Let ζ:IJ\zeta:I\to J be a map of finite sets. It defines a diagonal map

Δζ:XJXI,(xj)jJ(xζ(i))iI.\Delta_\zeta:X^J\longrightarrow X^I, \qquad (x_j)_{j\in J}\longmapsto(x_{\zeta(i)})_{i\in I}.

Coalescence of shtuka legs is the canonical fusion isomorphism that identifies the pullback of the II-leg shtuka cohomology along Δζ\Delta_\zeta with the JJ-leg cohomology in which all legs in one fiber of ζ\zeta have merged.

Representation-theoretic label

If WW is a representation of the G^I\widehat G^I, restriction along

G^JG^I,(gj)(gζ(i))\widehat G^J\longrightarrow\widehat G^I, \qquad (g_j)\longmapsto(g_{\zeta(i)})

gives a representation WζW^\zeta of G^J\widehat G^J. Writing HI,W\mathcal H_{I,W} for the relevant cohomology sheaf, coalescence has the form

ΔζHI,WHJ,Wζ.\Delta_\zeta^*\mathcal H_{I,W} \simeq \mathcal H_{J,W^\zeta}.
Geometric origin

The isomorphism comes from the factorization or fusion structure of the Beilinson–Drinfeld and the . It remains meaningful on diagonals where modifications collide; it is more than the evident identification on the open locus of distinct legs.

Excursion-operator role

Starting with no legs, an invariant vector x:1Wx:\mathbf 1\to W creates several coincident legs. Coalescence separates or groups the representation labels, supplies independent Galois actions, and a covector ξ:W1\xi:W\to\mathbf 1 annihilates the legs. Functoriality of coalescence is essential for the relations among .

References
  1. Vincent Lafforgue, “Chtoucas pour les groupes réductifs et paramétrisation de Langlands globale,” Chapter 4. arXiv.
  2. Beilinson and Drinfeld, Quantization of Hitchin's Integrable System and Hecke Eigensheaves, factorization construction.