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By: Marino Protti 1 , Victor González 1 , Andrew V. Newman 2* , Timothy H. Dixon 3 , Susan Y. Schwartz 4 , Jeffrey S. Marshall 5 , Lujia Feng 6 , Jacob I. Walter 2 , Rocco Malservisi 3 , Susan E. Owen 7 Marino Protti 1 , Victor González 1 , Andrew V. Newman 2* , Timothy H. Dixon 3 , Susan Y. Schwartz 4 , Jeffrey S. Marshall 5 , Lujia Feng 6 , Jacob I. Walter 2 , Rocco Malservisi 3 , Susan E. Owen 7 1. Observatorio Vulcanológico y Sismológico de Costa Rica (OVSICORI), Universidad Nacional, Apartado 1718-3000, Heredia 3000, Costa Rica 2. School of Earth and Atmospheric Sciences, Georgia Institute of Technology, 311 Ferst Drive, Atlanta, GA 30332-0340, USA 3. Department of Geology, University of South Florida, 4202 E Fowler Ave, Tampa, FL 33620, USA 4. Department of Earth and Planetary Sciences, University of California Santa Cruz, Santa Cruz, CA 95064, USA. 5. Geological Sciences Department, Cal Poly Pomona, 3801 West Temple Ave., Pomona, CA, 91768, USA 6. Earth Observatory of Singapore, Nanyang Technological University, 50 Nanyang Avenue, Block N2-1A-15, 639798, Singapore. 7. Jet Propulsion Laboratory, MS 238-600, 4800 Oak Grove Drive, Pasadena, CA 91109 * corresponding author Nicoya earthquake rupture anticipated by geodetic measurement of the locked plate interface SUPPLEMENTARY INFORMATION DOI: 10.1038/NGEO2038 NATURE GEOSCIENCE | www.nature.com/naturegeoscience 1 © 2013 Macmillan Publishers Limited. All rights reserved.

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Page 1: Nicoya earthquake rupture anticipated by geodetic ......Supplementary Text for “Nicoya earthquake rupture anticipated by geodetic measurement of the locked plate interface” By:

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Supplementary Text for “Nicoya earthquake rupture anticipated by geodetic measurement of the locked plate interface”

By: Marino Protti1, Victor González1, Andrew V. Newman2*, Timothy H. Dixon3, Susan Y. Schwartz4, Jeffrey S. Marshall5, Lujia Feng6, Jacob I. Walter2, Rocco Malservisi3, Susan E. Owen7

Marino Protti1, Victor González1, Andrew V. Newman2*, Timothy H. Dixon3, Susan Y. Schwartz4, Jeffrey S. Marshall5, Lujia Feng6, Jacob I. Walter2, Rocco Malservisi3, Susan E. Owen7

1. Observatorio Vulcanológico y Sismológico de Costa Rica (OVSICORI), Universidad Nacional, Apartado 1718-3000, Heredia 3000, Costa Rica

2. School of Earth and Atmospheric Sciences, Georgia Institute of Technology, 311 Ferst Drive, Atlanta, GA 30332-0340, USA

3. Department of Geology, University of South Florida, 4202 E Fowler Ave, Tampa, FL 33620, USA

4. Department of Earth and Planetary Sciences, University of California Santa Cruz, Santa Cruz, CA 95064, USA.

5. Geological Sciences Department, Cal Poly Pomona, 3801 West Temple Ave., Pomona, CA, 91768, USA

6. Earth Observatory of Singapore, Nanyang Technological University, 50 Nanyang Avenue, Block N2-1A-15, 639798, Singapore.

7. Jet Propulsion Laboratory, MS 238-600, 4800 Oak Grove Drive, Pasadena, CA 91109

* corresponding author

Nicoya earthquake rupture anticipated by geodetic measurement of the locked plate interface

SUPPLEMENTARY INFORMATIONDOI: 10.1038/NGEO2038

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© 2013 Macmillan Publishers Limited. All rights reserved.

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Seismic methods:

From seismic data recorded by the University of California Santa Cruz and Georgia Tech seismic networks on Nicoya, we identify the P and S phase arrivals utilizing a tuned automatic Short-term/Long-term average ratio filter provided with the Antelope Seismic Database software (www.brtt.com). The automatic choice of phase arrivals and event associations are subsequently reviewed by an analyst for accuracy and consistency. The phase information were then used to relocate events within a local three-dimensional velocity model1 using the software SIMULPS2. Figure 1 includes aftershocks that indicate horizontal formal errors of less than 1 km based on travel-time residuals between predicted and observed station arrival times. The epicenter of the mainshock is shown as the first-motion point source, based on the network-observed initial P-wave arrivals.

GPS processing and coseismic displacement fields:

Using funding obtained by the NSF-RAPIDS program, within 3 days of the earthquake a team comprising individuals from OVSICORI, University of South Florida, Georgia Tech, UC Santa Cruz, and Cal Poly Pomona began arriving in Nicoya to repair continuous GPS and seismic stations, and perform a rapid field campaign. All campaign GPS sites were occupied for a minimum of three-days, while several remained longer to capture ongoing postseismic deformation.

Syn-field Processing: Following the earthquake, daily and 5-minute kinematic positions for both campaign and

continuous data were processed as they were downloaded, either through routine telemetric communications already established or from individuals during the field deployment. The data were processed using single station bias fixing3 and point-positioning4 with JPL’s GIPSY-OASIS software. For the rapid estimates immediately following the earthquake, the JPL Rapid orbit and clock files were used5.

These early results were used during the active field campaign to evaluate the quality of GPS coverage in order to establish priorities for additional data collection from new and already measured stations, and for prioritizing continuous GPS repairs. Once early displacement fields were made, preliminary slip inversions were also made to evaluate the spatial extent of rupture. Post-Processing:

All GPS data collected during the field experiment were processed or reprocessed later and in a consistent manor using JPL’s final orbit products at the USF Geodesy lab. From these data the final GPS displacement field was created from the combination of data from campaign and continuous GPS data collected before and after the earthquake.

Displacements: For all GPS data the displacements ud were determined by differencing the post-event

position u1 and the combination of the last observed pre-event position u0 and the expected continued interseismic deformation from the product of the observed velocity v as reported in the Feng study6, and the time lapse between observation and earthquake t, such that:

ud = u1 ! (u0 + vt) .

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For the 21 campaign sites, the estimated pre-event positions were measured during a campaign in March 2010, leaving t = 2.53 years. After the earthquake, new stations were occupied as rapidly as possible, causing many sites to have very short-observations on their first day. To avoid problems introduced with such error-prone results, the post-earthquake positions were taken from the first subsequent daily-averaged GPS solution with a formal horizontal position error under 5 mm.

For the 18 continuous GPS stations, the displacement determination was performed in the same manner as the campaign sites. For the 9 stations that were operational through the earthquake daily solutions were taken from the days immediately preceding and following the event. Two stations were differenced using data with less than 2 weeks separation around the event. The remaining 7 stations had measurement lapses between about 50 and 500 days before the event. Errors:

The displacement errors σd were determined assuming the errors reported for the interseismic velocities σv (ref. 6), the pre-event positions σ0, and post-event positions σ1 were all independent7, such that:

! d = ! 02 +!1

2 + (! vt)2

where t is the time lapse between the earthquake and the prior event measurement. Errors were on average, approximately 3.2% and 6.7% of the displacement magnitudes for continuous and campaign sites, respectively. As expected, the errors are larger compared to displacements for sites away from the rupture, where deformation falls off. All stations positions, velocities, errors, and measurement lapses are reported in Table S1.

Field Geomorphic Methods:

Geomorphic field measurements were made 5-16 days after the earthquake to constrain coseismic uplift along the Nicoya coast. Uplift was measured at 22 sites using six different methods: 1) pre- vs. post-earthquake rapid altimeter surveying of coastal monuments, 2) reoccupation of pre-earthquake hand-level survey lines, 3) hand-level surveying of pre- vs. post-earthquake high tide debris lines, 4) spot measurements of displaced tidal notches and rock staining, 5) spot measurements of vertical extent of mortality (VEM) for sessile intertidal organisms8,9, 6) spot measurements of coastal stream incision and mangrove root exposure10.

The local survey datum at each site was the tidal still water level (SWL) at the time of surveying. Survey data were adjusted to the mean lower low water (MLLW) datum for regional tidal predictions11-13, and then corrected to corresponding elevations above mean sea level (MSL). An additional correction for wave run-up was applied based on local variations in beach slope14. The results were also adjusted for minor post-seismic deformation as observed by near-field GPS sites during the time period between the earthquake and geomorphic fieldwork.

Measurable coseismic uplift occurred along ~80 km of coastline between Playa Avellanas and Punta Coyote. Pronounced uplift (≥50 cm) occurred along ~30 km of coast from Nosara to Islita, with maximum uplift (≥80 cm) near Puerto Carrillo onshore of the epicenter

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(Figure 3). The observed geomorphic uplift pattern is consistent with that recorded by continuous GPS stations (although GPS values are systematically lower), and with seismic and geodetic inversions for primary slip centered beneath the Nicoya coast (Figure S1). All geomorphic uplift results are reported in Table S2.

Details of Geodetic Inversion methods:

To model the coseismic deformation of the 5 September 2012 Nicoya earthquake, we used the campaign and continuous GPS data, but excluded the geomorphic data collected here because of the increased errors and spatial redundancy with the GPS data. The model geometry, smoothing, and inversion method are the same as those used in the interseismic model and are described in the Feng study6. Although the interseismic and coseismic models share many similarities, they have three major differences: (1) only trench-normal and vertical interseismic annual velocities were used in the interseismic modeling, while all three components of coseismic offsets were used in the coseismic modeling; (2) only the dip-slip component of locking was considered in the interseismic modeling, while both dip-slip and strike-slip components were inverted in the coseismic modeling; (3) virtual back slip was assumed in the interseismic modeling with maximum back slip constrained by the plate convergence, while no maximum slip was applied in the coseismic modeling.

We conducted a separate checkerboard resolution test for the coseismic modeling to assess the spatial resolution of the GPS network on resolving dip-slip and strike-slip along the assumed subduction interface (Figure S2). In these tests we’ve included weighting based on per-station error estimates from the observed displacement field (Table S1) to account for the relative, but small error observed in the real data. Because of the reduced resolution toward the model boundaries, we only consider the high-resolution area that was observable at both low smoothing (κ = 1) and smoothing at the same level as the final model shown in Figure 4 (κ = 18,000).

We ran inversion models at a wide range of smoothing levels. The preferred model at κ = 18,000 (Figure S3b) was chosen because of its location in the inflection corner of the trade-off curve between roughness and misfit (Figure S3d), which introduces substantial smoothing but without the cost of large increasing misfit. For comparison, examples of under-smoothed (Figure S3a) and possibly over-smoothed (Figure S3c) are also provided. All three cases show a major slip patch underneath the Nicoya peninsula and some slip offshore. To test if the slip patch offshore is indeed required, we conducted another set of models with the offshore area constrained to have no coseismic slip. The fits of the constrained models were systematically and substantially worse than the models that allow some slip offshore. However, a more detailed analysis of this shallow slip patch was not conducted due to the low resolution offshore.

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Table S1: Displacement field obtained from a combination of the continuous and campaign GPS stations shown in Figure 2.

        Displacement   Error       time  lapse  Stat   Long.   Lat.   Elev.   E   N   V   E   N   V   Date-­‐0   Date-­‐1  

 [°]   [°]   [m]   [mm]   [mm]   [mm]   [mm]   [mm]   [mm]   [yr]   [yr]   [yr]  

Continuous                        BIJA   -­‐84.577   9.750   555.6   -­‐1.9   -­‐17.5   -­‐61.3   4.4   5.1   15.7   2011.381   2012.724   1.343  

BON2   -­‐85.203   9.765   28.0   -­‐17.7   -­‐280.2   230.5   1.7   1.6   6.6   2011.647   2012.705   1.058  CABA   -­‐85.344   10.238   27.0   -­‐192.1   -­‐302.9   -­‐112.2   0.8   0.7   2.8   2012.675   2012.680   0.005  ELVI   -­‐85.446   10.395   81.9   -­‐128.9   -­‐318.6   -­‐90.4   1.2   0.9   4.3   2012.642   2012.713   0.071  EPZA   -­‐85.568   10.141   668.4   -­‐95.0   -­‐192.3   270.9   0.8   0.7   2.8   2012.675   2012.680   0.005  GRZA   -­‐85.636   9.916   39.3   -­‐431.2   -­‐524.7   460.7   1.7   1.2   5.3   2012.658   2012.697   0.038  HATI   -­‐85.710   10.292   58.6   -­‐67.6   -­‐105.7   99.5   1.3   0.9   4.1   2012.544   2012.686   0.142  HUA2   -­‐85.352   10.018   593.9   -­‐99.1   -­‐230.6   196.2   0.9   0.6   2.7   2012.555   2012.686   0.131  IND1   -­‐85.502   9.865   75.3   -­‐204.4   -­‐600.7   505.6   1.0   0.9   4.0   2012.374   2012.686   0.311  LAFE   -­‐84.960   9.807   65.2   -­‐23.2   -­‐65.5   12.3   0.8   0.7   3.8   2012.675   2012.680   0.005  LEPA   -­‐85.031   9.945   20.9   -­‐115.5   -­‐131.6   11.6   1.3   1.0   4.4   2012.189   2012.708   0.519  LMNL   -­‐85.053   10.268   103.0   -­‐153.5   -­‐157.5   -­‐69.1   0.8   0.6   2.6   2012.675   2012.680   0.005  PNE2   -­‐85.829   10.196   19.5   -­‐234.3   -­‐107.7   185.6   1.9   1.7   8.2   2011.400   2012.705   1.305  PUJE   -­‐85.272   10.114   30.1   -­‐169.7   -­‐241.9   -­‐60.7   0.8   0.6   2.6   2012.675   2012.680   0.005  PUMO  

-­‐84.967   10.064   18.0   -­‐129.4   -­‐112.4   -­‐48.8   0.8   0.7   3.2   2012.675   2012.686   0.011  QSEC   -­‐85.357   9.840   17.4   -­‐46.7   -­‐391.7   395.4   0.8   0.7   2.8   2012.675   2012.680   0.005  SAJU   -­‐85.711   10.067   73.4   -­‐343.0   -­‐251.9   439.0   0.8   0.7   3.0   2012.675   2012.680   0.005  VERA   -­‐84.869   10.854   64.3   -­‐45.7   -­‐64.6   -­‐5.7   1.0   0.8   3.5   2012.675   2012.680   0.005  Campaign    

                     BAGA   -­‐85.261   10.541   123.4   -­‐89.0   -­‐159.8   -­‐75.8   6.5   2.5   11.4   2010.173   2012.702   2.529  BALL   -­‐85.448   10.383   118.0   -­‐121.9   -­‐304.1   -­‐148.6   5.1   2.0   8.1   2010.175   2012.708   2.533  BONG   -­‐85.207   9.744   21.6   1.8   -­‐283.0   254.4   4.6   2.6   8.9   2010.181   2012.694   2.513  CEBA   -­‐85.776   10.249   90.4   -­‐125.6   -­‐67.9   175.1   6.5   2.5   10.3   2010.181   2012.697   2.516  CRUZ   -­‐85.634   11.054   267.2   18.3   -­‐49.1   -­‐40.2   7.8   4.0   15.1   2010.189   2012.710   2.521  DIRI   -­‐85.611   10.272   82.0   -­‐50.5   -­‐199.3   -­‐24.7   5.8   2.2   10.0   2010.181   2012.694   2.513  GRAN   -­‐85.653   10.562   122.2   -­‐12.3   -­‐162.2   -­‐79.8   4.5   2.0   8.4   2010.184   2012.702   2.518  GUAR   -­‐85.450   10.140   136.3   -­‐115.1   -­‐281.0   45.1   6.2   1.9   9.9   2010.162   2012.691   2.529  GUIO   -­‐85.659   9.923   31.4   -­‐412.4   -­‐467.9   368.1   4.8   2.3   8.6   2010.170   2012.691   2.521  HOJA   -­‐85.382   10.079   241.0   -­‐131.3   -­‐249.2   55.4   7.5   2.3   10.6   2010.175   2012.689   2.514  JICA   -­‐85.136   9.975   61.4   -­‐102.0   -­‐156.9   -­‐31.1   5.1   2.2   9.4   2010.175   2012.699   2.524  LEON   -­‐85.187   9.937   276.9   -­‐33.2   -­‐151.3   63.0   5.3   2.1   8.7   2010.170   2012.689   2.519  MATA   -­‐85.813   10.355   77.8   -­‐34.5   -­‐61.9   46.4   6.3   3.0   15.0   2010.186   2012.697   2.511  PALO   -­‐85.220   10.241   40.0   -­‐206.0   -­‐247.1   -­‐84.5   6.6   2.7   10.7   2010.186   2012.702   2.516  PAQU   -­‐84.955   9.832   80.3   -­‐28.5   -­‐72.0   -­‐11.3   6.3   2.4   10.1   2010.167   2012.702   2.535  POTR   -­‐85.569   10.847   155.7   6.1   -­‐90.5   -­‐66.7   6.3   2.5   10.0   2010.189   2012.713   2.524  SAMA   -­‐85.549   9.889   45.9   -­‐286.7   -­‐601.6   531.4   4.6   2.1   8.0   2010.170   2012.691   2.521  SJOS   -­‐84.948   10.366   1062.1   -­‐105.7   -­‐120.3   -­‐120.7   5.1   2.1   8.3   2010.195   2012.702   2.507  SJUA   -­‐85.757   10.063   44.6   -­‐373.7   -­‐271.6   319.4   6.4   2.6   10.5   2010.186   2012.713   2.527  TENO   -­‐85.098   10.602   373.4   -­‐79.0   -­‐139.3   -­‐57.9   5.2   2.3   9.1   2010.189   2012.716   2.527  VENA   -­‐85.792   10.161   24.9   -­‐258.1   -­‐137.7   242.9   5.2   2.1   8.4   2010.184   2012.697   2.513  

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Table S2: Geomorphic uplift results shown in Figure 2 and S1.

        Ucs-­‐m   ΔR   Ups-­‐gps   Ucs-­‐a                  #   Location   Measured   Wave  Run-­‐Up   Post-­‐Seismic   Adjusted   RSS   Field   Site   Site  

    Uplift     Correction     Correction     Uplift     Error   Method   Latitude   Longitude           (m)     (m)     (m)     (m)     (±  m)         (deg  N)     (deg  W)                        1   Playa  Langosta  (Tamarindo)   0.00   n/a   n/a   0.00   0.20     A,B   10.2873   -­‐85.8516  2   Playa  Avellanas  (Avellanas)   0.28   -­‐0.04   -­‐0.02   0.22   0.20     A,B,C   10.2288   -­‐85.8376  3   Playa  Callejones  (Pochotes)   0.42   -­‐0.06   -­‐0.02   0.34   0.20     B,C,F   10.1851   -­‐85.8239  4   Playa  Junquillal  (Iguanazul)   0.40   n/a   -­‐0.02   0.38   0.10     A,E   10.1754   -­‐85.8175  5   Playa  Cocal  (San  Juanillo)   0.72   -­‐0.11   -­‐0.02   0.59   0.20   B,C   10.0314   -­‐85.7416  6   Playa  Peladas  (Nosara)   0.66   -­‐0.10   -­‐0.03   0.53   0.20   A,C   9.9537   -­‐85.6753  7   Playa  Guiones  Sur    

(Punta  Guiones)  0.80   -­‐0.12   -­‐0.03   0.65   0.20   A,B,C   9.9221   -­‐85.6608  

8   Playa  Garza  Oeste    (Punta  Guiones)  

0.76   -­‐0.11   -­‐0.03   0.62   0.20   B,C   9.9075   -­‐85.6509  

9   Playa  Sámara  Oeste  (Sámara)  

0.72   -­‐0.11   -­‐0.05   0.56   0.20   C   9.8772   -­‐85.5331  

10   Playa  Sámara  Este    (Punta  Indio)  

0.73   -­‐0.11   -­‐0.05   0.57   0.20   C   9.8683   -­‐85.5072  

11   Playa  Carrillo  Oeste    (Punta  Indio)  

0.72   -­‐0.11   -­‐0.05   0.56   0.20   C,F   9.8692   -­‐85.4991  

12   Playa  Carrillo  Este    (Puerto  Carrillo)  

0.85   -­‐0.13   -­‐0.05   0.67   0.20   A,B,C,G   9.8663   -­‐85.4828  

13   Playa  Bejuco  (Bejuco)   0.55   n/a   -­‐0.03   0.52   0.10   E   9.8181   -­‐85.3329  14   Playa  Caletas  

 (Punta  Coyote)  0.46   -­‐0.07   -­‐0.03   0.36   0.20   A,B,C   9.7595   -­‐85.2692  

15   Playa  Carmen  (Malpaís)   0.00   n/a   n/a   0.00   0.20   C   9.6267   85.1522                                                              

Explanation                  Ucs-­‐m      =  Measured  Co-­‐Seismic  Uplift  (Tide  corrected)                ΔR    =  Wave  Run-­‐Up  Correction  (ΔR  =  Rpre-­‐EQ  -­‐  Rpost-­‐EQ)              

Ups-­‐gps      =  Post-­‐Seismic  Uplift  Correction  (Measured  at  nearest  continuous  GPS  station)          Ucs-­‐a      =  Adjusted  Co-­‐Seismic  Uplift  (Ucs-­‐a  =  Ucs-­‐m  –  ΔR  –  Ups-­‐gps)                                  

Field  Methods                  A   Pre/Post  Earthquake  Rapid  Coastal  Monument  Survey  (Barometric  Altimeter)            B   Pre/Post  Earthquake  Beach  Profile  Survey  (Hand  Level  &  Stadia  Rod)            C   Pre/Post  Earthquake  High  Tide  Debris  Line  Survey  (Hand  Level  &  Stadia  Rod)              D   Displaced  High  Tide  Notches  &  Rock  Staining  (Stadia  Rod)              E   Vertical  Extent  of  Mortality  for  Sessile  Intertidal  Organisms  (Stadia  Rod)            F   Depth  of  Stream  Incision  &  Mangrove  Root  Exposure  (Stadia  Rod)            

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Table S2: Geomorphic uplift results shown in Figure 2 and S1.

        Ucs-­‐m   ΔR   Ups-­‐gps   Ucs-­‐a                  #   Location   Measured   Wave  Run-­‐Up   Post-­‐Seismic   Adjusted   RSS   Field   Site   Site  

    Uplift     Correction     Correction     Uplift     Error   Method   Latitude   Longitude           (m)     (m)     (m)     (m)     (±  m)         (deg  N)     (deg  W)                        1   Playa  Langosta  (Tamarindo)   0.00   n/a   n/a   0.00   0.20     A,B   10.2873   -­‐85.8516  2   Playa  Avellanas  (Avellanas)   0.28   -­‐0.04   -­‐0.02   0.22   0.20     A,B,C   10.2288   -­‐85.8376  3   Playa  Callejones  (Pochotes)   0.42   -­‐0.06   -­‐0.02   0.34   0.20     B,C,F   10.1851   -­‐85.8239  4   Playa  Junquillal  (Iguanazul)   0.40   n/a   -­‐0.02   0.38   0.10     A,E   10.1754   -­‐85.8175  5   Playa  Cocal  (San  Juanillo)   0.72   -­‐0.11   -­‐0.02   0.59   0.20   B,C   10.0314   -­‐85.7416  6   Playa  Peladas  (Nosara)   0.66   -­‐0.10   -­‐0.03   0.53   0.20   A,C   9.9537   -­‐85.6753  7   Playa  Guiones  Sur    

(Punta  Guiones)  0.80   -­‐0.12   -­‐0.03   0.65   0.20   A,B,C   9.9221   -­‐85.6608  

8   Playa  Garza  Oeste    (Punta  Guiones)  

0.76   -­‐0.11   -­‐0.03   0.62   0.20   B,C   9.9075   -­‐85.6509  

9   Playa  Sámara  Oeste  (Sámara)  

0.72   -­‐0.11   -­‐0.05   0.56   0.20   C   9.8772   -­‐85.5331  

10   Playa  Sámara  Este    (Punta  Indio)  

0.73   -­‐0.11   -­‐0.05   0.57   0.20   C   9.8683   -­‐85.5072  

11   Playa  Carrillo  Oeste    (Punta  Indio)  

0.72   -­‐0.11   -­‐0.05   0.56   0.20   C,F   9.8692   -­‐85.4991  

12   Playa  Carrillo  Este    (Puerto  Carrillo)  

0.85   -­‐0.13   -­‐0.05   0.67   0.20   A,B,C,G   9.8663   -­‐85.4828  

13   Playa  Bejuco  (Bejuco)   0.55   n/a   -­‐0.03   0.52   0.10   E   9.8181   -­‐85.3329  14   Playa  Caletas  

 (Punta  Coyote)  0.46   -­‐0.07   -­‐0.03   0.36   0.20   A,B,C   9.7595   -­‐85.2692  

15   Playa  Carmen  (Malpaís)   0.00   n/a   n/a   0.00   0.20   C   9.6267   85.1522                                                              

Explanation                  Ucs-­‐m      =  Measured  Co-­‐Seismic  Uplift  (Tide  corrected)                ΔR    =  Wave  Run-­‐Up  Correction  (ΔR  =  Rpre-­‐EQ  -­‐  Rpost-­‐EQ)              

Ups-­‐gps      =  Post-­‐Seismic  Uplift  Correction  (Measured  at  nearest  continuous  GPS  station)          Ucs-­‐a      =  Adjusted  Co-­‐Seismic  Uplift  (Ucs-­‐a  =  Ucs-­‐m  –  ΔR  –  Ups-­‐gps)                                  

Field  Methods                  A   Pre/Post  Earthquake  Rapid  Coastal  Monument  Survey  (Barometric  Altimeter)            B   Pre/Post  Earthquake  Beach  Profile  Survey  (Hand  Level  &  Stadia  Rod)            C   Pre/Post  Earthquake  High  Tide  Debris  Line  Survey  (Hand  Level  &  Stadia  Rod)              D   Displaced  High  Tide  Notches  &  Rock  Staining  (Stadia  Rod)              E   Vertical  Extent  of  Mortality  for  Sessile  Intertidal  Organisms  (Stadia  Rod)            F   Depth  of  Stream  Incision  &  Mangrove  Root  Exposure  (Stadia  Rod)            

7

Figure S1: Comparison of vertical uplift as measured by coastal continuous and campaign GPS site (green and orange) and as determined by geomorphic field observations. The spatial extent and amplitude of the geomorphic results largely agrees with those determined using GPS data, though with substantially greater error. This result highlights the utility of rapid geomorphic studies for the evaluation of coseismic deformation, particularly when pre-existing GPS measurements are not available. The same data are shown in Figure 2b and are repeated here without inland data for visual clarity.

−86˚ −85.5˚ −85˚9.5˚

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Figure S2: Checkerboard test on the spatial resolution of the dense Nicoya GPS network. (a) Synthetic input slip distribution; (b) Inverted best fit slip distribution at = 1; and (c) best-fit slip distribution at = 18,000. The green line outlines the best-resolved region, comparable to the area found in Feng et al., [2012]. The red vectors show the orientation and magnitude of input and predicted slip. The red diamonds and yellow circles are the campaign and continuous sites, respectively.

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Figure S3: The best-fit coseismic slip distribution for the 5 September 2012 Nicoya earthquake at different smoothing levels: (a) = 5000, (b) = 18,000, and (c) = 40,000. As smoothing increases, slip becomes more distributed, but more poorly match the data. (d) A trade-off curve between decreased roughness and increased misfit, represent as reduced chi-square. Our preferred model at = 18,000 is chosen in near the inflection-point of the curve.

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Supplementary References:

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2. Thurber, C. H. Local earthquake tomography: velocities and vp /vs theory, in: Seismic Tomography: Theory and Practice. eds. H. M. lyer and K. Hirahara, Chapman and Hall, London, 563-583, (1993).

3. Bertiger, W. et al. Single receiver phase ambiguity resolution with GPS data. J. Geodesy, 84(5), 327-337, (2010).

4. Zumberge, J. F., Heflin, M. B., Jefferson, D. C. ,Watkins, M. M. & Webb, F. H. Precise point positioning for the efficient and robust analysis of GPS data from large networks. J. Geophys. Res. 102(B3), 5005-5017, (1997).

5. Desai, S.D. et al. Results from the Reanalysis of Global GPS Data in the IGS08 Reference Frame. Trans. Amer. Geophys. Union, G53B-0904 [abstract], (2011).

6. Feng, L. et al. Active deformation near the Nicoya Peninsula, northwestern Costa Rica, between 1996 and 2010: Interseismic megathrust coupling. J. Geophys. Res. 117(B6), B06407. (2012).

7. Press, W. H., Teukolsky, S. A., Vetterling, W. T. & Flannery, B. P. Numerical Recipes in FORTRAN. Cambridge University Press, Cambridge, MA, 964 pp., (1992).

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11. Flater, D. A brief introduction to XTide. Linux Journal 32, 51-57 (1996). 12. Gill, S.K., & Schultz, J.R. Tidal datums and their applications. NOAA Special

Publication NOS CO-OPS 1, U.S. Department of Commerce, National Ocean Service, Center for Operational Oceanographic Products and Services, Silver Springs, Maryland, 112 p., (2001).

13. Pentcheff, D. & Flater, D., WWW Tide/Current Predictor, University of South Carolina, http://tbone.biol.sc.edu/tide/index.html (Accessed September 5, 2012).

14. Nielsen, P. and Hanslow, D.J., 1991, Wave runup distributions on natural beaches, Journal of Coastal Research, v. 7, no. 4, p. 1139-1152, (1991).

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