The 1983 classification of unitary highest weight modules over Hermitian symmetric Lie groups by Enright-Howe-Wallach and Jakobsen has recently been re-proved by elementary means (Dirac inequality plus PRV tensoring) for the classical families sp(2n,R), so*(2n), su(p,q), and, by a 2025 sequel, for the remaining families so(2,n), e6(-14), e7(-25); the unitary set has also been described at fixed infinitesimal character for all six families in the integral case. The sequel resolves the principal deferred item of the source paper; the surviving open core of the source paper's further-work program is: (i) explicit algebraic constructions of the first-reduction-point unitary modules in the so*(2n) subcases where unitarity is currently certified only by a continuity argument on the Shapovalov form; and (ii) elementary constructions of the discrete-part unitary modules in the exceptional cases e6(-14) and e7(-25), where the authors state that PRV products do not realize them and theta correspondence is used instead. Extending the fixed-infinitesimal-character description to the non-integral characters of su(p,q) and so*(2n) is a further optional direction beyond the sources' stated program, not part of the open core.

Background

Let GG be a connected simple Lie group of Hermitian type, meaning that the symmetric space G/KG/K (KK a maximal compact subgroup) carries a GG-invariant complex structure. On the Lie algebra level this is equivalent to the complexified Lie algebra decomposing as g=k⊕p+⊕p−\mathfrak{g}=\mathfrak{k}\oplus\mathfrak{p}^+\oplus\mathfrak{p}^- with p±\mathfrak{p}^\pm abelian, and the simple real Lie algebras of Hermitian type are exactly sp(2n,R)\mathfrak{sp}(2n,\mathbb{R}), so∗(2n)\mathfrak{so}^*(2n), su(p,q)\mathfrak{su}(p,q), so(2,n)\mathfrak{so}(2,n), e6(−14)\mathfrak{e}_{6(-14)} (the Lie algebra of the exceptional symmetric space E III) and e7(−25)\mathfrak{e}_{7(-25)} (E VII). A (g,K)(\mathfrak{g},K)-module (Harish-Chandra module) is called a highest weight module if it is generated by a weight vector annihilated by all positive root spaces of g\mathfrak{g}; its highest weight λ\lambda is then dominant and integral for k\mathfrak{k}, and the module is the unique irreducible quotient L(λ)L(\lambda) of the generalized Verma module N(λ)=U(g)⊗U(k⊕p+)FλN(\lambda)=U(\mathfrak{g})\otimes_{U(\mathfrak{k}\oplus\mathfrak{p}^+)}F_\lambda, where FλF_\lambda is the irreducible k\mathfrak{k}-module of highest weight λ\lambda. Unitary highest weight modules include the holomorphic discrete series and small representations such as the Segal-Shale-Weil (metaplectic) representation, and they are basic building blocks in the harmonic analysis of Hermitian symmetric spaces. The infinitesimal character, represented by the Harish-Chandra parameter Λ=λ+ρ\Lambda=\lambda+\rho modulo the Weyl group (ρ\rho being half the sum of the positive roots), is the standard invariant by which irreducible modules are organized.

Which L(λ)L(\lambda) are unitary was classified in 1983 by Enright-Howe-Wallach and independently by Jakobsen. The answer is organized along lines: fixing the highest weight, one studies the line λ0+zζ\lambda_0+z\zeta parameterized by z∈Rz\in\mathbb{R}, where ζ\zeta is the element orthogonal to the compact roots normalized against the maximal noncompact root. For zz sufficiently negative, N(λ0+zζ)N(\lambda_0+z\zeta) is a holomorphic discrete series module, irreducible and unitary; the smallest aa for which N(λ0+aζ)N(\lambda_0+a\zeta) is reducible is the first reduction point, and the unitary points on the line form a continuous part z<az<a together with finitely many discrete points, one of which may sit at z=az=a. Enright-Howe-Wallach proved unitarity on the continuous part and at z=az=a by a continuity argument on the Shapovalov form (the invariant Hermitian form on N(λ)N(\lambda), positive definite for z<az<a and positive semidefinite at z=az=a by passage to the limit), and constructed the discrete modules via theta correspondence, i.e. the transfer of representations between the two members of a dual pair of subgroups realized on a common Weil representation.

The source paper, by Pandžić-Prlić-Souček-Tuček, re-proves the classification for sp(2n,R)\mathfrak{sp}(2n,\mathbb{R}), so∗(2n)\mathfrak{so}^*(2n) and su(p,q)\mathfrak{su}(p,q) by elementary means. Its two main tools are, first, the Dirac inequality of Parthasarathy, a necessary condition for unitarity of the form ∥(λ−s)++ρk∥2≥∥λ+ρ∥2\|(\lambda-s)^++\rho_{\mathfrak{k}}\|^2\ge\|\lambda+\rho\|^2 for every Schmid KK-submodule with lowest weight −s-s of the symmetric algebra S(p−)S(\mathfrak{p}^-) (here ρk\rho_{\mathfrak{k}} is half the sum of the positive compact roots and (⋅)+(\cdot)^+ denotes the k\mathfrak{k}-dominant rearrangement), used at full strength through refined versions proved in the authors' Dirac-inequality papers; and second, PRV products, the technique going back to Parthasarathy-Ranga Rao-Varadarajan of realizing extreme KK-types FF inside tensor products of unitary modules and taking the generated submodule U(p−)FU(\mathfrak{p}^-)F, which is then an irreducible unitary highest weight module. Starting from basic modules obtained from the Weil representation, this tensoring construction produces all discrete unitary modules in most cases. The same authors, with Savin, completed the remaining families so(2,n)\mathfrak{so}(2,n), e6(−14)\mathfrak{e}_{6(-14)} and e7(−25)\mathfrak{e}_{7(-25)} in 2025, and the unitary set has since been described at fixed infinitesimal character for all six families in the integral case. What the elementary account still lacks is the subject of the problem below: in certain so∗(2n)\mathfrak{so}^*(2n) subcases the first-reduction-point modules are certified unitary only by the continuity argument (Lemma 1.11 of the source paper), and in the exceptional cases the discrete modules are reached only through theta correspondence. The non-integral infinitesimal characters of su(p,q)\mathfrak{su}(p,q) and so∗(2n)\mathfrak{so}^*(2n) are also untreated; that extension is noted below as an optional direction beyond the sources' stated program, not as part of the open core. For SU(1,2)SU(1,2), Kubo and Ørsted have recently exhibited the shape such completions can take, realizing the first-reduction-point modules as kernels and images of explicit intertwining differential operators built from Bernstein-Gelfand-Gelfand (BGG) resolutions, i.e. algebraic resolutions of highest weight modules by direct sums of Verma-type modules.

Problem Statement

Complete the constructive, elementary account of unitary highest weight modules for the Hermitian symmetric groups, removing the remaining non-algebraic steps. The classification itself (which L(λ)L(\lambda) are unitary) is closed, so the question is not which modules are unitary but whether each unitary module can be produced and certified by a direct algebraic construction. Concretely, with the notation of the Background:

  1. For the so∗(2n)\mathfrak{so}^*(2n) lines λ0+zζ\lambda_0+z\zeta in the subcases where the tensoring/PRV technique of the source paper produces all discrete unitary points except the first reduction point z=az=a — of which the Case-1 lines with λ1>λ2\lambda_1>\lambda_2, on which the unique discrete point is the endpoint of the continuous part, are the instances the source singles out, the target being the whole class rather than these instances alone — give a direct algebraic construction of L(λ0+aζ)L(\lambda_0+a\zeta), together with a proof of unitarity and irreducibility that does not pass through the continuity argument of Lemma 1.11 of the source paper.

  2. Give an elementary algebraic construction of the discrete-part unitary highest weight modules of the exceptional Hermitian groups E6(−14)E_{6(-14)} and E7(−25)E_{7(-25)}, extending or replacing the tensoring/PRV program of the source papers — basic modules from Segal-Shale-Weil/Weil representations, tensor products and PRV products. The sequel classification (arXiv:2412.06317, Section 1) states explicitly that PRV products do not construct the discrete part in these cases; the existing certifications — the E6E_6 dual-pair exceptional theta correspondence of Section 6 of that paper and, for E7E_7, the Enright-Howe-Wallach second-tensor-power argument cited there — are the current non-elementary state of the art and do not provide such a construction.

Parts 1 and 2 above jointly constitute one objective: a fully constructive, algebraic account of the unitary highest weight modules for all six Hermitian symmetric families, with no step certified only by continuity or theta correspondence.

Optional extension (not part of the completion criterion): the 2026 fixed-infinitesimal-character treatment of su(p,q)\mathfrak{su}(p,q) and so∗(2n)\mathfrak{so}^*(2n) deliberately restricts to integral infinitesimal characters, with a stated rationale, and announces no follow-up. Describing the unitary set at the non-integral infinitesimal characters of these two families is a meaningful further direction, but solving it is not required to close the problem.

References

  1. Pavle Pandžić, Ana Prlić, Vladimír Souček, Vít Tuček, 'On the classification of unitary highest weight modules', Japanese Journal of Mathematics (2026), DOI 10.1007/s11537-026-2451-5; arXiv:2305.15892, https://arxiv.org/abs/2305.15892.
  2. Pavle Pandžić, Ana Prlić, Gordan Savin, Vladimír Souček, Vít Tuček, 'On the classification of unitary highest weight modules in the exceptional cases', Journal of Algebra 684 (2025) 524-562, DOI 10.1016/j.jalgebra.2025.07.018; arXiv:2412.06317, https://arxiv.org/abs/2412.06317.
  3. Pavle Pandžić, Ana Prlić, Vladimír Souček, Vít Tuček, 'Unitary highest weight modules for su(p,q)\mathfrak{su}(p,q) and so∗(2n)\mathfrak{so}^*(2n) with fixed integral infinitesimal character', arXiv:2604.20566 (2026), https://arxiv.org/abs/2604.20566.
  4. Toshihisa Kubo, Bent Ørsted, 'On the intertwining differential operators between vector bundles over the real projective space of dimension two', arXiv:2503.22323 (2025), https://arxiv.org/abs/2503.22323.
  5. T. J. Enright, R. Howe, N. Wallach, 'A classification of unitary highest weight modules', in Representation Theory of Reductive Groups (Park City, Utah, 1982), Progress in Mathematics 40, Birkhäuser, Boston, 1983, pp. 97-143, DOI 10.1007/978-1-4684-6730-7_7, https://doi.org/10.1007/978-1-4684-6730-7_7.
  6. H. P. Jakobsen, 'Hermitian symmetric spaces and their unitary highest weight modules', Journal of Functional Analysis 52 (1983) 385-412, DOI 10.1016/0022-1236(83)90076-9, https://doi.org/10.1016/0022-1236(83)90076-9.
  7. R. Parthasarathy, 'Criteria for the unitarizability of some highest weight modules', Proceedings of the Indian Academy of Sciences Section A 89 (1980) 1-24, DOI 10.1007/BF02881021, https://doi.org/10.1007/BF02881021.
  8. M. Davidson, T. Enright, R. Stanke, 'Differential operators and highest weight representations', Memoirs of the American Mathematical Society 455 (1991), DOI 10.1090/memo/0455, https://doi.org/10.1090/memo/0455.
  9. T. Enright, A. Joseph, 'An intrinsic analysis of unitarizable highest weight modules', Mathematische Annalen 288 (1990) 571-594, DOI 10.1007/BF01444551, https://doi.org/10.1007/BF01444551.
  10. Pavle Pandžić, Ana Prlić, Vladimír Souček, Vít Tuček, 'Dirac inequality for highest weight Harish-Chandra modules I', Mathematical Inequalities and Applications 26 (2023) 233-265, DOI 10.7153/mia-2023-26-17, https://doi.org/10.7153/mia-2023-26-17.