nLab K3 surface




A K3 surface is a Calabi-Yau variety of dimension 22 whose Picard variety is zero-dimensional. In other words, it is a complex algebraic surface with trivial canonical bundle (ω X= 2Ω X𝒪 X\omega_X=\wedge^2\Omega_X\simeq \mathcal{O}_X) and with H 1(X,𝒪 X)=0H^1(X, \mathcal{O}_X)=0.

The term “K3” is

in honor of Kummer, Kähler, Kodaira, and the beautiful K2 mountain in Kashmir

(Weil 79, p. 546)



Compact hyperkähler structure

Over the complex numbers K3 surfaces are all Kähler, and even hyperkähler.

The only known examples of compact hyperkähler manifolds are Hilbert schemes of points X [n+1]X^{[n+1]} (for nn \in \mathbb{N}) for XX either

  1. a K3-surface

  2. a 4-torus (in which case the compact hyperkähler manifolds is really the fiber of (𝕋 4) [n]𝕋 4(\mathbb{T}^4)^{[n]} \to \mathbb{T}^4)

(Beauville 83) and two exceptional examples (O’Grady 99, O’Grady 03 ), see Sawon 04, Sec. 5.3.




(integral cohomology of K3-surface)

The integral cohomology of a K3-surface XX is

H n(X,){ | n=0 0 | n=1 22 | n=2 0 | n=3 | n=4 H^n(X,\mathbb{Z}) \;\simeq\; \left\{ \array{ \mathbb{Z} &\vert& n = 0 \\ 0 &\vert& n = 1 \\ \mathbb{Z}^{22} &\vert& n = 2 \\ 0 &\vert& n = 3 \\ \mathbb{Z} &\vert& n = 4 } \right.

(e.g. Barth-Peters-Van den Ven 84, VIII Prop. 3.2)


(Betti numbers of a K3-surface)

The Hodge diamond? is completely determined (even in positive characteristic) and hence the Hodge-de Rham spectral sequence degenerates at E 1E_1. This also implies that the Betti numbers are completely determined as 1,0,22,0,11, 0, 22, 0, 1:

h 0,0 h 1,0 h 0,1 h 2,0 h 1,1 h 0,2 h 2,1 h 1,2 h 2,2= 1 0 0 1 20 1 0 0 1 \array{ && h^{0,0} \\ & h^{1,0} && h^{0,1} \\ h^{2,0} & & h^{1,1} & & h^{0,2} \\ & h^{2,1} & & h^{1,2} \\ && h^{2,2} } \;\;\;=\;\;\; \array{ && 1 \\ & 0 && 0 \\ 1 & & 20 & & 1 \\ & 0 & & 0 \\ && 1 }

(e.g. Barth-Peters-Van den Ven 84, VIII Prop. 3.3)



(K3-surface spans SU-bordism ring in degree 4)

The canonical degree-4 generator y 4Ω 4 SUy_4 \in \Omega^{SU}_4 in the SU-bordism ring (this Prop.) is represented by minus the class of any (non-torus) K3-surface:

Ω 4 SU[12][K3]. \Omega^{SU}_4 \;\simeq\; \mathbb{Z}\big[ \tfrac{1}{2}\big]\big\langle -[K3] \big\rangle \,.

(LLP 17, Lemma 1.5, Example 3.1, CLP 19, Theorem 13.5a, see at Calabi-Yau manifolds in SU-bordism theory)

Characteristic classes

We discuss some characteristic classes of (the tangent bundle of) K3, and their evaluation on (the fundamental class of) K3K3 (i.e. their integration over K3K3).

Of K3K3


(Euler characteristic of K3)

The Euler characteristic of K3 is 24:

χ 4[K3]=24. \chi_4[K3] \;=\; 24 \,.

(first Chern class of K3)

The first Chern class of K3 vanishes:

c 1(K3)=0. c_1(K3) \;=\; 0 \,.

(second Chern class of K3)

The second Chern class of K3 evaluates to 24:

c 2[K3]=24. c_2[K3] \;=\; 24 \,.

For every closed complex manifold the evaluation of the top degree Chern class equals the Euler characteristic. Hence the statement follows from Prop. .


(first Chern class of K3)

The first Pontryagin class of K3 evaluates to 48:

p 1[K3]=48. p_1[K3] \;=\; -48 \,.

(see also e.g. Duff-Liu-Minasian 95 (5.10))


For a complex manifold the first Pontryagin class is the following polynomial in the first Chern class and the second Chern class. By Prop. the first Chern class vanishes, and by Prop. the second Chern class evaluates to 24:

p 1[K3] =c 1c 1=0[K3]2c 2[K3]24 =48. \begin{aligned} p_1[K3] & =\; \underset{= 0}{\underbrace{c_1 \cup c_1}}[K3] - 2 \underset{24}{\underbrace{c_2[K3]}} \\ & = - 48 \end{aligned} \,.

Of K3×K3K3 \times K3

Now consider the Cartesian product space K3×K3K3 \times K3.

See also at C-field tadpole cancellation the section Integrality on K3×K3K3 \times K3.


(Euler characteristic of K3×\timesK3)

The Euler characteristic of K3×K3K3 \times K3 is 24 224^2:

χ 8[K3×K3]=24 2. \chi_8[K3\times K3] \;=\; 24^2 \,.

By the Whitney sum formula for the Euler class we have χ 8[K3×K3]=(χ 4[K3]) 2\chi_8[K3 \times K3] = (\chi_4[K3])^2. Hence the statement follows by Prop. .


(first Pontryagin class of K3×\timesK3)

The first Pontryagin class evaluated on K3×K3K3 \times K3 is:

p 1[K3×K3]=2×48 p_1[K3 \times K3] \;=\; - 2 \times 48

By the general formula for Pontryagin classes of product spaces we have

p 1(K3×K3) =p 0(K3)p 1(K3)+p 1(K3)p 0(K3) =2p 1(K3) \begin{aligned} p_1(K3 \times K3) & =\; p_0(K3) \smile p_1(K3) + p_1(K3) \smile p_0(K3) \\ & = 2 p_1(K3) \end{aligned}

With this, the statement follows by Prop. .

Of K3×X 4K3 \times X^4

Now consider the Cartesian product space K3×X 4K3 \times X^4 of K3 with some 4-manifold.


(Euler characteristic of K3×X 4\times X^4)

The Euler characteristic of K3×K3K3 \times K3 is 2424 times the Euler characteristic of X 4X^4:

χ 8[K3×X 4]=24χ 4[X 4]. \chi_8[K3\times X^4] \;=\; 24 \cdot \chi_4[X^4] \,.

By the Whitney sum formula for the Euler class we have χ 8[K3×X 4]=χ 4[K3]χ 4[X 4]\chi_8[K3 \times X^4] = \chi_4[K3] \cdot \chi_4[X^4]. Hence the statement follows by Prop. .


(first Pontryagin class of K3×X 4\times X^4)

The first Pontryagin class evaluated on K3×X 4K3 \times X^4 is:

p 1[K3×X 4]=p 1[X 4]48 p_1[K3 \times X^4] \;=\; p_1[X^4] - 48

By the general formula for Pontryagin classes of product spaces we have

p 1[K3×X 4] =p 0[K3]p 1[X 4]+p 1[K3]p 0[X 4] =p 1[X 4]+p 1[K3] \begin{aligned} p_1[K3 \times X^4] & =\; p_0[K3] \smile p_1[X^4] + p_1[K3] \smile p_0[X^4] \\ & = p_1[X^4] + p_1[K3] \end{aligned}

With this, the statement follows by Prop. .

Moduli of higher line bundles and deformation theory

In positive characteristic pp:

The Néron-Severi group of a K3 is a free abelian group

The formal Brauer group is

  • either the formal additive group, in which case it has height h=h = \infty, by definition;

  • or its height is 1h101 \leq h \leq 10, and every value may occur

(Artin 74), see also (Artin-Mazur 77, p. 5 (of 46))

moduli spaces of line n-bundles with connection on nn-dimensional XX

nnCalabi-Yau n-foldline n-bundlemoduli of line n-bundlesmoduli of flat/degree-0 n-bundlesArtin-Mazur formal group of deformation moduli of line n-bundlescomplex oriented cohomology theorymodular functor/self-dual higher gauge theory of higher dimensional Chern-Simons theory
n=0n = 0unit in structure sheafmultiplicative group/group of unitsformal multiplicative groupcomplex K-theory
n=1n = 1elliptic curveline bundlePicard group/Picard schemeJacobianformal Picard groupelliptic cohomology3d Chern-Simons theory/WZW model
n=2n = 2K3 surfaceline 2-bundleBrauer groupintermediate Jacobianformal Brauer groupK3 cohomology
n=3n = 3Calabi-Yau 3-foldline 3-bundleintermediate JacobianCY3 cohomology7d Chern-Simons theory/M5-brane
nnintermediate Jacobian

Relation to third stably framed bordism group

The third stable homotopy group of spheres (the third stable stem) is the cyclic group of order 24:

π 3 s /24 [h ] [1] \array{ \pi_3^s &\simeq& \mathbb{Z}/24 \\ [h_{\mathbb{H}}] &\leftrightarrow& [1] }

where the generator [1]/24[1] \in \mathbb{Z}/24 is represented by the quaternionic Hopf fibration S 7h S 4S^7 \overset{h_{\mathbb{H}}}{\longrightarrow} S^4.

Under the Pontrjagin-Thom isomorphism, identifying the stable homotopy groups of spheres with the bordism ring Ω fr\Omega^{fr}_\bullet of stably framed manifolds (see at MFr), this generator is represented by the 3-sphere (with its left-invariant framing induced from the identification with the Lie group SU(2) \simeq Sp(1) )

π 3 s Ω 3 fr [h ] [S 3]. \array{ \pi_3^s & \simeq & \Omega_3^{fr} \\ [h_{\mathbb{H}}] & \leftrightarrow & [S^3] \,. }

Moreover, the relation 24[S 3]02 4 [S^3] \,\simeq\, 0 is represented by the bordism which is the complement of 24 open balls inside the K3-manifold (Wang-Xu 10, Sec. 2.6).

Elliptic fibration

See at elliptically fibered K3-surface.

As a fiber space in string compactifications




Original sources:

  • Michael Artin, Supersingular K3 Surfaces, Annal. Sc. d, l’Éc Norm. Sup. 4e séries, T. 7, fasc. 4, 1974, pp. 543-568

  • Andre Weil, Final report on contract AF 18 (603)-57. In Scientific works. Collected papers. Vol. II (1951-1964). 1979.

Textbook accounts include

  • W. Barth, C. Peters, A. Van den Ven, chapter VII of Compact complex surfaces, Springer 1984

Lecture notes:

Discussion of the deformation theory of K3-surfaces (of their Picard schemes) is (see also at Artin-Mazur formal group) in

Systematic construction of Ricci flat Riemannian metrics on K3 orbifolds:

Elliptic fibrations

  • O. Lecacheux, Weierstrass Equations for the Elliptic Fibrations of a K3 Surface In: Balakrishnan J., Folsom A., Lalín M., Manes M. (eds.) Research Directions in Number Theory Association for Women in Mathematics Series, vol 19. Springer (2019) (doi:10.1007/978-3-030-19478-9_4)

  • Marie Bertin, Elliptic Fibrations on K3 surfaces, 2013 (pdf)

In string theory

In string theory, the KK-compactification of type IIA string theory/M-theory/F-theory on K3-fibers is supposed to exhibit te duality between M/F-theory and heterotic string theory, originally due to

Review includes

Further discussion includes

Specifically in relation to orbifold string theory:

Specifically in relation to the putative K-theory-classification of D-brane charge:

Specifically in M-theory on G2-manifolds:

Specifically in relation to Moonshine:

Specifically in relation to little string theory:

Last revised on March 31, 2024 at 09:16:33. See the history of this page for a list of all contributions to it.