Constraints on transition zone discontinuities from surface wave overtone measurements Ueli Meier Jeannot Trampert Andrew Curtis.

Slides:



Advertisements
Similar presentations
A Partition Modelling Approach to Tomographic Problems Thomas Bodin & Malcolm Sambridge Research School of Earth Sciences, Australian National University.
Advertisements

SPP 1257 Modelling of the Dynamic Earth from an Integrative Analysis of Potential Fields, Seismic Tomography and other Geophysical Data M. Kaban, A. Baranov.
Lithospheric Plates The lithosphere can be defined thermally by an isotherm at the base of the lithosphere which should be around 1350 o C. Mantle rocks.
Conclusions… Challenge: 1)Seismic waves are affected by variations in temperature, pressure, composition, mineralogy, structure (layering, scales and distribution.
Upper mantle of the Bohemian Massif (Central Europe) studied by surface waves from Kurile Islands M8.1 and M8.3 earthquakes Petr Kolinsky Jiri Malek Institute.
Constraints on the LAB from Seismology, Petrology and Geodynamics/Mineral Physics fundamentals/10h.html A. Bengston, M. Blondes,
Neural Network Approach to Modeling the Laser Material-Removal Process By Basem. F. Yousef London, Canada, N6A 5B9 December 2001.
The Earth’s Structure Seismology and the Earth’s Deep Interior The Earth’s Structure from Travel Times Spherically symmetric structure: PREM - Crustal.
Dynamic topography, phase boundary topography and latent-heat release Bernhard Steinberger Center for Geodynamics, NGU, Trondheim, Norway.
Probabilistic tomography
Thermal structure of old continental lithosphere from the inversion of surface-wave dispersion with thermodynamic a-priori constraints N. Shapiro, M. Ritzwoller,
Measureable seismic properties
SPICE Research and Training Workshop III, July 22-28, Kinsale, Ireland Seismic wave Propagation and Imaging in Complex media: a European.
Clines Cline means ‘rapid change in’ Thermocline is a rapid change in temperature Pycnocline is a rapid change in density.
3D seismic imaging of the earth’s mantle Barbara Romanowicz Department of Earth and Planetary Science U.C. Berkeley.
How well do we know density in the Earth?. Velocity in the Earth is well known.
Low frequency coda decay: separating the different components of amplitude loss. Patrick Smith Supervisor: Jürgen Neuberg School of Earth and Environment,
The Earth in three dimensions From seismology to composition and temperature.
Seismic refraction surveys
A low velocity layer (LVZ) at the top of the subducting plate has been detected in a majority of subduction zones. LVZ may be a hydrated layer of oceanic.
Geophysical Inverse Problems with a focus on seismic tomography CIDER2012- KITP- Santa Barbara.
Surface wave tomography: part3: waveform inversion, adjoint tomography
Body Waves and Ray Theory
Intro to Geomorphology (Geos 450/550) Lecture 5: watershed analyses field trip #3 – Walnut Gulch watersheds estimating flood discharges.
Complexity in Carbonate Systems Jon Hill 1 Andrew Curtis 1 Rachel Wood 2 Dan Tetzlaff 3 1 Univeristy of Edinburgh 2 Schlumberger Cambridge Research and.
Surface wave tomography : 1. dispersion or phase based approaches (part A) Huajian Yao USTC April 19, 2013.
Seismology – Lecture 2 Normal modes and surface waves Barbara Romanowicz Univ. of California, Berkeley CIDER Summer KITP.
Cooling of the Earth: A parameterized convection study of whole versus layered models by McNamara and Van Keken 2000 Presentation on 15 Feb 2005 by Group.
Department of Geology & Geophysics
Probing Earth’s deep interior using mantle discontinuities Arwen Deuss University of Cambridge, UK also: Jennifer Andrews, Kit Chambers, Simon Redfern,
Surface waves Earthquakes generate both body waves (P, S) and surface waves Surface waves are generated along any free surface in the medium In the Earth,
The modeling of the channel deformations in the rivers flowing into permafrost with an increase in ambient temperature E. Debolskaya, E. Zamjatina, I.Gritsuk.
Seismological observations Earth’s deep interior, and their geodynamical and mineral physical interpretation Arwen Deuss, Jennifer Andrews University of.
The Lithosphere There term lithosphere is in a variety of ways. The most general use is as: The lithosphere is the upper region of the crust and mantle.
SOES6002: Modelling in Environmental and Earth System Science CSEM Lecture 1 Martin Sinha School of Ocean & Earth Science University of Southampton.
Which Mantle Interfaces Do Seismologists See? Peter Shearer* IGPP/SIO/U.C. San Diego * With figures from Castle, Deuss, Dueker, Fei, Flanagan, Gao, Gu,
Water in the Mantle ? Can be stored: 1)Hydrous minerals - only stable shallow 2) Dissolved in normally anhydrous minerals 3)A hydrous silica-rich fluid.
SPICE Research and Training Workshop III, July 22-28, Kinsale, Ireland Seismic wave Propagation and Imaging in Complex media: a European.
The good sides of Bayes Jeannot Trampert Utrecht University.
Global seismic tomography and its CIDER applications Adam M. Dziewonski KITP, July 14, 2008.
Earthquakes and the Interior  Earthquakes are definitely a geologic hazard for people living in earthquake regions, but the seismic waves generated by.
Adam M. Dziewonski in cooperation with Ved Lekic and Barbara Romanowicz Terra Incognita Again ; Five zones in the mantle KITP July 19, 2012.
EVIDENCE THAT RIDGES ARE FED FROM THE TRANSITION ZONE BUT NOT AS CONTINUOUS UPWELLING SHEETS. WHEN A TZ UPWELLING COMES UP DIRECTLY UNDER A RIDGE IT IS.
Lithospheric Structure of the Gulf of California – Salton Trough Region, NARS-Baja Array Working Group: Robert Clayton, Caltech Don Forsyth, Brown Antonio.
Global Tomography -150 km depth
Seismological Analysis Methods Receiver FunctionsBody Wave Tomography Surface (Rayleigh) wave tomography Good for: Imaging discontinuities (Moho, sed/rock.
Constraints on the observation of mantle plumes using global seismology Arwen Deuss University of Cambridge, UK.
1 Wavefield Calibration Using Regional Network Data R. B. Herrmann Saint Louis University.
Barbara Romanowicz1, Aimin Cao2, M. Panning3, F
Reference Earth model: heat-producing elements & geoneutrino flux *Yu Huang, Roberta Rudnick, and Bill McDonough Geology, U Maryland *Slava Chubakov, Fabio.
SPICE Research and Training Workshop III, July 22-28, Kinsale, Ireland Seismic wave Propagation and Imaging in Complex media: a European.
How can global seismic tomography help in studies of “Early Earth” Berkeley, December 10, 2011.
Seismic waves Mathilde B. Sørensen and Jens Havskov.
Rocks and the Earth’s Interior
Global Tomography -150 km depth
Azimuthal anisotropy layering in the Pacific upper mantle
Island Arc Magmatism Eruption of Anatahan Volcano,
Susan L. Beck George Zandt Kevin M. Ward Jonathan R. Delph.
Douglas A. Wiens & James Conder
Nils Holzrichter, Jörg Ebbing
Transition Zone Discontinuities
1-D Mississippi embayment sediment velocity structure and anisotropy: constraint from ambient noise analysis on a dense array Chunyu,Liu1; Charles A. Langston1.
Length scale of heterogeneity
Mixture Density Networks
Skeletonized Wave-Equation Surface Wave Dispersion (WD) Inversion
Phase Velocity & Group Velocity.
Bell Ringer 1. What physical layer of the Earth makes up all of the crust and the very upper portion of the mantle? 2. The core can be broken up into.
Does AVO Inversion Really Reveal Rock Properties?
Geophysics/Tectonics
Machine Learning and Wave Equation Inversion of Skeletonized Data
Presentation transcript:

Constraints on transition zone discontinuities from surface wave overtone measurements Ueli Meier Jeannot Trampert Andrew Curtis

Non-linear inversion of probability density functions of phase velocity maps Visser et al. 2008

The neural network (NN) approach: Bishop 1995, MacKay 2003 A neural network can be seen as a non-linear filter between any input and output The NN is an approximation to a non-linear function g where d=g(m), forward or inverse A training set is used to calculate the coefficients of the NN by non-linear optimisation

1) Generate a training set: D={d n,m n } Network Input: Observed or synthetic data for training Neural Network dndn p(m|d n,w) Network Output: Conditional probability density 2) Network training:3) Forward propagating a new datum through the trained network (i.e. solving the inverse problem) d obs p(m|d obs,w*)

Topography (Sediment) Moho Depth 220 km Discontinuity Vpv, Vph, Vsv, Vsh,  Vs (Vp,  linearly scaled) % Prem +- 5 % Prem 8 layers 3 layers Model Parameterization 9 layers 24 layers down to 1500 km below Prem 400 km Discontinuity 660 km Discontinuity 8 layers Vpv, Vph, Vsv, Vsh,  20km +- 5 % Prem 20km 30km

Example of a model realisation

Data At each geographical point, we use local dispersion curves and their Gaussian uncertainties (Visser et al. 2008) Periods between 35 s and 175 s Rayleigh waves up to 6 th overtone Love waves up to 5 th overtone

Mean dlnVs model

Discontinuities

Trade-offs between parameters

Interpretation Mixture of olivine, wadsleydite and melt Surface waves see top of discontinuity SS underside reflections see bottom of discontinuity ~30 km ~0.8wt% water The nature of the average 410km discontinuity 394 km 418 km

Interpretation dlnVs and dhTZ  dT and dOH Romanowicz and Gung 2002

Interpretation Average nature of discontinuities: 660-km relatively sharp: surface waves and SS underside reflection are consistent 410-km is ~30km broad: corresponds to an average of 08wt% of water

Interpretation Lateral variations in the transition zone: Temperature variations agree with tectonic expectations Water variations show a remarkable correlations with maps of global attenuation Slabs unlikely to transport water to the TZ Water is likely a remnant of deep magma ocean  water filter model