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>0, it is the vector bundle BX:=coker(OX→F∗OX); on Witt vectors, it is the quotient W(R)/im(F); in invariant theory, it appears as R/Rp for the Frobenius map on a graded ring; and in recent random-matrix models, cokernels of polynomial endomorphisms over Zp 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 X be a smooth projective variety over an algebraically closed field k of characteristic p>0, and let
F:X→X,F♯:OX→OX,f↦fp
be the absolute Frobenius morphism. Since X is reduced, there is a canonical injective map
BX:=coker(OX→F∗OX)0
The Frobenius cokernel is defined by
BX:=coker(OX→F∗OX)1
so that one has a short exact sequence of locally free sheaves
BX:=coker(OX→F∗OX)2
Using Grothendieck duality for the finite morphism BX:=coker(OX→F∗OX)3, one identifies
BX:=coker(OX→F∗OX)4
so the dual of the Frobenius cokernel is the kernel of the Frobenius trace map (Mallory, 3 Oct 2025).
For the BX:=coker(OX→F∗OX)5-th iterate BX:=coker(OX→F∗OX)6, with BX:=coker(OX→F∗OX)7, one writes
BX:=coker(OX→F∗OX)8
and obtains the exact sequences
BX:=coker(OX→F∗OX)9
and
W(R)/im(F)0
Thus the cokernel of the Frobenius endomorphism is exactly W(R)/im(F)1, while W(R)/im(F)2 is the Frobenius trace kernel. These sequences are locally split, and W(R)/im(F)3 is locally free of rank W(R)/im(F)4 when W(R)/im(F)5 (Carvajal-Rojas et al., 2021).
The same formal pattern recurs in higher degree. If
W(R)/im(F)6
then the Cartier isomorphism yields short exact sequences
W(R)/im(F)7
and W(R)/im(F)8 is the kernel of the higher Cartier operator W(R)/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/Rp0 is nef, then R/Rp1 is nef; if R/Rp2 is ample, then R/Rp3 is ample, so R/Rp4 is Fano. If R/Rp5 is globally generated and R/Rp6 is R/Rp7-split, then R/Rp8 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/Rp9 is a fibration with smooth general fiber and Zp0 is ample, then the general fibers are zero-dimensional, and all fibers are zero-dimensional if Zp1 is flat. Blow-ups in codimension Zp2 likewise destroy ampleness of the dual Frobenius trace bundle, because the restriction of Zp3 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 Zp4-finite field of characteristic Zp5,
Zp6
This equivalence is proved by analyzing the Katz–Sun filtration on Zp7, whose graded pieces are truncated symmetric powers Zp8. 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 Zp9 is ample, the variety is forced toward Fano-type geometry; when X0 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 X1,
X2
Hence X3 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 X4 is a smooth projective curve and X5 is ample, then X6. If X7 is a smooth projective surface, then X8 is ample if and only if X9. For smooth projective threefolds, ampleness of k0 forces k1 to be a Fano threefold of Picard rank k2 (Carvajal-Rojas et al., 2021).
The threefold classification was sharpened later. If k3 is a smooth Fano threefold over an algebraically closed field of characteristic k4, then
k5
The key obstruction is geometric: if k6 contains a smooth positive-dimensional subvariety k7 with normal bundle k8 such that k9 is effective, then p>00 is not ample. In particular, if p>01 contains a smooth rational curve p>02 with p>03, then p>04 is not ample. This excludes Fano threefolds containing lines or conics with respect to p>05 (Mallory, 3 Oct 2025).
The naive projective-space characterization fails in higher dimension. Quadrics provide the basic counterexample: for p>06, p>07 is ample if and only if p>08, and p>09 is ample for all F:X→X,F♯:OX→OX,f↦fp0 (Carvajal-Rojas et al., 2021). More broadly, for F:X→X,F♯:OX→OX,f↦fp1 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:X→X,F♯:OX→OX,f↦fp2.
Complete intersections furnish another obstruction class. If F:X→X,F♯:OX→OX,f↦fp3 is a smooth complete intersection of degrees F:X→X,F♯:OX→OX,f↦fp4 with F:X→X,F♯:OX→OX,f↦fp5 and F:X→X,F♯:OX→OX,f↦fp6 or F:X→X,F♯:OX→OX,f↦fp7, then F:X→X,F♯:OX→OX,f↦fp8 is not ample. The argument uses the existence of lines in F:X→X,F♯:OX→OX,f↦fp9 together with the inequality X0 for such lines (Mallory, 3 Oct 2025).
4. Witt vector Frobenius and its cokernel
For a commutative ring X1 and a primeX2, the X3-typical Witt vector Frobenius
X4
and its finite-level truncations
X5
provide another classical setting for the Frobenius cokernel. Here
X6
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
X7
An element X8 occurs as the first component of an element in
X9 if and only if BX:=coker(OX→F∗OX)00 (Davis et al., 2014).
The finite-level cokernel vanishes precisely under a ring-theoretic BX:=coker(OX→F∗OX)01-root condition. Surjectivity of
BX:=coker(OX→F∗OX)02
is equivalent to surjectivity of the BX:=coker(OX→F∗OX)03-th power map on each quotient BX:=coker(OX→F∗OX)04. At infinite level, surjectivity is stricter: BX:=coker(OX→F∗OX)05
Equivalently, full surjectivity is characterized by finite-level surjectivity together with Teichmüller density, or by surjectivity of the BX:=coker(OX→F∗OX)06-th power map on BX:=coker(OX→F∗OX)07 together with the same completeness condition (Davis et al., 2014).
Examples show that finite and infinite behavior diverge sharply. For BX:=coker(OX→F∗OX)08, finite-level surjectivity fails, so the Frobenius cokernel is already nonzero at finite levels. For the ring of integers BX:=coker(OX→F∗OX)09 in an algebraic closure of BX:=coker(OX→F∗OX)10, finite-level Frobenius is surjective for all BX:=coker(OX→F∗OX)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(OX→F∗OX)12
be the homogeneous coordinate ring of the Grassmannian BX:=coker(OX→F∗OX)13, with BX:=coker(OX→F∗OX)14 and BX:=coker(OX→F∗OX)15. The Frobenius on BX:=coker(OX→F∗OX)16 is
BX:=coker(OX→F∗OX)17
with image BX:=coker(OX→F∗OX)18. Viewing BX:=coker(OX→F∗OX)19 as an BX:=coker(OX→F∗OX)20-module, the Frobenius cokernel is
BX:=coker(OX→F∗OX)21
The decomposition of BX:=coker(OX→F∗OX)22 as a graded BX:=coker(OX→F∗OX)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(OX→F∗OX)24 and certain indecomposable Cohen–Macaulay modules BX:=coker(OX→F∗OX)25. Forgetting degrees, the Frobenius summands of BX:=coker(OX→F∗OX)26 lie among
BX:=coker(OX→F∗OX)27
and all of these appear when BX:=coker(OX→F∗OX)28. This is the paper’s explicit instance of BX:=coker(OX→F∗OX)29-uniformity: for sufficiently large BX:=coker(OX→F∗OX)30, the set of indecomposable summands does not depend on BX:=coker(OX→F∗OX)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(OX→F∗OX)32 into indecomposable homogeneous bundles. Up to multiplicity, the summands are twists of BX:=coker(OX→F∗OX)33, the bundles BX:=coker(OX→F∗OX)34, and twists of BX:=coker(OX→F∗OX)35. This Frobenius pushforward is a tilting bundle only for BX:=coker(OX→F∗OX)36 and BX:=coker(OX→F∗OX)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(OX→F∗OX)38 contribute to the nonfree part of BX:=coker(OX→F∗OX)39 over BX:=coker(OX→F∗OX)40, and hence to the nonfree part of the Frobenius cokernel. The same summands are then used to construct a noncommutative resolution BX:=coker(OX→F∗OX)41 of finite global dimension for a suitable direct sum BX:=coker(OX→F∗OX)42 of Frobenius summands (Raedschelders et al., 2017).
6. Random and cohomological analogues
Recent random-matrix work treats polynomial cokernels over BX:=coker(OX→F∗OX)43 as direct analogues of Frobenius cokernels. For
BX:=coker(OX→F∗OX)44
with BX:=coker(OX→F∗OX)45 fixed and BX:=coker(OX→F∗OX)46 random, and for a non-constant monic polynomial BX:=coker(OX→F∗OX)47, the central object is
BX:=coker(OX→F∗OX)48
More naturally, one equips it with the structure of an BX:=coker(OX→F∗OX)49-module for
BX:=coker(OX→F∗OX)50
via letting the image of BX:=coker(OX→F∗OX)51 act by BX:=coker(OX→F∗OX)52. The key linearization is
BX:=coker(OX→F∗OX)53
which replaces a polynomial in BX:=coker(OX→F∗OX)54 by an BX:=coker(OX→F∗OX)55-linear map. The paper proves exact finite-BX:=coker(OX→F∗OX)56 formulas for the distribution of BX:=coker(OX→F∗OX)57 when BX:=coker(OX→F∗OX)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(OX→F∗OX)59 of a BX:=coker(OX→F∗OX)60-adic module and the modules
BX:=coker(OX→F∗OX)61
while the random model replaces BX:=coker(OX→F∗OX)62 by BX:=coker(OX→F∗OX)63. The resulting distribution depends on BX:=coker(OX→F∗OX)64 and on the factorization of BX:=coker(OX→F∗OX)65, and in the squarefree case becomes a direct generalization of the Cohen–Lenstra measure to modules over BX:=coker(OX→F∗OX)66 (Cheong et al., 2023).
A complementary universality principle holds for random integral matrices. For an BX:=coker(OX→F∗OX)67 random integral matrix BX:=coker(OX→F∗OX)68 with independent entries from a very broad class of distributions, the limiting probability that BX:=coker(OX→F∗OX)69 is
BX:=coker(OX→F∗OX)70
This is a Cohen–Lenstra-type law, and it agrees with the distribution defined by the Haar model on BX:=coker(OX→F∗OX)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(OX→F∗OX)72-th Frobenius kernels BX:=coker(OX→F∗OX)73, the cohomology ring BX:=coker(OX→F∗OX)74 is Cohen–Macaulay, and its maximal ideal spectrum is homeomorphic to BX:=coker(OX→F∗OX)75. That work is about kernels of Frobenius rather than cokernels, but it is formulated so that explicit knowledge of BX:=coker(OX→F∗OX)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(OX→F∗OX)77; in Witt theory it measures the failure of Frobenius surjectivity on BX:=coker(OX→F∗OX)78; in invariant theory it records the nonfree part of BX:=coker(OX→F∗OX)79 over BX:=coker(OX→F∗OX)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).