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A multivariate function form quite different from the tensor-product construct is the scattered translates form, or stform for short. As the name suggests, it
uses arbitrary or scattered translates ψ(·
–*c*_{j}) of one fixed
function ψ, in addition to some polynomial terms. Explicitly, such a form describes a
function

$$f\left(x\right)={\displaystyle \sum _{j=1}^{n-k}\psi \left(x-{c}_{j}\right){a}_{j}+p\left(x\right)}$$

in terms of the *basis function* ψ, a sequence
(*c*_{j}) of sites called *centers* and a corresponding sequence
(*a*_{j}) of
*n* coefficients, with the final *k* coefficients,
*a*_{n-k+1},...,*a*_{n},
involved in the *polynomial part*, *p*.

When the basis function is radially symmetric, meaning that ψ(*x*)
depends only on the Euclidean length |*x*| of its argument,
*x*, then ψ is called a *radial basis function*, and, correspondingly,
*f* is then often called an RBF.

At present, the toolbox works with just one kind of stform, namely a bivariate
thin-plate spline and its first partial derivatives. For the thin-plate spline, the
basis function is ψ(*x*) =
φ(|*x*|^{2}), with φ(*t*) =
*t*log*t*, i.e., a radial basis function. Its
polynomial part is a linear polynomial, i.e., *p*(*x*)=*x*(1)*a*_{n
–
2}+*x*(2)*a*_{n
–
1}+*a*_{n}. The first partial derivative with respect to its first argument uses,
correspondingly, the basis function ψ(*x*)=φ(|*x*|^{2}), with φ(*t*) =
(*D*_{1}t)·(log*t*+1) and *D*_{1}*t *=
*D*_{1}*t*(*x*)
= 2*x*(1), and *p*(*x*) =
*a*_{n}.

A function in stform can be put together from its center sequence `centers`

and
its coefficient sequence `coefs`

by the command

f = stmak(centers, coefs, type);

with the string `type`

one of `'tp00'`

, `'tp10'`

, `'tp01'`

,
to indicate, respectively, a thin-plate spline, a first partial of
a thin-plate spline with respect to the first argument, and a first
partial of a thin-plate spline with respect to the second argument.
There is one other choice, `'tp'`

; it denotes a thin-plate
spline without any polynomial part and is likely to be used only during
the construction of a thin-plate spline, as in `tpaps`

.

A function *f* in stform depends linearly on
its coefficients, meaning that

$$f\left(x\right)={\displaystyle \sum _{j=1}^{n}{\psi}_{j}\left(x\right){a}_{j}}$$

with ψ_{j} either a translate of the
basis function Ψ or else some polynomial. Suppose you wanted
to determine these coefficients *a*_{j} so
that the function *f* matches prescribed values at
prescribed sites *x*_{i}.
Then you would need the collocation matrix (ψ_{j}(x_{i})).
You can obtain this matrix by the command `stcol`

`(centers,x,type)`

.
In fact, because the stform has *a*_{j} as
the *j*th *column*, `coefs(:,j)`

,
of its coefficient array, it is worth noting that `stcol`

can also supply the *transpose* of
the collocation matrix. Thus, the command

values = coefs*stcol(centers,x,type,'tr');

would provide the values at the entries of `x`

of
the st function specified by `centers`

and `type`

.

The stform is attractive because, in contrast to piecewise polynomial forms, its complexity is the same in any number of variables. It is quite simple, yet, because of the complete freedom in the choice of centers, very flexible and adaptable.

On the negative side, the most attractive choices for a radial
basis function share with the thin-plate spline that the evaluation
at any site involves all coefficients. For example, plotting a scalar-valued
thin-plate spline via `fnplt`

involves
evaluation at a 51-by-51 grid of sites, a nontrivial task when there
are 1000 coefficients or more. The situation is worse when you want
to determine these 1000 coefficients so as to obtain the stform of
a function that matches function values at 1000 data sites, as this
calls for solving a full linear system of order 1000, a task requiring
O(10^9) flops if done by a direct method. Just the construction of
the collocation matrix for this linear system (by `stcol`

)
takes O(10^6) flops.

The command `tpaps`

, which
constructs thin-plate spline interpolants and approximants, uses iterative
methods when there are more than 728 data points, but convergence
of such iteration may be slow.

After you have constructed an approximating or interpolating
thin-plate spline `st`

with the aid of `tpaps`

(or directly via `stmak`

), you can use the following commands:

`fnbrk`

to obtain its parts or change its basic interval,`fnval`

to evaluate it`fnplt`

to plot it`fnder`

to construct its two first partial derivatives, but no higher order derivatives as they become infinite at the centers.This is just one indication that the stform is quite different in nature from the other forms in this toolbox, hence other

`fn...`

commands by and large don't work with stforms. For example, it makes no sense to use`fnjmp`

, and`fnmin`

or`fnzeros`

only work for univariate functions. It also makes no sense to use`fnint`

on a function in stform because such functions cannot be integrated in closed form.The command

`Ast =`

`fncmb`

`(st,A)`

can be used on`st`

, provided`A`

is something that can be applied to the values of the function described by`st`

. For example,`A`

might be`'sin'`

, in which case`Ast`

is the stform of the function whose coefficients are the sine of the coefficients of`st`

. In effect,`Ast`

describes the function obtained by composing`A`

with`st`

. But, because of the singularities in the higher-order derivatives of a thin-plate spline, there seems little point to make`fndir`

or`fntlr`

applicable to such a`st`

.