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Wavelets, ridgelets, curvelets on the sphere

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Title: Wavelets, ridgelets, curvelets on the sphere


1
Wavelets, ridgelets, curvelets on the sphere and
applications
Y. Moudden, J.-L. Starck P. Abrial Service
dAstrophysique CEA Saclay, France
2
Wavelets, ridgelets, curvelets on the sphere and
applications
Y. Moudden, J.-L. Starck P. Abrial Service
dAstrophysique CEA Saclay, France
  • Outline
  • - Motivations
  • - Isotropic undecimated wavelet transform on the
    sphere
  • - Ridgelets and Curvelets on the sphere
  • - Applications to astrophysical data
    denoising, source separation

3
Introduction - Motivations
  • Numerous applications in astrophysics,
    geophysics, medical imaging, computer graphics,
    etc. where data are given on the sphere e.g.
  • - imaging the Earths surface with POLDER

http//polder.cnes.fr
4
Introduction - Motivations
  • Numerous applications in astrophysics,
    geophysics, medical imaging, computer graphics,
    etc. where data are given on the sphere e.g.
  • - imaging the Earths surface with POLDER
  • - mapping CMB fluctuations with WMAP

http//map.gsfc.nasa.gov
5
Introduction - Motivations
  • Numerous applications in astrophysics,
    geophysics, medical imaging, computer graphics,
    etc. where data are given on the sphere e.g.
  • - imaging the Earths surface with POLDER
  • - mapping CMB fluctuations with WMAP

Need for specific data processing tools, inspired
from successful methods in flat-land wavelets,
ridgelets and curvelets.
6
Wavelet transform on the sphere
  • Related work
  • P. Schroder and W. Sweldens (Orthogonal Haar
    WT), 1995.
  • M. Holschneider, Continuous WT, 1996.
  • W. Freeden and T. Maier, OWT, 1998.
  • J.P. Antoine and P. Vandergheynst, Continuous
    WT, 1999.
  • L. Tenerio, A.H. Jaffe, Haar Spherical CWT,
    (CMB), 1999.
  • L. Cayon, J.L Sanz, E. Martinez-Gonzales,
    Mexican Hat CWT, 2001.
  • J.P. Antoine and L. Demanet, Directional CWT,
    2002.
  • M. Hobson, Directional CWT, 2005.
  • Present implementation
  • isotropic wavelet transform
  • similar to the a trous algorithm, undecimated,
    simple inversion
  • algorithm based on the spherical harmonics
    transform

7
The isotropic undecimatedwavelet transform on
the sphere
  • Spherical harmonics expansion
  • We consider an axisymetric bandlimited scaling
    (low pass) function
  • Spherical correlation theorem

8
The isotropic undecimatedwavelet transform on
the sphere
  • Multiresolution decomposition
  • Can be obtained recursively
  • where
  • Possible scaling function

9
The isotropic undecimatedwavelet transform on
the sphere
  • Wavelet coefficients can be computed as
  • Hence the wavelet function
  • Recursively

10
The isotropic undecimatedwavelet transform on
the sphere
  • Reconstruction is a simple sum
  • Recursively, using conjugate filters
  • where

11
The isotropic undecimatedwavelet transform on
the sphere
12
The isotropic undecimatedwavelet transform on
the sphere
j1
j2
j3
j4
13
Healpix
  • Curvilinear hierarchical partition of the
    sphere.
  • 12 base resolution quadrilateral faces, each
    has nside2 pixels.
  • Equal area quadrilateral pixels of varying
    shape.
  • Pixel centers are regularly spaced on
    isolatitude rings.
  • Software package includes forward and inverse
    spherical harmonic transform.

K.M. Gorski et al., 1999, astro-ph/9812350http//
www.eso.org/science/healpix
14
The isotropic pyramidalwavelet transform on the
sphere
j2
j3
j4
15
Warping
Healpix provides a natural invertible mapping of
the quadrilateral base resolution pixels onto
flat square images.
16
Ridgelets on the sphere
Obtained by applying the euclidean digital
ridgelet transform to the 12 base resolution
faces.
  • Continuous ridgelet transform (Candes, 1998)

17
Ridgelets on the sphere
Obtained by applying the euclidean digital
ridgelet transform to the 12 Healpix base
resolution faces.
  • Continuous ridgelet transform (Candes, 1998)
  • Connection with the Radon transform

18
Ridgelets on the sphere
Obtained by applying the euclidean digital
ridgelet transform to the 12 base resolution
faces.
19
Ridgelets on the sphere
Back-projection of ridgelet coefficients at
different scales and orientations.
20
Digital Curvelet transform
  • local ridgelets
  • with proper scaling

Width Length2
21
Curvelets on the sphere
Obtained by applying the euclidean digital
curvelet transform to the 12 Healpix base
resolution faces.
Algorithm
22
Curvelets on the sphere
23
Denoising full-sky astrophysical maps
  • hard thresholding of spherical wavelet
    coefficients
  • hard thresholding of spherical curvelet
    coefficients
  • combined filtering

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30
Results
Top Details of the original and noisy
synchrotrn maps. Bottom Detail of the map
obtained using the combined filtering technique,
and the residual.
31
Full-sky CMB data analysis
  • CMB is a relic radiation from the early Universe.
  • Full-sky observations from WMAP and
    Planck-Surveyor.
  • The spectrum of its spatial fluctuations is of
    major importance in cosmology.
  • Foregrounds
  • Detector noise
  • Galactic dust
  • Synchrotron
  • Free - Free
  • Thermal SZ

32
A static linear mixture model
33
Foreground removal using ICA
  • Different classes of ICA methods
  • Algorithms based on non-gaussianity i.e.
    higher order statistics.
  • Most mainstream ICA techniques fastICA, Jade,
    Infomax, etc.
  • Techniques based on the diversity (non
    proportionality)
  • of variance (energy) profiles in a given
    representation such as
  • in time, space, Fourier, wavelet joint
    diagonalization of
  • covariance matrices, SMICA, etc.
  • CMB is well modeled by a stationary Gaussian
    random field.
  • Use Spectral matching ICA
  • But, non stationary noise process and Galactic
    emissions. Strongly emitting regions are masked.
  • in a wavelet representation, to preserve scale
    space information.

34
Spectral Matching ICA in wavelet space
  • Apply the undecimated isotropic spherical wavelet
    transform to the multichannel data.
  • For each scale j, compute empirical estimates of
    the covariance matrices of the multichannel
    wavelet coefficients (avoiding for instance
    masked regions)

35
Spectral Matching ICA in wavelet space
  • Apply the undecimated isotropic spherical wavelet
    transform to the multichannel data.
  • For each scale j, compute empirical estimates of
    the covariance matrices of the multichannel
    wavelet coefficients (avoiding for instance
    masked regions)
  • Fit the model covariance matrices to the
    estimated covariance matrices by minimizing the
    covariance mismatch measure

36
Spectral Matching ICA in wavelet space
  • The components may be estimated via Wiener
    filtering in each scale before inverting the
    wavelet transform

37
Experiment
  • Three independent components
  • Galactic region masked
  • Simulated observations in the six channels of
    the Planck HFI
  • Nominal noise standard deviation and 6dB, 3dB
  • Separation using wSMICA and SMICA in six scales
    and corresponding spectral bands.

38
Results
39
Conclusion
  • We have introduced new multiscale decompositions
    on the sphere.
  • Shown their usefulness in denoising and source
    separation.
  • More can be found on http //jstarck.free.fr
  • Software package should be released soon !?
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