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Geometric Tevelev Degrees

Updated 9 July 2026
  • Geometric Tevelev degrees are fixed-domain invariants that count morphisms from a fixed smooth pointed curve to a target variety under exact incidence conditions.
  • They connect theories such as Hurwitz, Schubert calculus, and quantum cohomology, providing explicit formulas and recursions in various geometric settings.
  • The framework distinguishes between geometric and virtual counts, with discrepancies arising from boundary phenomena and non-transversal map contributions.

Searching arXiv for papers on geometric Tevelev degrees and related tropical/logarithmic variants. Geometric Tevelev degrees are fixed-domain enumerative invariants attached to maps from a general pointed smooth curve to a target variety under the maximal number of point or incidence constraints compatible with a finite count. In the basic formulation, one studies the forgetful/evaluation morphism

τ:Mg,n(X,β)Mg,n×Xn\tau:\overline M_{g,n}(X,\beta)\to \overline M_{g,n}\times X^n

for a nonsingular projective target XX of dimension rr, genus gg, nn markings, and curve class β\beta, under the expected-dimension condition

βc1(TX)=r(n+g1).\int_\beta c_1(T_X)=r(n+g-1).

When every irreducible component dominating Mg,n×Xn\overline M_{g,n}\times X^n is generically smooth of expected dimension, the geometric Tevelev degree is the degree of τ\tau, equivalently the number of maps from a general nn-pointed genus-XX0 curve through XX1 general target points (Lian et al., 2021, Lian, 2023).

1. Fixed-domain definition and conceptual scope

The defining feature of a geometric Tevelev degree is that the source curve has fixed complex structure. One fixes a general pointed smooth curve XX2, chooses general target conditions, and counts morphisms XX3 in class XX4 satisfying those conditions. The count is expected to be finite precisely when

XX5

which is the equality between the virtual dimension of XX6 and the dimension of XX7 (Lian et al., 2021, Buch et al., 2021).

This notion is distinct from the virtual Tevelev degree. The virtual invariant is defined by pushing forward the virtual fundamental class,

XX8

whereas the geometric degree requires actual finiteness and transversality on a general fiber (Lian et al., 2021, Buch et al., 2021). A persistent theme in the literature is that virtual Tevelev degrees often admit very simple formulas, but geometric and virtual counts need not agree; discrepancies come from boundary stable maps, contracted components, rational tails, or other non-enumerative contributions (Lian, 2023, Lian et al., 2021).

Geometric Tevelev degrees count maps, not embedded image curves modulo reparametrization. If two distinct morphisms from the fixed source have the same image, they are counted separately. This map-counting perspective is fundamental in the fixed-domain interpolation problem and aligns Tevelev degrees with Brill–Noether theory, linear series, Hurwitz theory, and the geometry of evaluation maps on moduli spaces (Lian et al., 2021, Lian, 2023).

2. Hurwitz-theoretic origins and the XX9 case

The original Tevelev degree arises from Hurwitz moduli. For degree-rr0 simply branched covers rr1 of genus rr2 with rr3 marked unramified points, the admissible-cover compactification rr4 carries a natural morphism

rr5

In Tevelev’s original situation,

rr6

this map is finite, and the degree

rr7

counts degree-rr8 maps from a general rr9-pointed genus-gg0 curve to a general gg1-pointed rational curve, up to the ordering of the gg2 simple ramification points. The resulting formula is

gg3

(Cela et al., 2021).

The Hurwitz-space interpretation extends to the two-parameter family

gg4

For these parameters the source and target of the corresponding Hurwitz forgetful map still have equal dimension, and the generalized degrees gg5 count covers in which gg6 distinguished marked points lie in one common fiber. The central recursion is

gg7

obtained by excess intersection on boundary strata of admissible-cover spaces. In the classical sector gg8 this specializes to gg9; in other regimes it interpolates with projective geometry of lines and with Castelnuovo’s count of pencils (Cela et al., 2021).

For nn0, the theory admits a further geometric generalization allowing arbitrary ramification profiles over marked target points and equal-image constraints among marked source points. If nn1 are ramification profiles over nn2 marked target points, with

nn3

the generalized degree

nn4

counts admissible covers with prescribed grouped ramification, where

nn5

A basic structural simplification is that the degree depends on each nn6 only through its total size nn7. The theory admits both a genus recursion and explicit closed formulas, and it can also be expressed by Schubert-calculus formulas on nn8 via limit linear series (Cela et al., 2021).

3. Projective-space geometric Tevelev degrees

For nn9, the fixed-domain point-interpolation problem is especially rigid. If β\beta0 is a general pointed smooth curve of genus β\beta1, and β\beta2 are general points, the geometric Tevelev degree

β\beta3

is the number of degree-β\beta4 maps β\beta5 with β\beta6, under the balance

β\beta7

(Lian, 2023, Lian et al., 27 Aug 2025).

The projective-space case is now known in all degrees allowed by this dimension constraint. The main formula is an explicit Grassmannian intersection: β\beta8 obtained by degenerating the fixed source curve and replacing naïve map spaces by spaces of complete collineations. This resolves excess intersections coming from linear dependence and base-point phenomena and yields a complete geometric answer for point conditions in β\beta9, as well as a complete answer in βc1(TX)=r(n+g1).\int_\beta c_1(T_X)=r(n+g-1).0 with arbitrary point and line conditions (Lian, 2023).

The projective-space theory sharply distinguishes geometric from virtual counts. For βc1(TX)=r(n+g1).\int_\beta c_1(T_X)=r(n+g-1).1, the virtual answer is

βc1(TX)=r(n+g1).\int_\beta c_1(T_X)=r(n+g-1).2

when the dimension constraint holds, but geometric and virtual degrees differ outside the large-degree regime. In βc1(TX)=r(n+g1).\int_\beta c_1(T_X)=r(n+g-1).3, the first non-large-degree case βc1(TX)=r(n+g1).\int_\beta c_1(T_X)=r(n+g-1).4 has

βc1(TX)=r(n+g1).\int_\beta c_1(T_X)=r(n+g-1).5

and for βc1(TX)=r(n+g1).\int_\beta c_1(T_X)=r(n+g-1).6 one gets

βc1(TX)=r(n+g1).\int_\beta c_1(T_X)=r(n+g-1).7

(Lian, 2023).

A later combinatorial reformulation uses the RSK correspondence. Under

βc1(TX)=r(n+g1).\int_\beta c_1(T_X)=r(n+g-1).8

βc1(TX)=r(n+g1).\int_\beta c_1(T_X)=r(n+g-1).9 equals the number of Mg,n×Xn\overline M_{g,n}\times X^n0-ary words of length Mg,n×Xn\overline M_{g,n}\times X^n1 satisfying three subsequence conditions: there exist at least Mg,n×Xn\overline M_{g,n}\times X^n2 disjoint decreasing subsequences of length Mg,n×Xn\overline M_{g,n}\times X^n3; there is no nondecreasing subsequence of length Mg,n×Xn\overline M_{g,n}\times X^n4; and there is no Mg,n×Xn\overline M_{g,n}\times X^n5-subsequence of length Mg,n×Xn\overline M_{g,n}\times X^n6. This converts the Schubert formula into a manifestly positive word count and explains why the large-degree regime collapses to

Mg,n×Xn\overline M_{g,n}\times X^n7

(Lian et al., 27 Aug 2025).

4. Virtual theory, enumerativity, and logarithmic variants

Virtual Tevelev degrees admit a uniform quantum-cohomological expression. For a nonsingular projective target Mg,n×Xn\overline M_{g,n}\times X^n8, point class Mg,n×Xn\overline M_{g,n}\times X^n9, and quantum Euler class

τ\tau0

the virtual invariant satisfies

τ\tau1

This reduction to small quantum cohomology yields exact formulas for projective spaces, quadrics, cominuscule homogeneous spaces, and low-degree complete intersections (Buch et al., 2021).

Enumerativity is a separate issue. A central asymptotic result proves that for fixed genus and sufficiently positive curve class, virtual Tevelev degrees are enumerative for all homogeneous varieties and for hypersurfaces of sufficiently low degree compared to the dimension. The mechanism is twofold: smooth-domain maps in a general fiber become unobstructed and transverse, while boundary strata with rational tails fail to dominate the incidence target. In genus τ\tau2, stronger non-asymptotic statements hold in the same classes (Lian et al., 2021).

For hypersurfaces, there is also a direct geometric computation. If τ\tau3 is a smooth hypersurface of degree τ\tau4, with

τ\tau5

then

τ\tau6

for all τ\tau7 if τ\tau8, and for sufficiently large τ\tau9 if nn0. This reproves, by projective geometry, the asymptotic geometric count previously obtained by combining virtual formulas with enumerativity results (Lian, 2022).

Logarithmic variants enlarge the theory to toric targets with tangency conditions. For a toric variety nn1, discrete data nn2, and the logarithmic moduli space nn3, one studies

nn4

In genus nn5, under the fixed-domain dimension condition

nn6

the virtual logarithmic Tevelev degree equals the actual number of logarithmic stable maps from a general fixed source curve, provided boundary and toric-fixed-point degeneracies are excluded. For Hirzebruch surfaces nn7, the genus-nn8 tropical and logarithmic counts coincide and admit explicit closed formulas in the contact partitions nn9 (Cela et al., 2023).

For Fano complete intersections of dimension XX00, the quantum Euler class has been computed explicitly, leading to formulas for all virtual Tevelev degrees in classes XX01 satisfying

XX02

That work does not prove general geometric enumerativity, but it gives the full virtual answer and an algorithm reducing the remaining computation to genus-XX03 two-point hyperplane invariants (Cela, 2022).

5. Tropical Tevelev degrees and correspondence theorems

The tropical counterpart is defined by replacing admissible covers with tropical admissible covers and replacing Deligne–Mumford spaces with tropical moduli spaces. In the classical Hurwitz case

XX04

one has a finite tropical forgetful map

XX05

and the tropical Tevelev degree is

XX06

Because the simple branch ends are already unmarked on the tropical side, there is no XX07 denominator. The main tropical theorem is

XX08

proved by a correspondence theorem via Berkovich skeletons together with a direct combinatorial count of tropical admissible covers (Cavalieri et al., 2024).

The tropical computation is highly explicit. One chooses a special point in

XX09

whose source curve has a chain of XX10 loops and whose target is a caterpillar-like tree. Each loop contributes one of exactly two allowed local fragments, XX11 or XX12, altering the active-path degree by XX13. The genus part is therefore encoded by lattice paths that never cross below XX14, and the marked-tree part is reconstructed by cut-and-join operations along the active path. A binomial recursion counts the genus possibilities, and every resulting tropical cover has multiplicity XX15, so the degree is literally the number of covers (Cavalieri et al., 2024).

This tropical framework has recently been generalized by introducing the parameter XX16, so that

XX17

For positive XX18, the tropical degree remains unchanged: XX19 For negative XX20, one obtains an explicit defect formula: XX21 The same paper also defines generalized tropical Tevelev degrees with ramification profiles XX22, giving closed formulas that tropicalize the generalized algebraic degrees studied for XX23 (Dawson, 29 Jan 2026).

A recurring conceptual point is that tropical Tevelev degrees are not merely analogous to the algebraic ones. In the classical case XX24 is proved by tropicalization of moduli spaces and comparison of local analytic and tropical degrees, and the later generalized work is explicitly framed as tropicalizing the algebraic theories of Cela–Pandharipande–Schmitt and Cela–Lian (Cavalieri et al., 2024, Dawson, 29 Jan 2026).

6. Vanishing phenomena, exceptional targets, and adjacent degree theories

Geometric Tevelev degrees are not uniformly positive. A sharp vanishing result holds for Hirzebruch surfaces

XX25

If the expected-dimension condition

XX26

holds and XX27 (or XX28 and XX29), then no irreducible component of XX30 dominates XX31, except in the single case

XX32

Hence, outside that case,

XX33

The proof uses semistability of XX34 for general counted maps as a necessary condition for interpolation (Cela et al., 26 Mar 2025).

The exceptional case reduces exactly to XX35. For

XX36

one has

XX37

Geometrically, a map XX38 in class XX39 is equivalent to a degree-XX40 pencil XX41 together with a section of XX42, and the marked-point conditions determine that section uniquely. Thus the only nonzero Hirzebruch-surface counts for XX43 are inherited from the already-computed geometric Tevelev degrees of XX44 (Cela et al., 26 Mar 2025).

A broader but related multidegree theory is provided by Kapranov degrees on XX45. These are top intersections of divisor classes

XX46

equivalently multidegrees of the product of forgetful and Kapranov maps. They include the Castravet–Tevelev case as a special situation, and their positivity is characterized by the Cerberus condition

XX47

In the specialization XX48 for all XX49, the Kapranov degree is either XX50 or XX51, recovering the Castravet–Tevelev phenomenon inside a larger multidegree formalism (Brakensiek et al., 2023).

Taken together, these developments show that geometric Tevelev degrees form a moduli-theoretic family of fixed-domain interpolation invariants with several distinct faces: Hurwitz-theoretic for XX52, Schubert-theoretic for projective space, quantum-cohomological on the virtual side, logarithmic for toric targets with tangency, and tropical through correspondence theorems. The subject is marked by two complementary facts: in some regimes the answers are unexpectedly rigid, such as XX53 or XX54; in others, boundary contributions, semistability obstructions, or ramification constraints force genuine deviations from the virtual or large-degree picture (Lian, 2023, Lian et al., 2021).

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