The first algebra exists. Let with truncated convolution
The Tonelli theorem gives
Commutativity follows by replacing with ; associativity follows from the Fubini theorem applied to the simplex , . Together with completeness of , this makes a commutative Banach algebra, not necessarily unital. Adjoin an identity using unitization:
This norm is complete and submultiplicative by the preceding bound, and is the identity. This is the Volterra convolution algebra on a finite interval with an identity adjoined.
Take , where . Direct induction under convolution gives
Thus no power vanishes. For every the series
converges absolutely, since its norms have factorial denominators. Multiplication by telescopes to , so it is an inverse. On the other hand cannot be invertible: its scalar coordinate is zero, and scalar coordinates multiply, so can never equal . Hence
This explicitly exhibits a nonnilpotent quasinilpotent element without assuming a spectral-radius formula.
The second algebra does not exist. Suppose it did, and choose a nonscalar . Nonemptiness of its spectrum of an element, together with , gives . But is still nonscalar: if , then . By translation of the spectrum by a scalar,
This contradicts the required zero spectral radius for every nonscalar element. The contradiction already uses the spectral condition alone; the nonvanishing-power condition cannot remedy it.
A complex Banach algebra is an associative complex algebra with a complete norm satisfying submultiplicativity, . A field has a nonzero identity , and every nonzero element is invertible. We derive the Gelfand-Mazur theorem from these facts.
If , the series converges in the complete algebra. Multiplying its partial sums by and passing to the limit proves the Neumann series inverse. In particular, for any and ,
This resolvent of an element tends to zero in norm at infinity; the estimate follows from the geometric bound on .
We next prove that the spectrum of an element cannot be empty. Suppose every were invertible. At each , write
The Neumann series on a small disk about proves that is analytic there. Consequently, for each continuous linear functional , the function is entire. It is bounded outside a large disk by the estimate above and bounded on that disk by continuity. The Liouville theorem makes it constant; its zero limit at infinity makes the constant zero.
Continuous complex linear functionals separate points of . Here is the needed consequence of the Hahn-Banach theorem: for , define on the real span of and extend it as a bounded real linear functional of norm one. Then is complex linear and continuous, and . The real extension theorem is proved explicitly in Question 4(i) below. Thus for every forces , contradicting . This proves the nonemptiness of the Banach-algebra spectrum.
Choose . Since is a field, the noninvertible element must be zero. Hence every is a scalar multiple of . The map
is therefore a bijective unital complex-algebra homomorphism. It and its inverse are bounded, since . Thus it is an isomorphism of Banach algebras. If the usual normalization is included in the definition, it is an isometry; without that normalization, it is still the required continuous algebra isomorphism.
For , write and . Separate continuity and linearity make both maps bounded linear operators. For each fixed ,
The Uniform boundedness principle therefore gives such that whenever . Scaling yields
For completeness, the relevant Uniform boundedness principle follows from the Baire category theorem as follows. For a pointwise bounded family of bounded linear operators on a Banach space, the closed sets cover the space. One contains an open ball . Subtracting the bounds for and , with , gives . Applying this to , , bounds every operator norm by .
Define the new norm by
It is a norm because , so implies . The triangle inequality and scalar homogeneity follow from those of the operator norm. Moreover,
so it is equivalent to the original norm and remains complete. By associativity, , and the submultiplicativity of the operator norm proves
This is renorming a separately continuous Banach algebra. It even gives . If the algebra is the zero space, the conclusion is immediate separately.
Let be the convex hull of all terms of the sequence, meaning the set of their finite convex combinations. Suppose . Part (ii) then gives a continuous linear functional with for every . In particular for every , contradicting . Therefore the ball meets .
A point of that intersection is a finite combination with nonnegative coefficients summing to one. Set , combine repeated indices and insert zero coefficients for omitted indices. This gives
Thus zero lies in the norm closure of the convex hull. The same argument applies to every tail of the sequence and, by choosing errors tending to zero, also gives the usual Mazur lemma. Completeness of is not required for this conclusion.
The hypothesis needed is precisely convergence to zero against every continuous linear functional, namely weak convergence. The PDF says only “continuous” for the testing maps. If that is interpreted as including arbitrary nonlinear continuous maps, the constant map makes the hypothesis impossible. The proof above establishes the substantive conclusion under the intended, weaker linear-testing hypothesis, and therefore also the implication under the literal stronger wording.
Let be the Minkowski functional of :
The contained ball makes absorbing, so is finite, nonnegative and satisfies . It is positively homogeneous. To check subadditivity, if and , the defining property of a convex set gives , whence ; let decrease to the respective infima. Thus is a sublinear functional. We have for every . Also : otherwise for some , which would put in because is a convex set and .
We prove the dominated form of the Hahn-Banach theorem needed here. Suppose is linear on a subspace and there. To extend it to with , choose the value at between
Every lower candidate is at most every upper candidate, because
Taking among the candidates shows the two endpoints are finite: the lower supremum is at least and at most , and the upper infimum lies between them and . Define . For , the upper inequality applied to gives domination by . For , apply the lower inequality to and multiply by . At domination already holds. Hence this is a dominated one-dimensional extension.
Order all dominated extensions by inclusion of their domains. Chain unions preserve linearity and domination, so Zorn's lemma gives a maximal extension. The one-dimensional argument shows its domain is the whole vector space. This proves the requisite dominated Hahn-Banach theorem, rather than invoking an unproved separation form.
On the line , start with . For this equals ; for it is nonpositive and therefore at most . Extend it to on . Then
Applying domination to and also gives
Thus is a continuous linear functional, and
This proves separation from an absorbing convex set with no closedness assumption on . The proof also gives the norm-preserving real extension theorem used earlier: take when the original functional has norm at most .
Take and . The Lp space is strictly convex because is strictly convex: for distinct unit functions its pointwise midpoint inequality is strict on a set of positive measure, hence integration gives norm strictly below one. The finite-dimensional linear subspace has a best approximant: any minimizing sequence is bounded by , and finite-dimensional compactness gives a convergent subsequence whose limit minimizes the continuous error. Uniqueness follows from part 1.
Write that unique minimizer as and its residual as . Translation on the circle preserves the Lp norm. Since , the translated polynomial is another minimizer. Uniqueness forces
Also . Therefore the polynomial has residual , with the same norm as , and is again a minimizer. Hence
To extract the consequence, write the trigonometric polynomial as . The first identity gives . Only in the indicated frequency range is a multiple of , so is constant. The second identity makes this constant its own negative and therefore zero. Thus the lower-frequency Lp approximation to a single harmonic is
For the space already consists only of constants, and the negative-translation argument gives the same result.
Let and write the interpolating spline as . The interpolation equations are , so . Since is defined as a unique interpolant for arbitrary data, its B-spline collocation matrix is invertible. Ordered sites satisfying diagonal positivity ensure this by question 7. Positivity alone without admissible ordering does not: two equal sites in overlapping basis supports could give two identical rows. The norm argument below uses the existence of the operator stipulated here.
Standard partition-normalized B-splines satisfy and . The latter is a subpartition of unity for B-splines: extending the knot sequence gives a full partition of unity, and discarding basis functions cannot increase its sum. Hence
Taking the supremum over and then over unit-norm gives the B-spline interpolation operator norm estimate
Here the matrix norm is the induced maximum-row-sum norm, not the maximum of its individual entries. The proof only needs nonnegative basis functions, their sum at most one, and invertible interpolation.
The centered quadratic spline interpolation matrix is the symmetric tridiagonal Toeplitz matrix
For , this means simply . To evaluate the inverse norm exactly, let and . If is the nonnegative adjacency matrix of the path, then and . The convergent Neumann series
therefore has nonnegative entries. Since , its entrywise absolute values are . Let . Then , or
The homogeneous characteristic roots are . Put . The particular solution and the two boundary conditions give
These row sums are symmetric and increase toward the centre: the exponential sum in the numerator is minimized at the middle integer or pair of integers. With , the exact finite-size inverse norm is thus
For example it equals at and at , tending to as . Stating only the bound two would not evaluate the finite matrix norm requested here.
The general estimate from part 1 and the exact inverse norm from part 2b imply
and in particular , uniformly in the number of knots. This bound concerns the support-centred sites ; shifting the sampling sites changes the B-spline collocation matrix and can destroy uniform stability.