B-splines of the order 0 and 1 coincide with the nearest neighbor and linear interpolants (2) and (3) respectively. B-splines of a higher order n can be defined by a repetitive convolution of the zeroth-order spline (the box function) with itself:
Both the support length and the smoothness of B-splines increase with the order. In the limit, B-slines converge to the Gaussian function. Figures and show the third- and seventh-order splines and and their continuous spectra.
It is important to realize the difference between B-splines and the corresponding interpolants W(x,n), which are sometimes called cardinal splines . An explicit computation of the cardinal splines is impractical, because they have infinitely long support. Typically, they are constructed implicitly by the two-step interpolation method, outlined in the previous subsection. The cardinal splines of orders 3 and 7 and their spectra are shown in Figures and . As B-splines converge to the Gaussian function, the corresponding interpolants rapidly converge to the sinc function (4). A good convergence is achieved with the help of the infinitely long support, which results from recursive filtering at the first step of the interpolation procedure.
In practice, the recursive filtering step adds only marginally to the total interpolation cost. Therefore, an n-th order B-spline interpolation is comparable in cost with any other method with an (n+1)-point interpolant. The comparison in accuracy usually turns out in favor of B-splines. Figures and compare interpolation errors of B-splines and other similar-cost methods on the example from Figure .
Figure 15 Interpolation error of the cubic convolution interpolant (dashed line) compared to that of the third-order B-spline (solid line).
Figure 16 Interpolation error of the 8-point windowed sinc interpolant (dashed line) compared to that of the seventh-order B-spline (solid line).
Similarly to Figures and , we can also compare the discrete responses of B-spline interpolation with those of other methods. The right plots in Figures and show that the discrete spectra of the effective B-spline interpolants are genuinely flat at low frequencies and wider than those of the competitive methods. Although the B-spline responses are infinitely long because of the recursive filtering step, they exhibit a fast amplitude decay.
Figure 17 Discrete interpolation responses of cubic convolution and third-order B-spline interpolants (left) and their discrete spectra (right) for x=0.7.
Figure 18 Discrete interpolation responses of 8-point windowed sinc and seventh-order B-spline interpolants (left) and their discrete spectra (right) for x=0.7.