Eikonal basin tomography

Part 10 — Real-field capstones

Learning objectives

  • Close the forward-operator loop: PINN-eikonal as inverse-problem driver
  • Recognise body-wave first-arrival tomography vs ANT (§10.3) — same shape, different sources
  • Apply Tikhonov-regularised LS on event-station travel times
  • Connect to production EikoNet (Smith et al 2021) and PINNeik (Bin Waheed 2021)
  • Quantify recovery quality vs ray-coverage density

§10.3 inverted continental-scale velocity from AMBIENT-NOISE station-pair travel times. §10.7 closes the forward-operator loop: invert basin-scale velocity from BODY-WAVE first-arrival travel times — many earthquakes (or quarry blasts, or controlled active sources) propagating to a regional receiver array. Same Tikhonov-regularised least-squares inverse problem, same algorithmic shape, different forward-source configuration.

The PINN-eikonal connection

The cost of basin tomography is dominated by the FORWARD MODEL: computing predicted travel time from each event to each receiver through the candidate velocity field, repeated at every gradient-descent iteration. Classical FSM costs O(N_grid × N_sweeps) per event. For 1000 events × 100 stations × 100 inversion iterations = 10^7 FSM solves at ~50 ms each → 50 hours of compute. Production scale demands faster.

PINN-EIKONAL replaces FSM with a pre-trained neural network that takes (event_x, event_y, station_x, station_y, velocity_field) as input and outputs travel time as a single network forward pass — typically 100× faster than FSM. Smith et al 2021 EikoNet and Bin Waheed et al 2021 PINNeik formalise this. Once trained, the PINN-eikonal forward call costs ~0.5 ms; the same 50-hour FSM-based tomography becomes ~30 minutes.

Crucially, the INVERSE PROBLEM has the same shape regardless of which forward operator produces the travel times — Tikhonov-regularised LS on the slowness perturbation field. This widget uses straight-ray as a proxy for PINN-eikonal output (production codes use the trained PINN; the inversion code is unchanged).

Try it

Eikonal equation: first-arrival traveltime fieldsurface (z=0)high-V lensV = 3500 m/sbackground V = 2000 m/st=0.1t=0.2t=0.3t=0.4t=0.5t=0.6t=0.7sourcex (m) →depth (m) ↓

Setup: a 100 × 60 km regional sedimentary basin (e.g., Los Angeles or Imperial Valley scale):

  • Reference body-wave velocity 4.5 km/s (typical mid-crustal P-wave)
  • Truth: 2 anomalies — a SLOW sedimentary basin fill (Δv = −10%, σ = 14 km) and a FAST crystalline basement ridge (Δv = +6%, σ = 11 km)
  • 25 events distributed over the region (mimicking seismicity along regional faults) + 30 stations on a quasi-regular grid
  • ~750 event-station pairs after distance filtering, σ_pick = 0.4 s
  • Inversion: 540-cell slowness map, 250 iters of Tikhonov-regularised gradient descent, λ = 0.8 (moderate smoothing)

Two panels:

  • Truth velocity map: red = slow basin, blue = fast ridge, white squares = stations, yellow circles = events.
  • Recovered velocity map: same colormap, after Tikhonov inversion. Compare amplitudes + spatial extent to truth.

Below the panels, summary box reports per-anomaly recovered amplitude as percentage of truth + correct-sign indicator. Expected behaviour: both anomalies recovered with correct sign and 50-100% of true amplitude on most seeds.

Production basin tomography

Real basin tomography has been done at:

  • Los Angeles Basin (Hauksson 2000, Lin et al 2010, Shaw et al 2015): 50,000+ earthquake events recorded by Southern California Seismic Network, inverted for 3-D Vp + Vs over the Los Angeles region. Established the Puente Hills + Palos Verdes blind thrust faults. PINN-eikonal extensions by Smith et al 2021.
  • Imperial Valley: Salton Trough geothermal area; magmatic + faulting structure resolved at 2-5 km lateral resolution.
  • Cascadia subduction zone: deep events tomographically mapping the subducting slab.
  • Yellowstone: high-resolution P + S body-wave tomography revealing the upper-mantle plume (Smith et al 2009).

What §10.8 will do

§10.8 closes the textbook with a META capstone: take a CURRENT arXiv PINN paper (or a recent Geophysics journal paper) and walk through reproducing the central result end-to-end. Less a new physics topic, more a "you now have the tools — here's how to read the literature."

References

  • Smith, J.D., Azizzadenesheli, K., Ross, Z.E. (2021). EikoNet: Solving the eikonal equation with deep neural networks. IEEE Trans. Geosci. Remote Sens. 59(12), 10685–10696. PINN-eikonal forward operator usable in basin tomography.
  • Bin Waheed, U., Haghighat, E., Alkhalifah, T., Song, C., Hao, Q. (2021). PINNeik: Eikonal solution using physics-informed neural networks. Computers & Geosciences 155, 104833. Independent PINN-eikonal formulation.
  • Hauksson, E. (2000). Crustal structure and seismicity distribution adjacent to the Pacific and North America plate boundary in southern California. JGR 105(B6), 13875–13903. Production LA-basin tomography.
  • Lin, G., Thurber, C.H., Zhang, H., Hauksson, E., Shearer, P.M., Waldhauser, F., Brocher, T.M., Hardebeck, J. (2010). A California statewide three-dimensional seismic velocity model from both absolute and differential times. Bull. Seismol. Soc. Am. 100(1), 225–240. Continental-scale body-wave tomography.
  • Shaw, J.H., Plesch, A., Tape, C., Suess, M.P., Jordan, T.H., Ely, G., Hauksson, E., Tromp, J., Tanimoto, T., Graves, R., Olsen, K., Nicholson, C., Maechling, P.J., Rivero, C., Lovely, P., Brankman, C.M., Munster, J. (2015). Unified Structural Representation of the southern California crust and upper mantle. Earth Planet. Sci. Lett. 415, 1–15. Modern integrated SoCal velocity model.

This page is prerendered for SEO and accessibility. The interactive widgets above hydrate on JavaScript load.