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Motivic Height Zeta Functions

Updated 6 July 2026
  • Motivic height zeta functions are generating series in Grothendieck rings that encode moduli spaces of sections of prescribed degree over smooth projective curves.
  • They capture geometric analogues of classical height zeta functions via explicit formulas, functional equations, and rationality properties in settings like projective bundles and toric varieties.
  • Analytic methods, including Poisson summation and weight convergence, reveal pole structures and asymptotic behaviors that extend the Manin–Peyre principle in arithmetic geometry.

Searching arXiv for recent and foundational papers on motivic height zeta functions. Motivic height zeta functions are generating series in Grothendieck rings that encode spaces of sections or maps of prescribed degree over the function field of a curve. In the simplest form, one fixes a smooth projective curve CC over a field kk, a flat projective morphism π:X→C\pi:X\to C, and a line bundle or log-anticanonical class that plays the role of a height; one then forms a series whose dd-th coefficient is the class of the moduli space of sections of degree dd. This construction is a geometric analogue of classical height zeta functions over number fields and function fields, but its coefficients lie in motivic coefficient rings such as K0(Vark)K_0(\mathrm{Var}_k), localizations by the Lefschetz motive, or their completions. The subject has developed along several parallel lines: explicit formulas and functional equations for projective bundles, rationality and pole analysis for equivariant compactifications of vector groups, Poisson-summation methods for split toric varieties, and weighted refinements for elliptic surfaces (Maruyama, 2015, Chambert-Loir et al., 2013, Bilu et al., 3 Apr 2026).

1. Basic setup and definitions

A foundational formulation starts with a smooth projective curve C/kC/k, a function field F=k(C)F=k(C), and a family X→CX\to C whose generic fibre XηX_\eta carries a natural height datum. For each integer kk0, one considers a moduli space of sections of degree kk1, typically quasi-projective by a Hilbert-scheme argument, and defines a generating series in a Grothendieck ring. In the additive-group setting, if kk2 is the log-anticanonical bundle and kk3 denotes sections kk4 with kk5 and kk6, then

kk7

In the projective-bundle setting, if kk8 is a vector bundle on kk9 and π:X→C\pi:X\to C0 is the associated projective bundle, then

π:X→C\pi:X\to C1

where π:X→C\pi:X\to C2 is the quasi-projective scheme of sections π:X→C\pi:X\to C3 with π:X→C\pi:X\to C4 (Chambert-Loir et al., 2013, Maruyama, 2015).

The coefficient rings vary with the analytic regime under study. For projective bundles one passes from π:X→C\pi:X\to C5 to π:X→C\pi:X\to C6, the quotient identifying radicial surjections, sets π:X→C\pi:X\to C7, and localizes to π:X→C\pi:X\to C8. In toric and convergence-theoretic work one instead uses

π:X→C\pi:X\to C9

or its completion by the virtual-dimension filtration. Over finite fields, the count-points morphism or zeta measure sends the motivic series to more classical counting series, so the motivic formalism refines the arithmetic one rather than replacing it (Maruyama, 2015, Bilu et al., 3 Apr 2026).

A second basic feature is that “height” is not unique. In projective-bundle and additive-group settings it is usually a scalar degree. For split toric varieties one often has a multidegree height with values in dd0, and the single-variable anticanonical series is obtained by specializing along the anticanonical ray. This multivariable viewpoint is essential for the explicit Euler-product and residue formulas in the toric case (Bilu et al., 3 Apr 2026).

2. Projective bundles, Kapranov zeta, and functional equations

For a vector bundle dd1 of rank dd2 on dd3, the projective bundle dd4 provides one of the cleanest motivic height-zeta theories. The key auxiliary series is Kapranov’s motivic zeta function of the base curve,

dd5

with dd6. A Schwarzenberger-type construction produces varieties dd7, where dd8 is the dd9 of the coherent sheaf

dd0

on dd1, and yields the identity

dd2

in dd3 (Maruyama, 2015).

The main motivic theorem states that in dd4, the product dd5 is rational and satisfies a motivic functional equation. More precisely,

dd6

is a polynomial of degree dd7, and

dd8

Thus the denominator has exactly two critical factors, dd9 and K0(Vark)K_0(\mathrm{Var}_k)0, and the involution K0(Vark)K_0(\mathrm{Var}_k)1 exchanges the two sides (Maruyama, 2015).

The structural input is a motivic Riemann–Roch relation for the family K0(Vark)K_0(\mathrm{Var}_k)2: K0(Vark)K_0(\mathrm{Var}_k)3 where K0(Vark)K_0(\mathrm{Var}_k)4. The local system

K0(Vark)K_0(\mathrm{Var}_k)5

has rank difference K0(Vark)K_0(\mathrm{Var}_k)6, so the corresponding projective bundles differ motivically by a projective-space class. Summing in K0(Vark)K_0(\mathrm{Var}_k)7 forces both the two-term denominator and the involution in the functional equation. The paper presents this as the exact analogue of the Arakelov–Tate Riemann–Roch method used earlier in the analytic setting (Maruyama, 2015).

The ruled-surface case K0(Vark)K_0(\mathrm{Var}_k)8, K0(Vark)K_0(\mathrm{Var}_k)9 with C/kC/k0, gives the Hirzebruch surface C/kC/k1. In that case

C/kC/k2

and one again obtains a functional equation together with the denominator C/kC/k3. The geometry of the ruled surface stratifies the amplitudes of poles of C/kC/k4, and the two critical factors C/kC/k5 and C/kC/k6 allow one to read off the decomposition of the effective cone of C/kC/k7 (Maruyama, 2015).

3. Additive-group compactifications and motivic Poisson summation

A broader theory treats equivariant compactifications of the vector group C/kC/k8. Here C/kC/k9 is an algebraically closed field of characteristic zero, F=k(C)F=k(C)0 is a smooth projective connected curve, F=k(C)F=k(C)1 is a dense open subset, F=k(C)F=k(C)2, and F=k(C)F=k(C)3 is a smooth projective F=k(C)F=k(C)4-equivariant compactification of F=k(C)F=k(C)5. The boundary

F=k(C)F=k(C)6

is assumed to have strict normal crossings, with each F=k(C)F=k(C)7 smooth and geometrically irreducible. One chooses a flat model F=k(C)F=k(C)8 of F=k(C)F=k(C)9 over X→CX\to C0, extends to a good model X→CX\to C1, and denotes the vertical irreducible components over X→CX\to C2 by X→CX\to C3. The relevant height is defined by the log-anticanonical divisor

X→CX\to C4

and X→CX\to C5 is the constructible moduli space of sections X→CX\to C6 of height X→CX\to C7 whose generic value lies in X→CX\to C8 and whose restriction to X→CX\to C9 lands in XηX_\eta0 (Chambert-Loir et al., 2013).

The main rationality theorem asserts that XηX_\eta1 lies in the subring XηX_\eta2 of rational power series generated by inverses of XηX_\eta3. More precisely, there exist integers XηX_\eta4, XηX_\eta5, and a polynomial XηX_\eta6 in XηX_\eta7 such that XηX_\eta8 is an effective nonzero element of XηX_\eta9 and

kk00

The same work identifies the largest pole: it is at kk01, and its order is

kk02

where kk03 is the analytic Clemens complex of the special fibre at kk04, with vertices given by the horizontal components kk05 and the vertical components kk06, and faces given by their nonempty intersections (Chambert-Loir et al., 2013).

The proof is adelic and Fourier-theoretic. One rewrites the section-counting problem as a sum over kk07 with local intersection data, decomposes

kk08

and studies each kk09 as a product of local Fourier transforms kk10. The motivic Poisson summation formula, in the Hrushovski–Kazhdan framework, replaces classical harmonic analysis on kk11. Local analysis shows that the kk12 term has the maximal possible pole, contributed by the full Clemens complex, while for kk13 the pole order drops by at least kk14. This isolates the geometric origin of the leading pole (Chambert-Loir et al., 2013).

This setting is explicitly described as the geometric analogue of a number-field result of Chambert-Loir and Tschinkel. Counting sections kk15 of bounded log-anticanonical degree parallels counting integral points of bounded height, and motivic integration on arc spaces replaces the classical local Igusa integrals appearing in arithmetic Poisson summation (Chambert-Loir et al., 2013).

4. Split toric varieties and the motivic Manin–Peyre picture

For a split projective toric variety kk16 over a field kk17 of characteristic zero, with open torus kk18, fan kk19, character lattice kk20, and cocharacter lattice kk21, the height can be made multigraded by recording local intersection indices with the kk22-invariant divisors kk23, kk24. The motivic height zeta function is then

kk25

or, in the single-variable anticanonical case,

kk26

where kk27 denotes the moduli of maps of multidegree kk28 (Bilu et al., 3 Apr 2026).

The central analytic tool is a motivic Poisson formula for split algebraic tori. If kk29, a Schwartz–Bruhat motivic function on kk30 is an element of kk31 supported on finitely many cocharacters, and its Fourier transform is

kk32

Applied fibrewise on symmetric products of kk33, this gives a global Poisson identity that rewrites the height zeta function as a motivic integral of the Fourier transform over characters trivial on principal divisors. The local Fourier transform has the explicit form

kk34

with kk35 determined by the fan kk36 (Bilu et al., 3 Apr 2026).

The resulting analytic statements parallel the classical Batyrev–Tschinkel theory. In multivariable form,

kk37

for some kk38. After specializing to the anticanonical ray kk39, the series converges for kk40 and has a unique principal pole at kk41. Its order is kk42, and the residue is expressed as

kk43

where kk44 is the volume of the dual effective cone and kk45 is the motivic Tamagawa factor involving kk46, kk47, and the product over places kk48 (Bilu et al., 3 Apr 2026).

A direct consequence is a motivic Manin–Peyre statement: as kk49 tends to infinity in the effective cone, the classes

kk50

stabilize in the virtual-dimension completion to the constant kk51. For kk52, the toric theory recovers

kk53

with principal pole at kk54 of order kk55 and residue kk56 (Bilu et al., 3 Apr 2026).

5. Topologies, convergence, and asymptotic extraction

Motivic height zeta functions are studied not only as formal rational expressions but also as analytic objects in completed coefficient rings. One important framework uses the weight filtration coming from mixed Hodge theory. Over kk57, the Hodge realization

kk58

pulls back the standard weight filtration to a filtration on kk59, and the completion kk60 is defined so that a series kk61 converges when the weights of kk62 tend to kk63 fast enough. In the setting of partial equivariant compactifications of kk64, there exist a nonzero kk65 and kk66 such that

kk67

converges for kk68 and takes the value kk69 at kk70. In particular, kk71 has a pole of order kk72 at kk73 and no other poles in that disc; the integer kk74 is expressed in terms of kk75 and the simplicial complexes kk76 attached to bad fibres (Bilu, 2018).

This convergence theorem has asymptotic consequences for Hodge–Deligne polynomials of the section spaces. If kk77 has such a controlled pole, then for each congruence class modulo a fixed integer either kk78, or else

kk79

for some integer kk80, and the number of components of top dimension grows like kk81. Moreover, a positive proportion of congruence classes achieve the maximal dimension growth. In this way, the motivic pole structure is converted into geometric asymptotics for the moduli spaces of sections (Bilu, 2018).

A different completion arises from the Witt-ring and Hadamard-function viewpoint. Let kk82 be the rational Witt ring of rational functions kk83 with kk84, equipped with the Hadamard topology defined by the divisor norm

kk85

Its completion is identified with a space kk86 of meromorphic functions called Hadamard functions. Over a finite field, the zeta measure sends motivic classes to rational Witt vectors, and therefore maps completed motivic rings to kk87. For the toric motivic height-zeta series, the renormalized series

kk88

converges in the dimensional topology to a nonzero limit, and after applying the zeta measure one obtains convergence of

kk89

in the point-counting topology and, for kk90 above an explicit combinatorial bound, also in the Hadamard topology. This is presented as evidence for a meta-conjecture that natural sequences whose zeta-images converge in both the weight and point-counting topologies should converge in the stronger Hadamard topology as well (Bilu et al., 2020).

These two analytic regimes show that “pole” and “convergence” are not uniform notions in the subject. Rationality in a localized Grothendieck ring, convergence in the weight topology, and convergence in the Hadamard topology are distinct statements, each tailored to a different part of the motivic-height-zeta formalism (Bilu, 2018, Bilu et al., 2020).

6. Weighted refinements, elliptic surfaces, and limits of rationality

A recent refinement replaces plain section-counting by weighted counting in a moduli stack of elliptic curves over kk91. Let kk92 be the Deligne–Mumford stack parametrizing kk93-rational points of kk94-height kk95 on kk96, equivalently minimal elliptic curves kk97 of discriminant degree kk98. If kk99 is the associated relatively minimal elliptic surface with section, one defines

π:X→C\pi:X\to C00

where π:X→C\pi:X\to C01 is the rank of the trivial lattice in π:X→C\pi:X\to C02 and π:X→C\pi:X\to C03 is the Mordell–Weil rank. The Shioda–Tate formula reads

π:X→C\pi:X\to C04

Thus the series refines the height distribution simultaneously by trivial-lattice rank and Mordell–Weil rank (Park, 21 Jan 2026).

The rationality result applies to the trivial-lattice specialization

π:X→C\pi:X\to C05

Because π:X→C\pi:X\to C06 is determined by fibre types, the moduli stack decomposes into finitely many Kodaira strata on which π:X→C\pi:X\to C07 is constant. After introducing a multivariate series indexed by elementary local patterns and using a power-structure Euler product, one obtains a finite Euler product

π:X→C\pi:X\to C08

in π:X→C\pi:X\to C09. In particular, π:X→C\pi:X\to C10 is rational in π:X→C\pi:X\to C11 after inverting π:X→C\pi:X\to C12 (Park, 21 Jan 2026).

By contrast, the Mordell–Weil and Néron–Severi specializations are conjectured to be irrational: π:X→C\pi:X\to C13 The stated reason is geometric: on a fixed Kodaira stratum the trivial lattice is constant, whereas π:X→C\pi:X\to C14 and π:X→C\pi:X\to C15 vary along Noether–Lefschetz or Hodge jump loci, which are in general countable unions of closed algebraic subsets rather than a finite stratification. This creates a sharp distinction between locally determined weights, which admit finite Euler products, and globally varying lattice invariants, which are expected not to (Park, 21 Jan 2026).

π:X→C\pi:X\to C16

Taken together, these developments delineate the current scope of the subject. Projective bundles exhibit explicit functional equations and low-degree denominators; equivariant compactifications of π:X→C\pi:X\to C17 yield rationality and pole orders governed by Clemens complexes; split toric varieties admit a motivic Poisson theory compatible with a motivic Manin–Peyre principle; convergence can be studied in weight and Hadamard topologies; and weighted variants for elliptic surfaces show that rationality can depend sensitively on whether the chosen invariant is locally stratifiable or controlled by global jump loci (Maruyama, 2015, Chambert-Loir et al., 2013, Bilu et al., 3 Apr 2026, Bilu, 2018, Bilu et al., 2020, Park, 21 Jan 2026).

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