrialba (5) with plugged conduits show a negative response, Lee, 1998). Although our modeling was rela- whereas low-viscosity tively simple and did not account for finite fault -100 -50 0 50 100 volcanic systems show a complexity (i.e., directivity), we do not feel that Volcano response (%) positive response.

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Downloaded from http://pubs.geoscienceworld.org/gsa/geology/article-pdf/45/8/715/2315612/715.pdf by guest on 26 September 2021 include conduit plugging by more viscous mag- (pumping of gas into preexisting bubbles; e.g., emissions until the degassing pathway is reestab-

mas seem to demonstrate reduced SO2 degassing Brodsky et al., 1998) or sloshing (or another lished. The cyclic nature of many dome-forming following such earthquakes (negative response; mass redistribution process) in a bubbly magma eruptions (e.g., Melnik and Sparks, 2005) may e.g., Merapi, Fuego, Bagana). In this study, body (e.g., Carbone et al., 2009; Namiki et al., also be a dominant control on degassing, render- only Rabaul-Ulawun did not show a measur- 2016). Disregarding rectified diffusion as inef- ing them less susceptible to earthquake-induced able degassing response to earthquake-induced ficient (e.g., Ichihara and Brodsky, 2006), and effects. It is notable that Bebbington and Mar- dynamic stress; this could provide insight into given that the estimated PDS is commensurate zocchi (2011) found no statistical evidence for the state of their magmatic plumbing systems. with the stresses expected to weaken crystal- significant earthquake triggering of eruptions at Here we focus on our most significant results, rich magma (e.g., Sumita and Manga, 2008), we Merapi, Semeru, or Bromo. i.e., the positive response of Ambrym-Gaua and favor a scenario whereby pockets of accumulated The earthquake sample size was lower for the negative response of Merapi-Semeru-Bromo bubbles in the plumbing system are disrupted our other target volcanoes (Tables DR3–DR9),

(Fig. 2). Ambrym-Gaua showed increased SO2 by dynamic strains, either mobilizing bubbles but the results concur with our proposed inter- emissions following 63% of earthquakes generat- or increasing permeability via bubble wall col- pretation. Villarrica hosts an active and

ing PDS of at least 5 kPa (Fig. 2), whereas higher lapse. Stacked plots of SO2 emissions (Fig. 3A) shows a positive degassing response (Fig. 2).

SO2 would be expected following only 41% of indicate that peak SO2 degassing occurs after a Persistent, open-vent SO2 emissions at Turri-

days selected at random. A stacked SO2 emis- few days, suggesting that SO2 release at the sur- alba (e.g., Campion et al., 2012), coupled with

sion plot (Fig. 3) indicates that SO2 degassing at face lags behind the triggering event (however, its positive response, point to the involvement

Ambrym (the dominant SO2 source) consistently we have no constraints on the behavior of other of low-viscosity magma supplying the emitted

increased in response to earthquake-generated volatiles, e.g., H2O). gases. This demonstrates the insight into vol- PDS. Ambrym hosted at least one active lava Merapi-Semeru-Bromo exhibited a negative canic systems that analysis of their response to lake during the study period, likely maintained by response at all PDS levels (e.g., Fig. 2). This earthquakes can yield. the convection of low-viscosity within the suggests minimal susceptibility to the effect of Negative responses similar to Merapi- lake and conduit, driven by degassing-induced dynamic stress, at least with respect to degassing Semeru-Bromo were also observed at Fuego- density variations (e.g., Stevenson and Blake, activity detectable from space. Figure 3B indi- Pacaya and Bagana (Fig. 2). The near-surface 1998). This suggests that a steady-state volca- cates a consistent decrease in degassing follow- viscosity of conduit plugs and likely exerts nic system that can maintain active lava lakes is ing each earthquake, with small post-event spikes a strong control on activity at both Fuego and

more easily perturbed by small dynamic stresses that are less than pre-earthquake SO2 emissions. Bagana (e.g., Lyons et al., 2009; McCormick et (5 kPa; Fig. 3), and that the system responds by We attribute this to the influence of higher viscos- al., 2012), with permeability governed by tran-

degassing SO2 as it re-equilibrates. ity basaltic-andesite or andesite magmas at these sient pore networks and cracks that could be sus- Given that our calculated PDS values are volcanoes, which typically erupt lava domes. In ceptible to dynamic stresses (e.g., Heap and Ken- likely far below the supersaturation pressures such systems, bubble rise is inhibited and degas- nedy, 2016). Thus in these cases permeability required for bubble nucleation (a few MPa in sing occurs primarily along permeable fracture controls on degassing are likely dominant. The silicic magmas; e.g., Hurwitz and Navon, 1994), networks in the conduit (e.g., Edmonds et al., only neutral result in our analysis was found at possible mechanisms to explain earthquake- 2003). Earthquake-induced stresses could act to Rabaul-Ulawun, which displayed no clear degas-

triggered degassing include rectified diffusion modify or close existing fractures, reducing SO2 sing response. There are many possible reasons for this, including opposing responses at each volcano (canceling out any net degassing signal), Ambrym-Gaua Merapi-Semeru-Bromo or the effects of static stress changes or fault rup- 6 1.2 ture directivity (e.g., Delle Donne et al., 2010). ABOur results indicate a striking dependence of

5 1 the volcanic degassing response to earthquake- induced stresses on magma viscosity and eruptive style. We therefore recommend that interpreta- 4 0.8 tion of SO2 emission time series at actively degas- sing volcanoes takes into account the potential 3 0.6 effects of large earthquakes on observed trends. emission (kt) emission (kt) 2 2 More significant insights into the nature of volca- nic responses to earthquake-induced stresses are 2 0.4 sure to arise from the coming years of observa- erage SO erage SO tions of volcanic activity from space. Av Av 1 0.2 ACKNOWLEDGMENTS We acknowledge R. Hermann for his help with the CPS 0 0 (Computer Programs in Seismology) code. Ben Kennedy -15 -10-50 51015 -15-10 -5 0510 15 and Michael Manga provided constructive reviews that Days relative to earthquake Days relative to earthquake greatly improved the paper. This work was supported by the Michigan Space Grant Consortium (Avouris) and Figure 3. Stacked SO emission time series covering 15 days before and after earthquakes 2 NASA (Aura Science Team grant NNX11AF42G and that produced estimated peak dynamic stress (PDS) of at least 5 kPa at 2 volcano clusters. A: MEaSUREs grant NNX13AF50G to Carn). Ambrym-Gaua (Vanuatu). B: Merapi-Semeru-Bromo (Indonesia). Each plot shows the mean (bold line), median (dashed line), and individual time series (gray lines). In addition to the PDS REFERENCES CITED calculation, the number of time series varies depending on availability of SO2 data: 6 (A) and Bebbington, M.S., and Marzocchi, W., 2011, Stochas- 13 (B). At Ambrym and Gaua, the results suggest a delayed increase in SO2 emissions begin- tic models for earthquake triggering of volcanic ning ~5 d after an earthquake. Conversely, at Merapi-Semeru-Bromo, SO2 emissions appear to decrease following earthquakes. Figure DR2 (see footnote 1) shows the same plot for a eruptions: Journal of Geophysical Research, PDS of at least 25 kPa. v. 116, B05204, doi:​10​.1029​/2010JB008114.

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Downloaded from http://pubs.geoscienceworld.org/gsa/geology/article-pdf/45/8/715/2315612/715.pdf by guest on 26 September 2021 Brodsky, E.E., Sturtevant, B., and Kanamori, H., time-series analysis of volcanic emissions: Re- Volcanology and Geothermal Research, v. 320, 1998, Earthquakes, volcanoes, and rectified dif- mote Sensing of Environment, v. 183, p. 282–293, p. 156–171, doi:10​ .1016​ /j​ .jvolgeores​ .2016​ .03​ .010.​ fusion: Journal of Geophysical Research, v. 103, doi:​10​.1016​/j​.rse​.2016​.05​.022. Stevenson, D.S., and Blake, S., 1998, Modelling the p. 23,827–23,838, doi:​10​.1029​/98JB02130. Harris, A.J.L., and Ripepe, M., 2007, Regional earth- dynamics and thermodynamics of volcanic de- Campion, R., Martinez-Cruz, M., Lecoq, T., Caudron, quake as a trigger for enhanced volcanic activity: gassing: Bulletin of Volcanology, v. 60, p. 307– C., Pacheco, J., Pinardi, G., Hermans, C., Carn, S., Evidence from MODIS thermal data: Geophysi- 317, doi:​10​.1007​/s004450050234. and Bernard, A., 2012, Space- and ground-based cal Research Letters, v. 34, L02304, doi:​10.1029​ ​ Sumita, I., and Manga, M., 2008, Suspension rheol- measurements of sulphur dioxide emissions from /2006GL028251. ogy under oscillatory shear and its geophysical Turrialba Volcano (Costa Rica): Bulletin of Volca- Heap, M.J., and Kennedy, B.M., 2016, Exploring the implications: Earth and Planetary Science Let- nology, v. 74, p. 1757–1770, doi:10​ .1007​ /s00445​ ​ scale-dependent permeability of fractured andes- ters, v. 269, p. 468–477, doi:​10​.1016​/j​.epsl​.2008​ -012​-0631​-z. ite: Earth and Planetary Science Letters, v. 447, .02​.043. Carbone, D., Jousset, P., and Musumeci, C., 2009, p. 139–150, doi:​10​.1016​/j​.epsl​.2016​.05​.004. van der Lee, S., 1998, Observations and origin of Ray- Gravity ‘steps’ at Mt. Etna volcano (Italy): In- Herrmann, R.B., 2013, Computer programs in seis- leigh-wave amplitude anomalies: Geophysical strumental effects or evidences of earthquake- mology: An evolving tool for instruction and Journal International, v. 135, p. 691–699, doi:​10​ triggered magma density changes?: Geophysi- research: Seismological Research Letters, v. 84, .1046​/j​.1365​-246x​.1998​.00678​.x. cal Research Letters, v. 36, L02301, doi:​10.1029​ ​ p. 1081–1088, doi:​10​.1785​/0220110096. Velasco, A.A., Ammon, C.J., Farrell, J., and Pankow, /2008GL036179. Holland, P., translator, 1601, The historie of the world, K., 2004, Rupture directivity of the 3 November Carn, S.A., Krotkov, N.A., Yang, K., and Krueger, A.J., commonly called, The naturall historie of C. Plin- 2002 Denali fault earthquake determined from 2013, Measuring global volcanic degassing with ius Secundus: London, A. Islip, p. 1–49: http:// surface waves: Seismological Society of Amer- the Ozone Monitoring Instrument (OMI), in Pyle, penelope.uchicago.edu/holland/index.html (ac- ica Bulletin, v. 94, p. S293–S299, doi:​10​.1785​ D.M., et al., eds., Remote sensing of volcanoes cessed March 2017). /0120040624. and volcanic processes: Integrating observation Hurwitz, S., and Navon, O., 1994, Bubble nucleation Venzke, E., ed., 2013, Volcanoes of the World, v. 4.5.0: and modeling: Geological Society of London in rhyolitic melts: Experiments at high pressure, Washington, D.C., Smithsonian Institution Global Special Publication 380, p. 229–257, doi:​10.1144​ temperature, and water content: Earth and Plan- Volcanism Program, doi:10​ .5479​ /si​ .GVP​ .VOTW4​ ​ /SP380​.12. etary Science Letters, v. 122, p. 267–280, doi:10​ ​ -2013 (accessed 22 August 2016). Carn, S.A., Fioletov, V., McLinden, C.A., Li, C., and .1016​/0012​-821X​(94)90001​-9. Walter, T.R., and Amelung, F., 2007, Volcanic erup- Krotkov, N.A., 2017, A decade of global volca- Ichihara, M., and Brodsky, E.E., 2006, A limit on the tions following M ≥ 9 megathrust earthquakes:

nic SO2 emissions measured from space: Scien- effect of rectified diffusion in volcanic systems: Implications for the Sumatra-Andaman volca- tific Reports, v. 7, 44095, p. 1–12, doi:​10​.1038​ Geophysical Research Letters, v. 33, L02316, doi:​ noes: Geology, v. 35, p. 539–542, doi:10​ ​.1130​ /srep44095. 10​.1029​/2005GL024753. /G23429A​.1. Cigolini, C., Laiolo, M., and Coppola, D., 2007, Earth- Linde, A.T., and Sacks, I.S., 1998, Triggering of vol- Walter, T.R., Wang, R., Zimmer, M., Grosser, H., Lühr, quake-volcano interactions detected from radon canic eruptions: Nature, v. 395, p. 888–890, doi:​ B., and Ratdomopurbo, A., 2007, Volcanic activ- degassing at Stromboli (Italy): Earth and Plan- 10​.1038​/27650. ity influenced by tectonic earthquakes: Static and etary Science Letters, v. 257, p. 511–525, doi:10​ ​ Lyons, J.J., Waite, G.P., Rose, W.I., and Chigna, G., dynamic stress triggering at Mt. Merapi: Geo- .1016​/j​.epsl​.2007​.03​.022. 2009, Patterns in open vent, Strombolian behavior physical Research Letters, v. 34, L05304, doi:​ De la Cruz-Reyna, S., Tárraga, M., Ortiz, R., and Mar- at Fuego volcano, Guatemala, 2005–2007: Bul- 10.1029​/2006GL028710. tínez-Bringas, A., 2010, Tectonic earthquakes trig- letin of Volcanology, v. 72, p. 1–15, doi:10​ ​.1007​ Watt, S., Pyle, D.M., and Mather, T.A., 2009, The in- gering volcanic seismicity and eruptions. Case /s00445​-009​-0305​-7. fluence of great earthquakes on volcanic eruption studies at Tungurahua and Popocatépetl volca- Manga, M., and Brodsky, E., 2006, Seismic trigger- rate along the Chilean subduction zone: Earth noes: Journal of Volcanology and Geothermal Re- ing of eruptions in the far field: Volcanoes and and Planetary Science Letters, v. 277, p. 399–407, search, v. 193, p. 37–48, doi:10​ .1016​ /j​ .jvolgeores​ ​ geysers: Annual Review of Earth and Planetary doi:​10​.1016​/j​.epsl​.2008​.11​.005. .2010.03​ .005.​ Sciences, v. 34, p. 263–291, doi:10​ .1146​ /annurev​ ​ Yang, K., Krotkov, N.A., Krueger, A.J., Carn, S.A., Delle Donne, D., Harris, A.J.L., Ripepe, M., and .earth​.34​.031405​.125125. Bhartia, P.K., and Levelt, P.F., 2007, Retrieval of

Wright, R., 2010, Earthquake-induced thermal McCormick, B.T., Edmonds, M., Mather, T.A., and large volcanic SO2 columns from the Aura ozone anomalies at active volcanoes: Geology, v. 38, Carn, S.A., 2012, First synoptic analysis of volca- monitoring instrument: Comparison and limita- p. 771–774, doi:​10​.1130​/G30984​.1. nic degassing in Papua New Guinea: Geochemis- tions: Journal of Geophysical Research, v. 112, Edmonds, M., Oppenheimer, C., Pyle, D.M., Herd, try, Geophysics, Geosystems, v. 13, Q03008, doi:​ D24S43, doi:​10​.1029​/2007JD008825.

R.A., and Thompson, G., 2003, SO2 emissions 10​.1029​/2011GC003945. from Soufrière Hills Volcano and their relation- Melnik, O., and Sparks, R.S.J., 2005, Controls on con- ship to conduit permeability, hydrothermal inter- duit magma flow dynamics during lava dome build- action and degassing regime: Journal of Volcanol- ing eruptions: Journal of Geophysical Research, Manuscript received 17 February 2017 ogy and Geothermal Research, v. 124, p. 23–43, v. 110, B02209, doi:​10​.1029​/2004JB003183. Revised manuscript received 2 April 2017 doi:​10​.1016​/S0377​-0273​(03)00041​-6. Namiki, A., Rivalta, E., Woith, H., and Walter, T.R., Manuscript accepted 19 April 2017 Flower, V.J.B., Carn, S.A., and Wright, R., 2016, The 2016, Sloshing of a bubbly magma reservoir as impact of satellite sensor viewing geometry on a mechanism of triggered eruptions: Journal of Printed in USA

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