The ordinary interpolation formulation is unambiguous for strictly increasing knots; repeated knots require specified confluent interpolation or a limiting convention. First take distinct knots and , and for fixed write . The two degree-at-most- Lagrange interpolation polynomials and agree at the shared knots . Their difference is therefore
This remains valid if their difference has lower degree: the coefficient is then zero. The leading coefficient of a degree-at-most- interpolant is its order- divided difference. Comparing leading coefficients and using the divided-difference recursion gives
Consequently the Lee interpolation identity holds for every real :
No differentiability of the truncated power in its argument was needed for this distinct-node proof.
Sum the identity over . The right side telescopes, giving . When , all the nodes for lie below , so its interpolation data are zero and . All the nodes for lie above , where is already a polynomial of the admissible degree. Uniqueness of polynomial interpolation gives . Therefore the Marsden identity is
For order one the empty product is one, the interpolants are constants and a consistent half-open interval convention for gives the same telescoping proof. Nondecreasing repeated-knot sequences can be treated by the appropriate confluent or limiting convention wherever that definition is valid; merely specifying repeated data values does not uniquely determine the interpolation polynomials. The basic open knot interval in the Marsden identity avoids endpoint convention ambiguity.
For fixed , put , a truncated power function. Begin with distinct increasing knots. The two interpolation polynomials and agree at their shared knots. Their difference has degree at most , so
For the empty product is one and the same assertion holds for constant interpolants. The leading coefficient of a degree-at-most- interpolant on nodes is its order- divided difference, by the Newton interpolation polynomial. Therefore
This proves the Lee interpolation identity
The identity holds for every real , with the usual convention for the order-zero truncated power. Admissible repeated knots are handled by the corresponding confluent divided differences and consistent one-sided limits at breakpoints; taking these limits preserves the Lee interpolation identity.
Sum over to telescope:
If , the first knot values of are zero, so . At the last knots , the function agrees with the polynomial , so uniqueness of polynomial interpolation gives . Thus the Marsden identity is
Write . Begin with distinct increasing knots so ordinary polynomial interpolation is unambiguous. The two interpolants agree at the common knots . Their difference is consequently a scalar multiple of the monic polynomial of degree .
The leading coefficient of an interpolant is its highest divided difference. Thus this scalar is
The equality is precisely the divided-difference recurrence. This proves the Lee interpolation identity:
For the common-knot product is empty; the same argument is a difference of constants. Interpret as to obtain the usual half-open order-one B-splines. Repeated knots use the standard confluent or limiting interpretation, where the interpolation data are defined.
Sum over . The right side telescopes to . When , the first interpolation nodes all lie below , so . The last interpolation nodes all lie above , so interpolates the polynomial of degree and equals it identically. Hence the Marsden identity follows: