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Pairwise circuit data and the ternary projective model


This note asks whether the ordered-realization criterion of the collision-trade note, applied to overlapping circuits, can make the short and long circuits forced in a hypothetical counterexample incompatible. Through pairs of circuits whose orientations are free it cannot: all such data, including every restriction on mixed-sign overlaps, is satisfied by a model with (3d−1)/2(3^d-1)/2 points that contains circuits of every size. A common increasing positive realization requires one choice of element signs making every circuit two-sided, and the model already fails this necessary condition. Orientation of single relations in a common order, with unique completion, already gives the target for d≤3d\le3; whether the ordered pairwise conditions imply it for larger dd is open. The arguments below are Plasma AI's author-recorded deductions; none proves or refutes the target. The sign-free countermodel is not a model of the global cone condition.

Notation follows the collision-trade note. P={p1<⋯<pn}P=\{p_1<\cdots<p_n\} is a set of positive reals, d=d(P)d=d(P) is the maximum cardinality of a dissociated subset, LL is the real span of the ternary relations of PP, and τ(u)j=∑i≥jui\tau(u)_j=\sum_{i\ge j}u_i. A circuit is an inclusion-minimal support of a nonzero ternary relation; its relation uC∈{±1}Cu_C\in\{\pm1\}^C is unique up to sign. Every ternary vector of LL is a relation, since L⊆p⊥L\subseteq p^\perp.

The realization cone with free signs and order

Proposition 1. Let L⊆RnL\subseteq\mathbb R^n be spanned by integer vectors. The following are equivalent.

  1. For some permutation π\pi of the coordinates and some signs σ∈{±1}n\sigma\in\{\pm1\}^n, the subspace πσL\pi\sigma L satisfies the criterion τ(πσL)∩R≥0n={0}\tau(\pi\sigma L)\cap\mathbb R^n_{\ge0}=\{0\}.
  2. LL contains no nonzero ternary vector whose support has at most two elements.

When the second condition holds, there are signs σ\sigma and distinct positive integers ∣a1∣,…,∣an∣|a_1|,\ldots,|a_n| whose ternary relations are exactly the vectors σt\sigma t with tt a nonzero ternary vector of LL. In particular the dependent subsets of that positive set are exactly the subsets of [n][n] that support a nonzero ternary vector of LL.

Proof. If increasing positive reals annihilate πσL\pi\sigma L, undoing π\pi and σ\sigma gives a vector a⊥La\perp L whose coordinates are nonzero and have distinct absolute values. A ternary vector ±ei\pm e_i in LL would force ai=0a_i=0, and ±ei±ej\pm e_i\pm e_j would force ∣ai∣=∣aj∣|a_i|=|a_j|.

Conversely, L⊥L^\perp is a rational subspace and (L⊥)⊥=L(L^\perp)^\perp=L. Under the second condition the subspaces L⊥∩{xi=0}L^\perp\cap\{x_i=0\} and L⊥∩{xi=±xj}L^\perp\cap\{x_i=\pm x_j\} are proper, as is L⊥∩r⊥L^\perp\cap r^\perp for every ternary r∉Lr\notin L. Choose a rational point a∈L⊥a\in L^\perp outside their finite union and clear denominators. Put σi=sign⁡ai\sigma_i=\operatorname{sign}a_i. The integers ∣ai∣|a_i| are positive and distinct. A ternary tt is a relation of (∣ai∣)(|a_i|) exactly when σt⊥a\sigma t\perp a, that is, when σt∈L\sigma t\in L. Sorting the ∣ai∣|a_i| gives π\pi, and the criterion holds by its necessity half, summation by parts. □\square

Thus, once signs and order are free, the cone criterion says only that the relation space implies no relation of the form eie_i or ei±eje_i\pm e_j. This is the column condition of the corank-one note (distinct nonzero columns with no antipodal pair) in dual form. Thus the sign-free realization question is exactly whether the full real span contains one of these forbidden vectors. For prescribed signs and order, merely making every circuit two-sided is necessary but not sufficient: the cone condition still applies to all real linear combinations. The sections below keep these distinct requirements separate.

Two-circuit spans

Proposition 2. Let uu and vv be the relations of distinct circuits CC and DD, and put I=C∩DI=C\cap D. Fix an orientation of vv and put

I+={i∈I:ui=vi},I−={i∈I:ui=−vi}.I_+=\{i\in I:u_i=v_i\},\qquad I_-=\{i\in I:u_i=-v_i\}.

The nonzero ternary vectors of span⁡(u,v)\operatorname{span}(u,v) are exactly:

  • ±u\pm u, ±v\pm v and ±u±v\pm u\pm v when II is empty;
  • ±u\pm u, ±v\pm v and ±(u−v)\pm(u-v) when II is nonempty and I−I_- is empty, a compatible pair (the case of empty I+I_+ is the same after reversing vv);
  • ±u\pm u and ±v\pm v only, when I+I_+ and I−I_- are both nonempty, a mixed pair.

Proof. Neither circuit contains the other, so C∖DC\setminus D and D∖CD\setminus C are nonempty. On them αu+βv\alpha u+\beta v equals αu\alpha u and βv\beta v, so a ternary combination has α,β∈{−1,0,1}\alpha,\beta\in\{-1,0,1\}. On I+I_+ and I−I_- it equals (α+β)u(\alpha+\beta)u and (α−β)u(\alpha-\beta)u, which must also be ternary when those sets are nonempty. Enumerating the eight nonzero pairs (α,β)(\alpha,\beta) gives the list. □\square

By Proposition 1 applied to span⁡(u,v)\operatorname{span}(u,v), two circuits restrict each other only when a listed vector has support at most two. The circuits have at least three points, and C∪DC\cup D has at least six when they are disjoint. For a compatible pair, ∣C△D∣=∣C∖D∣+∣D∖C∣≥2|C\triangle D|=|C\setminus D|+|D\setminus C|\ge2, with equality exactly when C=T∪{x}C=T\cup\{x\} and D=T∪{y}D=T\cup\{y\} and the relations agree on TT up to sign: a compatible exchange pair. Every other pair is realized by positive integers having exactly the relations of its span. Consequently:

  1. Circuits of different sizes never restrict each other pairwise. In particular a short circuit and a long circuit do not, whatever their overlap and relative signs.
  2. A mixed overlap of any size imposes no pairwise restriction.
  3. The only pairwise restriction is unique completion: for an (s−1)(s-1)-set TT and a sign pattern on TT, at most one point completes a circuit. This is precisely the input of the circuit-covering inequality (2) of the collision-trade note. A compatible pair also forces a relation on C△DC\triangle D, so that set contains a circuit. This closure is a further constraint on the whole family, but the model below satisfies it too.

The ternary projective model

Let XX be a set of representatives of the (3d−1)/2(3^d-1)/2 classes {±x}\{\pm x\} of nonzero vectors of F3d\mathbb F_3^d. Over F3\mathbb F_3 the coefficients −1,0,1-1,0,1 are all the coefficients, so the ternary relations on XX are its linear relations, and its circuits are those of the projective geometry PG(d−1,3)\mathrm{PG}(d-1,3), each with its coefficient vector.

Theorem 3.

  1. Every (d+1)(d+1)-subset of XX supports a circuit, and a basis supports none.
  2. Each circuit has one relation up to sign; no two circuits form a compatible exchange pair; and for every compatible pair the set C△DC\triangle D contains a circuit.
  3. For every ss with 3≤s≤d+13\le s\le d+1 there is a circuit with ss points.
  4. ∣X∣=(3d−1)/2|X|=(3^d-1)/2, which is at least 2d2^d for every d≥2d\ge2.

Conversely, let a family of signed sets with at least three points each be given on [n][n], with no two members forming a compatible exchange pair, such that every (d+1)(d+1)-subset contains a member and some dd-subset contains none. Then n≤(3d−1)/2n\le(3^d-1)/2.

Proof. For the first item, a subset is dependent over F3\mathbb F_3 exactly when it supports a nonzero ternary relation. Two relations on one circuit that are not proportional have a combination vanishing at a point of the circuit, leaving a relation on a proper subset; the only scalars are ±1\pm1. If C=T∪{x}C=T\cup\{x\} and D=T∪{y}D=T\cup\{y\} have relations agreeing on TT, then uxx=−∑t∈Tutt=vyyu_xx=-\sum_{t\in T}u_tt=v_yy, so x=±yx=\pm y, which is impossible for distinct representatives. For a compatible pair, u−vu-v is an integer vector with entries in {−1,0,1}\{-1,0,1\} that vanishes on C∩DC\cap D; it is a nonzero relation, so its support contains a circuit. For the third item take e1,…,es−1,e1+⋯+es−1e_1,\ldots,e_{s-1},e_1+\cdots+e_{s-1}: they are dependent, and every s−1s-1 of them are independent.

For the converse, let DD be a dd-subset containing no member. For each x∉Dx\notin D, the set D∪{x}D\cup\{x\} contains a member CxC_x, which must contain xx. Normalize its relation to have coefficient 11 at xx and let εx∈{−1,0,1}D\varepsilon_x\in\{-1,0,1\}^D be minus its restriction to DD; its support has at least two points. If εx=±εy\varepsilon_x=\pm\varepsilon_y for x≠yx\ne y, then CxC_x and CyC_y are a compatible exchange pair. Hence x↦±εxx\mapsto\pm\varepsilon_x is injective into the classes of ternary vectors on DD with support at least two, and

n−d≤3d−12−d.□n-d\le\frac{3^d-1}2-d. \qquad\square

So (3d−1)/2(3^d-1)/2 is the exact maximum permitted by pairwise circuit data when orientations are free, and it is the trivial ternary bound. The model satisfies the circuit-covering inequality (2) because that inequality uses only such data. For d≥9d\ge9 it has both a circuit of at most six points and circuits with more than θ(d+1)\theta(d+1) points, and it has n≥2dn\ge2^d. An overlap restriction derived from pairs of circuits with free orientation, including every restriction on mixed overlaps, holds in this model, so it cannot make the forced short and long circuits incompatible.

For d=2d=2 the model is four signed triples on four points. With x1=(1,0)x_1=(1,0), x2=(0,1)x_2=(0,1), x3=(1,1)x_3=(1,1) and x4=(1,2)x_4=(1,2), three of its relations are

u1=e1+e2−e3,u2=e1−e2−e4,u3=e1+e3+e4,u_1=e_1+e_2-e_3,\qquad u_2=e_1-e_2-e_4,\qquad u_3=e_1+e_3+e_4,

and every two of its four triples meet in a mixed pair of points. Over the reals, u1+u2+u3=3e1u_1+u_2+u_3=3e_1, so these three circuits imply p1=0p_1=0.

Where characteristic zero enters

As sign-free data, the model differs from a real set only through combinations of at least three circuits. Two such combinations are the following.

Lemma 4 (mixed overlaps). For a mixed pair, put t±=u∣C∖D±v∣D∖Ct_\pm=u|_{C\setminus D}\pm v|_{D\setminus C}. Then

u±v=2u∣I±+t±.u\pm v=2u|_{I_\pm}+t_\pm .

For a real set, no ternary vector t±+c u∣I±t_\pm+c\,u|_{I_\pm} with c∈{−1,0,1}c\in\{-1,0,1\} is a relation. In the projective model t±−u∣I±t_\pm-u|_{I_\pm} is always a relation.

Proof. The vector u∣I±u|_{I_\pm} is a nonzero ternary vector on a proper subset of the circuit CC, so it is not in LL. Since t±+c u∣I±=(u±v)+(c−2)u∣I±t_\pm+c\,u|_{I_\pm}=(u\pm v)+(c-2)u|_{I_\pm}, it lies in LL only for c=2c=2. Modulo three, 2≡−12\equiv-1. □\square

Thus replacing the coefficient two by minus one gives a ternary relation over F3\mathbb F_3, whose support contains a circuit, but never a relation over the reals. Minimality of the whole new support is not asserted. The relations uu, vv and w=t+−u∣I+w=t_+-u|_{I_+} satisfy u+v−w=3u∣I+u+v-w=3u|_{I_+}; the four triples above are an instance.

Lemma 5 (completion paths). Fix a set UU and a sign vector σ\sigma on UU up to sign. Join xx and yy outside UU when U∪{x,y}U\cup\{x,y\} is a circuit whose relation, normalized to restrict to σ\sigma on UU, is σ+aex+bey\sigma+ae_x+be_y. For a real set this graph is a disjoint union of paths.

Proof. Unique completion allows at most one edge at xx for each sign aa, and two edges at xx carry opposite signs there. Along a cycle x1,…,xkx_1,\ldots,x_k with relations ui=σ+aiexi+biexi+1u_i=\sigma+a_ie_{x_i}+b_ie_{x_{i+1}} this gives bi−1=−aib_{i-1}=-a_i, so ∑iui=kσ∈L\sum_iu_i=k\sigma\in L. But σ\sigma is a nonzero ternary vector on a proper subset of a circuit. □\square

In positive terms every edge joins a pair with x+y=Gx+y=G or ∣x−y∣=G|x-y|=G, where G=∣σ⋅pU∣G=|\sigma\cdot p_U|. Along a path the signed values aipxia_ip_{x_i} change by σ⋅pU\sigma\cdot p_U at each step, so a path consists of the absolute values of consecutive terms of an arithmetic progression. In the projective model the progressions have period three and the graphs contain triangles.

Count each circuit of size ss once for each of its (s2)\binom s2 pairs, over the 2s−3(ns−2)2^{s-3}\binom n{s-2} choices of UU and ±σ\pm\sigma, with at most n−s+1n-s+1 edges in a forest on n−s+2n-s+2 vertices. Following the derivation of (2) then gives

∑s=3R2s−2(d+1s)n−s+2≥1,\sum_{s=3}^{R}\frac{2^{s-2}\binom{d+1}{s}}{n-s+2}\ge1,

improving the denominator n−s+1n-s+1 of (2). At d=2d=2 this gives n≤3n\le3, which is sharp, whereas (2) allows the four-point model. At d=3d=3 it gives n≤13n\le13 instead of 1414; the true maximum is six. Beyond small dd the gain is a factor (n−s+1)/(n−s+2)(n-s+1)/(n-s+2). It is another separate support count and does not separate the forced short and long circuits.

What positive orientation adds

In a positive real set, each circuit relation has both sides nonempty. For a family of signed sets, call a choice of element signs a positive orientation if it makes every relation two-sided.

Proposition 6. For d≥2d\ge2 the projective model has no positive orientation.

Proof. Changing element signs replaces XX by another set RR of representatives. Suppose every circuit relation on RR is two-sided. For distinct x,y∈Rx,y\in R, the vector x+yx+y is nonzero and not ±x\pm x or ±y\pm y; let r=±(x+y)r=\pm(x+y) be its representative. The triple {x,y,r}\{x,y,r\} is a circuit with relation x+y∓r=0x+y\mp r=0, one-sided when r=−(x+y)r=-(x+y). Hence x+y∈Rx+y\in R. Take distinct x,y∈Rx,y\in R. Then a=x+y∈Ra=x+y\in R, so a+y=x−ya+y=x-y and a+x=y−xa+x=y-x also lie in RR. These are opposite nonzero vectors, a contradiction. □\square

The ordered form of pairwise realizability is therefore strictly stronger. Its data are a linear order of [n][n] and a positive relation for each member of the family. Its conditions are that every two members are annihilated by one increasing positive vector, and that the support of the eliminated relation of a compatible pair contains a member. For a single relation uu the first condition says that τ(u)\tau(u) takes both signs; for a three-point circuit it says that the largest element is the sum of the other two. For a pair it says that the points (τ(u)j,τ(v)j)(\tau(u)_j,\tau(v)_j), 1≤j≤n1\le j\le n, positively span R2\mathbb R^2.

Orientation of single relations already gives a bound well below the projective model. Put

f(k)=2k−1−(k⌊k/2⌋)+[k even] 1k/2+1(kk/2).f(k)=2^{k-1}-\binom k{\lfloor k/2\rfloor} +[k\text{ even}]\,\frac{1}{k/2+1}\binom k{k/2}.

Proposition 7 (greedy set from the top). Fix a linear order of [n][n] and a family of members with at least three points each, each with a relation whose tail profile takes both signs. Suppose that no two members form a compatible exchange pair and that every (d+1)(d+1)-subset contains a member. Then

n≤d+∑k=2d(dk)f(k).n\le d+\sum_{k=2}^{d}\binom dk f(k).

Proof. Scan [n][n] downward from the largest position, keeping a set GG that contains no member and adding each position whose addition keeps it so. Then ∣G∣≤d|G|\le d. A rejected position xx completes a member CxC_x whose other points lie in GG above xx, so xx is the least point of CxC_x. Put S=Cx∖{x}S=C_x\setminus\{x\} and k=∣S∣≥2k=|S|\ge2, and read the signs of the relation on SS from the top down as a walk, normalized to start with +1+1. Apart from zeros above SS, the tail profile takes the partial sums tk=1,…,t1t_k=1,\ldots,t_1 of this walk above xx, and the value t1±1t_1\pm1 at and below xx. If the walk stays nonnegative and ends at t1≥1t_1\ge1, every value is nonnegative and the relation is not satisfiable. Of the 2k−12^{k-1} walks, (k⌊k/2⌋)\binom k{\lfloor k/2\rfloor} stay nonnegative, and those among them that end at zero, a Catalan number when kk is even, remain satisfiable with the sign −1-1 at xx. So f(k)f(k) classes are available on each kk-subset of GG. Unique completion makes x↦(S,±x\mapsto(S,\pm signs)) injective, and the right side increases with ∣G∣|G|. □\square

The bound equals 33 and 7=2d−17=2^d-1 for d=2,3d=2,3, where sign-free pairwise data allow 44 and 1313 and real sets reach 33 and 66. Thus positive orientation of single relations, with unique completion, proves the target for d≤3d\le3. For d=4,5d=4,5 the bound is 1818 and 5151, against the targets 1515 and 3131 and the proof sketch's bounds 1414 and 4242. Asymptotically it is 123d(1−Θ(d−1/2))\tfrac12 3^d(1-\Theta(d^{-1/2})): the walk restriction removes only a polynomial fraction of the ternary classes, so this count cannot reach 2d2^d. This is a limitation of the displayed count. It does not construct a family attaining it, or prove that the single-relation ordered assumptions themselves fail to imply the target. The unused requirement that all (d+1)(d+1)-subsets, including those with several rejected points, contain a member could impose further restrictions.

Two further facts are proved.

  1. One-sided circuits. The bound n≤2d−1n\le2^d-1 for one-sided circuits in the collision-trade note holds under the ordered conditions, with DD chosen to minimize the sum of the positions of its elements. Its proof uses only single relations (a root is the largest element of its circuit), unique completion, and the closure that places a circuit inside the elimination support of a compatible pair.
  2. Order constrains pairs. Proposition 2 permits pairs that the order excludes. With positions 1<⋯<61<\cdots<6, the relations p3=p1+p2p_3=p_1+p_2 and p4+p6=p1+p2+p5p_4+p_6=p_1+p_2+p_5 are each satisfiable and agree on {1,2}\{1,2\}, with a symmetric difference of four points. Under the first, p4+p6−p1−p2−p5=(p4−p3)+(p6−p5)>0p_4+p_6-p_1-p_2-p_5=(p_4-p_3)+(p_6-p_5)>0, so no increasing positive vector satisfies both.

For a three-point circuit the pair condition can be stated exactly. This is the quantitative overlap restriction that the cone imposes between a short circuit and any other circuit.

Proposition 8. Let uu be the relation pc=pa+pbp_c=p_a+p_b with a<b<ca<b<c, and let vv be the relation of another member, satisfiable on its own. No increasing positive vector satisfies both if and only if, for ϵ=1\epsilon=1 or ϵ=−1\epsilon=-1, the profile w=ϵτ(v)w=\epsilon\tau(v) is nonnegative on (a,b](a,b] and on (c,n](c,n], and

min⁡j≤awj+min⁡b<j≤cwj≥0.\min_{j\le a}w_j+\min_{b<j\le c}w_j\ge0.

Proof. The profile τ(u)\tau(u) equals −1-1 on [1,a][1,a], 00 on (a,b](a,b], 11 on (b,c](b,c] and 00 above cc. Infeasibility means ατ(u)+βτ(v)≥0\alpha\tau(u)+\beta\tau(v)\ge0 for some (α,β)≠0(\alpha,\beta)\ne0, the combination being nonzero because u,vu,v are independent and τ\tau is injective. Here β≠0\beta\ne0, since τ(u)\tau(u) takes both signs. Dividing by ∣β∣|\beta| and putting ϵ=sign⁡β\epsilon=\operatorname{sign}\beta and λ=α/∣β∣\lambda=\alpha/|\beta|, the condition reads w≥0w\ge0 on (a,b](a,b] and above cc, w≥λw\ge\lambda on [1,a][1,a], and w≥−λw\ge-\lambda on (b,c](b,c]. A suitable λ\lambda exists exactly when the displayed inequality holds. □\square

Above cc the restriction uses only the signs of the profile of vv. If it takes both signs above cc, or both signs on (a,b](a,b], the two relations are jointly realizable in the given order whatever their overlap. A long circuit whose profile changes sign above the largest element of a three-point circuit is therefore never excluded by it. Proposition 8 adds an orientation-dependent restriction to Proposition 2, but no contradiction between the forced short and long circuits follows from it.

Whether the ordered pairwise conditions, with the covering property, imply n≤2d−1n\le2^d-1 for d≥4d\ge4, or even n≤κdn\le\kappa^d for some κ<3\kappa<3, is open. A family satisfying them with n≥2dn\ge2^d would show that the ordered overlap restriction also fails. The projective model supplies no such family, and Proposition 7 is not evidence that one exists.

The pair condition for every short support

The cone test has an exact quantitative form for a pair of arbitrary circuit sizes, including all the short supports of sizes three through six forced by the high-girth argument. Put a=τ(u)a=\tau(u) and b=τ(v)b=\tau(v), where u,vu,v are independent and each profile takes both signs. Write J+J_+, J−J_- and J0J_0 for the coordinates where aa is positive, negative and zero. For ϵ∈{1,−1}\epsilon\in\{1,-1\} define

λϵ−=max⁡j∈J+−ϵbjaj,λϵ+=min⁡j∈J−−ϵbjaj.(5)\lambda_\epsilon^- =\max_{j\in J_+}\frac{-\epsilon b_j}{a_j},\qquad \lambda_\epsilon^+ =\min_{j\in J_-}\frac{-\epsilon b_j}{a_j}. \tag{5}

Proposition 9. No increasing positive vector annihilates both relations if and only if, for at least one choice of ϵ\epsilon,

ϵbj≥0(j∈J0),λϵ−≤λϵ+.(6)\epsilon b_j\ge0\quad(j\in J_0),\qquad \lambda_\epsilon^-\le\lambda_\epsilon^+. \tag{6}

Proof. By the cone criterion, infeasibility is equivalent to a nonzero combination αa+βb≥0\alpha a+\beta b\ge0. Since aa takes both signs, β≠0\beta\ne0. Divide by ∣β∣|\beta| and put λ=α/∣β∣\lambda=\alpha/|\beta| and ϵ=sign⁡β\epsilon=\operatorname{sign}\beta. The inequalities on J+J_+ say λ≥λϵ−\lambda\ge\lambda_\epsilon^-, those on J−J_- say λ≤λϵ+\lambda\le\lambda_\epsilon^+, and those on J0J_0 are exactly (6). Independence ensures that the resulting combination is nonzero. □\square

Thus every pair of actual circuits must violate (6) for both signs. This uses the relative positions and signs of the two circuits; their cardinalities and intersection size do not determine it. If bb takes both signs on J0J_0, both choices of ϵ\epsilon already fail. In particular, oscillation of the long relation's profile above the short circuit defeats this exclusion test. Proposition 8 is the case a=−1,0,1,0a=-1,0,1,0 on its four successive intervals.

No estimate has been obtained that combines these allowed profile patterns with covering every (d+1)(d+1)-set to contradict n≥2dn\ge2^d. The numerical inequality retained from the ordered argument is exactly Proposition 7: it gives n≤18n\le18 at d=4d=4, where the needed bound is 1515, and has base three asymptotically. The completion-path inequality is a separate support count, so it does not fill this gap. Passing the realization test for all pairs still leaves the full cone condition on combinations of three or more relations to be checked.

Retained examples

The 25-point K4,4K_{4,4} construction in the forest note contains both the four-point circuit

50025+19995=50010+2001050025+19995=50010+20010

and a seventeen-point circuit on D∪{50025}D\cup\{50025\}. The latter is

50025=2001(15+54+66+90+114+174+246−734),50025=2001\bigl(15+54+66+90+114+174+246-734\bigr),

where multiplication by 20012001 means using both copies of the eight-element block AA, once in AA and once in 2000A2000A. The forest note proves that DD is dissociated and this ternary representation is unique, so its full seventeen-element support is minimal. The four-point relation is minimal because its distinct positive entries have no additive triple. These circuits meet at 5002550025 and are jointly realized by the displayed positive integers; no cone certificate from them is possible. Here d=16d=16 and n=25n=25, far below the counterexample threshold. The coexistence therefore defeats an absolute ban on interacting short and long circuits, without testing the required exponential cardinality hypothesis.

In the seven-point set of the matching note every circuit has six points, each omitting one point, so every two circuits are an exchange pair sharing five points, and Proposition 2 forces every pair to be mixed. For example, the relations omitting 33 and 1515,

15+35+55=31+33+41,3+41+55=31+33+35,15+35+55=31+33+41,\qquad 3+41+55=31+33+35,

agree on 31,33,5531,33,55 and disagree on 35,4135,41. That set has only circuits of size d+1d+1, so it exhibits no coexistence of short and long circuits.

In the sharp six-point example {1,3,4,5,7,8}\{1,3,4,5,7,8\}, take u:p6=p1+p5u:p_6=p_1+p_5 and v:p1+p5=p2+p4v:p_1+p_5=p_2+p_4. Their profiles are (−1,0,0,0,0,1)(-1,0,0,0,0,1) and (0,−1,0,0,1,0)(0,-1,0,0,1,0), respectively. The second takes both signs where the first is zero, so (6) fails for both signs. Compatible elimination gives the existing circuit p6=p2+p4p_6=p_2+p_4. Conversely, the six-position infeasible example above has profiles (−1,0,1,0,0,0)(-1,0,1,0,0,0) and (−1,0,1,1,0,1)(-1,0,1,1,0,1): for ϵ=1\epsilon=1 both endpoints in (5) equal −1-1, and the second profile is nonnegative on J0J_0. Formula (6) excludes it.

For small dd the three relevant maxima compare as follows. At d=2d=2 real sets reach 33, sign-free pairwise data allow 44, and the ordered conditions allow 33. At d=3d=3 the values are 66, 1313 and at most 77. At d=4d=4 the real maximum is at most 1414, sign-free pairwise data allow 4040, and the ordered conditions allow at most 1818.

Remaining gap

The interaction between the two forced circuit sizes cannot come from pairs of circuits with free orientation; Theorem 3 rules this out at every dd. A successful inequality must use information beyond the sign-free pairwise conditions. Examples of such information are the fixed order and signs in (6), and combinations of at least three circuits, such as the characteristic three obstruction in Lemma 4. Other arguments may use the integer realization directly, as the high-girth bound and the binary residue tree of the proof sketch do. The projective model has no integer realization. The ordered conditions settle d≤3d\le3 through single relations. The remaining question is whether covering, compatible closure and the common-order restrictions imply the all-dd bound. The first undecided value for this weakened system is d=4d=4, where Proposition 7 gives 1818; the actual real-set case already has the stronger bound 1414. No ordered countermodel or coupled covering estimate is supplied. The target is unresolved.