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Propagation delays in InSAR
GE California Institute of Technology, 2013
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Propagation delays in InSAR
TerraSAR-X CosmoSkyMed Envisat ERS-1/2 RadarSat Sentinels Kollias et al, 2007, BAMS
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An example... - One month temporal baseline (no deformation)
- Topography <=> Atmospheric delay
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An example...
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An example...
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An example...
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Differential delay First pass Second Pass
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Differential delay First pass Second Pass
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A bit of theory Air Refractivity: : Total Pressure : Temperature
Refraction index : Total Pressure : Temperature : Cloud Water Content : Electron Density : Frequency : Constants
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A bit of theory - Small perturbation - Very hard to estimate
Air Refractivity: : Total Pressure : Temperature : Cloud Water Content : Electron Density Real-life range : Frequency - Small perturbation - Very hard to estimate : Constants Hanssen, 2001
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A bit of theory - Small perturbation - Very hard to estimate
Air Refractivity: : Total Pressure : Temperature : Cloud Water Content : Electron Density Real-life range : Frequency - Small perturbation - Very hard to estimate : Constants Hanssen, 2001
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A bit of theory Air Refractivity: : Total Pressure : Temperature
- Dispersive effect - Long wavelength perturbations (~100 km) - Effect is small in C-band (too short wavelength) - Significant in L-band : Cloud Water Content : Electron Density : Frequency : Constants
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Ionospheric perturbation
Shen et al., 2009, Nat. Geosci.
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Ionospheric perturbation
“clean” Interferogram Azimuth offsets Phase gradient - Estimate the azimuth offset - Compute the phase gradient - Extract the proportionality factor - Correct the interferogram Problem: Only works where there is no deformation along azimuth Interferogram Ionospheric phase screen Raucoules & de Michele, IEEE GRSL
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Ionosphere (not today)
A bit of theory Air Refractivity: : Total Pressure : Temperature Ionosphere (not today) : Cloud Water Content : Electron Density Troposphere (today) : Frequency : Constants
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A bit of theory Air Refractivity: Nadir Delay: and : Dry Air Pressure
: Total Pressure : Temperature : Specific Constant for dray air and vapor : Cloud Water Content : Gravitation : Electron Density : Partial pressure in Water Vapor : Frequency : Constants
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A bit of theory Delay along the Line-Of-Sight wrt. reference altitude:
: Dry Air Pressure : Total Pressure : Temperature : Specific Constant for dray air and vapor : Cloud Water Content : Gravitation : Electron Density : Partial pressure in Water Vapor : Frequency : Constants
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A bit of theory If I had a pressure profile...
Delay along the Line-Of-Sight wrt. reference altitude: If I had a pressure profile...
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... and a temperature profile...
A bit of theory Delay along the Line-Of-Sight wrt. reference altitude: ... and a temperature profile...
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... and a Water Vapor Partial Pressure profile...
A bit of theory Delay along the Line-Of-Sight wrt. reference altitude: ... and a Water Vapor Partial Pressure profile...
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... I could compute the total delay:
A bit of theory Delay along the Line-Of-Sight wrt. reference altitude: ... I could compute the total delay:
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? A bit of theory ... I could compute the total delay:
Delay along the Line-Of-Sight wrt. reference altitude: ? ... I could compute the total delay: But usually, I don’t have all those things (actually, never...).
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Do we really need to correct for that delay?
Can’t we just filter it, or whatever?
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Do we really need to correct for that delay?
Can’t we just filter it, or whatever? Yes, you can...
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Do we really need to correct for that delay?
Can’t we just filter it, or whatever? Yes, you can... ... but you should not.
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Single interferograms
Mw 7.7 Depth ~ 100 km
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Time filtering, then...? Stacking:
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Time filtering, then...? Stacking:
If we have independent interferograms, with random noise (in time)
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Time filtering, then...? Stacking:
If we have independent interferograms, with random noise (in time) Doin et al, 2009, J. App. Geophy.
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Now that we can do better, still no!!!
Time filtering, then...? Stacking: If we have independent interferograms, with random noise (in time) Now that we can do better, still no!!!
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==> Stacking or Time Series
How to correct then? Turbulent Delay Stratified Tropospheric Delay + ==> Stacking or Time Series - Random in Space and Time - Numerous Acquisitions to average or smooth the signal
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==> Stacking or Time Series
Separating the delay Turbulent Delay Stratified Tropospheric Delay + ==> Stacking or Time Series 2
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==> Stacking or Time Series
Separating the delay Turbulent Delay Stratified Tropospheric Delay + ==> Stacking or Time Series Semivariogram: Covariance:
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==> Stacking or Time Series
Separating the delay Turbulent Delay Stratified Tropospheric Delay + ==> Stacking or Time Series
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Estimating a phase/elevation relationship
Empirical Correction Estimating a phase/elevation relationship
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Empirical Methods Estimating a phase/elevation relationship
Joint inversion model/orbit/troposphere Cavalie et al, 2008; Jolivet et al., 2012
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Empirical Methods Estimating a phase/elevation relationship
Joint inversion model/orbit/troposphere Cavalie et al, 2008; Jolivet et al., 2012
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Estimating a phase/elevation relationship
Empirical Methods Estimating a phase/elevation relationship Multi-scale approach Lin et al, 2010
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- Deformation/Topography correlation
Empirical Methods - Deformation/Topography correlation
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Prediction Methods - Most methods focus on constructing vertical profiles of delay Available Data: GPS zenith delays Local Atmospheric data Multi-spectral imagery systems Global Re-analysis Available Methods: Interpolation (2D / 3D / Ray tracing) Meso-scale modeling
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Local Atmospheric Data
Prediction Methods Local Atmospheric Data - Data from a meteorological station - Radio sounding profile Delacourt et al. 1998, GRL
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Prediction Methods GPS zenith delays Onn & Zebker, 2006, JGR
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Prediction Methods GPS zenith delays Onn & Zebker, 2006, JGR
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Puyssegur et al, 2007, JGR; Li et al, 2012, GJI
Prediction Methods Multispectral Images Multi-spectral imagery system onboard Envisat: - Passive system (captures the electro-magnetic field reflected by the ground surface) - 15 Bands - Combination of band 14 and 15 gives the Integrated Precipitable Water Vapor - Integrated Wet delay and and : Specific Constant for dray air and vapor : Ratio of molecular masses of water vapor and dry air : Constants Puyssegur et al, 2007, JGR; Li et al, 2012, GJI
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Prediction Methods Multispectral Images Good:
Does not only correct for stratified features Predicts turbulence Bad: Does not work for night-time acquisitions Does not work if dense cloud cover Li et al, 2012, GJI
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Goal: Reproduce the turbulences using fine modeling
Prediction Methods Meso-Scale Modeling Goal: Reproduce the turbulences using fine modeling MM5 Modeling Interferogram Puyssegur et al, 2007, JGR
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Prediction Methods ERA-Interim Dee et al, 2011 Available Data:
GPS zenith delays Local Atmospheric data Multi-spectral imagery systems Global Re-analysis These data are not always available This is fine over SoCal, but Tibet is another story ERA-Interim Dee et al, 2011 - ECMWF atmospheric model - Global ~75 km grid - 4 solutions a day at 0 am, 6 am, 12 pm and 6 pm - Altitude, temperature and water vapor partial pressure at 37 pressure levels (surface to 50 km alt.)
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Computing Delay Maps from GAM
1 - Computing delay functions
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Computing Delay Maps from GAM
1 - Computing delay functions 2 - Spatial bilinear interpolation and spline interpolation for altitude
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Computing Delay Maps from GAM
One month temporal baseline == no deformation expected
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Computing Delay Maps from GAM
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Computing Delay Maps from GAM
ERA-Interim Dee et al, 2011 - ECMWF atmospheric model - Global ~75 km grid - 4 solutions a day at 0 am, 6 am, 12 pm and 6 pm - Altitude, temperature and water vapor partial pressure at 37 pressure levels (surface to 50 km alt.) North AmeRican Re-analysis Mesinger et al, 2006 - NOAA atmospheric model - North America (Canada, USA + Hawaii, Mexico), Lambert Conic grid, ~0.3 degrees - 8 solutions a day - Altitude, temperature and water vapor partial pressure at 29 pressure levels. Modern Era-Restrospective Analysis Rienecker et al, 2011 - NASA atmospheric model - Global ~0.5 deg - 4 solutions a day - Altitude, temperature and water vapor partial pressure at 42 pressure levels. Probably other models available, need to try these...
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Removing the atmosphere is great because...
... it allows to unwrap the phase where we thought it was impossible. - Atmosphere introduces high fringe rate over areas with rough topography. - High fringe rate is a problem for unwrapping (aliasing of fringe rates) - Correction “flattens” the phase field and allows for unwrapping Jolivet et al, 2011, GRL
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Removing the atmosphere is great because...
... it removes the seasonal oscillations in time series.
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Removing the atmosphere is great because...
... it removes the bias in rate estimates.
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Removing the atmosphere is great because...
... I hope it will allow to measure long wavelength deformations. - Long-wavelength tropospheric perturbation mimic orbital artifacts - Usually, we fit a first order polynomial function on the interferogram, pretending it comes from orbital errors - This long-wavelength is actually a combination of orbits + troposphere + tides (Hilary??)
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Bibliography - Kollias, P. et al., Millimeter-Wavelength Radars. Bulletin of the American Meteorological Society, pp.1–17. - Hanssen, R.F., Radar Interferometry, Data Interpretation and Error Analysis, Kulwer Academic Publishers. - Shen, Z.-K. et al., Slip maxima at fault junctions and rupturing of barriers during the 2008 Wenchuan earthquake. Nature Geoscience, 2(10), pp.718–724. - Raucoules, D. & de Michele, M., Assessing Ionospheric Influence on L-Band SAR Data: Implications on Coseismic Displacement Measurements of the 2008 Sichuan Earthquake. IEEE Geoscience and Remote Sensing Letters, 7(2), pp.286–290. - Doin, M.P. et al., Corrections of stratified tropospheric delays in SAR interferometry: Validation with global atmospheric models. Journal of Applied Geophysics, 69(1), pp.35–50. - Cavalié, O. et al., Measurement of interseismic strain across the Haiyuan fault (Gansu, China), by InSAR. Earth and Planetary Science Letters, 275(3-4), pp.246–257. - Lin, Y.-N.N. et al., A multiscale approach to estimating topographically correlated propagation delays in radar interferograms. Geochemistry Geophysics Geosystems, 11(9), p.Q09002. - Jolivet, R. et al., Shallow creep on the Haiyuan Fault (Gansu, China) revealed by SAR Interferometry. Journal of Geophysical Research, 117(B6). - Delacourt, C., Briole, P. & Achache, J., Tropospheric corrections of SAR interferograms with strong topography. Application to Etna. Geophysical Research Letters, {25}({15}), pp.{2849–2852}. - Onn, F. & Zebker, H.A., Correction for interferometric synthetic aperture radar atmospheric phase artifacts using time series of zenith wet delay observations from a GPS network. Journal of Geophysical Research, 111(B9). - Puysségur, B., Michel, R. & Avouac, J.-P., Tropospheric phase delay in interferometric synthetic aperture radar estimated from meteorological model and multispectral imagery. Journal of Geophysical Research, 112(B5). - Li, Z.W. et al., Correcting atmospheric effects on InSAR with MERIS water vapour data and elevation-dependent interpolation model. Geophysical Journal International, 189(2), pp.898–910. - Dee, D.P. et al., The ERA-Interim reanalysis: configuration and performance of the data assimilation system. Quarterly Journal of the Royal Meteorological Society, 137(656), pp.553–597. - Mesinger, F. et al., North American Regional Reanalysis. Bulletin of the American Meteorological Society, 87(3), pp.343–360. - Rienecker, M.M. et al., MERRA: NASA’s Modern-Era Retrospective Analysis for Research and Applications. Journal of Climate, 24(14), pp.3624–3648. - Jolivet, R. et al., Systematic InSAR tropospheric phase delay corrections from global meteorological reanalysis data. Geophysical Research Letters, 38(17).
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