Ugo Bruzzo’s research while affiliated with Federal University of Paraíba and other places

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Publications (39)


The paint group Tits Satake theory of hyperbolic symmetric spaces: the distance function, paint invariants and discrete subgroups
  • Preprint

February 2025

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3 Reads

Ugo Bruzzo

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Mario Trigiante

The present paper, which is partially a review, but also contains several completely new results, aims at presenting, in a unified mathematical framework, a complex and articulated lore regarding non-compact symmetric spaces, with negative curvature, whose isometry group is a non-compact, real simple Lie group. All such manifolds are Riemannian normal manifolds, according to Alekseevsky's definition, in the sense that they are metrically equivalent to a solvable Lie group manifold. This identification provides a vision in which, on one side one can derive quite explicit and challenging formulae for the unique distance function between points of the manifold, on the other one, one can organize the entire set of the available manifolds in universality classes distinguished by their common Tits Satake submanifold and, correspondingly, by their non-compact rank. The members of the class are distinguished by their different Paint Groups, the latter notion having been introduced by two of the present authors in an earlier collaboration. In relation to the construction of neural networks, these mathematical structures offer unique possibilities of replacing ad hoc activation functions with the naturally defined non-linear operations that relate Lie algebras to Lie Groups and vice-versa. The Paint Group invariants offer new tokens both to construct algorithms and inspect (hopefully to control) their working. A conspicuous part of the paper is devoted to the study and systematic construction of parabolic/elliptic discrete subgroups of the Lie groups SO(r,r+q), in view of discretization and/or tessellations of the space to which data are to be mapped. Furthermore, it is shown how the ingredients of Special K\"ahler Geometry and the c-map, well known in the supergravity literature, provide a unified classification scheme of the relevant Tits Satake universality classes with non-compact rank r<5.


Splitting of supervector bundles on projective superspaces

January 2025

We provide a splitting criterion for supervector bundles over the projective superspaces Pnm\mathbb{P}^{n|m}. More precisely, we prove that a rank pqp|q supervector bundle on Pnm\mathbb{P}^{n|m} with vanishing intermediate cohomology is isomorphic to the direct sum of even and odd line bundles, provided that n2n \geq 2. For n=1 we provide an example of a supervector bundle that cannot be written as a sum of line bundles.



Cox-Gorenstein algebras
  • Preprint
  • File available

July 2024

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26 Reads

This paper is a first step in the study of nonstandard graded algebras having Poincar\'e duality and their Lefschetz properties. We prove the equivalence between the toric setup and the G-graded one, generalize Macaulay-Matlis duality, introduce Lefschetz properties and prove a Hessian criteria in the G-graded setup. We prove a special case of the Codimension One Conjecture of Cattani-Cox-Dickenstein.

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Seiberg–Witten differentials on the Hitchin base

January 2024

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7 Reads

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1 Citation

Revista de la Real Academia de Ciencias Exactas, Físicas y Naturales. Serie A, Matemáticas

In this note we describe explicitly, in terms of Lie theory and cameral data, the covariant (Gauss–Manin) derivative of the Seiberg–Witten differential defined on the weight-one variation of Hodge structures that exists on a Zariski open subset of the base of the Hitchin fibration.



Deformation of pairs and Noether–Lefschetz loci in toric varieties

November 2023

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10 Reads

European Journal of Mathematics

We continue our study of the Noether–Lefschetz loci in toric varieties and investigate deformation of pairs (V, X) where V is a complete intersection subvariety and X a quasi-smooth hypersurface in a simplicial projective toric variety PΣ2k+1PΣ2k+1\mathbb {P}_{\Sigma }^{2k+1}, with V⊂XVXV\subset X. The hypersurface X is supposed to be of Macaulay type, which means that its toric Jacobian ideal is Cox–Gorenstein, a property that generalizes the notion of Gorenstein ideal in the standard polynomial ring. Under some assumptions, we prove that the class λV∈Hk,k(X)λVHk,k(X)\lambda _V\in H^{k,k}(X) deforms to an algebraic class if and only if it remains of type (k, k). Actually we prove that locally the Noether–Lefschetz locus is an irreducible component of a suitable Hilbert scheme. This generalizes Theorem 4.2 in our previous work (Bruzzo and Montoya 15(2):682–694, 2021) and the main theorem proved by Dan (in: Analytic and Algebraic Geometry. Hindustan Book Agency, New Delhi, pp 107–115, 2017).


On a Conjecture About Higgs Bundles and Some Inequalities

September 2023

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52 Reads

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1 Citation

Mediterranean Journal of Mathematics

We briefly review an open conjecture about Higgs bundles that are semistable after pulling back to any curve, and prove it in the rank 2 case. We also prove some results in higher rank under suitable additional assumptions. Moreover, we establish a set of inequalities holding for H-nef Higgs bundles that generalize some of the Fulton–Lazarsfeld inequalities for numerically effective vector bundles.


Positivity for Higgs vector bundles

July 2023

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9 Reads

Working in the category of smooth projective varieties over an algebraically closed field of characteristic 0, we review notions of ampleness and numerical nefness for Higgs bundles which "feel" the Higgs field and formulate criteria of the Barton-Kleiman type for these notions. We give an application to minimal surfaces of general type that saturate the Miyaoka-Yau inequality, showing that their cotangent bundle is ample. This will use results by Langer that imply that also for varieties over algebraically closed field of characteristic zero the so-called Simpson system is stable.


The universal polytope in the v,u2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathfrak {v},\frac{\mathfrak {u}}{2}$$\end{document} plane for all the metrics of the MB\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${\mathcal M}_B$$\end{document} manifolds considered in this paper and defined in equation (6.1)
A (left): Plot of the three functions CF1,2,3F2(v)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathcal{C}\mathcal{F}^{\mathbb {F}_2}_{1,2,3}(\mathfrak {v})$$\end{document} entering the intrinsic Riemann curvature tensor for the “Kronheimer” metric on F2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathbb {F}_2$$\end{document} with the choice of the parameter α=1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\alpha = 1$$\end{document}. B (right): Plot of the three functions CF1,2,3WW112(v)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathcal{C}\mathcal{F}^{\mathbb{W}\mathbb{W}_{112}}_{1,2,3}(\mathfrak {v})$$\end{document} entering the intrinsic Riemann curvature tensor for the Kronheimer metric on WP[1,1,2]\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathbb{W}\mathbb{P}[1,1,2]$$\end{document} with the choice of the parameter α=0\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\alpha = 0$$\end{document}. Comparing this picture with the one on the left, we see the discontinuity. In all smooth cases, the functions CF2,3F2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathcal{C}\mathcal{F}^{\mathbb {F}_2}_{2,3}$$\end{document} attain the same value in the lower endpoint of the interval while for the singular case of the weighted projective space, the initial values of CF2,3WP[1,1,2](v)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathcal{C}\mathcal{F}^{\mathbb{W}\mathbb{P}[1,1,2]}_{2,3}(\mathfrak {v})$$\end{document} are different
Plot of the three functions CF1,2,3KE(v)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathcal{C}\mathcal{F}^{\textrm{KE}}_{1,2,3}(\mathfrak {v})$$\end{document} entering the intrinsic Riemann curvature tensor for the KE metric with the choice of the parameter λ1=1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\lambda _1 = 1$$\end{document}, λ2=2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\lambda _2 = 2$$\end{document}
Plot of the three functions CF1,2,3F2ext(v)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathcal{C}\mathcal{F}^{F2ext}_{1,2,3}(\mathfrak {v})$$\end{document} entering the intrinsic Riemann curvature tensor for the extremal Kähler metrics on F2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$F_2$$\end{document} with two different choices of the parameter a=1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ a = 1$$\end{document}, b=2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ b = 2$$\end{document} and a=1/3\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ a = 1/3$$\end{document}, b=7/2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ b = 7/2$$\end{document}
Plot of three examples of the HKroF2(v)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {H}^{\mathbb {F}_2}_{Kro}(\mathfrak {v})$$\end{document} function for three different choices of the parameter α\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\alpha $$\end{document}

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D3-brane supergravity solutions from Ricci-flat metrics on canonical bundles of Kähler–Einstein surfaces

June 2023

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60 Reads

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1 Citation

Letters in Mathematical Physics

D3 brane solutions of type IIB supergravity can be obtained by means of a classical Ansatz involving a harmonic warp factor, H(y,y¯)H(y,yˉ)H(\textbf{y},\bar{\textbf{y}}) multiplying at power -1/21/2-1/2 the first summand, i.e., the Minkowski metric of the D3 brane world-sheet, and at power 1/2 the second summand, i.e., the Ricci-flat metric on a six-dimensional transverse space M6M6\mathcal {M}_6, whose complex coordinates y are the arguments of the warp factor. Of particular interest is the case where M6=tot[KMBM6=tot[K[(MB)]\mathcal {M}_6={\text {tot}}[ K\left[ \left( \mathcal {M}_B\right) \right] is the total space of the canonical bundle over a complex Kähler surface MBMB\mathcal {M}_B. This situation emerges in many cases while considering the resolution à la Kronheimer of singular manifolds of type M6=C3/ΓM6=C3/Γ\mathcal {M}_6=\mathbb {C}^3/\Gamma , where Γ⊂SU(3)ΓSU(3)\Gamma \subset \mathrm {SU(3)} is a discrete subgroup. When Γ=Z4Γ=Z4\Gamma = \mathbb {Z}_4, the surface MBMB\mathcal {M}_B is the second Hirzebruch surface endowed with a Kähler metric having SU(2)×U(1)SU(2)×U(1)\mathrm {SU(2)\times U(1)} isometry. There is an entire class Met(FV)Met(FV){\text {Met}}(\mathcal{F}\mathcal{V}) of such cohomogeneity one Kähler metrics parameterized by a single function FK(v)FK(v)\mathcal{F}\mathcal{K}(\mathfrak {v}) that are best described in the Abreu–Martelli–Sparks–Yau (AMSY) symplectic formalism. We study in detail a two-parameter subclass Met(FV)KE⊂Met(FV)Met(FV)KEMet(FV){\text {Met}}(\mathcal{F}\mathcal{V})_{\textrm{KE}}\subset {\text {Met}}(\mathcal{F}\mathcal{V}) of Kähler–Einstein metrics of the aforementioned class, defined on manifolds that are homeomorphic to S2×S2S2×S2S^2\times S^2, but are singular as complex manifolds. Actually, Met(FV)KE⊂Met(FV)ext⊂Met(FV)Met(FV)KEMet(FV)extMet(FV){\text {Met}}(\mathcal{F}\mathcal{V})_{\textrm{KE}}\subset {\text {Met}}(\mathcal{F}\mathcal{V})_{\textrm{ext}}\subset {\text {Met}}(\mathcal{F}\mathcal{V}) is a subset of a four parameter subclass Met(FV)extMet(FV)ext{\text {Met}}(\mathcal{F}\mathcal{V})_{\textrm{ext}} of cohomogeneity one extremal Kähler metrics originally introduced by Calabi in 1983 and translated by Abreu into the AMSY action-angle formalism.Met(FV)extMet(FV)ext{\text {Met}}(\mathcal{F}\mathcal{V})_{\textrm{ext}} contains also a two-parameter subclass Met(FV)extF2Met(FV)extF2{\text {Met}}(\mathcal{F}\mathcal{V})_{\textrm{ext}\mathbb {F}_2} disjoint from Met(FV)KEMet(FV)KE{\text {Met}}(\mathcal{F}\mathcal{V})_{\textrm{KE}} of extremal smooth metrics on the second Hirzebruch surface that we rederive using constraints on period integrals of the Ricci 2-form. The Kähler–Einstein nature of the metrics in Met(FV)KEMet(FV)KE{\text {Met}}(\mathcal{F}\mathcal{V})_{\textrm{KE}} allows the construction of the Ricci-flat metric on their canonical bundle via the Calabi Ansatz, which we recast in the AMSY formalism deriving some new elegant formulae. The metrics in Met(FV)KEMet(FV)KE{\text {Met}}(\mathcal{F}\mathcal{V})_{\textrm{KE}} are defined on the base manifolds of U(1) fibrations supporting the family of Sasaki–Einstein metrics SEmet5SEmet5\textrm{SEmet}_5 introduced by Gauntlett et al. (Adv Theor Math Phys 8:711–734, 2004), and already appeared in Gibbons and Pope (Commun Math Phys 66:267–290, 1979). However, as we show in detail using Weyl tensor polynomial invariants, the six-dimensional Ricci-flat metric on the metric cone of M5∈Met(SE)5M5Met(SE)5{\mathcal M}_5 \in {\text {Met}}(\textrm{SE})_5 is different from the Ricci-flat metric on tot[KMKEtot[K[(MKE)]{\text {tot}}[ K\left[ \left( \mathcal {M}_{\textrm{KE}}\right) \right] constructed via Calabi Ansatz. This opens new research perspectives. We also show the full integrability of the differential system of geodesics equations on MBMB\mathcal {M}_B thanks to a certain conserved quantity which is similar to the Carter constant in the case of the Kerr metric.


Citations (11)


... see also [BD24,eq. (8)]. Here λ SW is the Seiberg-Witten differential and ∇ GM the Gauss-Manin connection, see section 4. We review the discriminant D in section 2, but recall that it factors as D = D 1 D 2 , with the two factors corresponding to the products of roots of different lengths. ...

Reference:

Donagi-Markman cubics for Hitchin systems of type A2, B2. G2
Seiberg–Witten differentials on the Hitchin base

Revista de la Real Academia de Ciencias Exactas, Físicas y Naturales. Serie A, Matemáticas

... Remarks 0.1. Assuming K = C, the best of my knowledge, this conjecture has been proved in the following cases: a) r = 2, by [11,Theorems 4.5,4.8 and 4.9]; b) X has nef tangent bundle, by [14,Corollary 3.15]; c) dim(X) = 2 and the Kodaira dimension κ(X) of X is either −∞ or 0 ([14, Theorem 3.6, Propositions 3.11, 3.12, Corollary 3.8] and [13,Theorem 6.4]). d) dim(X) = 2, κ(X) = 1 and other technical hypotheses, see [15,Proposition 5.6]; e) X is a simply-connected Calabi-Yau variety, by [7,Theorem 4.1]; f) if X satisfies the Conjecture and Y is a fibred projective variety over X with rationally connected fibres, then Y does the same, by [14,Proposition 3.11]; g) if X satisfies the Conjecture then any finiteétale quotient Y of X does the same, by [14,Proposition 3.12]; h) E has a Jordan-Hölder filtration whose quotient are H-nflat and have rank at most 2, by [7, Theorem 3.2, Corollary 3.3] and previous item a; i) particular Higgs bundles described in [10]. ...

On a Conjecture About Higgs Bundles and Some Inequalities

Mediterranean Journal of Mathematics

... I plan to report on the advances obtained on the following special aspect of the gauge/gravity correspondence, within the context of quiver gauge-theories [18,19,20,21,22]: the relevance of the generalized Kronheimer construction [17,23,24,25] for the resolution of C 3 /Γ singularities. ...

D3-brane supergravity solutions from Ricci-flat metrics on canonical bundles of Kähler–Einstein surfaces

Letters in Mathematical Physics

... • Rationally connected varieties; • Abelian varieties; • Fibrations over a Higgs variety whose fibers are rationally connected; • Bases of finiteétale covers whose total space is a Higgs variety; • Varieties of dimension ≥ 3 containing an effective ample divisor which is a Higgs variety; • Varieties with nef tangent bundle (in dimension 2 and 3 these were classified in [10]); • Varieties birational to a Higgs variety. Moreover, in [7] it was shown that algebraic K3 surfaces are Higgs varieties, and this was extended, using different techniques, to simply connected Calabi-Yau varieties in [3]. Some results in the case of elliptic surfaces are proved in [9]. ...

Filtrations of numerically flat Higgs bundles and curve semistable Higgs bundles on Calabi–Yau varieties
  • Citing Article
  • March 2023

Advances in Geometry

... Assuming K = C, the best of my knowledge, this conjecture has been proved in the following cases: a) r = 2, by [11,Theorems 4.5,4.8 and 4.9]; b) X has nef tangent bundle, by [14,Corollary 3.15]; c) dim(X) = 2 and the Kodaira dimension κ(X) of X is either −∞ or 0 ([14, Theorem 3.6, Propositions 3.11, 3.12, Corollary 3.8] and [13,Theorem 6.4]). d) dim(X) = 2, κ(X) = 1 and other technical hypotheses, see [15,Proposition 5.6]; e) X is a simply-connected Calabi-Yau variety, by [7,Theorem 4.1]; f) if X satisfies the Conjecture and Y is a fibred projective variety over X with rationally connected fibres, then Y does the same, by [14,Proposition 3.11]; g) if X satisfies the Conjecture then any finiteétale quotient Y of X does the same, by [14,Proposition 3.12]; h) E has a Jordan-Hölder filtration whose quotient are H-nflat and have rank at most 2, by [7, Theorem 3.2, Corollary 3.3] and previous item a; i) particular Higgs bundles described in [10]. ♦ Using the previous "Lefschetz principle"-type theorem, I reduce this conjecture to complex case, i.e. it is enough to prove it on smooth complex projective varieties (cfr. ...

Semistable Higgs bundles on elliptic surfaces
  • Citing Article
  • April 2022

Advances in Geometry

... The grading group is the class group Cl(X) = Hom Z (C * × Z 3 , Z) = Z ⊕ Z 3 . Equation (5) suggests that in this case instead of a matrix P we have two matrices (actually, column vectors) P 0 , P 1 , providing the weights of the actions of C * and Z 3 , respectively: 1 ...

On the Hodge conjecture for quasi-smooth intersections in toric varieties

São Paulo Journal of Mathematical Sciences

... The mathematical formalization of the study of algebraic supergeometry, extending classical results from algebraic geometry, has opened new directions in exploring mathematical objects arising in physics, particularly in supersymmetric field theories and superstring theory. Supergeometry aims to provide the right environment for studying such structures as moduli space of supervector bundles and moduli space of supersymmetric curves [7,3], which are important in the perturbative approach to superstring theory [9,11]. In this context, understanding the arithmetically Cohen-Macaulay (ACM) bundles is a natural step towards classifying supervector bundles on superschemes. ...

The supermoduli of SUSY curves with Ramond punctures
  • Citing Article
  • July 2021

Revista de la Real Academia de Ciencias Exactas, Físicas y Naturales. Serie A, Matemáticas