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Enhanced inner core fine-scale heterogeneity towards Earth’s centre

Abstract

Earth’s inner core acquires texture as it solidifies within the fluid outer core. The size, shape and orientation of the mostly iron grains making up the texture record the growth of the inner core and may evolve over geologic time in response to geodynamical forces and torques1. Seismic waves from earthquakes can be used to image the texture, or fabric, of the inner core and gain insight into the history and evolution of Earth’s core2,3,4,5,6. Here, we observe and model seismic energy backscattered from the fine-scale (less than 10 km) heterogeneities7 that constitute inner core fabric at larger scales. We use a novel dataset created from a global array of small-aperture seismic arrays—designed to detect tiny signals from underground nuclear explosions—to create a three-dimensional model of inner core fine-scale heterogeneity. Our model shows that inner core scattering is ubiquitous, existing across all sampled longitudes and latitudes, and that it substantially increases in strength 500–800 km beneath the inner core boundary. The enhanced scattering in the deeper inner core is compatible with an era of rapid growth following delayed nucleation.

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Fig. 1: Example of ICS and map of arrays.
Fig. 2: ICS energy characteristics.
Fig. 3: Inner core 3D scattering structure.
Fig. 4: Variation of scattering strength and porosity in the equatorial plane viewed from Earth’s pole.

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Data availability

Requests for International Monitoring System array data can be completed online at https://www.ctbto.org/specials/vdec/. Data for ASAR and WRA can be downloaded from Incorporated Research Institutions for Seismology (IRIS; www.iris.edu) with network code AU. Data for ILAR, NVAR, PDAR and TXAR are available from IRIS with the network code IM; requests for YKA data can be submitted online at https://earthquakescanada.nrcan.gc.ca/fdsnws/. The seismic data for XHDR can be downloaded from IRIS with network code XH, and the seismic data of YDWG and YDWS are available from IRIS with the network code YD in 2013–2014. The Global Centroid Moment Tensor earthquake catalogue is available at https://www.globalcmt.org/CMTsearch.htmlSource data are provided with this paper.

Code availability

The seismic array processing code used in this study is available online at https://zenodo.org/record/6784342. The numerical code for the inner core compaction model is available online at https://github.com/MarineLasbleis/mushdynamics. The numerical code for the phonon simulation is available online at https://github.com/nmancinelli/psphoton. All figures were generated using pygmt (https://www.pygmt.org/latest/).

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Acknowledgements

We thank N. Mancinelli for sharing the phonon code and providing helpful modelling suggestions. We thank J. Vidale for helpful comments. This work was funded by the National Science Foundation (EAR-1722542). This work is approved for public release under LA-UR-22-28862.

Author information

Authors and Affiliations

Authors

Contributions

G.P. developed the array processing package gPar, analysed most array data, performed heterogeneity modelling and analysed inner core geodynamic evolution. K.D.K. supervised and acquired funding for the project and provided advice on data processing. S.-M.W. helped analyse array data. W.W. helped in the phonon scattering modelling. M.L. helped in the inner core compaction modelling. G.E. helped in funding acquisition and provided advice on data processing. All the authors contributed to the interpretation of the observations and in the preparation of the manuscript.

Corresponding author

Correspondence to Guanning Pang.

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Extended data figures and tables

Extended Data Fig. 1 Array geometries and station codes.

The triangles (blue for IMS arrays and green for Antarctica networks) are individual array elements and the dashed grey lines link the elements to the array reference points.

Extended Data Fig. 2 Example ICS observations in categories 1–3.

All three earthquakes were recorded in Chiang Mai, Thailand (CMAR) and had similar magnitudes (Mw ~6.3). The blue-dashed lines mark the predicted PKiKP arrival time and the red dashed lines mark the theoretical PKiKP slowness. Rows a through c (back azimuth, slowness, and beam amplitude) show the results from the sliding window slowness analysis, presented as a function of time relative to earthquake origin time. Row d shows envelopes of delay-and-sum beams formed at the theoretical PKiKP slowness. The red line is the best fitting curve to the background energy using the quasi-analytical coda decay model (Eq. (1)). Row e shows the denoised PKiKP envelopes as a function of time relative to PKiKP.

Extended Data Fig. 3 Overlapping PKiKP coda observations.

a, Locations of arrays AKASG (red triangle) and CMAR (blue triangle). The red star is a Category 1 earthquake recorded at AKASG and the blue stars are three Category 2 earthquakes recorded at CMAR. The solid lines are the ray paths from earthquakes to arrays and the dots are the corresponding bounce points on the ICB. These different earthquake-array combinations sample the same inner core region but different crust and mantle structure. Array response functions at 1 Hz with a slowness of 0 s/° are shown for b, AKASG and c, CMAR. d, Single (red) and stacked (blue) denoised PKiKP envelopes from AKASG and CMAR, respectively. e, Example delay-and-sum beam at the YKA seismic array in Canada. The earthquake (Mw 6.1, 2013/04/21 03:22:16 utc, 29.93°N, 138.89.62°E, 422 km depth, USGS-NEIC) occurred near Japan about 71°. Grey windows mark the signals used in f and g. f, Slowness vector analysis of the direct PKiKP phase (first grey window on e). Blue dots mark the theoretical slowness from AK135. White crosses indicate vertical incidence. Pink crosses represent bootstrap solutions determined by repeating the slowness analysis for 50 randomly resampled sets of array elements. g, Similar to f but for a time window deep in the coda (second grey window on e). Note that the coda energy has a lower ray parameter than the direct PKiKP wave but with a similar back azimuth, implying that it is arriving from great circle heterogeneity deep within the inner core beneath the PKiKP bounce point.

Extended Data Fig. 4 Geographic regions sampled in this study.

Names of regions located in the quasi-eastern hemisphere (longitude > 0) start with E. Names of regions in the quasi-western hemisphere (longitude <0) start with W. The colour is the number of earthquakes that sampled the region.

Extended Data Fig. 5 Observations and predictions of inner core scattered (ICS) energy.

The red lines are ICS envelope stacks sampling different inner core geographic regions (shown in Extended Data Fig. 4) observed at various arrays. The blue lines are the corresponding best-fitting simulations from the multiple scattering phonon approach.

Extended Data Fig. 6 Trade-off between a and ε.

a, Backscattered energy (D−1.5) as a function of correlation length (a) and root-mean-square velocity perturbation (ε). Stars mark the (a, ε) pairs used in generating synthetic envelopes shown in b. b, Synthetic envelopes from scattering models with the same diffusivity D but different (a, ε) pairs marked as stars in a.

Extended Data Fig. 7 Phonon models and model fitting algorithm.

a, A demonstration of the model fit using the algorithm in Eq. 4. The grey line is the observed ICS envelope. The red line is the best-fitting model prediction, and the blue line is a model prediction mismatching the observation by a factor of 4. b, All inner core heterogeneity models in this study. Green lines are the Class 1 models with uniform diffusivities. Red lines are the Class 2 models with stronger scattering strength in deep inner core. Blue lines are Class 3 models with weaker scattering with depth. The grey line is the same observation as in a. The brown line is the best-fit model.

Extended Data Fig. 8 Inner core two-stage growth model.

a, Inner core delayed nucleation and two-stage growth model. The inner core growth is in two steps: I. initial rapid growth stage (red segment); and II. Steady growth stage (blue). The right end of the x-axis is the present time. The left end, i.e., 0, is the moment when the centre of the primordial outer core cooled below its melting point. The y-axis is the normalized inner core radius at time t. RICB is the present inner core radius. The radius at the end of step I is a function of the supercooling temperature, which is shown in b. b, The initial inner core radius at the end of the early rapid growth step (step I) as a function of the supercooling temperature at historical Earth centre, modified from Huguet et al.30. The grey zone denotes the historical inner core radius at the end of Step I in the porosity evolution with delayed nucleation at 0.07–0.12τic, where τic is the presumed inner core age in the conventional growth model (dashed line in a).

Extended Data Fig. 9 Scattering strength and porosity along the radius of the inner core in the present day.

a, Global average scattering variation along the inner core radius. Inner core porosity structure based on three growth models: b, conventional inner core growth34, c, inner core nucleation delayed to 0.12τic, and d, inner core nucleation delayed nucleation delayed to 0.18τic. Yellow lines indicate 500 km below ICB, where the scattering strength increases globally.

Extended Data Table 1 Arrays in this study

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Pang, G., Koper, K.D., Wu, SM. et al. Enhanced inner core fine-scale heterogeneity towards Earth’s centre. Nature 620, 570–575 (2023). https://doi.org/10.1038/s41586-023-06213-2

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