Put . If minimizes distance, then for every and every real ,
Both signs of arbitrarily small force . In a complex inner product space, apply the same argument to to obtain the imaginary part too. Conversely, if is orthogonal to the subspace, the Pythagorean theorem for inner product spaces gives
Thus orthogonality characterizes the unique best approximation:
Finite dimension also guarantees existence by solving the invertible Gram matrix normal equations; completeness of the ambient inner product space is unnecessary.
Use the convention that the inner product is conjugate-linear in its first argument; the real case is the same without conjugates. Linear independence makes the Gram matrix positive definite, so exists and is Hermitian. Define the Riesz dual basis in an inner product space within by
Then . Its own Gram entries are
Hence the inverse Gram matrix is the Gram matrix of the dual vectors:
The dual vectors are required to lie in ; adding arbitrary vectors orthogonal to that subspace would preserve the displayed biorthogonality but would destroy this conclusion.
Use the standard partition normalization of B-splines, not rescaling each spline to have supremum exactly one. Let . Then . In the ordinary real inner product, the mixed-normalization spline Gram matrix is , where and . Since the form a basis, is positive definite; is invertible, so is invertible. The undeclared upper index in the printed matrix should be .
We need the standard positivity and normalization properties with their justification. The Cox-de Boor recurrence is
with zero-width terms interpreted as zero. It starts from nonnegative interval indicators. On each lower-order spline's support, its recurrence coefficients are nonnegative, so induction gives . Extend the finite knots outside their endpoints to a full knot sequence. In the full sum, coefficients of each lower-order spline add to one, so the recurrence preserves partition of unity. Our finite collection is a subset of nonnegative B-splines; therefore everywhere. The Marsden identity gives equality on the basic knot interval.
The divided-difference definition also gives support in : below the left endpoint the knot-data function is a polynomial of degree , whose order- divided difference vanishes; above the right endpoint the knot data vanish. Choose and . Integrating in and then taking the divided difference in its knot variable gives
because an order- divided difference of a monic degree- polynomial is one. The support lies inside , so .
Orthogonality of to the spline space gives , with . Since and has unit integral, . The induced matrix maximum norm is the absolute row-sum norm, so
Taking the supremum over nonzero proves the maximum-norm bound for spline projection:
The range is , so the printed phrase “onto ” must mean into , and onto . Continuity of the range requires continuous B-splines, for example and internal multiplicities at most . For order-one or discontinuous B-splines, the same bound is valid with codomain rather than .
Fix . If , all knot values of the function agree with a polynomial of degree . Its order- divided difference vanishes. If , all the knot values are zero, so the same divided difference again vanishes. Thus the support is finite:
The support and Gram bandwidth of B-splines also holds at repeated knots: the same conclusion follows with the standard limiting convention. If , then , so the two supports have no positive-length overlap. An endpoint intersection contributes zero to the integral defining . The case is identical. Hence
For strictly increasing knots, B-splines whose indices differ by overlap on a positive-length interval and their product is positive there, so this universal bound is sharp. In standard matrix terminology the half-bandwidth is and the full bandwidth is ; the paper's integer is .

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