Definition

Let EME\to M be a rank-rr Hermitian with structure group SU(r)SU(r) over a closed oriented four-manifold, and let AA be a with curvature FAF_A. Its instanton number is

k(E)=18π2Mtr(FAFA)=c2(E),[M]Z,k(E)= -\frac{1}{8\pi^2}\int_M\operatorname{tr}(F_A\wedge F_A) =\langle c_2(E),[M]\rangle\in\mathbb Z,

using the defining representation and the stated sign convention. It is the of EE, so it is independent of AA. When AA is a , this integer labels its topological sector but is not additional connection data.

Chern–Weil independence

The four-form

18π2tr(FAFA)-\frac{1}{8\pi^2}\operatorname{tr}(F_A\wedge F_A)

represents c2(E)c_2(E) because c1(E)=0c_1(E)=0 for an SU(r)SU(r)-bundle. Replacing AA by another connection changes this form by an exact , whose integral over closed MM vanishes. Thus the number depends on the bundle and orientation, not on the chosen representative connection.

For a general compact structure group, an “instanton number” requires choosing an invariant quadratic form normalized to represent an integral . The resulting charge need not use the displayed trace normalization.

Energy and self-duality

In four dimensions, decompose FA=FA++FAF_A=F_A^++F_A^- using the Hodge star. The Chern–Weil integral is proportional to

FAL22FA+L22\|F_A^-\|_{L^2}^2-\|F_A^+\|_{L^2}^2

with the present orientation and trace conventions. The Yang–Mills energy is the corresponding sum. Hence self-dual or saturate a topological proportional to k(E)|k(E)| Donaldson–Kronheimer, §2.1.

Reversing the orientation interchanges self-duality and anti-self-duality and changes the sign of the integral, while leaving its unchanged.

Related characteristic numbers

For a principal SU(2)SU(2)-bundle PP, the adjoint real rank-three bundle satisfies

p1(adP)=4c2(E)p_1(\operatorname{ad}P)=-4c_2(E)

under standard conventions. Thus “Pontryagin charge” may encode the same sector but with a sign or factor of four. It is not included as an alias because the normalization is not identical to the instanton number displayed here.

References
  1. Simon K. Donaldson and Peter B. Kronheimer, The Geometry of Four-Manifolds, Oxford University Press, 1990. DOI record. Relevant: §2.1, characteristic number, curvature decomposition, and the instanton energy bound.
  2. Daniel S. Freed and Karen K. Uhlenbeck, Instantons and Four-Manifolds, 2nd ed., Springer, 1991. DOI record. Relevant: chapter 2, Chern–Weil normalization and topological charge.