Home The twofold way of super holonomy
Article
Licensed
Unlicensed Requires Authentication

The twofold way of super holonomy

  • Josua Groeger EMAIL logo
Published/Copyright: May 5, 2016

Abstract

There are two different notions of holonomy in supergeometry, the supergroup introduced by Galaev and our functorial approach motivated by super Wilson loops. Either theory comes with its own version of invariance of vectors and subspaces under holonomy. By our first main result, the Twofold Theorem, these definitions are equivalent. Our proof is based on the Comparison Theorem, our second main result, which characterises Galaev’s holonomy algebra as an algebra of coefficients, building on previous results. As an application, we generalise some of Galaev’s results to S-points, utilising the holonomy functor. We obtain, in particular, a de Rham–Wu decomposition theorem for semi-Riemannian S-supermanifolds.

MSC 2010: 58A50; 53C29; 18F05

Communicated by Karl-Hermann Neeb


Funding statement: Research funded by the Institutional Strategy of the University of Cologne in the German Excellence Initiative.

A The fppf topology on the category of superpoints

For the purpose of studying the holonomy group functors it was natural to define the fppf-topology on the category 𝒫 of superpoints 0|L in the form of Definition 3.7. The objective of this appendix is to relate this definition to the one which is well known in algebraic geometry under the same name. For concreteness, we consider the 2-graded version used in [33, 22] of the classical notion (cf. [15, Section 5.2]), as follows.

Let SAlgK denote the category of supercommutative superalgebras over a field K with characteristic different from 2. Recall that a supercommutative superalgebra B over a superring A is said to be finitely presented if it is of the form A[t1,,tn|θ1,,θm]/I where I is a finitely generated ideal. An A-supermodule Y is said to be faithfully flat if the following holds: A sequence XXX′′ is exact if and only if the sequence XAYXAYX′′AY is exact (for all A-modules X,X,X′′).

Definition A.1

Definition A.1 (fppf)

The fppf topology on SAlgK is defined as collection of finite sets {RRi}iI (for R,RiSAlgK) such that the R-supermodule ×iIRi is faithfully flat and all Ri are finitely presented R-superalgebras.

Note that 𝒫 is naturally equivalent to the category Gr of Graßmann algebras over and, as such, can be considered as a full subcategory of SAlg. It makes sense to consider Definition A.1 restricted to 𝒫. Doing so results in our previous notion of fppf topology as shown by the following main result of this appendix.

Theorem A.2

The topology on P as defined in Definition 3.7 agrees with the one induced by Definition A.1.

Proof.

We note first that being finitely presented is no condition in the case of Graßmann algebras. Consider a covering consisting of morphisms φi:PiP as in Definition 3.7. By the following proposition, Proposition A.3, φi is a submersion if and only if Ri=𝒪Pi is flat as an R=𝒪P-module with respect to φ* (a morphism in Gr). All Ri being flat, in turn, is equivalent to the condition of Definition A.1 (by [4, Lemma I.2.2] and the implication (ii)  (i) in Proposition A.3). ∎

Concerning the preceding proof, we are obviously in the supercommutative rather than the commutative situation treated in [4]. However, the results relevant for our present purposes continue to hold unchanged.

In the following, we shall make no notational distinction between a morphism φ:0|L0|L and its pullback φ:LL.

Proposition A.3

Let φ:RS be a morphism in Gr, and consider S as an R-module via φ. Then the following are equivalent:

  1. S is faithfully flat.

  2. S is flat.

  3. S is free.

  4. (The associated morphism of superpoints corresponding to) φ is a submersion.

Proof.

(i)  (ii). In general, an R-module M is faithfully flat if and only if M is flat and MmM for every maximal ideal m (see [4, Proposition I.3.1]). In the case of a Graßmann algebra R, its nilpotent part Rnil is the unique maximal ideal and, obviously, Sφ(Rnil)S.

(ii)  (iii). The Jacobson radical of R is Rnil, and R/Rnil is a field. The equivalence follows from [4, Proposition II.3.5].

(iv)  (iii). A submersion is characterised by the existence of coordinates (θi)1in and (ηj)1jn+m on R and S, respectively, such that θiηi (see [5, Proposition 5.2.5]). Then any -basis of ηn+1,,ηn+m is an R-basis of S.

(ii)  (iv). This is a special case of [27, Proposition 3.6.1 (ii)]. ∎

Along with the proposition, also Theorem A.2 is established. We remark that the result by Schmitt in [27], used for the last implication, is really the hardest bit of the proof. While Schmitt’s results are stronger than needed here, his proofs involve a heavy algebraic machinery. We therefore consider it worth providing an independent, less abstract, proof of the implication (iii)  (iv) in Proposition A.3 in the remainder of this appendix. It is shown by induction over the number of R-Graßmann-generators, while the base case is established by means of ideal theory and reduction to a special case considered by Esin and Koç in [7]. The proof of the latter result, in turn, is rather concrete. We start with two easy lemmas needed in the inductive step, Proposition A.6 below.

Lemma A.4

Let φ:RnRm be a morphism of Graßmann algebras such that Rm is free. Then φ is injective. In particular, nm.

For the following lemma, we need the inclusion maps πj:n-1n with 1jn, defined by θkθk for k<j and θkθk+1 for kj, where we let (θk)1kn denote fixed coordinates of n and analogous for n-1. Unless said otherwise, we consider those corresponding to the standard bases of n and n-1, respectively.

Lemma A.5

Let φ:RnRm be a morphism of Graßmann algebras such that Rm is free. Then it is also free with respect to φπj:Rn-1Rm.

Proposition A.6

Assuming that every morphism ψ:RnRm, such that Rm is a free Rn-module with respect to ψ, is a submersion, the corresponding statement holds for all morphisms φ:Rn+1Rm.

Proof.

Let φ:n+1m be such that m is a free n+1-module. By Lemma A.5, it is also free with respect to the map φn+1:=φπn+1:nm which, by assumption, is a submersion. Therefore, there are coordinates of n and m, respectively, still denoted θ1,,θn and η1,,ηm, such that φn+1(θi)=ηi (see [5, Proposition 5.2.5]). Endowing the former coordinates with the original θn+1, φ obtains the form

φ(θ1)=η1,,φ(θn)=ηn,φ(θn+1)m.

We may assume that φ(θn+1)mη1,,ηn, for if not we can modify θn+1 by subtracting from it a suitable element of θ1,,θn. Denoting the associated morphism of superpoints still by φ, the differential at the single topological point 0 assumes the form

(dφ)0=(1n×n0(m-n)×n01×n(φ(θn+1)ηn+1|0)).

Observe that φ is a submersion if and only if the lower right submatrix is nonzero. This condition is satisfied by the following argument. The last line of (dφ)0 equals the differential (dφn+1)0 of the map φn+1:=φπ1πn, where the πj are defined with respect to the new coordinates. But φn+1 is a submersion by Lemma A.5 and the induction hypothesis for n=1. ∎

We now turn to the base case n=1. The following two lemmas provide equivalent characterisations of freeness in terms of ideal theory.

Lemma A.7

Let φ:R1RL be a morphism of Graßmann algebras. Then RL is free if and only if it has an R-basis of the form (v1,,v2L-1,φ(θ1)v1,,φ(θ1)v2L-1).

Proof.

This is shown analogous to the proof of Lemma A.5. ∎

Lemma A.8

Let μ(RL)1¯ and consider the ideal (μ) in RL generated by μ. Then RL admits an R-basis of the form (v1,,v2L-1,μv1,,μv2L-1) if and only if dimR(μ)2L-1. In this case, dimR(μ)=2L-1.

Proof.

If a basis as stated exists, then the vectors μvi(μ) are all linearly independent, thus the real dimension of (μ) is greater than or equal to their number, 2L-1.

Conversely, let (μw1,,μwd) denote a real basis of (μ) with d2L-1. We may endow this basis by vectors vj, 1jf, to a basis (v1,,vf,μw1,,μwd) of L. It follows that f+d=2L and thus f2L-1. Multiplying all vectors with μ and using μ2=0, one sees that the vectors (μv1,,μvf) span (μ), whence fdim(μ)=d2L-1, such that f=d=2L-1. In particular, (μv1,,μvd) is a basis of (μ). Endowed with the vectors vi, we obtain a basis of L as claimed. ∎

Our strategy for the base case will be to transform μ:=φ(θ1) to another odd element of some bigger Graßmann algebra with similar properties, and such that the associated ideal has the form treated by Esin and Koç in [7]. This is Proposition A.11 below. We now continue with two lemmas used in the proof of that algorithm. The first one is clear by Lemma A.8.

Lemma A.9

Let μ(RL)1¯. If dimR(μ)2L-1, then dimR(φ(μ))2L-1 for every Graßmann automorphism φ:RLRL.

Lemma A.10

Let μ(RL)1¯. Let r(RL)0¯ and consider μ^:=μ+ηL+1r(RL+1)1¯. If dimR(μ)2L-1 (with (μ) as an ideal in RL), then dimR(μ^)2L (as an ideal in RL+1).

Proof.

Writing elements of L+1 in the form v+ηL+1w with v,wL, we obtain

(μ^)={μv+ηL+1(rv-μw)v,wL}.

By assumption and Lemma A.8, L has a real basis (v1,,v2L-1,μv1,,μv2L-1). Let

V:=span(v1,,v2L-1)L.

There is a canonical map from VV to the space

{μv+ηL+1(rv-μw)v,wV}(μ^)

sending (v,w) to μv+ηL+1(rv-μw), which is clearly -linear and surjective. Assume μv+ηL+1(rv+μw)=0. Then, in particular, μv=0. By the definition of V, it follows that v=0. Then also μw=0 and, similarly, w=0. The aforementioned map is injective, and we conclude that dim(μ^)dim(VV)=2L. ∎

For the next proposition, we need the following notation. Let (ηi)i denote the coordinates of L corresponding to the standard basis of L. We write the expansion of μL with respect to these coordinates in the form

(A.1)μ=JCμJηJ,CμJ,ηJ=ηJ1ηJ|J|,

where the sum runs over all multiindices J of length |J| up to L.

Proposition A.11

Let μ(RL)1¯ be such that dimR(μ)2L-1. Then there are LL and μ(RL)1¯ such that the following conditions hold:

  1. There is a bijective correspondence

    λ:{JCμJ0}{JCμJ0}

    such that |J|=|λ(J)|.

  2. We have

    JCμJ0ηJ0.
  3. dim(μ)2L-1.

Proof.

We can successively built μ from μ as follows. Let j0 denote the smallest integer such that the generator ηj0 is contained in at least two monomials ηJ such that CμJ0. Let I denote one of k2 such multiindices. By assumption, there is r(L)0¯ such that ηI=ηj0r. Consider

μ^:=(μ-CμIηI)+(ηj0+ηL+1)CμIr.

By Lemma A.10, it satisfies dim(μ^)2L-1 with L=L+1. Consider next the automorphism

φ:LL

defined by ηiηi (i<L) and ηL(ηL-ηj0). Then the element φ(μ^) satisfies dim(φ(μ^))2L-1 by Lemma A.9. Moreover, the number of monomials containing ηj0 is reduced to k-1. It is also clear that the multiindex bijection required in the statement is satisfied.

Now start with μ replaced by φ(μ^) from the previous step, and repeat the construction until finally there is no generator ηj0 contained in more than one monomial. Since every step of the construction satisfies the first and third items in the statement, the same holds for the final result. As no two monomials therein share a common generator, the product over all is nonzero. ∎

Proof of (iii)  (iv) in Proposition A.3.

This remaining implication is proved by induction over n in R=n. It remains to show the base case as the inductive step was already established in Proposition A.6. Consider thus a morphism φ:1L such that L is free as an 1-module via φ. By Lemma A.7 and Lemma A.8, this property is characterised by dim(μ)2L-1 for μ:=φ(θ1). The algorithm of Proposition A.11 constructs another odd μ with a similar shape, but such that the product over all monomials with nonvanishing coefficients in (A.1) does not vanish. This is the case treated in [7]. In [7, Theorem 4], the dimension of (μ) is explicitly calculated to be

dim(μ)=2L-1(1-{JCμJ0}(1-21-|J|)).

Together with dim(μ)2L-1, this forces at least one of the multiindices J in the product to be of length |J|=1. But then the corresponding μ-multiindex λ-1(J) has also length 1. It follows that φ is a submersion. ∎

Acknowledgements

I would like to thank Jan Hakenberg for lending his algorithmic expertise and Alexander Alldridge and Dominik Ostermayr for making suggestions which helped to improve a previous version of the article. Moreover, I would like to thank the anonymous referee for helpful comments and suggestions.

References

[1] Bartocci C., Bruzzo U. and Hernández-Ruipérez D., The Geometry of Supermanifolds, Kluwer, Dordrecht, 1991. 10.1007/978-94-011-3504-7Search in Google Scholar

[2] Bartocci C., Bruzzo U., Hernández-Ruipérez D. and Pestov V., Quotient supermanifolds, Bull. Aust. Math. Soc. 58 (1998), 107–120. 10.1017/S0004972700032044Search in Google Scholar

[3] Belitsky A., Korchemsky G. and Sokatchev E., Are scattering amplitudes dual to super Wilson loops?, Nuclear Phys. B 855 (2012), 333–360. 10.1016/j.nuclphysb.2011.10.014Search in Google Scholar

[4] Bourbaki N., Commutative Algebra, Hermann, Paris, 1972. Search in Google Scholar

[5] Carmeli C., Caston L. and Fioresi R., Mathematical Foundations of Supersymmetry, European Mathematical Society, Zürich, 2011. 10.4171/097Search in Google Scholar

[6] Deligne P. and Freed D., Supersolutions, Quantum Fields and Strings: A Course for Mathematicians, American Mathematical Society, Providence, 1999. Search in Google Scholar

[7] Esin S. and Koç C., Annihilators of principal ideals in the exterior algebra, Taiwanese J. Math. 11 (2007), no. 4, 1019–1035. 10.11650/twjm/1500404799Search in Google Scholar

[8] Galaev A., Holonomy of supermanifolds, Abh. Math. Semin. Univ. Hambg. 79 (2009), 47–78. 10.1007/s12188-008-0015-7Search in Google Scholar

[9] Galaev A. and Leistner T., Recent developments in pseudo-Riemannian holonomy theory, Handbook of Pseudo-Riemannian Geometry and Supersymmetry, IRMA Lect. Math. Theor. Phys. 16, European Mathematical Society, Zürich (2010), 581–629. 10.4171/079-1/17Search in Google Scholar

[10] Gorbatsevich V., Onishchik A. and Vinberg E., Foundations of Lie Theory and Lie Transformation Groups, Springer, Berlin, 1997. Search in Google Scholar

[11] Groeger J., Holomorphic supercurves and supersymmetric sigma models, J. Math. Phys. 52 (2011), no. 12, Article ID 123505. 10.1063/1.3665710Search in Google Scholar

[12] Groeger J., Super Wilson loops and holonomy on supermanifolds, Commun. Math. 22 (2014), no. 2, 185–211. Search in Google Scholar

[13] Hanisch F., Variational Problems on Supermanifolds, Dissertation, Universität Potsdam, Potsdam, 2012. Search in Google Scholar

[14] Hélein F., An introduction to supermanifolds and supersymmetry, Systèmes Intégrables et Théorie des Champs Quantiques, Hermann, Paris (2009), 103–157. Search in Google Scholar

[15] Jantzen J., Representations of Algebraic Groups, Academic Press, Boston, 1987. Search in Google Scholar

[16] Joyce D., Compact Manifolds with Special Holonomy, Oxford University Press, Oxford, 2000. 10.1093/oso/9780198506010.001.0001Search in Google Scholar

[17] Khemar I., Supersymmetric harmonic maps into symmetric spaces, J. Geom. Phys. 57 (2007), no. 8, 1601–1630. 10.1016/j.geomphys.2007.01.005Search in Google Scholar

[18] Kobayashi S. and Nomizu K., Foundations of Differential Geometry, Vol. 1, Wiley Classics Libr., Wiley-Interscience, New York, 1996. Search in Google Scholar

[19] Leites D., Introduction to the theory of supermanifolds, Russian Math. Surveys 35 (1980), no. 1, 1–64. 10.1070/RM1980v035n01ABEH001545Search in Google Scholar

[20] Mac Lane S., Categories for the Working Mathematician, Springer, New York, 1998. Search in Google Scholar

[21] Mason L. and Skinner D., The complete planar S-matrix of N=4 SYM as a Wilson loop in twistor space, J. High Energy Phys. 2010 (2010), no. 12, Paper No. 018. 10.1007/JHEP12(2010)018Search in Google Scholar

[22] Masuoka A. and Zubkov A., Quotient sheaves of algebraic supergroups are superschemes, J. Algebra 348 (2011), no. 1, 135–170. 10.1016/j.jalgebra.2011.08.038Search in Google Scholar

[23] Merkulov S. and Schwachhöfer L., Classification of irreducible holonomies of torsion-free affine connections, Ann. of Math. (2) 150 (1999), no. 1, 77–149. 10.2307/121098Search in Google Scholar

[24] Molotkov V., Infinite-dimensional 2k-supermanifolds, ICTP preprint IC/84/183, ICTP, Trieste, 1984. Search in Google Scholar

[25] Sachse C., A categorical formulation of superalgebra and supergeometry, preprint 2008, http://arxiv.org/abs/0802.4067. Search in Google Scholar

[26] Santi A. and Spiro A., Super-Poincaré algebras, space-times, and supergravities (II), J. Math. Phys. 53 (2012), no. 3, Article ID 032505. 10.1063/1.3692323Search in Google Scholar

[27] Schmitt T., Regular sequences in 2-graded commutative algebra, J. Algebra 124 (1989), no. 1, 60–118. 10.1016/0021-8693(89)90153-1Search in Google Scholar

[28] Shvarts A., On the definition of superspace (in Russian), Teor. Mat. Fiz. 60 (1984), no. 1, 37–42. 10.1007/BF01018248Search in Google Scholar

[29] Varadarajan V., Supersymmetry for Mathematicians: An Introduction, American Mathematical Society, Providence, 2004. 10.1090/cln/011Search in Google Scholar

[30] Vistoli A., Grothendieck topologies, fibered categories and descent theory, Fundamental Algebraic Geometry, Math. Surveys Monogr. 123, American Mathematical Society, Providence (2005), 1–104. Search in Google Scholar

[31] Voronov A., Mappings of supermanifolds (in Russian), Teoret. Mat. Fiz. 60 (1984), no. 1, 43–48. 10.1007/BF01018249Search in Google Scholar

[32] Wu H., Holonomy groups of indefinite metrics, Pacific J. Math. 20 (1967), 351–382. 10.2140/pjm.1967.20.351Search in Google Scholar

[33] Zubkov A., Affine quotients of supergroups, Transform. Groups 14 (2009), no. 3, 713–145. 10.1007/s00031-009-9055-zSearch in Google Scholar

Received: 2015-7-16
Revised: 2016-1-19
Published Online: 2016-5-5
Published in Print: 2016-11-1

© 2016 by De Gruyter

Downloaded on 1.11.2025 from https://www.degruyterbrill.com/document/doi/10.1515/forum-2015-0139/html
Scroll to top button