TheoremComplete

Suslin's Rigidity Theorem

Suslin's rigidity theorem states that for algebraically closed fields, K-theory with finite coefficients depends only on the characteristic. This deep result connects algebraic K-theory over algebraically closed fields to topological K-theory and shows that, with finite coefficients, the transcendence degree is invisible.


Statement

Theorem6.5Suslin's Rigidity

Let kβ†ͺKk \hookrightarrow K be an extension of algebraically closed fields of the same characteristic. Then for any nβ‰₯0n \geq 0 and any mβ‰₯1m \geq 1:

Kn(k;Z/m)β†’β€…β€ŠβˆΌβ€…β€ŠKn(K;Z/m)K_n(k; \mathbb{Z}/m) \xrightarrow{\;\sim\;} K_n(K; \mathbb{Z}/m)

is an isomorphism. In particular, Kn(Fβ€Ύp;Z/m)β‰…Kn(kβ€Ύ;Z/m)K_n(\overline{\mathbb{F}}_p; \mathbb{Z}/m) \cong K_n(\overline{k}; \mathbb{Z}/m) for any algebraically closed field kk of characteristic pp.


Consequences

ExampleAlgebraic vs topological K-theory

Combining rigidity with the comparison to topological K-theory:

For k=Ck = \mathbb{C}: The map BGL(C)Ξ΄β†’BGL(C)BGL(\mathbb{C})^{\delta} \to BGL(\mathbb{C}) from the discrete to the continuous classifying space induces (by Suslin) an isomorphism with finite coefficients:

Kn(C;Z/m)β‰…Kntop(C;Z/m)=Ο€n(BU;Z/m)K_n(\mathbb{C}; \mathbb{Z}/m) \cong K_n^{\text{top}}(\mathbb{C}; \mathbb{Z}/m) = \pi_n(BU; \mathbb{Z}/m)

Since Ο€n(BU)={ZnΒ even0nΒ odd\pi_n(BU) = \begin{cases} \mathbb{Z} & n \text{ even} \\ 0 & n \text{ odd} \end{cases}, we get:

Kn(C;Z/m)β‰…{Z/mnΒ even0nΒ oddK_n(\mathbb{C}; \mathbb{Z}/m) \cong \begin{cases} \mathbb{Z}/m & n \text{ even} \\ 0 & n \text{ odd} \end{cases}

By rigidity, this holds for any algebraically closed field of characteristic 0:

Kn(Qβ€Ύ;Z/m)β‰…Kn(C;Z/m)β‰…Ο€n(BU;Z/m).K_n(\overline{\mathbb{Q}}; \mathbb{Z}/m) \cong K_n(\mathbb{C}; \mathbb{Z}/m) \cong \pi_n(BU; \mathbb{Z}/m).

ExamplePositive characteristic

For algebraically closed fields of characteristic p>0p > 0 and mm coprime to pp:

Kn(Fβ€Ύp;Z/m)β‰…Kn(kβ€Ύ;Z/m)K_n(\overline{\mathbb{F}}_p; \mathbb{Z}/m) \cong K_n(\overline{k}; \mathbb{Z}/m)

for any algebraically closed kk with char⁑(k)=p\operatorname{char}(k) = p. Since K2iβˆ’1(Fβ€Ύp)=lim→⁑K2iβˆ’1(Fpn)=lim→⁑Z/(pniβˆ’1)=Q/Z[prime-to-p]K_{2i-1}(\overline{\mathbb{F}}_p) = \varinjlim K_{2i-1}(\mathbb{F}_{p^n}) = \varinjlim \mathbb{Z}/(p^{ni} - 1) = \mathbb{Q}/\mathbb{Z}[\text{prime-to-}p], we get:

K2iβˆ’1(Fβ€Ύp;Z/m)β‰…Z/m(mΒ coprimeΒ toΒ p)K_{2i-1}(\overline{\mathbb{F}}_p; \mathbb{Z}/m) \cong \mathbb{Z}/m \quad (m \text{ coprime to } p)

K2i(Fβ€Ύp;Z/m)=0(mΒ coprimeΒ toΒ p)K_{2i}(\overline{\mathbb{F}}_p; \mathbb{Z}/m) = 0 \quad (m \text{ coprime to } p)

This matches the topological computation, confirming that algebraic K-theory of algebraically closed fields is "topological" with finite coefficients.


Proof sketch

Proof

The proof uses the theory of algebraic cycles and a norm argument.

Step 1: Reduction to extensions of transcendence degree 1. Write K=lim→⁑KΞ±K = \varinjlim K_\alpha as a directed union of subfields with tr.deg⁑(KΞ±/k)<∞\operatorname{tr.deg}(K_\alpha/k) < \infty. Since K-theory commutes with filtered colimits of rings, Kn(K;Z/m)=lim→⁑Kn(KΞ±;Z/m)K_n(K; \mathbb{Z}/m) = \varinjlim K_n(K_\alpha; \mathbb{Z}/m). It suffices to show Kn(k)β†’Kn(KΞ±)K_n(k) \to K_n(K_\alpha) is an isomorphism mod mm for each KΞ±K_\alpha, which reduces to the case tr.deg⁑(K/k)=1\operatorname{tr.deg}(K/k) = 1 by induction.

Step 2: The case of transcendence degree 1. Let K=k(C)‾K = \overline{k(C)} for a curve CC over kk. Choose a smooth projective model Cˉ\bar{C} over kk with function field k(C)k(C). We have:

Kn(k)β†’Kn(k(C))β†’Kn(K)K_n(k) \to K_n(k(C)) \to K_n(K)

For mm invertible in kk, the key is to show both maps are isomorphisms mod mm.

Step 3: Norm and transfer argument. For a closed point x∈CΛ‰x \in \bar{C} with residue field k(x)k(x) (which equals kk since kk is algebraically closed), the localization sequence gives:

β‹―β†’Kn+1(k(C);Z/m)β†’βˆ‚xKn(k;Z/m)β†’β‹―\cdots \to K_{n+1}(k(C); \mathbb{Z}/m) \xrightarrow{\partial_x} K_n(k; \mathbb{Z}/m) \to \cdots

The composite Kn(k;Z/m)β†’pullbackKn(k(C);Z/m)β†’normΒ viaΒ xKn(k;Z/m)K_n(k; \mathbb{Z}/m) \xrightarrow{\text{pullback}} K_n(k(C); \mathbb{Z}/m) \xrightarrow{\text{norm via } x} K_n(k; \mathbb{Z}/m) is multiplication by deg⁑(x)=1\deg(x) = 1, hence the identity.

Step 4: Injectivity. The pullback Kn(k;Z/m)β†’Kn(k(C);Z/m)K_n(k; \mathbb{Z}/m) \to K_n(k(C); \mathbb{Z}/m) has a left inverse (the norm via any rational point), so it is injective.

Step 5: Surjectivity. This is the harder direction. Suslin shows that every element of Kn(k(C);Z/m)K_n(k(C); \mathbb{Z}/m) can be "specialized" to an element of Kn(k;Z/m)K_n(k; \mathbb{Z}/m) by choosing appropriate specialization maps k(C)β†’kk(C) \to k. The key technical ingredient is the Suslin--Voevodsky theorem on relative algebraic cycles: the complex zp(C,βˆ™)z^p(C, \bullet) computing motivic cohomology satisfies a rigidity property when kk is algebraically closed.

Step 6: Passage to algebraic closure. Finally, Kn(k(C);Z/m)→Kn(K;Z/m)K_n(k(C); \mathbb{Z}/m) \to K_n(K; \mathbb{Z}/m) is an isomorphism because K=k(C)‾K = \overline{k(C)} and taking the algebraic closure does not change K-theory mod mm (by a Galois cohomology argument: Kn(F‾;Z/m)GF≅Kn(F;Z/m)K_n(\overline{F}; \mathbb{Z}/m)^{G_F} \cong K_n(F; \mathbb{Z}/m) is trivial when GFG_F acts trivially). ░\square

β– 

Related results

RemarkGabber's rigidity and generalizations

Gabber extended Suslin's rigidity to the following setting: for a Henselian local ring (R,m)(R, \mathfrak{m}) with residue field kk and mm invertible in RR:

Kn(R;Z/m)β†’β€…β€ŠβˆΌβ€…β€ŠKn(k;Z/m).K_n(R; \mathbb{Z}/m) \xrightarrow{\;\sim\;} K_n(k; \mathbb{Z}/m).

This Gabber rigidity theorem is the local analogue of Suslin's result. It implies:

  • KK-theory with finite coefficients is insensitive to Henselian thickenings.
  • For a smooth scheme XX over an algebraically closed field kk, Kn(X;Z/m)K_n(X; \mathbb{Z}/m) depends only on the etale homotopy type of XX (when mm is invertible in kk).

The combination of Suslin rigidity and Gabber rigidity shows that algebraic K-theory with finite coefficients is, in a precise sense, an etale-local invariant.