Summary
- 6 July
- §1.1 - §1.2
- Definition of Fourier Transform (L1 version)
- Motivated the inversion formula; stated these theorems:
- Jordan's theorem
- Pringsheim's theorem
- Algebraic properties of the FT
- linearity
- symmetry (even and odd functions)
- conjugacy (FT of complex conjugate of f)
- dilations; notation: Dag(t)=ga(t):=a g(a t)
- translation in time: tuf(t)
:= f(t-u)
- modulation (translation in frequency): twF(g)= F(g - w)
Time domain modualtion of f: e2ipwtf(t)
- Modulation example; band-limited functions
- HW -- 1.8(b,c)
- 7 July
- §1.3, 1.4.1, 1.5, 1.6.3
- Important functions
- sinc(x)=sin(px)/(px) or Dirichlet function d(x)=sin(x)/(px);
FT[1[-T,T]](g)=d2pT(g)
- Poisson function, Fejér function
- Gaussian, g(t)=exp(-t2)/p½
FT[ g ](g)=exp(-(pg)2)
- Analytic properties of the FT
- If f is L1, then F is uniformly continuous and vanishes
at infinity.
- FT[ f (m) ](g) = (2pig)m
F(g)
- FT[ (-2pit)m f(t) ](g) = F(m)(g)
- Convolution theorem: FT[ f*g ](g) =
F(g) G(g)
- Integral of sin(x)/x, all x, is p
- HW -- 1.19(a) and 1.31
- 8 July
- §1.7, 1.8.1
- Inversion formula for FT
- Dini conditions on f at t
- Expressions for "partial sums"
- Proof of result
- Solving a PDE (heat flow with a convective term) via FT
techniques
- HW -- 1.23(a) and 1.27
- 9 July
- §1.10
- Definition of FT on L2 (space of finite energy signals)
- If f is in both L1 and L2, then || F
||L2=|| f ||L2
- Parseval/Plancheral Theorem: If f and g are in L2, then
- || F ||L2=|| f ||L2
- < f,g > = < F,G > (Usual inner product.)
- HW -- 1.26 and 1.35
- 12 July
- §2.1-2.2 & §2.4
- Dirac's delta function
- Delta sequences (approximate identities)
- Distributions
- D, the space of infinitely differentiable, compactly
supported functions; convergence in this space
- D', the dual to D, comprising all
continuous linear functionals on D; these are the
distributions
- Examples: delta functions; locally integrable functions
- Elementary properties of distributions
- Linearity and continuity (definition)
- Equality of distributions
- Support of a distribution
- Sum of distributions
- Positive distributions
- Schwartz space, S
- Infinitely differentiable functions with ``fast'' decay
- Seminorms or metric generate topology
- HW -- 2.5(a) and 2.6
- 13 July
- §2.4, §2.7.8-2.7.10
- The Fourier transform of S is S.
- Tempered distributions
- S', continuous linear functionals on S
- Fourier transform of a distribution FT[T](f) := T(FT[f])
- Derivatives of distributions: T'(f) := - T(f')
- Translation of distributions: (tuT)(f) := T(t-uf)
- Examples involving Dirac delta functions
- Positive definite functions & Bochner's theorem
- Let f: R --> C be continuous. We say that f is
positive definite if, for every set of distinct points
{x1,...,xn} in R, the n×n matrix A
with entries Aj,k = f(xj - xk) is
positive semidefinite.
- Bochner's Theorem: f is positive definite if and only if f is the
FT (distribution sense) of a nonnegative measure m.
- HW -- 2.30, 2.34, 2.35
- 14 July
- Multidimensional Fourier transform (§7.5, G. Folland,
Fourier Analysis and Its Applications, Wadsworth &
Brooks/Cole, Belmont, CA, 1992)
- Definition
- Convolution and Inversion theorems
- Multidimensional Schwartz space
- FT of Gaussians in several dimensions
- Properties--same as for one dimensional case, except that we have
rotational invariance
- Radial functions
- Fourier series, §3.1
- Definition for a 2W periodic L1 function F(g)
- Fourier coefficients are regarded as a time series and F the
frequency representaion of the time series
- Partial sums SN(g)
- HW -- 3.1(a), 3.7; problem on linear change of variables in FT
- 15 July
- §3.3-3.4
- Showed DN(t)=sin((N+½)t)/sin(½t)
- Dini conditions for convergence of FS; proved using FT version of
results together with Dirichlet kernel
- Operations with Fourier series
- Addition and scalar multiplication
- Integration
- Differentiation
- Convolution theorem
- Fejér Kernel WN defined as the Cesáro
mean of DN
- HW -- 3.11(b)
- 16 July
- §3.4
- Properties of Fejér's kernel WN
- F*WN --> F (F continuous or L1)
- Approximate identity (delta sequence)
- Definition
- WN is an example
- Get same convergence results as for WN
- Uniqueness theorem for fourier coefficients of F in L1
- Weierstrass approximation theorem
- L2 results
- {exp(-inpg/W)} is an orthonormal
basis for square integrable 2W periodic
functions
- Parseval's formula
- Riesz-Fischer theorem
- HW -- 3.16
- 19 July
- §3.5 and Notes
- Wiener's Inversion Theorem
- A(T) is all 2W periodic
functions that are Fourier series for l 1
time series.
- Discrete convolution theorem
- Inversion theorem: If F is in A(T) and if F
never vanishes, then 1/F is also in A(T).
- Sampling Theorem
- Statement and proof in notes
- Band-limited functions
- Nyquist frequency
- Aliasing
- HW
- Show that the set {sinc(t - n)}n
e Z is orthogonal in L2(R).
- What is the L2(R) span of this set?
- 20 July
- §3.8 and notes on the DFT
- HW
- Prove that if f and g are in L(ZN), then so it
f*g.
- Prove that DFT[f*g] = DFT[f]DFT[g]
- Define the shift operator via tjf[n]=f[n-j]. Find the DFT of tjf in terms of the DFT of f.
-
- 21 July
- Midterm test
- 22 July
- §3.10 and class notes
- The Poisson summation formula
- FT of the Dirac Comb
- Application to Gaussians
- The discrete cosine transform (DCT)
- 23 July
- Inverting the DCT
- DCT and DFT
- DFT and the FT
- HW
- Show that if the kth entry of a row vector
Rn is given by Rn[k] = cos(np(k+½)/N), then
RnRmT is N if m=n=0, N/2, if
n=m>0, and 0 if m is not equal to n.
- Write out the connection between the DFT and DCT for N=4.
- 26 July
- §2.6.5-6 & class notes
- Translation invariant systems
- Subspace X of distributions invariant under translations
- Operator L taking X to X, with these properties:
- L is linear
- L is translation invariant: taL = Lta
- The operator L above is called a filter
- Structure of filters
- Eigenfunctions L[e2ipgt] = H(g) e2ipgt (g fixed, real)
- FT(L[f]) = H(g) F(g) (H is the transfer function)
- L[f]=h*f (h is the impulse response (IR))
- Causal filters
- "No output before input."
- Definition: L is causal if and only if f(t)=0 for all t < a
implies L[f] = 0 for all t < a.
- L is causal iff h(t) = 0 for all t < 0. (Showed the condition on h
was sufficient.)
- h(t) = 0 for all t < 0 iff H(g) is
the Laplace transform of h evaluated at s = 2ipg
- Ideal low-pass filter is not causal
- Discrete filters - act on two-sided sequences, the functions on
Z
- HW
- Suppose that X is the space L1. Show that if h
is in L1, then L[f] = h*f is a stable filter; i.e.,
||L[f]|| < (constant)× ||f||.
- Show that the condition h(t) = 0 for all t < 0 is necessary
for L to be causal.
- Show that if K and L are filters with IR functions g and h,
respectively, then KL is a filter with IR g*h. (Take everything in
L1). If L is causal, what conditions on g make KL causal?
- 27 July
- Surface fitting - class notes
- Problems come from geodesy, geophysics, graphics, map-making,
meteorology, neural nets, and other areas.
- Common features. The data sites are in Rn,
where n may be 2, 3, or higher; one neural net application requires
n=64. Sites where data are taken are scattered, possibly sparse. The
function that fits the data should not "ripple" too much.
- For the one dimensional case, cubic splines provide an example of
the type of solution that we want.
- Background
- Roland Hardy empirically discovered the Hardy multiquadric
approach, which uses interpolants that are linear combinations of
m(x-xj) =
(1+|x-xj|2)1/2
- Jean Duchon took a variational approach similar to that used for
splines, and got different interpolants. For the two dimensional
case, he minimized the integral of the square of Du, subject to constraints. He obtained
interpolants that are linear combinations of
s(x-xj) =
|x-xj| 2
log(|x-xj|2)
- Franke's conjecture. Richard Franke did a comparative sutdy of
scattered data interpolation methods. The winners? Hardy's
multiquadric method and Duchon's thin plate spline approach. Franke
conjectured the invertibility of the interpolation matrix for the
multiquadric.
- Madych/Nelson and Micchelli both proved the conjecture true. The
Madych/Nelson approach was variational -- similar to
Duchon's. Micchelli worked with "Laplace transforms" related to
Gaussians.
- HW
Let x1=0, x2=1, x3=2. For
each F below, find the eigenvalues for the interpolation matrix
Aj,k = F(|xj - xk|2 )
- F(r2)= exp(-r2) (Gaussian)
- F(r2)= (1+r2)1/2 (multiquadric)
- F(r2)= r2log( r2) (thin plate spline)
- References
- J. Duchon, Interpolation des Fonctions de Deux Variables Suivant
le Principe de la Flexion des Plaques Minces, Rairo Analyse
Numerique 10 (1976), 5-12.
- J. Duchon, Splines minimizing rotation invariant semi-norms in
Sobolev spaces, pp. 85-100 in Constructive Theory of Functions
of Several Variables, Oberwolfach 1976, W. Schempp and
K. Zeller, eds., Springer-Verlag, Berlin, 1977.
- R.L. Hardy, Multiquadric equations of topography and other
irregular surfaces, J. Geophys. Res. 76 (1971),
1905-1915.
- R.L. Hardy, Theory and Applications of the
Multiquadric-Biharmonic Method, Comput. Math. Appl.
19 (1990), 163-208.
- W.R. Madych and S.A. Nelson, Multivariate interpolation: a
variational theory, manuscript, 1983.
- W.R. Madych and S.A. Nelson, Multivariate interpolation and
conditionally positive definite functions, Approx. Theory and its
Applications 4 (1988), 77-79.
- C.A. Micchelli, Interpolation of scattered data: distances,
matrices, and conditionally positive definite functions, Const.
Approx. 2 (1986), 11-22.
- 28 July
- Radial basis functions & surface fitting
- Polynomial reproducing methods.
- Let X = {x1, ..., xN} be a
subset of Rn and let p and q be any polynomials of
degree m -1 or less. X is unisolvent if
p(xj) = q(xj) implies that p=q;
i.e., the two polynomials are identical.
- An interpolation method is polynomially reproducing if
it reproduces a polynomial p of degree m-1 or less from data
yj = p(xj) whenever X is unisolvent
- Conditionally positive definite functions of order m.
- Let P be a matrix whose jth row is a monomial of
degree m -1 or less evaluated at xj. The monomials
used should span all polynomials of degree m-1 or less and X should be
unisolvent.
- A continuous function h is said to be conditionlly positive
definite of order m if for every n×1 column vector c in the null
space of P we have c+Ac >= 0, with A=[h(
xk - xj )].
- h is strictly conditionally positive definite if for c
in the null space of P the equation c+Ac = 0 implies that
c=0.
- If h is conditonally positive definite of order m and if the
support of the distributional FT of h includes an open set in
Rn, then h is strictly CPD of order m.
- Interpolation using translates - two types
- No polynomial reproduction. Let h be a continuous strictly
positive definite function. Use linear combinations of h( x -
xj ).
- Degree m-1 polynomial reproduction is required. Let h be a
continuous strictly CPD function of order m. Use linear combinations
of h( x - xj ), together with all monomials
of degree m-1 or less.
- HW
- Show that X is unisolvent if and only if the rank of P mentioned
above is the dimension of the space of polynomials of degree m-1 or
less. Use this to show that if X contains a unisolvent subset, then X
is also unisolvent.
- Suppose that {x1, ..., xN} are distinct
real numbers. Show that if
c1exp(-2ipgx1) + ... + cNexp(-2ipgxN) = 0
holds for all g in R, then
cj = 0 for j = 1 ... N. (Note: the xj's are not
necessarily integers, so the exponentials are not orthogonal, in
general.)
-
- 29 July
- Radial basis functions & surface fitting (continued)
- Order 1 SCPD functions
- Reproducing the constants
-
Ydata=Ac+PTb, cTPT=0, where
PT = column of ones and b=scalar
- Hardy multiquadric is an example of an order 1 SCPD function
- Order m SCPD functions
- Reproducing the polynomials of degree less than or equal to m-1
- Let P be a matrix whose jth row is a monomial of
degree m -1 or less evaluated at xj, and let the
data sites be a unisolvent set.
- Equations: Ydata=Ac+PTb, P*c=0
- The thin plate spline is an example of an order 2 SCPD function
- HW
- Let P be the matrix described above, X a unisolvent set, and h is
an order m SCPD function. Show that the interpolant
f(x) = c1h( x - xj )+ ... +
cNh( x - xN ) + pm -
1(x),
where p is a polynomial of degree m - 1 or less, reproduces
polynomials if the equations below hold
Ydata=Ac+PTb, P*c=0
-
- 30 July
- Radial basis functions & surface fitting (continued)
- Order m radial CPDF
- CPD functions of order m in all dimensions
- Connection with completely monotonic functions
- Berstein-Widder theorem (completely monotonic functions)
- Schoenberg's theorem (order 0)
- Micchelli (order 1)
- Guo, Hu, & Sun (order m)
- Associated quadratic forms and SCPD order m radial functions
- HW
- Find the dimension of the space of polynomials of degree k in n variables.
- Show that the matrix below is invertible whenever h is order m
SCPD and the data sites are a unisolvent for the polynomials of degree
m in n variables.
-
-
- 2 August
- MATLAB demonstration of surface fitting with the Hardy multiquadrics
- Basics for S2
- Spherical coordinates
- Metric tensor
- Invariant volume element
- Geodesics (great circles)
- Laplace-Beltrami operator
- Connection with Laplacian on R3
- Fourier analysis on S2
- Homogeneous harmonic polynomials on R3
- Eigenfunctions of the Laplace-Beltrami operator, DS
- HW
- Let DS be the
Laplace-Beltrami operator on the 2-sphere. For the usual inner product
on S2, show that <DS f, g> = < f, DS g>
- Suppose DS Y + l Y = 0. Show that l =
- || Yq ||2 / || Y
||2
-
- 3 August
- Construction of the spherical harmonics
- Eigenvalues, eigenfunctions of the Laplace-Beltrami operator
- Ladder operators, L+ and L-
- Properties of the spherical harmonics
- Relation to harmonic polynomials on R3
- Orthonormal basis for L2
- HW
- Show that L+ DS = DS L+.
- Show that the eigenfunctions of DS (the spherical
harmonics)corresponding to the eigenvalue l(l+1) have the
form
sin|m|(q) ×
p(cos(q)) ×
exp(imj),
where p is a polynomial of degree l - |m|.
- Find all spherical harmonics of order 3.
-
- 4 August
- Rotations in R3
- Orthogonal matrices, O(3)
- Determinant one orthogonal matrices, SO(3)
- The space of harmonic polynpmials homogeneous of degree
l in R3 is invariant under rotations.
- Spherical harmonics of order l form a space invariant
under rotations
- The Addition Theorem
- Positive definite kernels and functions on S2
- HW
- Let t = x.y. Show that the sum
(1/4p)(P0(t) +
3P1(t) + ... + (2L+1)PL(t))
is a reproducing kernel on the space of spherical harmonics having
order L or less.
- Show that Pl(x.y) is positive
definite on S2. (Hint: Use the Addition Theorem.)
-
- 5 August
- Postive definite functions on spheres
- Schoenberg's theorem for S2
- Legendre expansions with nonnegative coefficients
- Strictly positive definite functions and Legendre series with
positive coefficients
- Schoenberg-Bingham Theorem
- Schur products of matrices
- (x.y)k is positive difinite on all spheres
- Functions strictly postive definite on all spheres
- Example: exp(x.y) is SPD on all spheres
- Interpolation with SPD functions and kernels
- Series for the gravitational potential exterior to a sphere
- HW
- Show that 1 is the maximum value of |Pl(t)|
on [-1,1]. (Hint: Let t = x . y; use the Addition Theorem.)
- Show that the Schur product of two positive sem-definite matrices
is also positive semi-definite.