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Multiplicative Hecke Operators

Updated 9 July 2026
  • Multiplicative Hecke operators are defined via explicit product formulas that capture local factor structures in classical modular form theory.
  • They extend to nonlinear settings by acting on meromorphic modular forms, identifying eta quotients as eigenforms and linking to Borcherds products and divisor maps.
  • In vector-valued and noncommutative frameworks, these operators satisfy modified product identities and recurrences, unveiling deeper arithmetic and geometric insights.

Multiplicative Hecke operators are a family of constructions in which the multiplicative structure of Hecke theory is made explicit either in the operator algebra, in the target on which the operators act, or in the resulting eigenvalue relations. In the classical linear setting, this appears through prime-by-prime factorization and commuting local Hecke actions; in a genuinely nonlinear setting, one replaces additive Hecke sums by products and lets the operators act on multiplicative groups of meromorphic modular forms; and in several recent generalizations the same theme reappears in noncommutative, vector-valued, geometric, and derived contexts (Walling, 2014, Kim et al., 2024, Hain, 2023).

1. Classical multiplicativity and local Hecke structure

In the standard theory of modular and Siegel modular forms, multiplicativity is encoded by commuting local operators and by the organization of the Hecke algebra prime by prime. For Siegel Eisenstein series of arbitrary degree nn, weight kk, level NN, and character χ\chi, Walling gives explicit formulas for the action of T(p)T(p) and Tj(p2)T_j(p^2), diagonalizes the Eisenstein space for all primes pNp\nmid N, and, in square-free level, also diagonalizes the operators at primes dividing the level. On the averaged basis Eσ,ψE_{\sigma,\psi}, the good-prime eigenvalue of T(p)T(p) is

λσ,ψ(p)=ψ1(p)ψ2(pn)i=1n(ψ2χ(p)pki+1),\lambda_{\sigma,\psi}(p)= \psi_1(p)\psi_2(p^n)\prod_{i=1}^n(\psi_2\chi(p)p^{k-i}+1),

and for the modified operators kk0 one gets

kk1

These product formulas are the clearest local manifestation of multiplicativity in that setting; in square-free level they lead to simultaneous diagonalization and a multiplicity-one theorem (Walling, 2014).

In half-integral weight Siegel theory, the relevant operators are kk2, not kk3: Walling states that “the half-integral weight Hecke operator kk4 is kk5 for any prime kk6.” The local Hecke algebra is therefore organized around the square-indexed operators, and alternate generators kk7 are introduced precisely because they simplify the Fourier-coefficient formulas and expose the local multiplicative structure. For Eisenstein series of level kk8 with kk9 odd and square-free, the resulting eigenvalues become explicit product expressions, for example

NN0

and the odd-prime Hecke operators commute, allowing simultaneous diagonalization and multiplicity-one on the relevant Eisenstein subspace. A closely related reorganization of the local half-integral weight Hecke algebra replaces the standard generators NN1 by NN2, turning twisted Gauss-sum formulas into representation numbers and making the local structure compatible with theta series and Jacobi theory (Walling, 2016, Walling, 2011).

These results do not identify a single universal notion of “multiplicative Hecke operator,” but they show that classical Hecke theory is already governed by local product formulas, commuting prime-indexed operators, and prime-power recursions. This suggests that later nonlinear or noncommutative versions are best understood as extensions of a prime-by-prime local paradigm rather than as completely unrelated constructions.

2. Genuine multiplicative Hecke operators on meromorphic modular forms

A literal multiplicative Hecke theory is developed for the multiplicative group NN3 of integral weight meromorphic modular forms for NN4, with unitary multiplier system, integer Fourier coefficients, and leading coefficient NN5. If NN6 has weight NN7, then for a prime NN8 and NN9 the multiplicative Hecke operator χ\chi0 is defined by a product of slash transforms, with different formulas according to whether χ\chi1 or χ\chi2, and χ\chi3 is the identity. For general

χ\chi4

If

χ\chi5

then χ\chi6 again has a product expansion, with weight and order transformed by

χ\chi7

where χ\chi8. For χ\chi9, the exponent formula simplifies at T(p)T(p)0 to

T(p)T(p)1

The core multiplicative relation is the product identity

T(p)T(p)2

so in particular T(p)T(p)3 when T(p)T(p)4. For T(p)T(p)5, the prime-power recursion is

T(p)T(p)6

while for T(p)T(p)7,

T(p)T(p)8

In this framework, a multiplicative Hecke eigenform is defined by

T(p)T(p)9

and the classification theorem states that for Tj(p2)T_j(p^2)0 the following are equivalent: Tj(p2)T_j(p^2)1 is a multiplicative Hecke eigenform; Tj(p2)T_j(p^2)2 has no zeros or poles on Tj(p2)T_j(p^2)3; and Tj(p2)T_j(p^2)4 is an eta quotient. Thus eta quotients are exactly the multiplicative Hecke eigenforms in this setting (Kim et al., 2024).

The same paper emphasizes that this theory is adapted to infinite-product exponents Tj(p2)T_j(p^2)5, divisors, and Borcherds products rather than to additive Fourier coefficients. A plausible implication is that “multiplicative Hecke operator” is most precise when the natural algebraic structure on the target is multiplication rather than addition.

3. Borcherds products, logarithmic derivatives, and divisors

The nonlinear Hecke formalism becomes especially effective when paired with Borcherds lifts and divisor maps. For a fundamental discriminant Tj(p2)T_j(p^2)6 and Tj(p2)T_j(p^2)7, the generalized Borcherds product of type Tj(p2)T_j(p^2)8

Tj(p2)T_j(p^2)9

sends a vector-valued harmonic weak Maass form to a meromorphic modular form for pNp\nmid N0 with unitary character, possibly of infinite order. On the additive side the relevant Hecke operator is pNp\nmid N1, and the equivariance theorem states that for primes pNp\nmid N2,

pNp\nmid N3

This extends Guerzhoy’s multiplicative Hecke operator to the generalized Borcherds setting attached to pNp\nmid N4 and the Weil representation (Jeon et al., 2022).

In the meromorphic-modular setting of Kim and Shin, the Borcherds product and the logarithmic derivative are Hecke equivariant for all pNp\nmid N5 coprime to the level and discriminant. If pNp\nmid N6 denotes the Borcherds product and

pNp\nmid N7

then

pNp\nmid N8

when pNp\nmid N9, and

Eσ,ψE_{\sigma,\psi}0

when Eσ,ψE_{\sigma,\psi}1. These identities are proved prime-power first and then extended by multiplicativity, and they place product expansions, divisor data, and additive Hecke theory in a single compatible formalism (Kim et al., 2024).

The divisor-theoretic version is even more direct. On

Eσ,ψE_{\sigma,\psi}2

the multiplicative Hecke action attached to a double coset Eσ,ψE_{\sigma,\psi}3 is

Eσ,ψE_{\sigma,\psi}4

The divisor map to Eσ,ψE_{\sigma,\psi}5 is then Hecke equivariant: for Eσ,ψE_{\sigma,\psi}6,

Eσ,ψE_{\sigma,\psi}7

This yields the divisor-sum identity

Eσ,ψE_{\sigma,\psi}8

and is applied to Bruinier–Kohnen–Ono type formulas, Rohrlich-type divisor sums, and recurrences for polyharmonic Maass forms. In this context the paper explicitly frames additive and multiplicative Hecke operators as two representations of the same Hecke algebra Eσ,ψE_{\sigma,\psi}9, with divisors naturally compatible with the multiplicative one (Jeon et al., 3 May 2025).

4. Nonabelian and noncommutative multiplicativity

A different generalization appears in Hain’s nonabelian Hecke theory on loops and conjugacy classes. Starting from a finite unramified covering T(p)T(p)0, one has pushforward and pullback on free homotopy classes, and the classical Hecke correspondences T(p)T(p)1 on the modular orbifold induce operators on

T(p)T(p)2

These operators preserve elliptic, parabolic, and hyperbolic classes, and the coprime multiplicativity relation survives: T(p)T(p)3 At a fixed prime T(p)T(p)4, however, the classical commutative local Hecke algebra is replaced by a noncommutative one. The auxiliary operator

T(p)T(p)5

enters the prime-power relation

T(p)T(p)6

which replaces the scalar correction term of the classical formula. On parabolic classes,

T(p)T(p)7

and

T(p)T(p)8

These formulas imply

T(p)T(p)9

so the algebra generated by the λσ,ψ(p)=ψ1(p)ψ2(pn)i=1n(ψ2χ(p)pki+1),\lambda_{\sigma,\psi}(p)= \psi_1(p)\psi_2(p^n)\prod_{i=1}^n(\psi_2\chi(p)p^{k-i}+1),0 is not commutative. Hain packages the local structure as

λσ,ψ(p)=ψ1(p)ψ2(pn)i=1n(ψ2χ(p)pki+1),\lambda_{\sigma,\psi}(p)= \psi_1(p)\psi_2(p^n)\prod_{i=1}^n(\psi_2\chi(p)p^{k-i}+1),1

with

λσ,ψ(p)=ψ1(p)ψ2(pn)i=1n(ψ2χ(p)pki+1),\lambda_{\sigma,\psi}(p)= \psi_1(p)\psi_2(p^n)\prod_{i=1}^n(\psi_2\chi(p)p^{k-i}+1),2

and recovers the classical Hecke algebra as the quotient obtained by imposing λσ,ψ(p)=ψ1(p)ψ2(pn)i=1n(ψ2χ(p)pki+1),\lambda_{\sigma,\psi}(p)= \psi_1(p)\psi_2(p^n)\prod_{i=1}^n(\psi_2\chi(p)p^{k-i}+1),3. Dually, the opposite algebra acts on the ring of class functions on the relative completion of λσ,ψ(p)=ψ1(p)ψ2(pn)i=1n(ψ2χ(p)pki+1),\lambda_{\sigma,\psi}(p)= \psi_1(p)\psi_2(p^n)\prod_{i=1}^n(\psi_2\chi(p)p^{k-i}+1),4, hence on conjugation-invariant iterated Shimura integrals, preserving mixed Hodge structures and commuting with the absolute Galois action (Hain, 2023).

This construction shows that multiplicativity need not imply commutativity. Here coprime factorization survives intact, but prime-power structure becomes operator-valued and noncentral.

5. Vector-valued, analytic, and formal variants

The expression “multiplicative Hecke operators” also appears in several nonclassical analytic settings. In rational conformal field theory, Hecke operators are defined on vector-valued modular functions of conductor λσ,ψ(p)=ψ1(p)ψ2(pn)i=1n(ψ2χ(p)pki+1),\lambda_{\sigma,\psi}(p)= \psi_1(p)\psi_2(p^n)\prod_{i=1}^n(\psi_2\chi(p)p^{k-i}+1),5. For a prime λσ,ψ(p)=ψ1(p)ψ2(pn)i=1n(ψ2χ(p)pki+1),\lambda_{\sigma,\psi}(p)= \psi_1(p)\psi_2(p^n)\prod_{i=1}^n(\psi_2\chi(p)p^{k-i}+1),6 with λσ,ψ(p)=ψ1(p)ψ2(pn)i=1n(ψ2χ(p)pki+1),\lambda_{\sigma,\psi}(p)= \psi_1(p)\psi_2(p^n)\prod_{i=1}^n(\psi_2\chi(p)p^{k-i}+1),7,

λσ,ψ(p)=ψ1(p)ψ2(pn)i=1n(ψ2χ(p)pki+1),\lambda_{\sigma,\psi}(p)= \psi_1(p)\psi_2(p^n)\prod_{i=1}^n(\psi_2\chi(p)p^{k-i}+1),8

and the transformed modular representation is

λσ,ψ(p)=ψ1(p)ψ2(pn)i=1n(ψ2χ(p)pki+1),\lambda_{\sigma,\psi}(p)= \psi_1(p)\psi_2(p^n)\prod_{i=1}^n(\psi_2\chi(p)p^{k-i}+1),9

These operators satisfy

kk00

and the prime-power recursion

kk01

At weight kk02, the correction term is kk03. The paper interprets this as an extension of Galois symmetry from modular data to full RCFT characters (Harvey et al., 2018).

For the Lerch zeta function, Lagarias and Li define two-variable operators

kk04

on twisted-periodic real-analytic function spaces. The exact semigroup law

kk05

holds on the twisted-periodic space, and for each kk06 there is a two-dimensional space kk07 generated by Lerch zeta functions on which every kk08 acts by the scalar kk09. Under twisted-periodicity and integrability hypotheses, this kk10 is the maximal simultaneous eigenspace for the family kk11 (Lagarias et al., 2015).

On formal power series and hypergeometric functions, the operators

kk12

satisfy

kk13

On the set of hypergeometric functions, the spectrum of kk14 is

kk15

and the principal eigenfunctions are polylogarithms and the rational functions kk16. Simultaneous eigenfunctions for all kk17 are exactly

kk18

which is equivalent to complete multiplicativity of the coefficient sequence (Moll et al., 2010).

Taken together, these examples show that multiplicative Hecke structures extend beyond scalar modular forms to vector-valued, two-variable, and purely formal settings. The common feature is an operator family indexed by positive integers whose composition law is encoded directly in multiplication.

6. Geometric and arithmetic extensions

Recent work has pushed multiplicative Hecke ideas into geometric representation theory, derived Hecke theory, and Archimedean harmonic analysis. In the Jacquet–Rallis relative trace formula over local function fields, the spherical Hecke module on the symmetric side and the spherical Hecke algebra on the unitary side are compared by a canonical transfer

kk19

and the fundamental lemma is proved using multiplicative Hitchin fibrations. For matching strongly regular semisimple elements kk20 and matching spherical test functions kk21, the main identity is

kk22

At the level of Satake functions, the corresponding orbital integrals are realized as point counts on affine Jacquet–Rallis fibers. In this setting, “multiplicative” refers primarily to multiplicative Hitchin fibrations and multiplicative affine Springer fibers rather than to product-valued Hecke operators (Wang et al., 2024).

For the multiplicative group kk23 over a number field, the derived Hecke algebra acquires an explicit local description: kk24 and the resulting operators act on cohomology by

kk25

When kk26, the paper proves non-vanishing of the degree-one derived Hecke action under mild assumptions. If kk27 does not divide the order of kk28, then the map

kk29

is an isomorphism of kk30-modules. The proof uses the Grunwald–Wang theorem to show that finitely many local mod-kk31 unit characters detect the global unit characters (Kim et al., 2024).

At the Archimedean place, the Hecke–Baxter operator for kk32 is the kk33-biinvariant kernel

kk34

an element of the spherical Hecke algebra. On spherical principal series it acts by scalar multiplication with the local Archimedean kk35-factor, and the paper reinterprets kk36 as a generalized Whittaker function for an extension of kk37 by a Heisenberg Lie group. It is then lifted to a corresponding extension of kk38. This gives a representation-theoretic realization of an Archimedean multiplicative Hecke kernel as a matrix coefficient (Gerasimov et al., 2024).

These developments suggest that multiplicative Hecke operators are no longer confined to a single formalism. They appear as nonlinear product operators on meromorphic modular forms, as local commuting or twisted semigroups on analytic function spaces, as noncommutative operators on loops and conjugacy classes, and as geometric or derived actions built from spherical Hecke categories, Heisenberg extensions, and arithmetic tori.

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