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Reduced-Dimensionality Inverse Scattering Using Basis Functions

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Title: Reduced-Dimensionality Inverse Scattering Using Basis Functions


1
Reduced-Dimensionality Inverse Scattering Using
Basis Functions
  • Andrew E. Yagle
  • Dept. of EECS, The University of Michigan
  • Ann Arbor, MI

2
Presentation Overview
  • Problem Statement
  • Basis Function Representation
  • Matrix Problem Formulation
  • Reformulation as Overdetermined Multiparameter
    Eigenvalue Problem
  • Use of Left Null Matrix
  • 1-D Illustrative Numerical Example

3
Inverse Problem Statement
  • GIVEN 1 monopole point source antenna 1
    frequency, moving platform (e.g., plane)
  • Unknown scatterer V(x) compact support
  • Unknown Greens function G(x,y)
  • Response at x to source at same x u(x)
  • GOAL Reconstruct V(x) from u(x)

4
Inverse Scattering Formulation
G(x,x)
V(x)

5
Inverse Problem Statement
Reciprocity G(x,y)G(y,x) x and y in ?3
Assume Born (single-scatter) approximation
6
Basis Function Representation
Assume Unknown linear combinations of known
basis functions, as follows
7
Basis Function Representation
  • Should not be separable in receiver x and source
    y locations (precludes deconvolution)
  • Dont confuse this with separable in (x,y,z)
  • Need not be orthonormal, complete, or
    biorthogonal to each other
  • Sample observations spatially uku(x-xk)
    special case impulse basis functions

8
Basis Function Representation
  • Selections of all of these basis functions are
    problem-dependent
  • Multilayered media Greens functionsum of
    several terms with unknown reflections
  • Multipole, wavelet, Fourier representations
  • Need (NM) independent observations u(x) either
    samples or coefficient dimensionality

9
Matrix Problem Formulation
Method-of-Moments (MoM) linear system
Insert expansions into integral equation
Where
10
Matrix Problem Formulation
Rewrite as huge (NM)X(NM) linear system
11
Matrix Problem Formulation
In principle Could solve this, and then
BUT Far too large to be practical!
12
Reformulation as Overdetermined Multiparameter
Eigenvalue Problem
Define N matrices Ai, each (NM)XN, as
13
Reformulation as Overdetermined Multiparameter
Eigenvalue Problem
Rewrite Previous (NM)X(NM) system as
14
Reformulation as Overdetermined Multiparameter
Eigenvalue Problem
Rewrite Multiparam eigenvalue problem
15
Reformulation as Overdetermined Multiparameter
Eigenvalue Problem
1. Heavily overdetermined (NMgtgtNM) 2. Actually
(NM) simultaneous polynomial equations in
(NM) unknowns gi and vj 3. But solution not easy
(see below) 4. Make use of (NM) data points as
follows
16
Use of Left Null Matrix
  • Apply recent procedure for multichannel blind
    deconvolution (both 1-D and 2-D)
  • Tall matrices (rowsgtcolumns) have left
    nullspaces basis can be computed
  • null vectorsXmatrix of unknowns0
  • This becomes linear system in unknowns
  • Now adapt this to the present problem

17
Use of Left Null Matrix
  • There is a reclining matrix B so that
  • BA1A2AN0 00
  • Ai is (NM)XM as defined previously
  • A1A2AN is thus (NM)X(N-1)M
  • B is MX(NM) where MNM-(N-1)M
  • B can be PRECOMPUTED from Ai!

18
Use of Left Null Matrix
Premult Huge linear system by known B
BUT MXM linear system, not (NM)X(NM)!
19
Use of Left Null Matrix
  • Instead of the huge (NM)X(NM) linear system, have
    small MXM linear system!
  • Precompute the left null vector B from known
    basis-function-derived A matrix Off-line
    computation do for many bases
  • Solve system directly for vi coefficients Can
    incorporate a priori information
  • Sufficient statistic M-point YBu

20
Use of Left Null Matrix Stochastic Formulation
  • Usually have a priori pdfs for coefficients
  • Compute MAP (Maximum A posteriori Probability)
    estimator instead of the ML (Maximum Likelihood)
    estimator
  • If noise and a priori information pdfs are
    Gaussian, get least-squares solution
  • Otherwise, use iterative algorithm (EM)

21
1-D Illustrative Numerical Example
  • 1-D problem entirely discrete space-time
  • u(i)response at i to impulsive source at i
  • G(i,j)response at i to impulse at j
  • u(i)? G(i,j)V(j)G(j,i)? G2(i,j)V(j)
  • GOAL Reconstruct V(j) from u(i)

22
1-D Illustrative Numerical Example
  • BASIS FUNCTION EXPANSIONS
  • G2(i,j)g1/(i-j)2g2/(ij)2 N2
  • Toeplitz-plus-Hankel structure (not exploited
    here, but not uncommon)
  • Symmetric G(i,j)G(j,i) (reciprocity)
  • V(j)v1?(j-1)v2?(j-2) M2
  • 2-point support for scatterer
  • u(i)? G(i,j)V(j)G(j,i)? G2(i,j)V(j)
  • GOAL Reconstruct V(j) from u(i)

23
1-D Illustrative Numerical Example
  • BASIS FUNCTIONS Greens function
  • ?1(i,,j)1/(i-j)2 ?2(i,j)1/(ij)2
  • ?j(n)?(n-j) (scatterer support 1,2)
  • ??k(n)?(n2-j) (sampled observations)
  • OBSERVATIONS

24
1-D Illustrative Numerical ExampleHuge Linear
System of Equations
25
1-D Illustrative Numerical ExampleHuge Linear
System of Equations
Solving this and arranging into matrix
SOLUTION V(j)3?(j-1)4?(j-2) to an unknowable
scale factor
26
1-D Illustrative Numerical ExampleTiny Linear
System of Equations
27
1-D Illustrative Numerical ExampleTiny Linear
System of Equations
28
1-D Illustrative Numerical ExampleTiny Linear
System of Equations
  • POINT Solving tiny 2X2 linear system
    instead of solving huge 4X4 linear system
  • Sufficient statistic YBu 4-vector to 2-vector
  • Null matrix B precomputed from basis functions
    ahead of time, off-line.

29
Reformulation as Overdetermined Multiparameter
Eigenvalue Problem
Recall This form of large linear system
30
Reformulation as Overdetermined Multiparameter
Eigenvalue Problem

Left-multiply by matrix C where
Cu0 0g1A1gnAnv so that we
have g1A1gnAn is rank-deficient
and Vecg1A1gnAn is linear
combination vecA1vecAnknown basis set.
31
Reformulation as Overdetermined Multiparameter
Eigenvalue Problem
  • g1A1gnAn can be computed
  • iteratively using Lift-and-Project method
  • Project g1A1gnAn rank-deficient
  • using SVD and setting smallest SV to 0
  • 2. Project vecg1A1gnAn onto
  • spanvecA1vecAn

32
Reformulation as Overdetermined Multiparameter
Eigenvalue Problem

Both of these are (Frobenius matrix)
norm-reducing operations. By Composite Mapping
Theorem, this is guaranteed to converge (maybe to
0!) Problem Takes long time to converge.
33
CONCLUSION
  • Solve inverse scattering problem in Born
    approximation with coincident point source and
    receiver on moving platform
  • Using precomputed null vectors, reduce (NM)X(NM)
    system to MXM system Mcoefficients
    representing scatterer Ncoefficients
    representing Greens
  • Sufficient statistic reduce data dimension

34
FUTURE WORK
  • Should need much less data NMltltNM
  • Apply the algorithms we are presently developing
    to solve non-overdetermined multiparameter
    eigenvalue problem
  • Sample data for well-conditioned problem
    adaptively choose the vehicle trajectory
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