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School of Earth and Environment Institute of Geophysics and Tectonics Robust corrections for topographically-correlated atmospheric noise in InSAR data from large deforming regions By David Bekaert Andy Hooper, Tim Wright and Richard Walters

School of Earth and Environment Institute of Geophysics and Tectonics Robust corrections for topographically- correlated atmospheric noise in InSAR data

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School of Earth and Environment

Institute of Geophysics and Tectonics

Robust corrections for topographically-correlated atmospheric noise in InSAR data from large deforming regions

By David Bekaert

Andy Hooper, Tim Wright and Richard Walters

School of Earth and Environment Why a tropospheric correction for InSAR?

Tectonic

Over 9 months

100 km

cm

-10 13.5

To extract smaller deformation signals

School of Earth and Environment

To extract smaller deformation signals

Tropospheric delays can reach up to 15 cm

With the tropospheric delay a superposition of

- Short wavelength turbulent component

- Topography correlated component

- Long wavelength component

Troposphere

1 interferogram

(ti –tj)

Tectonic

Over 9 months

100 km

cm

-10 13.5

Why a tropospheric correction for InSAR?

School of Earth and Environment

Auxiliary information (e.g.): Limitations

• GPS

• Weather models

• Spectrometer data

Station distribution

Accuracy and resolution

Cloud cover and temporal sampling

Tropospheric corrections for an interferogram

School of Earth and Environment

Auxiliary information (e.g.): Limitations

• GPS

• Weather models

• Spectrometer data

Interferometric phase

• Linear estimation (non-deforming region or band filtering)

Station distribution

Accuracy and resolution

Cloud cover and temporal sampling

Assumes a laterally uniform troposphere

isolines

Δφtropo =Kuniform ⋅ h +Const

Tropospheric corrections for an interferogram

School of Earth and Environment

A linear correction can work in small regions Interferogram

Tropo

GPS

InSAR and GPS data property of IGN

Linear est

isolines

Δφtropo =Kuniform ⋅ h +Const

A laterally uniform troposphere

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However

• Spatial variation of troposphere

est: Spectrometer & Linear

isolines

+ +

- +

A linear correction can work in small regions

Δφtropo =Kuniform ⋅ h +Const

A spatially varying troposphere

Topography

School of Earth and Environment

Allowing for spatial variation

Interferogram (Δɸ)Why not estimate a linear function locally?

Δφtropo =Kuniform ⋅ h +Const

-9.75 rad 9.97A spatially varying troposphere

School of Earth and Environment

Δφtropo =Kuniform ⋅ h +Const

-9.75 rad 9.97A spatially varying troposphere

Why not estimate a linear function locally?

Does not work as:

Const is also spatially-varying and

cannot be estimated from original phase!

Interferogram (Δɸ)

School of Earth and Environment

Δφtropo =Kspatial ⋅ h0 − h( )α

Δφtropo =Kuniform ⋅ h +Const

-9.75 rad 9.97

We propose a power-law relationship

that can be estimated locally

A spatially varying troposphere

Why not estimate a linear function locally?

Does not work as:

Const is also spatially-varying and

cannot be estimated from original phase!

Interferogram (Δɸ)

School of Earth and Environment

Δφtropo =Kspatial ⋅ h0 − h( )α

With h0 the lowest height at which the relative

tropospheric delays ~0

• 7-14 km from balloon sounding

Sounding data provided by the University of Wyoming

Allowing for spatial variation

School of Earth and Environment

Allowing for spatial variation

Δφtropo =Kspatial ⋅ h0 − h( )α

With h0 the lowest height at which the relative

tropospheric delays ~0

• 7-14 km from balloon sounding

With α a power-law describing the decay of

the tropospheric delay

• 1.3-2 from balloon sounding data

Allowing for spatial variation

Sounding data provided by the University of Wyoming

School of Earth and Environment Power-law example

Δφ =Kspatial ⋅ h0 − h( )α+ Δφdefo + ...

-9.75 rad 9.97

Interferogram (Δɸ)

School of Earth and Environment Power-law example

-9.75 rad 9.97

Δφband≈ Kspatial ⋅ h0 − h( )

α

band

Band filtered: phase (Δɸband) & topography (h0-h)αband

(Y. Lin et al., 2010, G3) for a linear approach

Interferogram (Δɸ)

School of Earth and Environment Power-law example

Δφband≈ Kspatial ⋅ h0 − h( )

α

band

Band filtered: phase (Δɸband) & topography (h0-h)αband

(Y. Lin et al., 2010, G3) for a linear approach

School of Earth and Environment Power-law example

Band filtered: phase (Δɸband) & topography (h0-h)αband €

Δφband≈ Kspatial ⋅ h0 − h( )

α

band

For each window:estimate Kspatial

(Y. Lin et al., 2010, G3) for a linear approach

Anti-correlated!

School of Earth and Environment Power-law example

Δφband≈ Kspatial ⋅ h0 − h( )

α

band

Band filtered: phase (Δɸband) & topography (h0-h)αband

For each window:estimate Kspatial

(Y. Lin et al., 2010, G3) for a linear approach

Anti-correlated!

School of Earth and Environment

Original phase (Δɸ)

Power-law example

Band filtered: phase (Δɸband) & topography (h0-h)αband Tropo variability (Kspatial) €

Δφband≈ Kspatial ⋅ h0 − h( )

α

band

rad/mα -1.1e-6 9.8e-5

School of Earth and Environment

Original phase (Δɸ)

Power-law example

Band filtered: phase (Δɸband) & topography (h-h0)αband Tropo variability (Kspatial) €

Δφtropo =Kspatial ⋅ h0 − h( )α

Topography (h0-h)α

-1.1e-6 9.8e-5rad/mα

-9.75 rad 9.97

Power-law est (Δɸtropo)

4.7e4 2.4e51/mα

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Allowing for spatial variation-9.75 rad 9.97 -9.75 rad 9.97 -9.75 rad 9.97

Original phase (Δɸ) Power-law est (Δɸtropo) Spectrometer est (Δɸtropo)

Power-law example

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Regions:

• El Hierro (Canary Island)

- GPS

- Weather model

- Uniform correction

- Non-uniform correction

• Guerrero (Mexico)

- MERIS spectrometer

- Weather model

- Uniform correction

- Non-uniform correction

Case study regions

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-11.2 rad 10.7

Interferograms(original)

El Hierro

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WRF(weather model)

El Hierro

-11.2 rad 10.7

Interferograms(original)

School of Earth and Environment

WRF(weather model)

El Hierro

-11.2 rad 10.7

Interferograms(original)

School of Earth and Environment

WRF(weather model)

Linear(uniform)

El Hierro

-11.2 rad 10.7

Interferograms(original)

School of Earth and Environment

WRF (weather model)

Linear(uniform)

Power-law(spatial var)

El Hierro

-11.2 rad 10.7

Interferograms(original)

School of Earth and Environment El Hierro quantification

ERA-I run at 75 km resolution WRF run at 3 km resolution

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MERIS MERIS

Mexico-9.75 rad 9.97

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MERIS MERIS

Clouds

Mexico-9.75 rad 9.97

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MERIS ERA-I MERIS ERA-I

Mexico-9.75 rad 9.97(Weather model)

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MERIS ERA-I MERIS ERA-I

Misfit near coast

Mexico-9.75 rad 9.97(Weather model)

School of Earth and Environment

MERIS ERA-I Linear MERIS ERA-I Linear

Mexico-9.75 rad 9.97(Weather model)

School of Earth and Environment

MERIS ERA-I Linear MERIS ERA-I Linear

Mexico-9.75 rad 9.97(Weather model)

School of Earth and Environment

MERIS ERA-I Linear Power-law MERIS ERA-I Linear Power-law

Mexico-9.75 rad 9.97(Weather model)

School of Earth and Environment

MERIS ERA-I Linear Power-law MERIS ERA-I Linear Power-law

Mexico-9.75 rad 9.97(Weather model)

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MERIS ERA-I

Linear Power-law

Mexico techniques compared: profile AA’

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MERIS accuracy

(Z. Li et al., 2006)

Mexico quantification

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• Fixing a reference at the ‘relative’ top of the troposphere allows us to deal with spatially-varying tropospheric delays.

• Band filtering can be used to separate tectonic and tropospheric components of the delay in a single interferogram

• A simple power-law relationship does a reasonable job of modelling the topographically-correlated part of the tropospheric delay.

• Results compare well with weather models, GPS and spectrometer correction methods.

• Unlike a linear correction, it is capable of capturing long-wavelength spatial variation of the troposphere.

Summary/Conclusions

Toolbox with presented techniques will be made available to the community