Hyperkähler manifold: Difference between revisions

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==Examples==
==Examples==
For any integer <math>n \ge 1</math>, the space <math>\mathbb{H}^n</math> of <math>n</math>-tuples of [[quaternion]]s endowed with the [[Riemannian_manifold#Euclidean_space|flat Euclidean metric]] is a hyperkähler manifold. The first non-trivial example discovered is the [[Eguchi–Hanson space|Eguchi–Hanson metric]] on the cotangent bundle <math>T^*S^2</math> of the [[Sphere|two-sphere]]. It was also independently discovered by [[Eugenio Calabi]], who showed the more general statement that cotangent bundle <math>T^*\mathbb{CP}^n</math> of any [[complex projective space]] has a [[Riemannian_manifold#Geodesic_completeness|complete]] hyperkähler metric.<ref name="calabi" /> More generally, Birte Feix and Dmitry Kaledin showed that the cotangent bundle of any [[Kähler manifold]] has a hyperkähler structure on a [[Neighbourhood (mathematics)|neighbourhood]] of its [[Vector_bundle#Sections_and_locally_free_sheaves|zero section]], although it is generally incomplete.<ref>Feix, B. Hyperkähler metrics on cotangent bundles. J. Reine Angew. Math. 532 (2001), 33–46.</ref><ref>Kaledin, D. A canonical hyperkähler metric on the total space of a cotangent bundle. Quaternionic structures in mathematics and physics (Rome, 1999), 195–230, Univ. Studi Roma "La Sapienza", Rome, 1999.</ref>
For any integer <math>n \ge 1</math>, the space <math>\mathbb{H}^n</math> of <math>n</math>-tuples of [[quaternion]]s endowed with the [[Riemannian_manifold#Euclidean_space|flat Euclidean metric]] is a hyperkähler manifold. The first non-trivial example discovered is the [[Eguchi–Hanson space|Eguchi–Hanson metric]] on the cotangent bundle <math>T^*S^2</math> of the [[Sphere|two-sphere]]. It was also independently discovered by [[Eugenio Calabi]], who showed the more general statement that cotangent bundle <math>T^*\mathbb{CP}^n</math> of any [[complex projective space]] has a [[Riemannian_manifold#Geodesic_completeness|complete]] hyperkähler metric.<ref name="calabi" /> More generally, Birte Feix and Dmitry Kaledin showed that the cotangent bundle of any [[Kähler manifold]] has a hyperkähler structure on a [[Neighbourhood (mathematics)|neighbourhood]] of its [[Vector_bundle#Sections_and_locally_free_sheaves|zero section]], although it is generally incomplete.<ref>{{cite journal |last=Feix |first=B. |title=Hyperkähler metrics on cotangent bundles |journal=J. Reine Angew. Math. |volume=532 |year=2001 |pages=33–46 |doi=10.1515/crll.2001.017 }}</ref><ref>{{cite book |last=Kaledin |first=D. |chapter=A canonical hyperkähler metric on the total space of a cotangent bundle |title=Quaternionic structures in mathematics and physics (Rome, 1999) |pages=195–230 |publisher=Univ. Studi Roma "La Sapienza" |location=Rome |year=1999 |doi=10.1142/9789812810038_0010 }}</ref>


Due to [[Kunihiko Kodaira]]'s classification of complex surfaces, we know that any [[compact space|compact]] hyperkähler 4-manifold is either a [[K3 surface]] or a compact [[Torus#n-dimensional torus|torus]] <math>T^4</math>. (Every [[Calabi–Yau manifold]] in 4 (real) dimensions is a hyperkähler manifold, because {{math|[[Special unitary group|SU(2)]]}} is isomorphic to {{math|[[Symplectic group|Sp(1)]]}}.)
Due to [[Kunihiko Kodaira]]'s classification of complex surfaces, we know that any [[compact space|compact]] hyperkähler 4-manifold is either a [[K3 surface]] or a compact [[Torus#n-dimensional torus|torus]] <math>T^4</math>. (Every [[Calabi–Yau manifold]] in 4 (real) dimensions is a hyperkähler manifold, because {{math|[[Special unitary group|SU(2)]]}} is isomorphic to {{math|[[Symplectic group|Sp(1)]]}}.)


As was discovered by Beauville,<ref name="beauville">Beauville, A. Variétés Kähleriennes dont la première classe de Chern est nulle. J. Differential Geom. 18 (1983), no. 4, 755–782 (1984).</ref> the [[Hilbert scheme]] of {{math|k}} points on a compact hyperkähler 4-manifold is a hyperkähler manifold of dimension {{math|4k}}. This gives rise to two series of compact examples: Hilbert schemes of points on a K3 surface and [[Hilbert scheme|generalized Kummer varieties]].
As was shown by Beauville, the [[Hilbert scheme]] of {{math|k}} points on a compact hyperkähler 4-manifold is a hyperkähler manifold of dimension {{math|4k}}.<ref name="beauville">{{cite journal |last=Beauville |first=A. |title=Variétés Kähleriennes dont la première classe de Chern est nulle |journal=J. Differential Geom. |volume=18 |year=1983 |issue=4 |pages=755–782 |doi= }}</ref> This gives rise to two series of compact examples: Hilbert schemes of points on a K3 surface and [[Hilbert scheme|generalized Kummer varieties]].


Non-compact, complete, hyperkähler 4-manifolds which are asymptotic to {{math|'''H'''/''G''}}, where {{math|'''H'''}} denotes the [[quaternion]]s and {{math|''G''}} is a finite [[subgroup]] of {{math|Sp(1)}}, are known as [[asymptotically locally Euclidean]], or ALE, spaces. These spaces, and various generalizations involving different asymptotic behaviors, are studied in [[physics]] under the name [[gravitational instanton]]s. The [[Gibbons–Hawking ansatz]] gives examples invariant under a circle action.
Non-compact, complete, hyperkähler 4-manifolds which are asymptotic to {{math|'''H'''/''G''}}, where {{math|'''H'''}} denotes the [[quaternion]]s and {{math|''G''}} is a finite [[subgroup]] of {{math|Sp(1)}}, are known as [[asymptotically locally Euclidean]], or ALE, spaces. These spaces, and various generalizations involving different asymptotic behaviors, are studied in [[physics]] under the name [[gravitational instanton]]s. The [[Gibbons–Hawking ansatz]] gives examples invariant under a circle action.


Many examples of noncompact hyperkähler manifolds arise as moduli spaces of solutions to certain gauge theory equations which arise from the dimensional reduction of the anti-self dual [[Yang–Mills theory|Yang–Mills equations]]: instanton moduli spaces,<ref>Maciocia, A. Metrics on the moduli spaces of instantons over Euclidean 4-space.
Many examples of noncompact hyperkähler manifolds arise as moduli spaces of solutions to certain gauge theory equations which arise from the dimensional reduction of the anti-self dual [[Yang–Mills theory|Yang–Mills equations]]: instanton moduli spaces,<ref>{{cite journal |last=Maciocia |first=A. |title=Metrics on the moduli spaces of instantons over Euclidean 4-space |journal=Comm. Math. Phys. |volume=135 |year=1991 |issue=3 |pages=467–482 |doi=10.1007/BF02104116 }}</ref> [[monopole moduli space]]s,<ref>{{cite book |last=Atiyah |first=M. |last2=Hitchin |first2=N. |title=The geometry and dynamics of magnetic monopoles |series=M. B. Porter Lectures |publisher=Princeton University Press |location=Princeton, NJ |year=1988 |isbn=0-691-08480-7 }}</ref> spaces of solutions to [[Nigel Hitchin]]'s [[Hitchin's equations|self-duality equations]] on [[Riemann surface]]s,<ref>{{cite journal |last=Hitchin |first=N. |title=The self-duality equations on a Riemann surface |journal=Proc. London Math. Soc. |series=s3 |volume=55 |year=1987 |issue=1 |pages=59–126 |doi=10.1112/plms/s3-55.1.59 }}</ref> space of solutions to [[Nahm equations]]. Another class of examples are the [[Hiraku Nakajima|Nakajima]] [[Quiver (mathematics)|quiver]] varieties,<ref>{{cite journal |last=Nakajima |first=H. |title=Instantons on ALE spaces, quiver varieties, and Kac-Moody algebras |journal=Duke Math. J. |volume=76 |year=1994 |issue=2 |pages=365–416 |doi=10.1215/S0012-7094-94-07613-8 }}</ref> which are of great importance in representation theory.
Comm. Math. Phys. 135 (1991), no. 3, 467–482.</ref> [[monopole moduli space]]s,<ref>Atiyah, M.; Hitchin, N. The geometry and dynamics of magnetic monopoles. M. B. Porter Lectures. Princeton University Press, Princeton, NJ, 1988.</ref> spaces of solutions to [[Nigel Hitchin]]'s [[Hitchin's equations|self-duality equations]] on [[Riemann surface]]s,<ref>Hitchin, N. The self-duality equations on a Riemann surface. Proc. London Math. Soc. (3) 55 (1987), no. 1, 59–126.</ref> space of solutions to [[Nahm equations]]. Another class of examples are the [[Hiraku Nakajima|Nakajima]] [[Quiver (mathematics)|quiver]] varieties,<ref>Nakajima, H. Instantons on ALE spaces, quiver varieties, and Kac-Moody algebras. Duke Math. J. 76 (1994), no. 2, 365–416.</ref> which are of great importance in representation theory.


==Cohomology==
==Cohomology==

Latest revision as of 19:43, 22 June 2025

In differential geometry, a hyperkähler manifold is a Riemannian manifold (M,g) endowed with three integrable almost complex structures I,J,K that are Kähler with respect to the Riemannian metric g and satisfy the quaternionic relations I2=J2=K2=IJK=1. In particular, it is a hypercomplex manifold. All hyperkähler manifolds are Ricci-flat and are thus Calabi–Yau manifolds.Template:Efn

Hyperkähler manifolds were first given this name by Eugenio Calabi in 1979.[1]

Early history

Marcel Berger's 1955 paper[2] on the classification of Riemannian holonomy groups first raised the issue of the existence of non-symmetric manifolds with holonomy Sp(n)·Sp(1). Interesting results were proved in the mid-1960s in pioneering work by Edmond Bonan[3] and Kraines[4] who have independently proven that any such manifold admits a parallel 4-form Ω. Bonan's later results[5] include a Lefschetz-type result: wedging with this powers of this 4-form induces isomorphisms Ωnk2kT*M=4n2kT*M.

Equivalent definition in terms of holonomy

Equivalently, a hyperkähler manifold is a Riemannian manifold (M,g) of dimension 4n whose holonomy group is contained in the [[Symplectic_group#Sp(n)|compact symplectic group Template:Math]].[1]

Indeed, if (M,g,I,J,K) is a hyperkähler manifold, then the tangent space Template:Math is a quaternionic vector space for each point Template:Math of Template:Math, i.e. it is isomorphic to n for some integer n, where is the algebra of quaternions. The [[Symplectic_group#Sp(n)|compact symplectic group Template:Math]] can be considered as the group of orthogonal transformations of n which are linear with respect to Template:Math, Template:Math and Template:Math. From this, it follows that the holonomy group of the Riemannian manifold (M,g) is contained in Template:Math. Conversely, if the holonomy group of a Riemannian manifold (M,g) of dimension 4n is contained in Template:Math, choose complex structures Template:Math, Template:Math and Template:Math on Template:Math which make Template:Math into a quaternionic vector space. Parallel transport of these complex structures gives the required complex structures I,J,K on Template:Math making (M,g,I,J,K) into a hyperkähler manifold.

Two-sphere of complex structures

Every hyperkähler manifold (M,g,I,J,K) has a 2-sphere of complex structures with respect to which the metric g is Kähler. Indeed, for any real numbers a,b,c such that

a2+b2+c2=1

the linear combination

aI+bJ+cK

is a complex structures that is Kähler with respect to g. If ωI,ωJ,ωK denotes the Kähler forms of (g,I),(g,J),(g,K), respectively, then the Kähler form of aI+bJ+cK is

aωI+bωJ+cωK.

Holomorphic symplectic form

A hyperkähler manifold (M,g,I,J,K), considered as a complex manifold (M,I), is holomorphically symplectic (equipped with a holomorphic, non-degenerate, closed 2-form). More precisely, if ωI,ωJ,ωK denotes the Kähler forms of (g,I),(g,J),(g,K), respectively, then

Ω:=ωJ+iωK

is holomorphic symplectic with respect to I.

Conversely, Shing-Tung Yau's proof of the Calabi conjecture implies that a compact, Kähler, holomorphically symplectic manifold (M,I,Ω) is always equipped with a compatible hyperkähler metric.[6] Such a metric is unique in a given Kähler class. Compact hyperkähler manifolds have been extensively studied using techniques from algebraic geometry, sometimes under the name holomorphically symplectic manifolds. The holonomy group of any Calabi–Yau metric on a simply connected compact holomorphically symplectic manifold of complex dimension 2n with H2,0(M)=1 is exactly Template:Math; and if the simply connected Calabi–Yau manifold instead has H2,0(M)2, it is just the Riemannian product of lower-dimensional hyperkähler manifolds. This fact immediately follows from the Bochner formula for holomorphic forms on a Kähler manifold, together the Berger classification of holonomy groups; ironically, it is often attributed to Bogomolov, who incorrectly went on to claim in the same paper that compact hyperkähler manifolds actually do not exist!

Examples

For any integer n1, the space n of n-tuples of quaternions endowed with the flat Euclidean metric is a hyperkähler manifold. The first non-trivial example discovered is the Eguchi–Hanson metric on the cotangent bundle T*S2 of the two-sphere. It was also independently discovered by Eugenio Calabi, who showed the more general statement that cotangent bundle T*n of any complex projective space has a complete hyperkähler metric.[1] More generally, Birte Feix and Dmitry Kaledin showed that the cotangent bundle of any Kähler manifold has a hyperkähler structure on a neighbourhood of its zero section, although it is generally incomplete.[7][8]

Due to Kunihiko Kodaira's classification of complex surfaces, we know that any compact hyperkähler 4-manifold is either a K3 surface or a compact torus T4. (Every Calabi–Yau manifold in 4 (real) dimensions is a hyperkähler manifold, because Template:Math is isomorphic to Template:Math.)

As was shown by Beauville, the Hilbert scheme of Template:Math points on a compact hyperkähler 4-manifold is a hyperkähler manifold of dimension Template:Math.[6] This gives rise to two series of compact examples: Hilbert schemes of points on a K3 surface and generalized Kummer varieties.

Non-compact, complete, hyperkähler 4-manifolds which are asymptotic to Template:Math, where Template:Math denotes the quaternions and Template:Math is a finite subgroup of Template:Math, are known as asymptotically locally Euclidean, or ALE, spaces. These spaces, and various generalizations involving different asymptotic behaviors, are studied in physics under the name gravitational instantons. The Gibbons–Hawking ansatz gives examples invariant under a circle action.

Many examples of noncompact hyperkähler manifolds arise as moduli spaces of solutions to certain gauge theory equations which arise from the dimensional reduction of the anti-self dual Yang–Mills equations: instanton moduli spaces,[9] monopole moduli spaces,[10] spaces of solutions to Nigel Hitchin's self-duality equations on Riemann surfaces,[11] space of solutions to Nahm equations. Another class of examples are the Nakajima quiver varieties,[12] which are of great importance in representation theory.

Cohomology

Template:Harvtxt show that the cohomology of any compact hyperkähler manifold embeds into the cohomology of a torus, in a way that preserves the Hodge structure.

Notes

Template:Notelist

See also

References

Template:Reflist

Template:String theory topics

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