Let kk be a field, put F=k((t))F=k((t)) and O=k[[t]]\mathcal O=k[[t]], and let GG be a . For a regular semisimple element γ\gamma of its g(F)\mathfrak g(F) whose Lie-algebra centralizer is a maximal torus (the Lie-algebra analogue of a ), the affine Springer fiber is the subspace

Mγ={gG(O)G(F)/G(O):Ad(g1)γg(O)}\mathcal M_\gamma= \left\{ gG(\mathcal O)\in G(F)/G(\mathcal O): \operatorname{Ad}(g^{-1})\gamma\in\mathfrak g(\mathcal O) \right\}

of the .

Interpretation and group version

It parametrizes integral GG-lattices preserved by γ\gamma.

There is also a group version in which γG(F)\gamma\in G(F) and the integrality condition is g1γgG(O)g^{-1}\gamma g\in G(\mathcal O).

Geometry

Affine Springer fibers are usually infinite-dimensional as ambient loci but have finite-dimensional reduced pieces under standard regularity hypotheses. They can be singular, reducible, and nonproper. A lattice in the loop of γ\gamma acts on them, often with a projective quotient.

Orbital integrals

Point counts and of affine Springer fibers encode . The places these local fibers inside a global family, allowing geometric comparison with endoscopic fibers in the proof of the .

References
  1. David Kazhdan and George Lusztig, “Fixed point varieties on affine flag manifolds,” Israel Journal of Mathematics 62 (1988), 129–168.
  2. Ngô Bảo Châu, “Survey on the fundamental lemma,” 2010, §§3–4. Author PDF.