In a unital Banach algebra, the Neumann series gives whenever : the series converges in norm by submultiplicativity and completeness, and multiplication of its partial sums on either side gives . Consequently, if is invertible and , write
The second factor has a Neumann series inverse, so is invertible. This exhibits a ball around each in the group of invertible elements of a Banach algebra, proving that group is an open set.
The same series proves continuity of inversion in a Banach algebra, with the useful quantitative estimate
The right side tends to zero as . Since applying inversion twice gives the original element, it is a bijection whose inverse is the same continuous map. Thus inversion is a homeomorphism of the open group of invertibles onto itself.
For the final unheaded request, define
It is open by the preceding argument and contains . If were a boundary point, a sequence would converge to , while openness gives . Then is a noninvertible limit of invertibles. The one-sided-inverse argument in part (ii) shows that this limit has neither a left inverse of an algebra element nor a right inverse of an algebra element, contradicting the hypothesis. Therefore has empty boundary; it is both open and closed in the connected complex plane, and .
For every nonzero , put . The identity proves invertibility, so the spectrum of an element is contained in . It is nonempty: if the resolvent of an element existed for all , it would be an entire algebra-valued function tending to zero at infinity by the Neumann series. Applying any bounded linear functional and then the Liouville theorem would make it zero; the Hahn-Banach theorem separates points and would force the resolvent itself to be zero, contradicting its inverse equation. Hence
If , then
is invertible by the Neumann series, a contradiction. Thus every satisfies
Here because is invertible and is not. Since , this proves the inverse norm divergence at noninvertible boundary points:
Suppose were a left inverse of an algebra element , so . Then , and is invertible for all sufficiently large by the Neumann series. For such , is a product of invertibles, hence invertible. The equation then gives , a contradiction.
If instead , then , so is eventually invertible. Now is invertible, and again , a contradiction. This proves that a noninvertible limit of invertibles has neither type of one-sided inverse. No finite-dimensional assumption is used.

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