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Frobenius Cokernel in Algebraic Geometry

Updated 14 July 2026
  • Frobenius cokernel is the cokernel of a Frobenius-induced map, capturing key exact sequences and duality in algebraic geometry.
  • It links positivity of vector bundles to geometrical features in projective spaces, complete intersections, and Fano varieties.
  • Its analogues extend to Witt vectors, invariant theory, and random-matrix models, underpinning universal cokernel distributions.

In algebraic geometry, arithmetic, and representation theory, the Frobenius cokernel denotes the cokernel of a Frobenius-induced map, but the concrete object depends on the ambient category. On a smooth projective variety in characteristic p>0p>0, it is the vector bundle BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X); on Witt vectors, it is the quotient W(R)/im(F)W(R)/\operatorname{im}(F); in invariant theory, it appears as R/RpR/R^p for the Frobenius map on a graded ring; and in recent random-matrix models, cokernels of polynomial endomorphisms over Zp\mathbb Z_p are treated as direct analogues of “Frobenius cokernels” (Carvajal-Rojas et al., 2021, Davis et al., 2014, Raedschelders et al., 2017, Cheong et al., 2023).

1. Basic definitions and exact sequences

Let XX be a smooth projective variety over an algebraically closed field kk of characteristic p>0p>0, and let

F:XX,F:OXOX, ffpF:X\to X,\qquad F^\sharp:\mathcal O_X\to\mathcal O_X,\ f\mapsto f^p

be the absolute Frobenius morphism. Since XX is reduced, there is a canonical injective map

BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)0

The Frobenius cokernel is defined by

BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)1

so that one has a short exact sequence of locally free sheaves

BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)2

Using Grothendieck duality for the finite morphism BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)3, one identifies

BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)4

so the dual of the Frobenius cokernel is the kernel of the Frobenius trace map (Mallory, 3 Oct 2025).

For the BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)5-th iterate BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)6, with BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)7, one writes

BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)8

and obtains the exact sequences

BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)9

and

W(R)/im(F)W(R)/\operatorname{im}(F)0

Thus the cokernel of the Frobenius endomorphism is exactly W(R)/im(F)W(R)/\operatorname{im}(F)1, while W(R)/im(F)W(R)/\operatorname{im}(F)2 is the Frobenius trace kernel. These sequences are locally split, and W(R)/im(F)W(R)/\operatorname{im}(F)3 is locally free of rank W(R)/im(F)W(R)/\operatorname{im}(F)4 when W(R)/im(F)W(R)/\operatorname{im}(F)5 (Carvajal-Rojas et al., 2021).

The same formal pattern recurs in higher degree. If

W(R)/im(F)W(R)/\operatorname{im}(F)6

then the Cartier isomorphism yields short exact sequences

W(R)/im(F)W(R)/\operatorname{im}(F)7

and W(R)/im(F)W(R)/\operatorname{im}(F)8 is the kernel of the higher Cartier operator W(R)/im(F)W(R)/\operatorname{im}(F)9 (Mallory, 3 Oct 2025).

2. Positivity, negativity, and the geometry they detect

A central theme is that positivity of the Frobenius trace kernel is equivalent to negativity of the Frobenius cokernel. If R/RpR/R^p0 is nef, then R/RpR/R^p1 is nef; if R/RpR/R^p2 is ample, then R/RpR/R^p3 is ample, so R/RpR/R^p4 is Fano. If R/RpR/R^p5 is globally generated and R/RpR/R^p6 is R/RpR/R^p7-split, then R/RpR/R^p8 is ample as well (Carvajal-Rojas et al., 2021).

These implications are not merely numerical. An ample Frobenius trace kernel rules out nontrivial smooth fibrations: if R/RpR/R^p9 is a fibration with smooth general fiber and Zp\mathbb Z_p0 is ample, then the general fibers are zero-dimensional, and all fibers are zero-dimensional if Zp\mathbb Z_p1 is flat. Blow-ups in codimension Zp\mathbb Z_p2 likewise destroy ampleness of the dual Frobenius trace bundle, because the restriction of Zp\mathbb Z_p3 to the exceptional divisor has a nontrivial trivial summand (Carvajal-Rojas et al., 2021).

The opposite positivity problem concerns the Frobenius cokernel itself rather than its dual. For a smooth projective variety over an Zp\mathbb Z_p4-finite field of characteristic Zp\mathbb Z_p5,

Zp\mathbb Z_p6

This equivalence is proved by analyzing the Katz–Sun filtration on Zp\mathbb Z_p7, whose graded pieces are truncated symmetric powers Zp\mathbb Z_p8. It gives a direct bridge between classical positivity of the cotangent bundle and Frobenius-based positivity (Mallory, 3 Oct 2025).

This suggests two complementary regimes. When Zp\mathbb Z_p9 is ample, the variety is forced toward Fano-type geometry; when XX0 is ample, the cotangent bundle is ample, so the geometry is controlled by strong negativity of the tangent bundle. The literature treats these as distinct but formally parallel manifestations of Frobenius-controlled positivity (Carvajal-Rojas et al., 2021, Mallory, 3 Oct 2025).

3. Projective space, quadrics, and classification results

Projective space is the basic model. On XX1,

XX2

Hence XX3 is ample, and the Frobenius cokernel is strongly negative. This behavior motivated the question whether ampleness of the Frobenius trace kernel characterizes projective space (Carvajal-Rojas et al., 2021).

In low dimension, the answer is affirmative. If XX4 is a smooth projective curve and XX5 is ample, then XX6. If XX7 is a smooth projective surface, then XX8 is ample if and only if XX9. For smooth projective threefolds, ampleness of kk0 forces kk1 to be a Fano threefold of Picard rank kk2 (Carvajal-Rojas et al., 2021).

The threefold classification was sharpened later. If kk3 is a smooth Fano threefold over an algebraically closed field of characteristic kk4, then

kk5

The key obstruction is geometric: if kk6 contains a smooth positive-dimensional subvariety kk7 with normal bundle kk8 such that kk9 is effective, then p>0p>00 is not ample. In particular, if p>0p>01 contains a smooth rational curve p>0p>02 with p>0p>03, then p>0p>04 is not ample. This excludes Fano threefolds containing lines or conics with respect to p>0p>05 (Mallory, 3 Oct 2025).

The naive projective-space characterization fails in higher dimension. Quadrics provide the basic counterexample: for p>0p>06, p>0p>07 is ample if and only if p>0p>08, and p>0p>09 is ample for all F:XX,F:OXOX, ffpF:X\to X,\qquad F^\sharp:\mathcal O_X\to\mathcal O_X,\ f\mapsto f^p0 (Carvajal-Rojas et al., 2021). More broadly, for F:XX,F:OXOX, ffpF:X\to X,\qquad F^\sharp:\mathcal O_X\to\mathcal O_X,\ f\mapsto f^p1 and quadric hypersurfaces, the full set of kernels of the higher Cartier operators does not characterize projective space (Mallory, 3 Oct 2025). This is the main correction to the optimistic expectation that Frobenius positivity should single out F:XX,F:OXOX, ffpF:X\to X,\qquad F^\sharp:\mathcal O_X\to\mathcal O_X,\ f\mapsto f^p2.

Complete intersections furnish another obstruction class. If F:XX,F:OXOX, ffpF:X\to X,\qquad F^\sharp:\mathcal O_X\to\mathcal O_X,\ f\mapsto f^p3 is a smooth complete intersection of degrees F:XX,F:OXOX, ffpF:X\to X,\qquad F^\sharp:\mathcal O_X\to\mathcal O_X,\ f\mapsto f^p4 with F:XX,F:OXOX, ffpF:X\to X,\qquad F^\sharp:\mathcal O_X\to\mathcal O_X,\ f\mapsto f^p5 and F:XX,F:OXOX, ffpF:X\to X,\qquad F^\sharp:\mathcal O_X\to\mathcal O_X,\ f\mapsto f^p6 or F:XX,F:OXOX, ffpF:X\to X,\qquad F^\sharp:\mathcal O_X\to\mathcal O_X,\ f\mapsto f^p7, then F:XX,F:OXOX, ffpF:X\to X,\qquad F^\sharp:\mathcal O_X\to\mathcal O_X,\ f\mapsto f^p8 is not ample. The argument uses the existence of lines in F:XX,F:OXOX, ffpF:X\to X,\qquad F^\sharp:\mathcal O_X\to\mathcal O_X,\ f\mapsto f^p9 together with the inequality XX0 for such lines (Mallory, 3 Oct 2025).

4. Witt vector Frobenius and its cokernel

For a commutative ring XX1 and a prime XX2, the XX3-typical Witt vector Frobenius

XX4

and its finite-level truncations

XX5

provide another classical setting for the Frobenius cokernel. Here

XX6

and vanishing of the cokernel is equivalent to surjectivity of the Frobenius map (Davis et al., 2014).

The structure of the kernel is governed by a descending sequence of ideals

XX7

An element XX8 occurs as the first component of an element in XX9 if and only if BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)00 (Davis et al., 2014).

The finite-level cokernel vanishes precisely under a ring-theoretic BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)01-root condition. Surjectivity of

BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)02

is equivalent to surjectivity of the BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)03-th power map on each quotient BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)04. At infinite level, surjectivity is stricter: BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)05 Equivalently, full surjectivity is characterized by finite-level surjectivity together with Teichmüller density, or by surjectivity of the BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)06-th power map on BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)07 together with the same completeness condition (Davis et al., 2014).

Examples show that finite and infinite behavior diverge sharply. For BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)08, finite-level surjectivity fails, so the Frobenius cokernel is already nonzero at finite levels. For the ring of integers BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)09 in an algebraic closure of BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)10, finite-level Frobenius is surjective for all BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)11, but spherical completeness fails, so the infinite-level cokernel is nonzero. For a spherically complete valuation ring of the kind constructed by Poonen, the infinite Witt Frobenius is surjective (Davis et al., 2014).

In the mixed-characteristic direction, the finite-level vanishing of the Frobenius cokernel is described as the integral perfectoid condition of Scholze, repackaged in Witt-vector language. The same condition is stable under certain integral extensions and underlies the almost-purity statement proved there (Davis et al., 2014).

5. Graded rings, invariant theory, and homogeneous varieties

In invariant theory, the Frobenius cokernel appears module-theoretically. Let

BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)12

be the homogeneous coordinate ring of the Grassmannian BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)13, with BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)14 and BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)15. The Frobenius on BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)16 is

BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)17

with image BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)18. Viewing BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)19 as an BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)20-module, the Frobenius cokernel is

BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)21

The decomposition of BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)22 as a graded BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)23-module therefore controls the structure of the cokernel (Raedschelders et al., 2017).

The indecomposable Frobenius summands are expressed in terms of modules of covariants BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)24 and certain indecomposable Cohen–Macaulay modules BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)25. Forgetting degrees, the Frobenius summands of BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)26 lie among

BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)27

and all of these appear when BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)28. This is the paper’s explicit instance of BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)29-uniformity: for sufficiently large BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)30, the set of indecomposable summands does not depend on BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)31, although multiplicities and grading shifts still vary (Raedschelders et al., 2017).

Geometrically, the same analysis yields a decomposition of the Frobenius pushforward BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)32 into indecomposable homogeneous bundles. Up to multiplicity, the summands are twists of BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)33, the bundles BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)34, and twists of BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)35. This Frobenius pushforward is a tilting bundle only for BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)36 and BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)37; otherwise it is not tilting (Raedschelders et al., 2017).

The module-theoretic consequence for the cokernel is that the Frobenius cokernel is far from projective in general. The nonfree indecomposable summands BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)38 contribute to the nonfree part of BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)39 over BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)40, and hence to the nonfree part of the Frobenius cokernel. The same summands are then used to construct a noncommutative resolution BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)41 of finite global dimension for a suitable direct sum BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)42 of Frobenius summands (Raedschelders et al., 2017).

6. Random and cohomological analogues

Recent random-matrix work treats polynomial cokernels over BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)43 as direct analogues of Frobenius cokernels. For

BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)44

with BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)45 fixed and BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)46 random, and for a non-constant monic polynomial BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)47, the central object is

BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)48

More naturally, one equips it with the structure of an BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)49-module for

BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)50

via letting the image of BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)51 act by BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)52. The key linearization is

BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)53

which replaces a polynomial in BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)54 by an BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)55-linear map. The paper proves exact finite-BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)56 formulas for the distribution of BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)57 when BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)58 is Haar-random, establishes universality for a broader concentrated-residue class, and derives a Cohen–Lenstra style limit law in the non-concentrated regime (Cheong et al., 2023).

This random-matrix perspective is explicitly presented as directly analogous to “Frobenius cokernels.” Conceptually, one studies an endomorphism BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)59 of a BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)60-adic module and the modules

BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)61

while the random model replaces BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)62 by BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)63. The resulting distribution depends on BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)64 and on the factorization of BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)65, and in the squarefree case becomes a direct generalization of the Cohen–Lenstra measure to modules over BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)66 (Cheong et al., 2023).

A complementary universality principle holds for random integral matrices. For an BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)67 random integral matrix BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)68 with independent entries from a very broad class of distributions, the limiting probability that BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)69 is

BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)70

This is a Cohen–Lenstra-type law, and it agrees with the distribution defined by the Haar model on BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)71. The paper interprets this as support for the principle that random endomorphisms modelling Frobenius produce canonical cokernel distributions independent of microscopic details of the entry distribution (Nguyen et al., 2018).

Representation-theoretic work on Frobenius kernels gives a different, but related, analogue. For the BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)72-th Frobenius kernels BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)73, the cohomology ring BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)74 is Cohen–Macaulay, and its maximal ideal spectrum is homeomorphic to BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)75. That work is about kernels of Frobenius rather than cokernels, but it is formulated so that explicit knowledge of BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)76 constrains possible kernels and cokernels of Frobenius-induced maps on cohomology (Ngo, 2012).

Across these settings, the Frobenius cokernel is best viewed not as a single invariant but as a family of formally parallel constructions. In geometry it is a vector bundle attached to BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)77; in Witt theory it measures the failure of Frobenius surjectivity on BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)78; in invariant theory it records the nonfree part of BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)79 over BX:=coker(OXFOX)\mathcal B_X:=\operatorname{coker}(\mathcal O_X\to F_*\mathcal O_X)80; and in random-matrix models it becomes a probabilistic proxy for cokernels of polynomial functions of Frobenius-like endomorphisms (Carvajal-Rojas et al., 2021, Davis et al., 2014, Raedschelders et al., 2017, Cheong et al., 2023).

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