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Reduction Operations and Structural Characterizations of S1S^1-Flows in Graphs

Published 19 Aug 2026 in math.CO | (2608.18725v1)

Abstract: While every graph admitting a nowhere-zero $3$-flow also admits an S<sup>1S<sup>1-flow, the converse does not hold in general as shown by Thomassen (2014). In this paper, we develop reduction techniques for S<sup>1S<sup>1-flows based on graph operations including bull-growth, $2$-sums, and wheel contractions. A key tool is the two-terminal S<sup>1S<sup>1-preflow, which enables us to prove that if a $2$-connected graph contains an odd wheel as a proper subgraph and contracting the wheel yields a graph with a nowhere-zero $3$-flow, then the original graph admits an S<sup>1S<sup>1-flow. As applications, we completely characterize S<sup>1S<sup>1-flows in two graph classes: a triangularly connected graph admits an S<sup>1S<sup>1-flow if and only if it is not an odd wheel; and a graph containing a spanning triangle-tree admits an S<sup>1S<sup>1-flow if and only if it is not an odd crystal.

Authors (4)

Summary

  • The paper develops bull-growth, generalized 2-sum, wheel-contraction, and preflow techniques that preserve or construct S¹-flows under structural reductions.
  • Bridgeless triangularly connected graphs admit an S¹-flow exactly when they are not odd wheels, covering locally connected, squared, and 2-connected chordal graph classes.
  • Graphs with a spanning triangle-tree admit an S¹-flow exactly when they are not odd crystals, while the paper conjectures that every S¹-flow graph has a nowhere-zero 4-flow.

Context and motivation

Integer flow theory, introduced by Tutte as the dual of vertex coloring, has been extended to real-valued flows by Goddyn, Tarsi, and Zhang, and further to vector flows by Jain and Thomassen. This paper, by Li, Li, Luo, and Su (2608.18725), concerns S1S^1-flows: assignments of unit vectors in R2\mathbb{R}^2 to edges satisfying the conservation condition f(v)=0\partial f(v)=\mathbf{0} at every vertex. Thomassen established that every graph with a nowhere-zero $3$-flow admits an S1S^1-flow (via an R3R_3-flow of cube roots of unity), that the converse holds for cubic graphs if and only if the graph is bipartite, but fails in general: graphs built by repeated $2$-sums of copies of K4K_4 admit S1S^1-flows yet no nowhere-zero $3$-flow. Wang et al. posed the problem of characterizing conditions under which an R2\mathbb{R}^20-flow forces a nowhere-zero R2\mathbb{R}^21-flow, obtaining partial results via rank conditions on the flow and degree-R2\mathbb{R}^22 structure. The present paper attacks this problem from the structural side, developing reduction operations—bull-growth, generalized R2\mathbb{R}^23-sums, and wheel contractions—and using them to obtain complete characterizations of R2\mathbb{R}^24-flows in two graph classes.

Reduction operations

The first reduction shows that the bull-growth operation preserves R2\mathbb{R}^25-flows. Given a graph R2\mathbb{R}^26, the bull-growth replaces an edge R2\mathbb{R}^27 (or a non-edge when R2\mathbb{R}^28) by two adjacent R2\mathbb{R}^29-vertices f(v)=0\partial f(v)=\mathbf{0}0 sharing a common neighbor f(v)=0\partial f(v)=\mathbf{0}1. The proof in the case f(v)=0\partial f(v)=\mathbf{0}2 is a direct construction: orient all edges into f(v)=0\partial f(v)=\mathbf{0}3 and out of f(v)=0\partial f(v)=\mathbf{0}4, copy the value f(v)=0\partial f(v)=\mathbf{0}5 onto f(v)=0\partial f(v)=\mathbf{0}6 and f(v)=0\partial f(v)=\mathbf{0}7, and use the fact that any unit vector extends to a triple of unit vectors summing to zero to fill the remaining three edges. Consequently, if f(v)=0\partial f(v)=\mathbf{0}8 admits an f(v)=0\partial f(v)=\mathbf{0}9-flow then so does its bull-growth; this is used later in contrapositive form, since it implies bull-reductions of counterexamples remain counterexamples.

For $3$0-sums, the paper proves a closure theorem stronger than mere preservation: if $3$1 and both factors admit $3$2-flows, then replacing $3$3 by any number $3$4 of parallel edges still yields an $3$5-flow. The argument rotates one factor's flow so that the values on the common edge are either opposite ($3$6 even) or separated by $3$7 ($3$8 odd), then distributes their sum across the parallel edges. The mixed case—where one factor has only a nowhere-zero $3$9-flow after contracting S1S^10—is handled by two complementary tools:

The two-terminal preflow lemma: if S1S^11 has a nowhere-zero S1S^12-flow, then for any distinct vertices S1S^13 and any prescribed unit vector S1S^14, there exists an S1S^15-preflow on S1S^16 whose boundary is S1S^17 at S1S^18, S1S^19 at R3R_30, and zero elsewhere. The construction modifies a R3R_31-valued R3R_32-flow along a directed R3R_33–R3R_34 path, extracts an Euler-trail parity decomposition, and encodes the result geometrically using the vertices of an equilateral triangle, so that each edge receives a vector of norm exactly R3R_35.

A boundary lemma for odd wheels: every nonzero zero-sum boundary R3R_36 on an odd wheel can be realized by a nowhere-zero R3R_37-flow, via a sign-change recursion along the rim. A companion lemma gives odd wheels the analogous preflow property with arbitrary boundary vectors of norm R3R_38, constructed explicitly in the complex plane using sixth roots of unity.

Combining these yields the main reduction theorem for R3R_39-sums: if each factor either admits an $2$0-flow or has a contraction $2$1 admitting a nowhere-zero $2$2-flow, then the sum admits an $2$3-flow. In the hardest subcase (both factors have only contractive $2$4-flows), the preflow lemma supplies prefows on $2$5 and $2$6 whose boundary directions are chosen so that the angle between them satisfies $2$7, making the compensating value on $2$8 itself a unit vector.

Finally, the wheel-contraction theorem states that if a $2$9-connected graph contains a wheel K4K_40 as a proper subgraph and K4K_41 admits a nowhere-zero K4K_42-flow, then K4K_43 admits an K4K_44-flow. If K4K_45 is even or non-induced, K4K_46 contains a K4K_47-connected subgraph (using that K4K_48 and even wheels are K4K_49-connected), so S1S^10 actually has a nowhere-zero S1S^11-flow. For induced odd wheels, the boundary induced by the flow on S1S^12 is either nonzero—in which case the boundary lemma extends it to a genuine S1S^13-flow—or identically zero, in which case a component of S1S^14 meeting the wheel in at least two vertices (guaranteed by S1S^15-connectivity) is matched against the wheel via the two preflow lemmas with a common boundary vector.

Triangularly connected graphs

A graph is triangularly connected if every pair of edges lies on a common triangle-path. Fan et al. characterized such graphs without nowhere-zero S1S^16-flows as those reducible by S1S^17-sums to odd wheels. Building on this, the paper proves:

Theorem. A bridgeless triangularly connected graph admits an S1S^18-flow if and only if it is not an odd wheel.

The necessity direction uses Wang et al.'s criterion: in an odd wheel, the degree-S1S^19 vertices induce a connected cycle while removing them leaves an acyclic graph, and odd wheels have no $3$0-flow. For sufficiency, a minimal counterexample must decompose as a $3$1-sum $3$2 with $3$3 an odd wheel and $3$4 triangularly connected without a $3$5-flow; minimality forces $3$6 to be an odd wheel, and since $3$7 always admits a $3$8-flow (proved via planar duality and explicit colorings), the general $3$9-sum theorem produces an R2\mathbb{R}^200-flow—a contradiction. Because locally connected graphs, squares of connected graphs, and R2\mathbb{R}^201-connected chordal graphs are triangularly connected, the result immediately applies to these classes: every bridgeless member other than an odd wheel admits an R2\mathbb{R}^202-flow.

Graphs with spanning triangle-trees

A triangle-tree is built from a triangle by repeatedly adding a vertex adjacent to exactly two adjacent existing vertices; a crystal is a triangle-path plus an edge joining its two leaves, and is odd if all degrees are odd. The second main characterization reads:

Theorem. A bridgeless graph containing a spanning triangle-tree admits an R2\mathbb{R}^203-flow if and only if it is not an odd crystal.

The exclusion of odd crystals rests on a rigidity argument. At any R2\mathbb{R}^204-vertex carrying an R2\mathbb{R}^205-flow, the incident values (up to sign) form a regular hexagon on the unit circle. An algebraic lemma over the Eisenstein integers R2\mathbb{R}^206 then shows that if several hexagon vertices plus two additional unit vectors sum to zero with the latter not canceling, the two extra vectors must also be hexagon vertices—the key cases being squared norms R2\mathbb{R}^207, with R2\mathbb{R}^208 excluded by the congruence R2\mathbb{R}^209. Using the canonical outerplane embedding of a triangle-path (whose backbone is a path with pendant degree-R2\mathbb{R}^210 vertices), a minimal-counterexample argument propagates hexagon membership from one leaf across the backbone; the propagation must break at some backbone vertex R2\mathbb{R}^211, but the lemma forces the two exceptional edges back into the hexagon unless they cancel—which would allow a splitting operation producing a smaller odd crystal with an R2\mathbb{R}^212-flow, contradicting minimality. Hence no odd crystal admits an R2\mathbb{R}^213-flow.

For the converse, the paper invokes Li, Li, and Wang's structure theorem: a graph with a spanning triangle-tree and no R2\mathbb{R}^214-flow is either R2\mathbb{R}^215 or a bull-growth of a smaller such graph. Minimality reduces to the case where the smaller graph is an odd crystal, and a combinatorial lemma shows that bull-growing an odd crystal either destroys the spanning triangle-tree property, yields another odd crystal, or produces an R2\mathbb{R}^216-flow (via a R2\mathbb{R}^217-sum with R2\mathbb{R}^218 or with a wheel)—each alternative contradicting the choice of counterexample.

Notably, the two classes characterized are incomparable: the paper exhibits a triangularly connected graph (a wheel with rim-pendant triangles) containing no spanning triangle-tree, and a crystal that is not triangularly connected because its added edge lies in no triangle.

Limitations and open questions

The paper concedes that its reduction techniques do not settle the general relationship between R2\mathbb{R}^219-flows and integer flows. All known classes of graphs with R2\mathbb{R}^220-flows also admit nowhere-zero R2\mathbb{R}^221-flows, motivating the conjecture that every R2\mathbb{R}^222-flow graph admits a nowhere-zero R2\mathbb{R}^223-flow; the authors note that a minimal counterexample would have to be non-planar, non-cubic, and essentially R2\mathbb{R}^224-edge-connected, but state plainly that they have neither proof nor disproof. They also leave open whether the wheel in the contraction theorem can be replaced by arbitrary one-edge-deletions of R2\mathbb{R}^225-connected graphs, observing that R2\mathbb{R}^226 shows some finite exceptions are unavoidable. Similar contraction results for graph classes beyond wheels are deferred to future work. The sufficiency proofs also rely structurally on prior characterizations (Fan et al.; Li–Li–Wang), so the method's reach is bounded by the availability of analogous structure theorems for other classes.

Conclusion

This paper develops a coherent toolkit—bull-growth preservation, parallel-edge closure under R2\mathbb{R}^227-sums, two-terminal R2\mathbb{R}^228-preflows with R2\mathbb{R}^229-norm boundaries, and boundary-realization lemmas for odd wheels—for lifting flows from reduced graphs to larger ones. Its main results give exact structural obstructions to R2\mathbb{R}^230-flows in two natural classes: odd wheels among triangularly connected graphs, and odd crystals among graphs with spanning triangle-trees. In both cases the obstruction coincides with the absence of a nowhere-zero R2\mathbb{R}^231-flow, providing new instances where the R2\mathbb{R}^232-flow and R2\mathbb{R}^233-flow existence questions align, while the authors' own conjecture on R2\mathbb{R}^234-flows marks precisely where current understanding ends.

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