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Line graph obstruction


Proved. A least color in a hypothetical counterexample cannot be the line graph of any loopless multigraph, with no multiplicity restriction. The heavy-pair and final-triple arguments close the earlier unrestricted-multiplicity gap. This excludes a construction family, not arbitrary colorings; no reduction of general least colors to line graphs is known.

Throughout, r≥3r\ge3, N=r2+1N=r^2+1, and GG satisfies

α(G)≤r,ω(G)≤r,e(G)≤rN2,e(G[W])≤Dr(∣W∣)(W⊆V(G)),(1)\alpha(G)\le r,\qquad \omega(G)\le r,\qquad e(G)\le\frac{rN}{2},\qquad e(G[W])\le D_r(|W|)\quad(W\subseteq V(G)), \tag{1}

with DrD_r and prp_r as in the reductions. These are necessary conditions for a least color.

Matching reduction

Suppose G=L(F)G=L(F), with FF a simple graph or loopless multigraph. Then

e(F)=N,ν(F)=α(G)≤r,Δ(F)≤r.(2)e(F)=N,\qquad \nu(F)=\alpha(G)\le r,\qquad \Delta(F)\le r. \tag{2}

Here multiplicities are counted in degrees and edge counts. The last inequality follows because the edges at any vertex of FF form a clique in L(F)L(F).

The Tutte--Berge formula is

ν(F)=min⁡S⊆V(F)∣V(F)∣+∣S∣−o(F−S)2,(3)\nu(F)=\min_{S\subseteq V(F)} \frac{|V(F)|+|S|-o(F-S)}2, \tag{3}

where oo counts odd-order components. Its statement and proof were checked in Douglas B. West, A short proof of the Berge--Tutte Formula and the Gallai--Edmonds Structure Theorem, European Journal of Combinatorics 32 (2011), 674--676, Theorem 4, author preprint p. 3. West defines def⁡(F)=max⁡S(o(F−S)−∣S∣)\operatorname{def}(F)=\max_S(o(F-S)-|S|) and states ν(F)=(∣V(F)∣−def⁡(F))/2\nu(F)=(|V(F)|-\operatorname{def}(F))/2, exactly (3). For multigraphs, apply this theorem to the underlying simple graph.

Choose a minimizing SS. If CC ranges over the components of F−SF-S, then

ν(F)=∣S∣+∑C⌊∣C∣2⌋.(4)\nu(F)=|S|+\sum_C\left\lfloor\frac{|C|}{2}\right\rfloor. \tag{4}

Edges having an endpoint in SS number at most r∣S∣r|S|, and an even component CC has at most r∣C∣/2r|C|/2 edges. Since e(F)>rν(F)e(F)>r\nu(F), some odd component must satisfy

∣C∣=2a+1,m=e(C)=ar+b,1≤a≤r,1≤b≤⌊r/2⌋.(5)|C|=2a+1,\qquad m=e(C)=ar+b,\qquad 1\le a\le r,\qquad 1\le b\le\lfloor r/2\rfloor. \tag{5}

Otherwise summing the component bounds in (4) would give e(F)≤rν(F)e(F)\le r\nu(F). The upper bound on bb follows from Δ(F)≤r\Delta(F)\le r. The vertices of GG corresponding to E(C)E(C) induce exactly L(C)L(C).

Simple line graphs

Assume first that FF is simple. An adjacent pair of its edges has a unique common endpoint, so Cauchy--Schwarz gives

e(L(C))=∑x∈C(dC(x)2)≥2m22a+1−m.(6)e(L(C))=\sum_{x\in C}\binom{d_C(x)}2 \ge\frac{2m^2}{2a+1}-m. \tag{6}

For the parameters in (5),

2Dr(ar+b)=ar2+a(a−2)r+b(b−1)+2ab.(7)2D_r(ar+b)=ar^2+a(a-2)r+b(b-1)+2ab. \tag{7}

We show that a≤r−1a\le r-1 makes (6) exceed this inherited cap. Put

P(a,r,b)=2(2a+1)(2(ar+b)22a+1−(ar+b)−Dr(ar+b)).P(a,r,b)=2(2a+1) \left(\frac{2(ar+b)^2}{2a+1}-(ar+b)-D_r(ar+b)\right).

Direct expansion yields

P(a,r,b)−P(a,r,1)=(b−1)(−4a2−2ab+8ar−6a+3b+2).P(a,r,b)-P(a,r,1) =(b-1)(-4a^2-2ab+8ar-6a+3b+2).

Since b≤r/2b\le r/2 and r≥a+1r\ge a+1, the second factor is at least a(7r−4a−6)+3b+2>0a(7r-4a-6)+3b+2>0. Writing t=r−a−1≥0t=r-a-1\ge0 gives

P(a,r,1)=3a2+a+2+a(2a2+a+6)t+a(2a−1)t2>0.P(a,r,1)=3a^2+a+2+a(2a^2+a+6)t+a(2a-1)t^2>0.

This proves the required strict violation. Hence a=ra=r.

Equation (4) now forces S=∅S=\varnothing and every other component of FF to be a singleton. Thus all NN edges lie in CC, of order 2r+12r+1. By (6),

e(G)≥2N22r+1−N>rN2,e(G)\ge\frac{2N^2}{2r+1}-N>\frac{rN}{2},

where the strict inequality is equivalent to

4N−(r+2)(2r+1)=(2r−1)(r−2)>0.4N-(r+2)(2r+1)=(2r-1)(r-2)>0.

This contradicts (1) and proves the simple-line-graph obstruction.

Bounded multiplicity

For a loopless multigraph, the correct edge identity is

e(L(F))=∑x(dF(x)2)−∑xy(μxy2).(8)e(L(F))=\sum_x\binom{d_F(x)}2 -\sum_{xy}\binom{\mu_{xy}}2. \tag{8}

The subtracted term is essential: C5[Kt]C_5[K_t] is the line graph of a five-cycle with edge multiplicity tt. Therefore the preceding simple proof does not already exclude the local-cap counterfamily.

Assume every multiplicity is at most hh and r≥8hr\ge8h. The matching reduction still gives (5), and (8) implies

e(L(C))≥2m22a+1−h+12m.(9)e(L(C))\ge\frac{2m^2}{2a+1}-\frac{h+1}{2}m. \tag{9}

The case a=1a=1 is impossible: any two edges of a loopless multigraph on three vertices are incident, so m≥r+1m\ge r+1 would give a forbidden clique. Thus a≥2a\ge2.

If a≤r−2ha\le r-2h, define, on 0≤b≤r/20\le b\le r/2,

f(b)=2(ar+b)22a+1−h+12(ar+b)−Dr(ar+b),f(b)=\frac{2(ar+b)^2}{2a+1} -\frac{h+1}{2}(ar+b)-D_r(ar+b),

interpreting the last term by the polynomial (7). Its derivative

f′(b)=4(ar+b)2a+1−a−b−h2f'(b)=\frac{4(ar+b)}{2a+1}-a-b-\frac h2

decreases with bb, and even at b=r/2b=r/2 is 3r/2−a−h/2>03r/2-a-h/2>0. Also

f(0)=ar2((2a−1)r2a+1−a+1−h)>0,f(0)=\frac{ar}{2} \left(\frac{(2a-1)r}{2a+1}-a+1-h\right)>0,

because r≥a+2hr\ge a+2h and

(2a−1)(a+2h)−(2a+1)(a+h−1)=h(2a−3)+1>0.(2a-1)(a+2h)-(2a+1)(a+h-1)=h(2a-3)+1>0.

Thus inherited density forces a>r−2h≥3r/4a>r-2h\ge3r/4.

In particular 2a+1>r2a+1>r, so m≥arm\ge ar gives

2m2a+1−h+12>r−h+32>0.\frac{2m}{2a+1}-\frac{h+1}{2} >r-\frac{h+3}{2}>0.

Factoring (9) into mm times this positive bracket yields

e(G)>r(r−2h)(r−h+32)>r(r2+1)2.e(G)>r(r-2h)\left(r-\frac{h+3}{2}\right) >\frac{r(r^2+1)}2.

The final comparison follows from

r2−(5h+3)r+2h2+6h−1>0:r^2-(5h+3)r+2h^2+6h-1>0:

for r≥8hr\ge8h, we have r−5h−3≥0r-5h-3\ge0 and 2h2+6h−1>02h^2+6h-1>0. This again contradicts (1).

Consequently all line-graph construction families with maximum multiplicity o(r)o(r) fail for sufficiently large parameters.

Unrestricted multiplicity: constraints on a minimal odd core

The following established reductions are used in the unrestricted proof below, which closes the concentration gap they leave. Within the component from (5), choose an inclusion-minimal odd vertex set UU with

∣U∣=2a+1,m=e(F[U])=ar+b>ar.|U|=2a+1,\qquad m=e(F[U])=ar+b>ar.

Then a≤ra\le r and 1≤b≤r/21\le b\le r/2. All degrees below refer to F[U]F[U]. Set

δu=r−d(u),∑u∈Uδu=r−2b.(10)\delta_u=r-d(u),\qquad \sum_{u\in U}\delta_u=r-2b. \tag{10}

Deleting any pair leaves a proper odd set, so minimality gives

d(u)+d(v)−μuv≥r+b.(11)d(u)+d(v)-\mu_{uv}\ge r+b. \tag{11}

For μ=μuv≥1\mu=\mu_{uv}\ge1, the two star cliques in L(F[U])L(F[U]) have orders r−δu,r−δvr-\delta_u,r-\delta_v, intersect in μ\mu vertices, and their union has r+sr+s vertices, where

s=r−δu−δv−μ≥b≥1.s=r-\delta_u-\delta_v-\mu\ge b\ge1.

Its edge count is at least the sum of the two clique edge counts minus (μ2)\binom\mu2. Applying inherited density and using Dr(r+s)=(r2)+(s+12)D_r(r+s)=\binom r2+\binom{s+1}{2} gives exactly

(μ−1)s≤δuδv.(12)(\mu-1)s\le\delta_u\delta_v. \tag{12}

If μ≥2\mu\ge2, the concave quadratic (μ−1)(r−δu−δv−μ)(\mu-1)(r-\delta_u-\delta_v-\mu) has minimum r−δu−δv−2r-\delta_u-\delta_v-2 on 2≤μ≤r−δu−δv−12\le\mu\le r-\delta_u-\delta_v-1. Thus

(δu+1)(δv+1)≥r−1whenever μuv≥2.(13)(\delta_u+1)(\delta_v+1)\ge r-1 \qquad\text{whenever }\mu_{uv}\ge2. \tag{13}

In particular, parallel edges require substantial endpoint deficits, while their total is only r−2br-2b.

There is also an averaged edge lower bound. Include the whole star at uu, together with δu+1\delta_u+1 edges at vv not incident with uu; (11) ensures that enough exist. This (r+1)(r+1)-set has at most (d(u)−μuv)(δu+1)(d(u)-\mu_{uv})(\delta_u+1) nonedges. The local cap therefore gives

μuv≤d(u)−r−1δu+1.\mu_{uv}\le d(u)-\frac{r-1}{\delta_u+1}.

Using this in (8) and averaging the endpoint bounds yields

e(L(F[U]))≥14∑u∈U(d(u)2−d(u)+(r−1)d(u)r+1−d(u)).e(L(F[U]))\ge\frac14\sum_{u\in U} \left(d(u)^2-d(u)+\frac{(r-1)d(u)}{r+1-d(u)}\right).

The summand has second derivative 2+2(r2−1)/(r+1−d)3>02+2(r^2-1)/(r+1-d)^3>0. Jensen's inequality consequently gives

e(L(F[U]))≥m22a+1−m2+(2a+1)(r−1)m2(2a+1+r−2b).(14)e(L(F[U]))\ge \frac{m^2}{2a+1}-\frac m2+ \frac{(2a+1)(r-1)m}{2(2a+1+r-2b)}. \tag{14}

The next two reductions show that a surviving core must have a<r/2a<\sqrt{r/2}. Below that range the concentration argument in the final section applies.

No degree-rr vertex in the minimal core

Suppose d(u)=rd(u)=r for some u∈Uu\in U. If vv is a neighbor of uu, (11) gives

d(v)−μuv≥b≥1.d(v)-\mu_{uv}\ge b\ge1.

Thus an edge at vv exists outside the star at uu. The latter star is a KrK_r in GG, and an external vertex can have at most one neighbor in such a clique. It follows that μuv=1\mu_{uv}=1. The same property forbids an edge between any two distinct neighbors of uu: that edge would have two neighbors in the star clique.

Hence NF(u)N_F(u) is an independent set of exactly rr vertices, and its complement in UU is a vertex cover of size 2a+1−r2a+1-r. Consequently

ar+b=e(F[U])≤r(2a+1−r),ar+b=e(F[U])\le r(2a+1-r),

which forces a=ra=r because a≤ra\le r and b>0b>0.

When a=ra=r, (10) shows that at least

(2r+1)−(r−2b)=r+2b+1≥r+3(2r+1)-(r-2b)=r+2b+1\ge r+3

vertices have degree rr. Their star cliques have pairwise disjoint edge sets in L(F[U])L(F[U]): each edge incident with a degree-rr vertex has multiplicity one, so two such stars intersect in at most one vertex. Therefore

e(G)≥(r+3)(r2)>r(r2+1)2,e(G)\ge(r+3)\binom r2>\frac{r(r^2+1)}2,

the difference being r(r−2)>0r(r-2)>0. This contradicts (1).

Thus every vertex of the minimal core has degree at most r−1r-1. Equation (10) now yields

2a+1≤r−2b≤r−2,a≤r−32.(15)2a+1\le r-2b\le r-2,\qquad a\le\frac{r-3}{2}. \tag{15}

The core has a<r/2a<\sqrt{r/2}

Let L(b)L(b) denote the right side of (14), and set D(b)=Dr(ar+b)D(b)=D_r(ar+b). Regarding these as real functions on 1≤b≤r/21\le b\le r/2,

(L−D)′(b)=2(ar+b)2a+1−a−b+(r2−1)(2a+1)22(2a+1+r−2b)2>0.(L-D)'(b)= \frac{2(ar+b)}{2a+1}-a-b+ \frac{(r^2-1)(2a+1)^2}{2(2a+1+r-2b)^2}>0.

Indeed, the first three terms decrease with bb and at b=r/2b=r/2 equal r/2−a>0r/2-a>0 by (15). Thus it suffices to compare L(1)L(1) and D(1)D(1).

Put

P=2(2a+1)(2a+r−1)(L(1)−D(1)).P=2(2a+1)(2a+r-1)\bigl(L(1)-D(1)\bigr).

Expansion gives

Pr=ar(2a2+3a+7−r)−4a4+5a2−6a+2−8a3+8a2−2a+2r.(16)\frac Pr= ar(2a^2+3a+7-r)-4a^4+5a^2-6a+2 -\frac{8a^3+8a^2-2a+2}{r}. \tag{16}

Suppose, contrary to the claimed bound, that r≤2a2r\le2a^2. Together with (15), this puts rr in [2a,2a2][2a,2a^2]. The concave function ar(2a2+3a+7−r)ar(2a^2+3a+7-r) has its minimum over this interval at an endpoint. The endpoint at 2a22a^2 exceeds that at 2a2a by 2a2(a−1)(a+7)≥02a^2(a-1)(a+7)\ge0. Hence the first term in (16) is at least 4a4+2a3+14a24a^4+2a^3+14a^2.

Since r≥2ar\ge2a and 8a3+8a2−2a+2>08a^3+8a^2-2a+2>0, (16) now gives

Pr≥2a3+15a2−10a+3−1a>0.\frac Pr\ge 2a^3+15a^2-10a+3-\frac1a>0.

Thus (14) exceeds inherited density, a contradiction. We conclude

a<r2.(17)a<\sqrt{\frac r2}. \tag{17}

Combining this with the hereditary span bound further restricts a possible core to

r64<a<r2.\sqrt{\frac r{64}}<a<\sqrt{\frac r2}.

For the lower bound, if r≥64a2r\ge64a^2, any ar+1ar+1 of the core's edge vertices give an induced graph of independence at most aa, contradicting that theorem. This intermediate range is eliminated in the final section.

Heavy near-perfect matchings in the root are excluded

Here FF is the minimal odd root above: ∣F∣=2a+1|F|=2a+1, m=e(F)=ar+bm=e(F)=ar+b, 1≤b≤r/21\le b\le r/2, and Δ(F)≤r\Delta(F)\le r. For r≥4r\ge4, it cannot have a matching uiviu_iv_i, 1≤i≤a1\le i\le a, whose multiplicities μi\mu_i are all at least r/2r/2.

Write

ti=δui+δvi,ci=r−μi,si=ci−ti≥b,T=∑iti.t_i=\delta_{u_i}+\delta_{v_i},\quad c_i=r-\mu_i,\quad s_i=c_i-t_i\ge b,\quad T=\sum_i t_i.

The two-star cap (12) gives

δuiδvi≥(μi−1)si≥(r/2−1)b.\delta_{u_i}\delta_{v_i}\ge(\mu_i-1)s_i\ge(r/2-1)b.

Thus ti2≥2(r−2)bt_i^2\ge2(r-2)b and titj≥2(r−2)bt_it_j\ge2(r-2)b. Every matched endpoint has positive integer deficit, so T≥2aT\ge2a. The unmatched vertex zz has degree T+2bT+2b, by (10).

Call all pairs outside the matching light. The total light multiplicity at uiu_i is δvi+si\delta_{v_i}+s_i, and vice versa. Every light pair has at least one matched endpoint. Squaring these residual degrees consequently gives

∑light uvμuv2≤∑i((δui+si)2+(δvi+si)2).\sum_{\text{light }uv}\mu_{uv}^2 \le\sum_i\bigl((\delta_{u_i}+s_i)^2+ (\delta_{v_i}+s_i)^2\bigr).

Use the identity 2e(L(F))=∑vd(v)2−∑uvμuv2−m2e(L(F))=\sum_v d(v)^2-\sum_{uv}\mu_{uv}^2-m to obtain

2e(L(F))≥ar2+T2−∑iti2+4bT+4b2+∑isi(2r−4ti−3si)−ar−b.\begin{aligned} 2e(L(F))\ge{}&ar^2+T^2-\sum_i t_i^2+4bT+4b^2\\ &+\sum_i s_i(2r-4t_i-3s_i)-ar-b. \end{aligned}

Since ti+si=ci≤r/2t_i+s_i=c_i\le r/2, the summands on the second line are at least si2s_i^2. Also T2−∑iti2≥2a(a−1)(r−2)bT^2-\sum_i t_i^2\ge2a(a-1)(r-2)b. Subtracting the inherited cap (7) gives

2e(L(F))−2Dr(ar+b)≥a(a−1)((2b−1)r−4b)+4bT+3b2−2ab+∑isi2>0.\begin{aligned} 2e(L(F))-2D_r(ar+b)\ge{}& a(a-1)((2b-1)r-4b)\\ &+4bT+3b^2-2ab+\sum_i s_i^2>0. \end{aligned}

The first bracket is nonnegative, and T≥2aT\ge2a makes the remaining expression positive. This proves the exclusion without using the least-color budget in this final step.

The minimal odd root is also factor-critical. If F−zF-z had no perfect matching, Tutte's theorem would give a set SS with q=o(F−z−S)≥∣S∣+2q=o(F-z-S)\ge|S|+2. Put K=S∪{z}K=S\cup\{z\} and k=∣K∣k=|K|. Each odd component CC of F−KF-K is a proper odd set, so minimality gives e(C)≤r(∣C∣−1)/2e(C)\le r(|C|-1)/2; even components have at most r∣C∣/2r|C|/2 edges. Edges incident with KK number at most rkrk. Therefore

m≤r2(∣F∣+k−q)≤ar,m\le\frac r2(|F|+k-q)\le ar,

a contradiction. This is the Tutte--Berge input already checked above, applied to the underlying simple graph.

These two additional arguments were checked by the author and are author-recorded. Heavy edges form a matching because the root has maximum degree at most r−1r-1. The next argument forces all but three vertices into this matching and then excludes that last possibility.

Unrestricted multiplicities: concentration and the last three vertices

Theorem. No graph satisfying (1) is the line graph of a loopless multigraph.

It remains to exclude the minimal odd root above. The case a=1a=1 gives a clique of order at least r+1r+1 in its line graph. The case a=2a=2 is excluded by the hereditary independence-two span bound: any 2r+12r+1 edge vertices have independence at most two. For r=3r=3 it is already excluded by (15). Thus assume

a≥3,r>2a2,r≥19.a\ge3,\qquad r>2a^2,\qquad r\ge19.

Call a root pair heavy if its multiplicity is at least r/2r/2. These pairs form a matching, of size h≤ah\le a. For each heavy pair uiviu_iv_i put

ti=δui+δvi,si=r−ti−μi≥b,ci=ti+si≤r/2,T=∑iti,S=∑isi.t_i=\delta_{u_i}+\delta_{v_i},\quad s_i=r-t_i-\mu_i\ge b,\quad c_i=t_i+s_i\le r/2, \qquad T=\sum_i t_i,\quad S=\sum_i s_i.

The two-star cap implies

ti2≥4δuiδvi≥4(μi−1)si≥2(r−2)b>(2a−1)2.t_i^2\ge4\delta_{u_i}\delta_{v_i} \ge4(\mu_i-1)s_i\ge2(r-2)b>(2a-1)^2.

Since tit_i is integral, ti≥2at_i\ge2a.

At least a−1a-1 heavy pairs

Write Q=∑uδu2Q=\sum_u\delta_u^2. The exact line-graph identity and ∑uδu=r−2b\sum_u\delta_u=r-2b give

∑uvμuv2≥(a−1)r2−a(a−1)r+Q+4br−b2−2ab.(18)\sum_{uv}\mu_{uv}^2\ge (a-1)r^2-a(a-1)r+Q+4br-b^2-2ab. \tag{18}

This follows by rearranging

2e(L(F))=∑ud(u)2−∑uvμuv2−m≤2Dr(ar+b).2e(L(F))=\sum_ud(u)^2-\sum_{uv}\mu_{uv}^2-m \le2D_r(ar+b).

On the other hand, heavy pairs contribute hr2−2r(T+S)+∑ici2hr^2-2r(T+S)+\sum_i c_i^2. Light pairs have total multiplicity (a−h)r+b+T+S(a-h)r+b+T+S, each less than r/2r/2. Since ci2≤rci/2c_i^2\le rc_i/2,

∑uvμuv2≤a+h2r2−r(T+S)+br2.(19)\sum_{uv}\mu_{uv}^2\le \frac{a+h}{2}r^2-r(T+S)+\frac{br}{2}. \tag{19}

Combining (18)--(19) yields

0≥a−h−22r2−a(a−1)r+r(T+S)+Q+b(7r2−b−2a).(20)0\ge\frac{a-h-2}{2}r^2-a(a-1)r+r(T+S)+Q +b\left(\frac{7r}{2}-b-2a\right). \tag{20}

The last term is positive. If h≤a−3h\le a-3, the first two terms already have positive sum, since r>2a2r>2a^2. If h=a−2h=a-2, then T≥2a(a−2)T\ge2a(a-2), and rT−a(a−1)r≥a(a−3)r≥0rT-a(a-1)r\ge a(a-3)r\ge0. Both cases are impossible. Therefore h≥a−1h\ge a-1. The heavy near-perfect matching lemma above excludes h=ah=a, leaving exactly h=a−1h=a-1.

Three unmatched root vertices

Let ZZ be these three vertices, and write

τ=e(F[Z])=r−k,k≥0.\tau=e(F[Z])=r-k,\qquad k\ge0.

Here k≥0k\ge0 follows from minimality applied to the proper odd set ZZ. For z∈Zz\in Z, let ℓz\ell_z count edges from zz to the matched endpoints, with multiplicity, and put B=∑z∈ZℓzB=\sum_{z\in Z}\ell_z. The total degree in ZZ is 2r+2b+T2r+2b+T, so

B=T+2b+2k.B=T+2b+2k.

The residual degrees at matched endpoints are δvi+si\delta_{v_i}+s_i and δui+si\delta_{u_i}+s_i, totaling T+2ST+2S. Thus k≤S−bk\le S-b. The two-star cap also gives

si≤ti22(r−2),S≤rT4(r−2)≤2T7,0≤k≤2T7.(21)s_i\le\frac{t_i^2}{2(r-2)},\qquad S\le\frac{rT}{4(r-2)}\le\frac{2T}{7}, \qquad 0\le k\le\frac{2T}{7}. \tag{21}

The last numerical inequality holds for r≥16r\ge16.

Every light pair not contained in ZZ has a matched endpoint. Its squared multiplicity is therefore accounted for at least once in the sum of squared residual degrees at matched endpoints. For a heavy pair with endpoint deficits x,yx,y, t=x+yt=x+y, and parameter ss,

(r−x)2+(r−y)2−(r−t−s)2−(y+s)2−(x+s)2=r2−t2+s(2r−4t−3s)≥r2−t2+s2,\begin{aligned} &(r-x)^2+(r-y)^2-(r-t-s)^2-(y+s)^2-(x+s)^2\\ &\hspace{15mm}=r^2-t^2+s(2r-4t-3s) \ge r^2-t^2+s^2, \end{aligned}

because t+s≤r/2t+s\le r/2. Consequently

2e(L(F))≥(a−1)r2−∑iti2+∑isi2+∑z∈Zd(z)2−∑uv⊂Zμuv2−ar−b.(22)2e(L(F))\ge(a-1)r^2-\sum_i t_i^2+\sum_i s_i^2 +\sum_{z\in Z}d(z)^2-\sum_{uv\subset Z}\mu_{uv}^2-ar-b. \tag{22}

Let wzw_z be the multiplicity on the pair opposite zz in ZZ, allowing zero. Then ∑zwz=τ\sum_z w_z=\tau and d(z)=τ−wz+ℓzd(z)=\tau-w_z+\ell_z. Direct expansion gives

∑z∈Zd(z)2−∑uv⊂Zμuv2=τ2+2∑z(τ−wz)ℓz+∑zℓz2.\sum_{z\in Z}d(z)^2-\sum_{uv\subset Z}\mu_{uv}^2 =\tau^2+2\sum_z(\tau-w_z)\ell_z+\sum_z\ell_z^2.

No pair in ZZ is heavy, so wz<r/2w_z<r/2 and τ−wz≥r/2−k\tau-w_z\ge r/2-k. By Cauchy--Schwarz the last display is at least

(r−k)2+(r−2k)B+B23.(r-k)^2+(r-2k)B+\frac{B^2}{3}.

Substitute B=T+2b+2kB=T+2b+2k into (22) and subtract (7). The resulting lower bound for 2e(L(F))−2Dr(ar+b)2e(L(F))-2D_r(ar+b) is

rT−a(a−1)r−∑iti2+T2−2kT−5k23+4b3(T−k)+b23+2b(r−a)+∑isi2.(23)\begin{aligned} &rT-a(a-1)r-\sum_i t_i^2 +\frac{T^2-2kT-5k^2}{3}\\ &\qquad+\frac{4b}{3}(T-k)+\frac{b^2}{3} +2b(r-a)+\sum_i s_i^2. \tag{23} \end{aligned}

By (21), the quadratic term is at least T2/147T^2/147, and all the following terms are nonnegative. Also

∑iti2≤rT2,T≥2a(a−1)>0.\sum_i t_i^2\le\frac{rT}{2},\qquad T\ge2a(a-1)>0.

Thus (23) is at least

rT2−a(a−1)r+T2147>0,\frac{rT}{2}-a(a-1)r+\frac{T^2}{147}>0,

contradicting the hereditary cap. This finishes the unrestricted multigraph proof.

Checks and limitations

The simple and bounded-multiplicity proofs, (10)--(14), and the two core reductions (15)--(17) were checked by the author and are author-recorded. The unrestricted concentration and three-vertex argument were also checked by the author; its three polynomial identities were verified symbolically as well as by expansion. The earlier symbolic expansions were also checked directly. No random or exhaustive construction search was used.

These arguments concern a least color: the global edge budget in (1) is essential. They do not show that an arbitrary selected color cannot be a line graph. Nor do they reduce general color graphs to line graphs, or prove the corresponding statement for all claw-free graphs.

Budget-free span for K_r-free line graphs

Theorem. If J=L(F)J=L(F) is the line graph of a loopless multigraph, is KrK_r-free, and satisfies every inherited upper cap, then

∣J∣≤rα(J).|J|\le r\alpha(J).

There is no restriction on ∣J∣|J| or α(J)\alpha(J), and no edge budget.

Suppose instead e(F)>rν(F)e(F)>r\nu(F). The Tutte--Berge decomposition used above supplies a minimal odd overfull root UU, of order 2a+12a+1 with ar+bar+b edges, b≥1b\ge1. Every root star is a clique, so now Δ(F)≤r−1\Delta(F)\le r-1 directly. Hence all deficits are positive and

∑u∈U(r−d(u))=r−2b,2a+1≤r−2b.\sum_{u\in U}(r-d(u))=r-2b,\qquad 2a+1\le r-2b.

This gives (15) without the degree-rr-vertex argument, which was the only use of the least-color budget in the unrestricted proof. The Jensen estimate, the reduction r>2a2r>2a^2, and the heavy-pair and final triple inequalities then apply unchanged. They exclude every such root, a contradiction. The small cases a=1,2a=1,2 are treated as above.

Thus either normalized core would be excluded by a valid line-graph reduction. The obstacle is not transferring the least-color budget; it is obtaining that structural reduction. The theorem also yields the general odd-clique inequalities.