
- Select a language for the TTS:
- UK English Female
- UK English Male
- US English Female
- US English Male
- Australian Female
- Australian Male
- Language selected: (auto detect) - EN
Play all audios:
ABSTRACT Plate tectonics successfully describes the surface of Earth as a mosaic of moving lithospheric plates. But it is not clear what happens at the base of the plates, the
lithosphere–asthenosphere boundary (LAB). The LAB has been well imaged with converted teleseismic waves1,2, whose 10–40-kilometre wavelength controls the structural resolution. Here we use
explosion-generated seismic waves (of about 0.5-kilometre wavelength) to form a high-resolution image for the base of an oceanic plate that is subducting beneath North Island, New Zealand.
Our 80-kilometre-wide image is based on P-wave reflections and shows an approximately 15° dipping, abrupt, seismic wave-speed transition (less than 1 kilometre thick) at a depth of about 100
kilometres. The boundary is parallel to the top of the plate and seismic attributes indicate a P-wave speed decrease of at least 8 ± 3 per cent across it. A parallel reflection event
approximately 10 kilometres deeper shows that the decrease in P-wave speed is confined to a channel at the base of the plate, which we interpret as a sheared zone of ponded partial melts or
volatiles. This is independent, high-resolution evidence for a low-viscosity channel at the LAB that decouples plates from mantle flow beneath, and allows plate tectonics to work. Access
through your institution Buy or subscribe This is a preview of subscription content, access via your institution ACCESS OPTIONS Access through your institution Subscribe to this journal
Receive 51 print issues and online access $199.00 per year only $3.90 per issue Learn more Buy this article * Purchase on SpringerLink * Instant access to full article PDF Buy now Prices may
be subject to local taxes which are calculated during checkout ADDITIONAL ACCESS OPTIONS: * Log in * Learn about institutional subscriptions * Read our FAQs * Contact customer support
SIMILAR CONTENT BEING VIEWED BY OTHERS DISCOVERY OF FLAT SEISMIC REFLECTIONS IN THE MANTLE BENEATH THE YOUNG JUAN DE FUCA PLATE Article Open access 17 August 2020 RAPID MAGMA ASCENT BENEATH
LA PALMA REVEALED BY SEISMIC TOMOGRAPHY Article Open access 21 October 2022 MEGATHRUST REFLECTIVITY REVEALS THE UPDIP LIMIT OF THE 2014 IQUIQUE EARTHQUAKE RUPTURE Article Open access 08 July
2022 REFERENCES * Rychert, C. A., Rondenay, S. & Fischer, K. M. P-to-S and S-to-P imaging of a sharp lithosphere-asthenosphere boundary beneath eastern North America. _J. Geophys. Res._
112, B08314 (2007) Article ADS Google Scholar * Kawakatsu, H. et al. Seismic evidence for sharp lithosphere-asthenosphere boundaries of oceanic plates. _Science_ 324, 499–502 (2009)
Article CAS ADS Google Scholar * Parsons, B. & McKenzie, D. Mantle convection and the thermal structure of plates. _J. Geophys. Res._ 83, 4485–4496 (1978) Article ADS Google
Scholar * Watts, A. B. _Isostasy and Flexure of the Lithosphere_ (Cambridge Univ. Press, 2001) Google Scholar * Fischer, K. M., Ford, H. A., Abt, D. L. & Rychert, C. A. The
lithosphere-asthenosphere boundary. _Annu. Rev. Earth Planet. Sci._ 38, 551–575 (2010) Article CAS ADS Google Scholar * Naif, S., Key, K., Constable, S. & Evans, R. L. Melt-rich
channel observed at the lithosphere–asthenosphere boundary. _Nature_ 495, 356–359 (2013) Article CAS ADS Google Scholar * Olugboji, T. M., Karato, S. & Park, J. Structures of the
oceanic lithosphere-asthenosphere boundary: mineral-physics modeling and seismological signatures. _Geochem. Geophys. Geosyst._ 14, 880–901 (2013) Article ADS Google Scholar * Jarchow, C.
M., Goodwin, E. B. & Catchings, R. D. Are large explosive sources applicable to resource exploration? _Leading Edge (Tulsa Okla.)_ 9, 12–17 (1990) Article Google Scholar * Steer, D.
N., Knapp, J. H. & Brown, L. D. Super deep reflection profiling: exploring the continental mantle lid. _Tectonophysics_ 286, 111–121 (1998) Article ADS Google Scholar * Henrys, S. A.
et al. SAHKE geophysical transect reveals crustal and subduction zone structure at the southern Hikurangi margin, New Zealand. _Geochem. Geophys. Geosyst._ 14, 2063–2083 (2013) Article ADS
Google Scholar * Lamb, S. H. Cenozoic tectonic evolution of the New Zealand plate-boundary zone: a paleomagnetic perspective. _Tectonophysics_ 509, 135–164 (2011) Article ADS Google
Scholar * Reyners, M., Eberhart-Phillips, D., Stuart, G. & Nishimura, Y. Imaging subduction from the trench to 300 km depth beneath the central North Island, New Zealand, with Vp and
Vp/Vs. _Geophys. J. Int._ 165, 565–583 (2006) Article ADS Google Scholar * Eberhart-Phillips, D., Reyners, M., Chadwick, M. & Chiu, J.-M. Crustal heterogeneity and subduction
processes: 3-D Vp, Vp/Vs and Q in the southern North Island, New Zealand. _Geophys. J. Int._ 162, 270–288 (2005) Article ADS Google Scholar * Warner, M. Free water and seismic
reflectivity in the lower continental crust. _J. Geophys. Eng._ 1, 88–101 (2004) Article Google Scholar * Bostock, M. G. Seismic waves converted from velocity gradient anomalies in the
Earth’s upper mantle. _Geophys. J. Int._ 138, 747–756 (1999) Article ADS Google Scholar * Zhou, H. _Practical Seismic Data Analysis_ (Cambridge Univ. Press, 2014) Book Google Scholar *
Sheriff, R. E. & Geldart, L. P. _Exploration Seismology_ 2nd edn (Cambridge Univ. Press, 1995) Book Google Scholar * Warner, M. & McGeary, S. E. Seismic reflection coefficients
from mantle fault zones. _Geophys. J. Int._ 89, 223–230 (1987) Article ADS Google Scholar * Hacker, B. R., Abers, G. A. & Peacock, S. M. Subduction factory 1. Theoretical mineralogy,
densities, seismic wave speeds, and H2O contents. _J. Geophys. Res._ 108 (B1). 2029 (2003) ADS Google Scholar * Yamamoto, J., Korenaga, J., Hirano, N. & Kagi, H. Melt-rich
lithosphere-asthenosphere boundary inferred from petit-spot volcanoes. _Geology_ 42, 967–970 (2014) Article ADS Google Scholar * Sakamaki, T. et al. Ponded melt at the boundary between
the lithosphere and asthenosphere. _Nature Geosci._ 6, 1041–1044 (2013) Article CAS ADS Google Scholar * Hirth, G. & Kohlstedt, D. L. Water in the oceanic upper mantle: implications
for rheology, melt extraction and the evolution of the lithosphere. _Earth Planet. Sci. Lett._ 144, 93–108 (1996) Article CAS ADS Google Scholar * Hammond, W. C. & Humphreys, E. D.
Upper mantle seismic wave velocity: effects of realistic partial melt geometries. _J. Geophys. Res._ 105, 10975–10986 (2000) Article ADS Google Scholar * Gripp, A. E. & Gordon, R. G.
Young tracks of hotspots and current plate velocities. _Geophys. J. Int._ 150, 321–361 (2002) Article ADS Google Scholar * Hall, C. E. & Parmentier, E. M. Spontaneous melt
localization in a deforming solid with viscosity variations due to water weakening. _Geophys. Res. Lett._ 27, 9–12 (2000) Article ADS Google Scholar * Lie, J., Pederson, T. & Husebye,
E. S. Observations of seismic reflectors in the lower lithosphere beneath the Skagerrak. _Nature_ 346, 165–168 (1990) Article ADS Google Scholar * Richardson, R. M. Ridge forces,
absolute plate motions, and the intraplate stress field. _J. Geophys. Res._ 97, 11739–11748 (1992) Article ADS Google Scholar * Savage, M., Park, J. & Todd, H. Velocity and anisotropy
structure of the Hikurangi subduction margin, New Zealand, from receiver functions. _Geophys. J. Int._ 168, 1034–1050 (2007) Article ADS Google Scholar * Duncan, G. & Beresford, G.
Median filter behaviour with seismic data. _Geophys. Prospect._ 43, 329–345 (1995) Article ADS Google Scholar * Taylor, J. R. _An Introduction to Error Analysis_ 2nd edn (University
Science Books, 1997) Google Scholar * Menke, W., Levin, V. & Sethi, R. Seismic attenuation in the crust at the mid-Atlantic plate boundary in south-west Iceland. _Geophys. J. Int._ 122,
175–182 (1995) Article ADS Google Scholar * Badley, M. E. _Practical Seismic Interpretation_ (International Human Resources Development Corporation, 1985) Google Scholar * Williams, C.
A. et al. Revised interface geometry for the Hikurangi Subduction Zone, New Zealand. _Seismol. Res. Lett._ 84, 1066–1073 (2013) Article Google Scholar * Seward, A. et al. _Seismic Array
HiKurangi Experiment II (SAHKE II)_ (Onshore Active Source Acquisition Report no. 2011/50, GNS Science, Lower Hutt, 2011) * Larsen, S. & Schultz, A. _ELAS3D:2D/3D Elastic
Finite-difference Wave Propagation Code_ (Lawrence Livermore National Laboratory Technical Report UCRL-MA-121792, 1995) Google Scholar Download references ACKNOWLEDGEMENTS The SAHKE project
was supported by public research funding from the Government of New Zealand, the Japanese Science and Technology Agency, and the National Science Foundation (NSF OCE-1061557). Explosives
and technical support was provided by Orica New Zealand Ltd. Individual land owners, Greater Wellington Regional Council, Transpower, and forestry companies allowed us onto their land. The
IRIS/Passcal instrument pool provided the land instruments and technical support. We thank colleagues E. Smith and W. Stratford for comments on initial versions of this paper. AUTHOR
INFORMATION AUTHORS AND AFFILIATIONS * Institute of Geophysics, Victoria University, Salamanca Road, Wellington 6140, New Zealand, T. A. Stern, M. K. Savage, S. Lamb & R. Sutherland *
Institute of Geological and Nuclear Sciences, 1 Fairway Drive, Lower Hutt 5010, New Zealand, S. A. Henrys & R. Sutherland * Department of Earth Sciences, University of Southern
California, 3651 Trousdale Parkway, Los Angeles, California 90210, USA, D. Okaya * Seismological Observatory, University of Nevada, 1664 North Virginia Street, Reno, Nevada 90210, USA, J. N.
Louie * Earthquake Research Institute, Tokyo University, 1-1-1 Yoyoi, Tokyo 113-0032, Japan, H. Sato & T. Iwasaki Authors * T. A. Stern View author publications You can also search for
this author inPubMed Google Scholar * S. A. Henrys View author publications You can also search for this author inPubMed Google Scholar * D. Okaya View author publications You can also
search for this author inPubMed Google Scholar * J. N. Louie View author publications You can also search for this author inPubMed Google Scholar * M. K. Savage View author publications You
can also search for this author inPubMed Google Scholar * S. Lamb View author publications You can also search for this author inPubMed Google Scholar * H. Sato View author publications You
can also search for this author inPubMed Google Scholar * R. Sutherland View author publications You can also search for this author inPubMed Google Scholar * T. Iwasaki View author
publications You can also search for this author inPubMed Google Scholar CONTRIBUTIONS All authors except J.N.L. and S.L. participated and led aspects of the data acquisition. J.N.L.
developed and applied the median filter to produce Fig. 3a and Extended Data Fig. 5a, c. T.A.S. wrote the initial manuscript. S.A.H. organized the shots and permissions, and did processing
for the pick migrations and the raw stack (Extended Data Figs 2 and 5b). D.O. and H.S. developed the initial shot gathers from the raw instrument data. T.A.S. and J.N.L. carried out
numerical modelling (Fig.4b, Extended Data Figs 1d, 6 and 9). All authors discussed and commented on various versions of the manuscript. CORRESPONDING AUTHOR Correspondence to T. A. Stern.
ETHICS DECLARATIONS COMPETING INTERESTS The authors declare no competing financial interests. EXTENDED DATA FIGURES AND TABLES EXTENDED DATA FIGURE 1 FREQUENCY SPECTRA AND ANALYSIS. A,
Frequency spectrum of the R2 reflection and the background noise. We only show frequencies above the 4.5-Hz cut-off frequency of the geophones used. B, Frequency spectrum of the R0 and R2
reflections. C, Table summarizing the frequency range for all events on the different shots; summaries of the geological conditions in each shot hole34 are also given. D, A spectral ratio
analysis16 between R2 and R0 reflections that yields a least squares linear fit to the data to give a gradient of −0.0627. Theoretically this gradient value can be equated to πΔ_t_/_Q_P
(ref. 16), where Δ_t_ is the TWTT between the R0 and R2 reflectors. For Δ_t_ = 20 s, we get an estimate of _Q_P (inverse attenuation) of 1,002 with a standard error of ±30 (based on least
squares linear regression). EXTENDED DATA FIGURE 2 PICK MIGRATION FOR R1 REFLECTOR AND SHOT GATHERS. A, Plan view of onshore and offshore SAHKE lines with shots 11 and 12 labelled. B, Pick
migrations for R1 reflection for shot 11 based on a laterally varying velocity model, which is derived from earthquake and shot data10. We use the velocity model created by 3D tomography to
carry out a migration of reflection picks10. Where the arcs converge to a constant solution gives the best structural interpretation of the reflector. We show the results for two shots (B,
shot 11; C, shot 12) and the common solution. The solution (black bar) appears to be a reflector in the mantle of the Australian plate, which dips to the southeast and is located within the
Taranaki Fault Zone. D, Shot gather for shot 11 with low band-pass filter of 5–10 Hz that brings out the low frequency, R1, southeast-dipping reflector (20 s depth at zero offset). It also
shows the R0 reflector (∼9 s at zero offset) for the top of the plate that dips to the northwest. Vertical axis is travel time (s) and horizontal axis is shot offset in km. Sg is the crustal
refracted S wave. E, Shot gather for shot 11 with band pass filter 16–30 Hz that shows up the R2 reflector with its broad frequency content, and suppresses the low frequency R1 reflection.
Rsed and PmP represent reflections interpreted to come from the upper surface of the sediment channel on top of the oceanic crust, and from the Moho of the oceanic Pacific plate,
respectively. EXTENDED DATA FIGURE 3 TWO SHOT GATHERS FROM EACH LINE END SHOWING REFLECTIONS R0 TO R3. A, Shot 12; B, shot 3. Both plots show data that have been band-passed between 8 and 25
Hz. The quality of the shots is highly dependent on the rock that the shot was placed in, with the drillers’ logs34 showing basement rock for shots 9, 10 and 11, and the very bottom of shot
hole 12. EXTENDED DATA FIGURE 4 STACKING AND MODEL SENSITIVITIES. A, Stacking chart for image shown in Fig. 3a. Colour scale shows magnitude of the fold, orange stars are shot points.
Numbers on the grid are metres north and east from the New Zealand Map Grid. B, Plots of seismic velocity versus depth12 and of stacking velocity (the root-mean-squared average seismic
velocity between the surface and a specific depth) versus depth used in the processing of the seismic section (Fig. 3). C, Plot of predicted plate thickness versus average _v_P for the
oceanic mantle; four plots are shown, each one derived using a different value of average crust _v_P (labelled). Based on the position in travel time for the reflectors at zero offset on
shot 11 (Extended Data Fig. 2c), we take the travel time in the oceanic crust to be 4 s and that in the oceanic mantle lid to be 14 s. The green dashed box represents the preferred range of
solutions based on likely velocities for the oceanic crust and oceanic upper mantle19. Note that the uncertainty in the thickness of plate determination is < ± 1 km. EXTENDED DATA FIGURE
5 STACKING TESTS. A, Stack as for Fig. 3a but without shot 11. This is a check to ascertain how much the high-quality, higher-frequency shot 11 dominated the stack. We still see the main
features in this stack, suggesting that the other shots are making a significant contribution. Dashed line shows our interpreted position for the Moho of the oceanic Pacific plate (PmP
reflection). B, A stack with no median filter applied. EXTENDED DATA FIGURE 6 WAVE-EQUATION MODELLING FOR A DIPPING PLATE MODEL. A, A model that simulates a highly simplified (oceanic crust
not included) SAHKE structure for input into wave equation modelling. A layer of low-wave-speed sediments is included at the base of the crust, so we can examine how multiples from this
channel interfere with the proposed R2 and R3 reflections at the base of the plate. The simulation is based on e3d35 and is run with _v_S = 0, so no S-wave reflections are created. B,
Synthetic shot gather for shot 11 geometry based on the model. RA. M EXTENDED DATA FIGURE 7 PRE-STACK DEPTH MIGRATION TESTS. A, The two azimuths used for 3D Kirchoff-sum, pre-stack depth
migration16 are in-line with the seismic line and at right angles to it (the cross-line). The velocity model used was an earlier version of that shown in Extended Data Fig. 5b with slightly
lower velocities. The input shot gathers for 3D migration were the instantaneous amplitude-attribute traces, heavily smoothed by median filtering as in Fig. 3b, then bandpass filtered to
produce an approximate zero-phase, low-frequency wavelet at each pre-stack reflection with strong amplitude. B, The in-line migration, showing coherency in the top 30 km with the dip of the
top of the plate evident. Here constant travel-time diffraction arcs are created from each shot point. Where energy is enhanced we interpret there to be reflectors, and conversely if there
is no enhancement, but just the diffraction arcs, we interpret this to be a lack of coherent structure. Coherent energy is seen at greater depths (90–100 km), which we ascribe to structure
of the LAB. C, Here the data of each shot gather are randomized (jack-knife test16), and put through the same migration. Comparing the randomized with the correct data migration shows what
are artefacts of the migration geometry, and what is signal. This confirms that images between 90 and 100 km depth seen in B are real. D, Result of migration in the cross-line direction; no
coherent alignments are seen. E, Jack-knife test for the cross-line migration. Note that E looks similar to D, suggesting there is no alignment of structure in the cross-line direction, and
that the reflections we are imaging are not side-swipe from out of plane structures. F, Schematic plot showing the relationship between the normalized thickness of the acoustic impedance
transition zone, _d_/_λ_, and the relative (that is, normalized to the value for a vanishingly thin transition zone) reflection coefficient. Here _d_ is the thickness of the zone, _λ_ is the
seismic wavelength, and the reflection coefficient is normalized to that for a impedance contrast of zero thickness14. Inset, schematic of the transition zone _d_ between two layers of
different velocities, _v_1 and _v_2. EXTENDED DATA FIGURE 8 GATHERS FOR SHOT 11 WHERE THE OFFSETS ARE PLOTTED IN-LINE AND CROSS-LINE. In A, the maximum offset from the shot is 70 km in a
northwest to southeast azimuth (see Extended Data Fig. 7a). In B, the maximum offset of seismic receivers from shot 11, in a southwest to northeast azimuth, is 7.5 km. These are gathers of
median filtered data (0.5 s by 41 traces), smoothed and passed through a 8–25 Hz bandpass filter, plotted in the 24–32 s range to bring out the R2 and R3 reflectors. Note the coherency in
the in-line direction and lack of coherency in the cross-line gather. This further corroborates evidence from the pre-stack depth migration that the R2 and R3 reflections come from a surface
below the northwest–southeast striking SAHKE04 line and are not side-swipe from out of plane reflections. EXTENDED DATA FIGURE 9 MODELS. A, Model of the structure and seismic velocities
just north of the SAHKE line based on receiver functions28. Note the proposed subduction channel of accreted sediments, in line with more recent work10, and the interpreted 13° dip, which is
in the 12°–15° range proposed in this study. B, A simple horizontal-layered model which is used as input for the synthetic wave equation modelling using software e3d35 shown in C. This is a
simplified approximation model for our observations beneath SAHKE04, although we ignore dip. C, Wave equation modelling35 based on input modelling shown in B for an input P wave and
vertical geophones. No gain control is applied. Strong primary reflections and multiples from the top of the plate and oceanic Moho are shown. In reality, the surface multiples are not that
strong because of scattering from topography. The R2 and R3 reflections can be seen as being weak events compared to R0. D, Wave equation modelling35 based on input modelling shown in B for
a input S wave and vertical geophones. Here the S-wave reflections are more prominent and S–P converted phases of R2 and R3 are predicted at about 38 and 41 s. Note that the S–P and S–S
reflections have no energy at zero incidence angle and significant energy only for offsets >30 km. As we are only stacking data with maximum offsets of 50 km, we expect that some, but
limited, S–P energy is contributing to the R4 phase of Fig. 3a. RELATED AUDIO KERRI SMITH CHATS TO TIM STERN ABOUT HIS EXPLOSIVE PLATE TECTONIC STUDIES POWERPOINT SLIDES POWERPOINT SLIDE FOR
FIG. 1 POWERPOINT SLIDE FOR FIG. 2 POWERPOINT SLIDE FOR FIG. 3 POWERPOINT SLIDE FOR FIG. 4 RIGHTS AND PERMISSIONS Reprints and permissions ABOUT THIS ARTICLE CITE THIS ARTICLE Stern, T.,
Henrys, S., Okaya, D. _et al._ A seismic reflection image for the base of a tectonic plate. _Nature_ 518, 85–88 (2015). https://doi.org/10.1038/nature14146 Download citation * Received: 15
March 2014 * Accepted: 03 December 2014 * Published: 04 February 2015 * Issue Date: 05 February 2015 * DOI: https://doi.org/10.1038/nature14146 SHARE THIS ARTICLE Anyone you share the
following link with will be able to read this content: Get shareable link Sorry, a shareable link is not currently available for this article. Copy to clipboard Provided by the Springer
Nature SharedIt content-sharing initiative