- The papers defines the class of operators $ \mathcal{M}_{mul}(H) of bounded operators that attain their minimum modulus on every reducing subspace.
- Self-adjoint operators in $\mathcal{ M}_{mul}(H)$ have a well-ordered point spectrum and are diagonalizable
- The class $\mathcal{ M}_{mul}(H)$ is dense in the space of all bounded operators, indicating prevalence in operator theory.
This paper introduces and develops the theory of operators that attain their minimum modulus on every nonzero reducing subspace. For a bounded operator T on a separable complex Hilbert space H, the minimum modulus is m(T)=inf{∥Tx∥:x∈SH}, and T is minimum attaining if this infimum is realized on the unit sphere. The authors define
Mr(H):={T∈B(H):T∣M∈M(M) for every nonzero M∈RT},
where RT denotes the lattice of reducing subspaces of T. This class interpolates between the absolutely minimum attaining operators AM(H) and the minimum attaining operators M(H):
T0
Both inclusions are shown to be strict. Strictness on the left follows because every idempotent lies in T1, while an idempotent with both range and kernel infinite dimensional fails to be AM (by a known characterization of AM idempotents). Strictness on the right follows from an explicit diagonal operator on T2 that attains its minimum at T3 but whose restriction to T4 has minimum modulus T5 that is not an eigenvalue. The definition parallels the T6-class of norm attaining operators studied by Ramesh and Osaka, where norm attainment is required on every reducing subspace; here all results are proved independently using the minimum-attainment property.
The paper also identifies broad natural subclasses contained in T7: every irreducible minimum attaining operator, all idempotents, orthogonal projections, partial isometries, Toeplitz operators with inner symbols, and Hankel operators T8 with T9 inner. Membership is invariant under unitary equivalence, and for WEP operators (H0), membership of H1 is equivalent to membership of H2. In general, however, H3 does not imply H4 or H5; a unilateral weighted shift example demonstrates all three failures simultaneously, including non-closed range.
A useful reduction is that H6 implies H7, since H8 and H9; for positive m(T)=inf{∥Tx∥:x∈SH}0, membership of m(T)=inf{∥Tx∥:x∈SH}1 is equivalent to that of m(T)=inf{∥Tx∥:x∈SH}2.
Spectral structure: well-ordered point spectra
The central spectral result concerns self-adjoint operators: if m(T)=inf{∥Tx∥:x∈SH}3 is self-adjoint, then m(T)=inf{∥Tx∥:x∈SH}4 admits an orthonormal basis of eigenvectors, and the set m(T)=inf{∥Tx∥:x∈SH}5 is a countable well-ordered subset of m(T)=inf{∥Tx∥:x∈SH}6. Consequently m(T)=inf{∥Tx∥:x∈SH}7 admits the strong-operator-topology representation m(T)=inf{∥Tx∥:x∈SH}8 over mutually orthogonal eigenprojections. The proof of diagonalizability is a Zorn's lemma argument: a maximal orthonormal set of eigenvectors spans a reducing subspace, and minimum attainment forces an eigenvector in any nonzero complement. Well-ordering follows from applying the defining condition to the reducing subspace spanned by eigenspaces indexed by an arbitrary subset m(T)=inf{∥Tx∥:x∈SH}9 of T0: minimum attainment forces T1 itself to lie in T2.
The mechanism behind well-ordering is transparent: a positive operator with strictly decreasing eigenvalues T3 fails membership, since the direct sum of the corresponding eigenspaces is reducing but the infimum T4 is not attained there. Combining necessity and sufficiency yields a complete characterization:
Characterization: A positive operator T5 belongs to T6 if and only if T7, where T8 is a bounded countable well-ordered set and T9 are mutually orthogonal projections summing to Mr(H):={T∈B(H):T∣M∈M(M) for every nonzero M∈RT},0 strongly. In particular Mr(H):={T∈B(H):T∣M∈M(M) for every nonzero M∈RT},1, so the spectrum of such an operator is countable with at most one accumulation point, namely its infimum.
There is also a clean bridge to the Mr(H):={T∈B(H):T∣M∈M(M) for every nonzero M∈RT},2-class: for positive Mr(H):={T∈B(H):T∣M∈M(M) for every nonzero M∈RT},3 with Mr(H):={T∈B(H):T∣M∈M(M) for every nonzero M∈RT},4, one has Mr(H):={T∈B(H):T∣M∈M(M) for every nonzero M∈RT},5 if and only if Mr(H):={T∈B(H):T∣M∈M(M) for every nonzero M∈RT},6. This affine correspondence reflects that, on positive operators, minimum attainment of Mr(H):={T∈B(H):T∣M∈M(M) for every nonzero M∈RT},7 coincides with norm attainment of its reflection about Mr(H):={T∈B(H):T∣M∈M(M) for every nonzero M∈RT},8.
Stability under perturbations and density
Two perturbation results show robustness of the class. First, adding a self-adjoint finite-rank operator commuting with each Mr(H):={T∈B(H):T∣M∈M(M) for every nonzero M∈RT},9 to a well-ordered spectral sum preserves membership, because finitely many points are removed from and adjoined to a well-ordered set. Second, subtracting a positive compact operator RT0 commuting with the RT1 and dominated by RT2 on each range RT3 also preserves membership; the proof shows that any putative decreasing sequence in RT4 would force either infinitely many increasing nonzero eigenvalues of a compact operator or a contradiction via compactness applied to an orthonormal sequence. These combine into a theorem covering RT5 perturbations of positive type, which in turn yields that finite direct sums of AM operators lie in RT6. Notably, this fails for infinite direct sums: RT7 has point spectrum without a least element and hence is not in the class.
The density results are the strongest quantitative statements in the paper:
RT8
The argument approximates RT9 on T0 by a finite-spectrum self-adjoint operator, forms T1 via the polar decomposition, notes T2 has finite spectrum and thus lies in the class, and concludes T3. Moreover, refining with a rank-one-type perturbation technique of Tcaciuc, the authors prove that the operators in T4 possessing a nontrivial invariant half-space are also norm dense in T5 — a strengthening relevant to the invariant subspace problem, since it shows dense subsets of T6 consist of operators guaranteed to have invariant subspaces of infinite dimension and codimension. Since T7, these density theorems strictly improve the known density of T8 due to Kulkarni and Ramesh.
Normal and multiplication operators
For quasinormal T9, membership of AM(H)0 is equivalent to AM(H)1; the proof shows quasinormality makes the closed span of eigenspaces of AM(H)2 reduce AM(H)3, allowing the Zorn-type argument to run for AM(H)4 directly. For normal operators this yields a full structural representation: AM(H)5 if and only if AM(H)6 decomposes as an orthogonal direct sum of pairwise orthogonal reducing subspaces AM(H)7, with AM(H)8 countable well-ordered, such that
AM(H)9
where each M(H)0 is unitary (with M(H)1 arbitrary on M(H)2). Three consequences follow immediately: normal members have adjoints in the class, normal members have closed range (since M(H)3 is injective and minimum attaining, hence bounded below), and multiplying a normal member on either side by an isometry preserves membership — the last requiring a careful case analysis when M(H)4.
As a concrete application, multiplication operators on M(H)5 are characterized symbol-theoretically: M(H)6 if and only if
M(H)7
with M(H)8 unimodular, M(H)9 pairwise essentially disjoint measurable sets of positive measure covering T00 up to null sets, and T01 a countable well-ordered subset of T02. Thus T03 qualifies exactly when T04 takes countably many values indexed by a well-ordered set.
General operators and the hypothesis T05
Without normality or quasinormality, T06 and T07 need not share reducing subspaces. Under the structural assumption T08, the equivalence T09 holds verbatim, and the paper obtains a complete representation: T10 belongs to the class if and only if
T11
where T12 is countable well-ordered, T13 are mutually orthogonal projections summing to T14, and T15 are partial isometries with initial spaces T16 satisfying T17; convergence is in the strong operator topology. This is obtained from the polar decomposition T18 by restricting the partial isometry to each spectral subspace.
Finally, the hypothesis itself is characterized through von Neumann algebras: writing T19, one has T20 if and only if the partial isometry T21 belongs to the bicommutant T22. The forward direction shows T23 commutes with every projection in T24 (handling T25 separately), then extends to the whole commutant by strong density of projections; the converse uses commutation with spectral projections of T26 to transfer reducibility. The authors explicitly pose as an open question the search for intrinsic necessary and sufficient conditions for T27 beyond this algebraic criterion.
Limitations and open questions
Several restrictions qualify the results. Membership is not preserved under taking adjoints or moduli in general, so much of the theory relies on auxiliary hypotheses (self-adjointness, quasinormality, normality, WEP, or T28). The spectral characterizations apply directly only to positive and self-adjoint operators; for arbitrary T29 no spectral description independent of the structural hypothesis is given. Infinite direct sums of AM operators fall outside the class, so the finite-sum stability result cannot be extended naively. The paper leaves open the characterization of T30 stated above, and the analogous question of whether the compact-perturbation results extend to broader classes of commuting perturbations is not addressed.
Conclusion
The paper establishes T31 as a properly intermediate class between absolutely minimum attaining and minimum attaining operators, gives complete spectral characterizations in the positive, normal, and structurally constrained settings via countable well-ordered spectra, proves norm denseness of the class — and of its subclass with nontrivial invariant half-spaces — in T32, and links membership for normal and multiplication operators to concrete decompositions. The remaining gap between the general theory and the cases governed by T33 defines the natural continuation of this line of work.