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Simplicial First Chern Class

Updated 7 July 2026
  • Simplicial First Chern Class is a universal representative of c₁ constructed on combinatorial and simplicial models rather than on smooth manifolds.
  • It is computed using methods like the Bott–Shulman–Stasheff de Rham complex, Čech nerves, and simplicial presheaf approaches to connect classical and discrete geometry.
  • The approach provides explicit cocycle formulas for triangulated S¹-bundles and aids in computational topology via transgression and combinatorial techniques.

Searching arXiv for the supplied papers and closely related work on simplicial first Chern classes, simplicial Chern–Weil theory, and combinatorial/simplicial representatives. arXiv search query: "simplicial first Chern class Bott-Shulman-Stasheff Chern-Weil triangulated circle bundle coherent analytic sheaves" The simplicial first Chern class is a representative of the first Chern class c1c_1 constructed on a simplicial or combinatorial model rather than directly on a smooth manifold. In the literature, this phrase covers several closely related settings: the Bott–Shulman–Stasheff simplicial de Rham complex of the nerve NGNG of a Lie group, Čech nerves of open covers, triangulated S1S^1-bundles and their combinatorial local formulas, and simplicial presheaves or stacks of bundles and coherent sheaves. In each case, the aim is the same: to realize the universal or geometric class c1c_1 by an explicit cocycle compatible with face maps, classifying maps, and transgression constructions (Suzuki, 2017).

1. Simplicial models for bundles and classifying spaces

For a Lie group GG, the standard simplicial models are the nerve

NG(q)=GqNG(q)=G^q

and the simplicial manifold

PG(q)=Gq+1,PG(q)=G^{q+1},

with face operators determined by multiplication in GG and by omission of factors. The simplicial map

γ:PGNG,γ(g0,,gq)=(g0g11,g1g21,,gq1gq1)\gamma:PG\to NG,\qquad \gamma(g_0,\dots,g_q)=(g_0g_1^{-1},\,g_1g_2^{-1},\,\dots,\,g_{q-1}g_q^{-1})

models the universal bundle EGBGEG\to BG after geometric realization. Bott–Shulman–Stasheff attach to any simplicial manifold NGNG0 the double complex

NGNG1

with

NGNG2

and total differential NGNG3. For NGNG4, one has

NGNG5

while for NGNG6,

NGNG7

Dupont’s simplicial forms NGNG8 and the integration map

NGNG9

give an equivalent cohomological model, and this is the basic framework in which simplicial characteristic classes are computed (Suzuki, 2017).

A broader geometric-categorical version replaces simplicial manifolds by smooth simplicial sets. For a Fréchet Lie group S1S^10 and a suitable Grothendieck universe S1S^11, one obtains a smooth Kan complex S1S^12 together with a universal simplicial S1S^13-bundle S1S^14. When S1S^15 has the homotopy type of a CW complex, there is a homotopy equivalence

S1S^16

and a universal Chern–Weil homomorphism

S1S^17

compatible with pullback to ordinary principal bundles (Savelyev, 2021).

2. Universal simplicial Chern–Weil construction and the degree-two class

On the universal simplicial bundle S1S^18, Dupont’s canonical simplicial connection is

S1S^19

where c1c_10 are barycentric coordinates on c1c_11 and each c1c_12 is the pullback of the Maurer–Cartan form from the c1c_13-th factor of c1c_14. Its curvature is

c1c_15

For an invariant polynomial c1c_16, the universal simplicial Chern–Weil map is

c1c_17

The resulting cocycles in c1c_18 are the Bott–Shulman–Stasheff forms (Suzuki, 2017).

For c1c_19, the first Chern class and first Chern character coincide: GG0 and the corresponding invariant polynomial is

GG1

In the universal simplicial context, the degree-two representative can be read off from the general formula for powers of the first Chern class. For GG2, Suzuki writes

GG3

a total degree-GG4 element representing the universal first Chern class, up to the choice of normalizing constants and sign conventions. Closedness is with respect to the total differential GG5 (Suzuki, 2017).

In the simplicial de Rham complex of GG6, the full Chern character is realized by explicit cocycles obtained from Dupont’s universal curvature. For GG7, the invariant polynomials

GG8

produce the universal classes GG9. The case NG(q)=GqNG(q)=G^q0 is precisely the simplicial realization of NG(q)=GqNG(q)=G^q1 (Suzuki, 2013).

The smooth simplicial set construction gives the same degree-two class in a different model. For NG(q)=GqNG(q)=G^q2 or NG(q)=GqNG(q)=G^q3, the universal class attached to the linear invariant polynomial NG(q)=GqNG(q)=G^q4 is the universal real first Chern class in

NG(q)=GqNG(q)=G^q5

and under NG(q)=GqNG(q)=G^q6 it becomes the ordinary universal NG(q)=GqNG(q)=G^q7 in NG(q)=GqNG(q)=G^q8 (Savelyev, 2021).

3. Transgression and simplicial Chern–Simons forms

Because NG(q)=GqNG(q)=G^q9 for PG(q)=Gq+1,PG(q)=G^{q+1},0, every Bott–Shulman–Stasheff cocycle on PG(q)=Gq+1,PG(q)=G^{q+1},1 pulls back to an exact cocycle on PG(q)=Gq+1,PG(q)=G^{q+1},2. If

PG(q)=Gq+1,PG(q)=G^{q+1},3

then

PG(q)=Gq+1,PG(q)=G^{q+1},4

for some PG(q)=Gq+1,PG(q)=G^{q+1},5-cochain PG(q)=Gq+1,PG(q)=G^{q+1},6. These are the simplicial Chern–Simons forms. For the first Chern class, the transgression identity is

PG(q)=Gq+1,PG(q)=G^{q+1},7

the direct simplicial analogue of the ordinary Chern–Simons transgression formula (Suzuki, 2017).

The torus case PG(q)=Gq+1,PG(q)=G^{q+1},8 is especially explicit. Writing PG(q)=Gq+1,PG(q)=G^{q+1},9 on GG0, Suzuki gives the GG1-th Chern character cocycle on GG2 by

GG3

For GG4,

GG5

The associated Chern–Simons form on GG6 is

GG7

and it satisfies

GG8

For GG9, the Chern class and Chern character formulas coincide, so this is the simplicial first Chern class together with its universal primitive (Suzuki, 2017).

A related transgressive description appears in the local truncated simplicial de Rham complex. Suzuki proves Brylinski’s conjecture by constructing a local cocycle γ:PGNG,γ(g0,,gq)=(g0g11,g1g21,,gq1gq1)\gamma:PG\to NG,\qquad \gamma(g_0,\dots,g_q)=(g_0g_1^{-1},\,g_1g_2^{-1},\,\dots,\,g_{q-1}g_q^{-1})0 whose boundary maps to the Bott–Shulman–Stasheff form representing γ:PGNG,γ(g0,,gq)=(g0g11,g1g21,,gq1gq1)\gamma:PG\to NG,\qquad \gamma(g_0,\dots,g_q)=(g_0g_1^{-1},\,g_1g_2^{-1},\,\dots,\,g_{q-1}g_q^{-1})1. The same mechanism applies in degree γ:PGNG,γ(g0,,gq)=(g0g11,g1g21,,gq1gq1)\gamma:PG\to NG,\qquad \gamma(g_0,\dots,g_q)=(g_0g_1^{-1},\,g_1g_2^{-1},\,\dots,\,g_{q-1}g_q^{-1})2, so the universal degree-one local cochain transgresses the simplicial representative of γ:PGNG,γ(g0,,gq)=(g0g11,g1g21,,gq1gq1)\gamma:PG\to NG,\qquad \gamma(g_0,\dots,g_q)=(g_0g_1^{-1},\,g_1g_2^{-1},\,\dots,\,g_{q-1}g_q^{-1})3 (Suzuki, 2013).

4. Combinatorial formulas on triangulated γ:PGNG,γ(g0,,gq)=(g0g11,g1g21,,gq1gq1)\gamma:PG\to NG,\qquad \gamma(g_0,\dots,g_q)=(g_0g_1^{-1},\,g_1g_2^{-1},\,\dots,\,g_{q-1}g_q^{-1})4-bundles

A different, explicitly combinatorial meaning of simplicial first Chern class arises for triangulated circle bundles. One paper states that a “trivial calculation” based on Kontsevich’s differential γ:PGNG,γ(g0,,gq)=(g0g11,g1g21,,gq1gq1)\gamma:PG\to NG,\qquad \gamma(g_0,\dots,g_q)=(g_0g_1^{-1},\,g_1g_2^{-1},\,\dots,\,g_{q-1}g_q^{-1})5-form yields “very simple rational combinatorial characteristics (we call it ‘curvature’) of a triangulated γ:PGNG,γ(g0,,gq)=(g0g11,g1g21,,gq1gq1)\gamma:PG\to NG,\qquad \gamma(g_0,\dots,g_q)=(g_0g_1^{-1},\,g_1g_2^{-1},\,\dots,\,g_{q-1}g_q^{-1})6 bundle over a 2-simplex, which is a local combinatorial formula for the first Chern class”. The curvature is “expressed in terms of cyclic word in 3-character alphabet associated to the bundle”, and “from the point of view of simplicial combinatorics the word is a canonical shelling of the total complex” (Mnev, 2011).

A more systematic formulation replaces cyclic words by necklaces. For an elementary simplicial circle bundle over an ordered simplex γ:PGNG,γ(g0,,gq)=(g0g11,g1g21,,gq1gq1)\gamma:PG\to NG,\qquad \gamma(g_0,\dots,g_q)=(g_0g_1^{-1},\,g_1g_2^{-1},\,\dots,\,g_{q-1}g_q^{-1})7, the oriented fiber circle determines a surjective word

γ:PGNG,γ(g0,,gq)=(g0g11,g1g21,,gq1gq1)\gamma:PG\to NG,\qquad \gamma(g_0,\dots,g_q)=(g_0g_1^{-1},\,g_1g_2^{-1},\,\dots,\,g_{q-1}g_q^{-1})8

well-defined up to cyclic shift, hence an oriented necklace. Proper subwords select exactly one occurrence of each symbol, and their permutation parity defines the rational parity

γ:PGNG,γ(g0,,gq)=(g0g11,g1g21,,gq1gq1)\gamma:PG\to NG,\qquad \gamma(g_0,\dots,g_q)=(g_0g_1^{-1},\,g_1g_2^{-1},\,\dots,\,g_{q-1}g_q^{-1})9

For an elementary simplicial circle bundle EGBGEG\to BG0, the local coefficient of EGBGEG\to BG1 is

EGBGEG\to BG2

where EGBGEG\to BG3 is the associated necklace. This defines a rational simplicial local formula for the EGBGEG\to BG4-th power of the first Chern class. In particular, for EGBGEG\to BG5,

EGBGEG\to BG6

so the first Chern class of a triangulated circle bundle is represented on each EGBGEG\to BG7-simplex by a rational number computed from the parity of the associated necklace (Mnev et al., 2016).

The derivation is again Chern–Weil in origin. The necklace determines a normalized matrix EGBGEG\to BG8, this matrix defines a map of simplices, and pullback of Kontsevich’s cyclic invariant connection form on the universal cyclic bundle yields the local coefficient after integration. In this sense, the simplicial first Chern class is simultaneously combinatorial and universal (Mnev et al., 2016).

5. Čech nerves, coherent sheaves, and holomorphic refinements

On a complex manifold EGBGEG\to BG9 with a locally finite Stein cover NGNG00, the Čech nerve

NGNG01

is a simplicial complex manifold. A global holomorphic vector bundle pulls back to a simplicial bundle on this nerve, and Green’s barycentric connection

NGNG02

is an admissible simplicial connection. Its curvature NGNG03 is an endomorphism-valued simplicial NGNG04-form, and the simplicial first Chern form is

NGNG05

Dupont fiber integration sends this to the Čech–de Rham bicomplex. For a global vector bundle NGNG06, the degree-one case recovers the classical Čech representative: NGNG07 and for a line bundle NGNG08 with transition functions NGNG09,

NGNG10

Thus the simplicial first Chern class agrees with the usual first Chern class from the exponential sequence (Hosgood, 2020).

The formal foundations for this construction are developed using admissible simplicial connections and Green complexes on Čech nerves. A simplicial connection generated in degree zero is built from local connections by barycentric interpolation, and on Green complexes such connections are admissible. This is the structural condition that makes evaluation of invariant polynomials on simplicial curvature possible (Hosgood, 2020).

There is also a purely holomorphic version in which the Chern character is a map of simplicial presheaves

NGNG11

After evaluation on the Čech nerve of a good cover and passage to totalization, a bundle with local holomorphic connections and transition functions NGNG12 maps to a Čech cocycle with components

NGNG13

For a line bundle, the degree-two component is the Čech NGNG14-cocycle

NGNG15

which represents the first Chern class in Hodge cohomology (Glass et al., 2019).

This simplicial-presheaf viewpoint extends further. The simplicial presheaf NGNG16 of infinity vector bundles carries a Chern character map NGNG17, and on connected components after Čech sheafification it recovers the Toledo–Tong and O’Brian–Toledo–Tong Chern character of coherent sheaves. The degree-two piece is therefore the first Chern class in the same generalized sense, now available for stacks and equivariant settings as well (Glass et al., 2022).

The adjective “simplicial” is used in several non-equivalent ways, and the distinction matters. In toric geometry, a complete simplicial toric variety is defined by a simplicial fan, and the codimension-one part of its Chern–Schwartz–MacPherson class is

NGNG18

When NGNG19 is smooth, this equals the ordinary first Chern class NGNG20; in the simplicial, possibly singular case, it is the natural degree-one extension appearing in the CSM framework (Helmer, 2015).

In Hodge-theoretic moduli problems, one encounters a stacky or simplicial interpretation rather than a simplicial manifold of group type. For moduli of polarized Calabi–Yau manifolds, the first Chern form of the tangent bundle with the Hodge metric or the Weil–Petersson metric extends as a current to a normal-crossing compactification and represents the first Chern class of the canonical extension of the tangent bundle. The paper also explains that, from a simplicial or stacky viewpoint, these curvature forms represent the first Chern class in stack cohomology once an atlas or simplicial resolution is chosen (Liu et al., 2014).

Differential cohomology gives yet another refinement. There is a unique natural transformation

NGNG21

compatible with the underlying topological NGNG22 and with the curvature map. Although not formulated in simplicial language, this construction is model-independent and adapts naturally to simplicial settings, because it is defined by universal homotopy-theoretic properties rather than by a particular differential form model (0907.2504).

A recent computational realization makes the simplicial first Chern class entirely discrete. For a complex line bundle of local polarization vectors over a simplicial mesh NGNG23 approximating a sphere around a Weyl point, one first passes to a real rank-NGNG24 bundle, computes edge rotations NGNG25 by an orthogonal Procrustes problem, extracts angles NGNG26, and then defines on each triangle

NGNG27

This integer NGNG28-cochain is the simplicial Euler class of the real bundle and hence the simplicial first Chern class of the original complex line bundle. The resulting Chern number is gauge invariant, derivative free, structure preserving, and robust to noise, and it is used to count topological interface modes via the spectral flow–monopole correspondence (Bohlsen et al., 1 Aug 2025).

Taken together, these constructions show that the simplicial first Chern class is not a single formula but a family of equivalent realizations of NGNG29 on simplicial objects: a universal Bott–Shulman–Stasheff cocycle on NGNG30, a transgressed class on NGNG31, a local rational cocycle on triangulated NGNG32-bundles, a Čech–simplicial representative on nerves of covers, a characteristic class of simplicial presheaves and stacks, and, in recent computational work, an integer NGNG33-cochain on a simplicial mesh. The unifying principle is that NGNG34 is represented by data compatible with faces, degeneracies, and classifying maps, so that simplicial or combinatorial models recover the same characteristic class as ordinary Chern–Weil theory.

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