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Adaptive frame bounds for the seven-cycle problem


This page preserves an earlier research route and its local standing. The completed threshold proof is in the solution note.

This continues the PSD lifting for fixed weighted templates. The transfer to arbitrary colored graphs requires a further argument.

The adaptive operator

Let AA be a zero-one symmetric template matrix, allowing loops; wi>0w_i>0, ∑iwi=1\sum_iw_i=1; W=diag⁡(wi)W=\operatorname{diag}(w_i); and P2=AWAP_2=AWA. Choose vectors aia_i with ⟨ai,aj⟩=(P2)ij\langle a_i,a_j\rangle=(P_2)_{ij}. A convenient realization is ai(p)=Apia_i(p)=A_{pi} in the weighted space L2(w)L^2(w).

Let L⪰0L\succeq0 have Gram vectors ℓi\ell_i, with Lij=0L_{ij}=0 whenever there is no three-walk from ii to jj, including the diagonal condition at nontriangular types. For an unordered edge type put

gij=ai⊗ℓj+aj⊗ℓi,mij=wiwj (i≠j),mii=wi2/2.g_{ij}=a_i\otimes\ell_j+a_j\otimes\ell_i,\qquad m_{ij}=w_iw_j\ (i\ne j),\quad m_{ii}=w_i^2/2.

The optimized physical-edge weighting in the template certificate is exactly

λmax⁡(FL),FL=∑ij: gij≠0mijgijgijT∥gij∥2.(1)\lambda_{\max}(F_L),\qquad F_L=\sum_{ij:\,g_{ij}\ne0} m_{ij}\frac{g_{ij}g_{ij}^{\mathsf T}}{\|g_{ij}\|^2}. \tag{1}

Indeed the weighted quotient is $|\sum m_{ij}z_{ij}g_{ij}|^2/ \sum m_{ij}z_{ij}^2|g_{ij}|^2$; its maximum is the squared operator norm of the matrix with columns mijgij/∥gij∥\sqrt{m_{ij}}g_{ij}/\|g_{ij}\|.

If all triangular types form a three-walk clique, joint optimization over L,zL,z can use rank-one LL: for fixed zz, the quotient is linear-fractional in an unrestricted PSD matrix on those types, so a rank-one summand attains at least the same ratio. This assertion is not made under arbitrary sparsity constraints on LL.

Uniform edge weights fail even after optimizing the vertex kernel

Take types U1,U2,A,B,CU_1,U_2,A,B,C with

w(U1)=w(U2)=w(A)=w(B)=a=(1−c)/4,w(C)=c,0<c<1.w(U_1)=w(U_2)=w(A)=w(B)=a=(1-c)/4,\qquad w(C)=c, \quad 0<c<1.

The edges are

U1U2, U1A, U2B, AB, AC, BC,U_1U_2,\ U_1A,\ U_2B,\ AB,\ AC,\ BC,

and a loop at CC. The density is q=1/4+c2/4>1/4q=1/4+c^2/4>1/4. Exactly Z={A,B,C}Z=\{A,B,C\} is triangular, and every pair in ZZ admits a three-walk. Thus admissible LL is an arbitrary PSD matrix on ZZ.

Put P4=AWAWAWAP_4=AWAWAWA, s=P2ws=P_2w, and

N=(WP4W)Z,D=(diag⁡(wisi)+W(A∘P2)W)Z.N=(WP_4W)_Z,\qquad D=\bigl(\operatorname{diag}(w_i s_i) +W(A\circ P_2)W\bigr)_Z .

With uniform edge weights the quotient is tr⁡(NL)/tr⁡(DL)\operatorname{tr}(NL)/\operatorname{tr}(DL). Direct first-order multiplication gives

D/8−Nc⟶1256(5−3−2−35−2−2−28)(c↓0).(2)\frac{D/8-N}{c}\longrightarrow \frac1{256} \begin{pmatrix} 5&-3&-2\\ -3&5&-2\\ -2&-2&8 \end{pmatrix} \qquad(c\downarrow0). \tag{2}

For example sA=1/4+c/4+c2/2s_A=1/4+c/4+c^2/2 and sC=(1+c)2/4s_C=(1+c)^2/4; the diagonal AAAA derivative of D/8D/8 is zero, while the corresponding derivative of NN is −5/256-5/256. The AB,AC,CCAB,AC,CC derivatives of D/8−ND/8-N are −3/256,−2/256,8/256-3/256,-2/256,8/256, respectively. Symmetry supplies the other entries in (2).

The matrix on the right has eigenvalues 8,5+17,5−178,5+\sqrt{17},5-\sqrt{17}, divided by 256256, all positive. Therefore for every sufficiently small positive cc, D/8−N≻0D/8-N\succ0. Every nonzero admissible LL then gives a quotient strictly below 1/81/8. Thus adapting LL alone cannot prove the desired universal bound with uniform physical edge weights.

This is a counterexample to that restricted certificate, not to the color bound or to the fully adaptive lifting.

A signed repair throughout the same family

Use scalar Gram vectors

f=(0,0,0,1,−1/2),L=ffT,f=(0,0,0,1,-1/2),\qquad L=ff^{\mathsf T},

in the order (U1,U2,A,B,C)(U_1,U_2,A,B,C), and test the frame operator against h=(1,0,0,1,1/2)h=(1,0,0,1,1/2) in L2(w)L^2(w). Its squared norm is (2−c)/4(2-c)/4. Set ze=⟨ge,h⟩/∥ge∥2z_e=\langle g_e,h\rangle/\|g_e\|^2 for nonzero geg_e. The nonzero weights are

zU2B=1,zAB=11+c,zAC=−21+c,zBC=23−c,zCC=−12.z_{U_2B}=1,\quad z_{AB}=\frac1{1+c},\quad z_{AC}=-\frac2{1+c},\quad z_{BC}=\frac2{3-c},\quad z_{CC}=-\frac12.

The frame Rayleigh quotient is

R(c)=42−c(2a3+a(a+c)2(1+c)+ac2(3−c)+c2(1+c)16).R(c)=\frac4{2-c} \left( 2a^3+\frac{a(a+c)}{2(1+c)} +\frac{ac}{2(3-c)} +\frac{c^2(1+c)}{16} \right).

These terms follow respectively from the types U2BU_2B, ABAB and ACAC, BCBC, and CCCC. Simplification gives

R(c)−18=−c(c4+3c3−14c2−c−1)8(c−3)(c−2)(c+1)>0(0<c<1).R(c)-\frac18 = -\frac{c(c^4+3c^3-14c^2-c-1)} {8(c-3)(c-2)(c+1)}>0 \qquad(0<c<1).

The denominator is positive, and c4+3c3≤4c2c^4+3c^3\le4c^2 makes the parenthesized polynomial negative. The actual weighted Gram quotient is at least R(c)R(c) by Cauchy--Schwarz, or directly by (1). Thus the failure in (2) is repaired by joint, signed adaptation.

Two explicit bounds avoiding a joint optimization

Let SS be a set of positive-degree triangular types such that (A3)ij>0(A^3)_{ij}>0 for every i,j∈Si,j\in S, including the diagonal. Put

di=(P2)ii,ui=ai/di,cij=⟨ui,uj⟩∈[0,1].d_i=(P_2)_{ii},\qquad u_i=a_i/\sqrt{d_i},\qquad c_{ij}=\langle u_i,u_j\rangle\in[0,1].

Isolated types contribute no edges and are omitted.

Define two PSD matrices MS,NSM_S,N_S by adding the following contributions for each unordered edge of mass m=mijm=m_{ij}.

For i∉S,j∈Si\notin S,j\in S, both receive muiuiTm u_i u_i^{\mathsf T}. For distinct i,j∈Si,j\in S, their contributions are respectively

m1+cij(uiuiT+ujujT)\frac{m}{1+c_{ij}} (u_i u_i^{\mathsf T}+u_j u_j^{\mathsf T})

and

m[uiuiT+ujujT−cij(uiujT+ujuiT)].m\bigl[ u_i u_i^{\mathsf T}+u_j u_j^{\mathsf T} -c_{ij}(u_i u_j^{\mathsf T}+u_j u_i^{\mathsf T}) \bigr].

For a loop iiii with i∈Si\in S, both receive miiuiuiTm_{ii}u_i u_i^{\mathsf T}. Edges outside SS contribute zero. The second internal contribution is PSD because (1−cij−cij1)⪰0\begin{pmatrix}1&-c_{ij}\\-c_{ij}&1\end{pmatrix}\succeq0. Then

sup⁡L admissibleλmax⁡(FL)≥max⁡{λmax⁡(MS),λmax⁡(NS)}.(3)\sup_{L\ {\rm admissible}}\lambda_{\max}(F_L) \ge \max\{\lambda_{\max}(M_S),\lambda_{\max}(N_S)\}. \tag{3}

For proof, take a generic unit feature vector xx, write ti=⟨x,ui⟩t_i=\langle x,u_i\rangle, and choose ℓi=di/ti\ell_i=\sqrt{d_i}/t_i on SS, zero outside. This gives an admissible rank-one LL. For an internal distinct edge, gijg_{ij} is parallel to tiui+tjujt_i u_i+t_j u_j, so its frame Rayleigh contribution divided by its mass is

(ti2+tj2)2ti2+tj2+2cijtitj.\frac{(t_i^2+t_j^2)^2} {t_i^2+t_j^2+2c_{ij}t_it_j}.

It is at least each of

ti2+tj21+cij,ti2+tj2−2cijtitj.\frac{t_i^2+t_j^2}{1+c_{ij}}, \qquad t_i^2+t_j^2-2c_{ij}t_it_j.

The first follows from 2titj≤ti2+tj22t_it_j\le t_i^2+t_j^2; the second follows by subtracting and obtaining a nonnegative square divided by the positive denominator. Crossing edges and loops give their listed contributions directly. Summing and maximizing over xx proves (3). Approximation handles zero projections tit_i. Attainment of the supremum over LL is not asserted.

The loop contribution must be treated separately: using the internal-distinct formula for NSN_S would incorrectly give zero.

Hierarchical positive scaling

There is a further lower bound using only nonnegative vertex and edge coefficients. Order an admissible three-walk clique SS, put ℓi=εrank⁡(i)\ell_i=\varepsilon^{\operatorname{rank}(i)} on SS, and put ℓi=0\ell_i=0 outside SS. As ε↓0\varepsilon\downarrow0, the normalized edge vector tends to uj=aj/dju_j=a_j/\sqrt{d_j}, where jj is the outside endpoint of a crossing edge, the later endpoint of an internal distinct edge, or the endpoint of a loop. Therefore the certificate supremum is at least

λmax⁡(QS,≺),QS,≺=∑emeutarget⁡(e)utarget⁡(e)T.\lambda_{\max}(Q_{S,\prec}),\qquad Q_{S,\prec}=\sum_e m_eu_{\operatorname{target}(e)} u_{\operatorname{target}(e)}^{\mathsf T}.

In the standard nonnegative coordinate representation of the aia_i, all finite-ε\varepsilon edge vectors are nonnegative. A largest Rayleigh vector can consequently be chosen nonnegative, so this bound is attainable as a supremum using nonnegative edge coefficients. The assertion does not require the nonpositive-support extension described in the PSD note.

Positive-coefficient repair of the five-type family

Let t=(1−c)/4t=(1-c)/4 and d=2t+cd=2t+c. Choosing ℓA=1,ℓC=ε,ℓB=0\ell_A=1,\ell_C=\varepsilon,\ell_B=0, with zeros on the two nontriangular types, gives the limiting frame

Q=t2uU1uU1T+t(t+c)uBuBT+cd2uCuCT.Q=t^2u_{U_1}u_{U_1}^{\mathsf T} +t(t+c)u_Bu_B^{\mathsf T} +\frac{cd}{2}u_Cu_C^{\mathsf T}.

In Euclidean coordinates ai(j)=Aijwja_i(j)=A_{ij}\sqrt{w_j}, the test vector x0=aU1+(c/2)eCx_0=a_{U_1}+(\sqrt c/2)e_C has Rayleigh quotient

R0=5c3+c+28(2−c)(1+c),R0−18=c2(5c+1)8(2−c)(1+c)>0.R_0=\frac{5c^3+c+2}{8(2-c)(1+c)},\qquad R_0-\frac18=\frac{c^2(5c+1)}{8(2-c)(1+c)}>0.

Thus negative coefficients are not necessary to repair that family.

In fact this also reaches the equivalent half-edge target from the half-edge reduction. For c≥1/4c\ge1/4,

R0−q2=c2(c2+4c−1)8(2−c)(1+c)>0.R_0-\frac q2 =\frac{c^2(c^2+4c-1)}{8(2-c)(1+c)}>0.

For 0<c≤1/40<c\le1/4, use

x1=(0,t,t+c4t,c4t,c2)x_1=\left(0,\sqrt t,\sqrt t+\frac{c}{4\sqrt t}, \frac{c}{4\sqrt t},\frac{\sqrt c}{2}\right)

in the order U1,U2,A,B,CU_1,U_2,A,B,C. Its Rayleigh quotient satisfies

R1−q2=−c2(18c3+11c2−12c−1)16(c+1)(c2−c+2)>0,R_1-\frac q2 =-\frac{c^2(18c^3+11c^2-12c-1)} {16(c+1)(c^2-c+2)}>0,

since 18c3+11c2≤31c/8<12c+118c^3+11c^2\le31c/8<12c+1 on this interval. These formulas follow by summing the three rank-one projection terms in QQ and dividing by ∥xi∥2\|x_i\|^2. Strictness permits a sufficiently small finite ε\varepsilon.

Scope of the hierarchical bound

This ordering construction cannot improve on the best physical rectangle for the same SS. Write Q=∑iγiaiaiT/diQ=\sum_i\gamma_i a_i a_i^{\mathsf T}/d_i. For the positive feature vector with coordinates wp\sqrt{w_p}, the row quotients are

∑i∈N(p)γi.\sum_{i\in N(p)}\gamma_i.

Each is the mass of those ordered active edges whose target lies in N(p)N(p), a subset of E(N(p),S)E(N(p),S). The elementary Collatz--Wielandt upper bound therefore gives

λmax⁡(QS,≺)≤max⁡pe(N(p),S).\lambda_{\max}(Q_{S,\prec})\le\max_p e(N(p),S).

This places the quantitative difficulty back in the physical-rectangle localization problem; it is not a proof of that localization.

Remaining quantitative gap

No proof or counterexample was obtained for the universal assertion sup⁡Lλmax⁡(FL)≥1/8\sup_L\lambda_{\max}(F_L)\ge1/8 above density 1/41/4. Nor is it proved that maximizing the explicit bounds in (3) over SS reaches 1/81/8. The five-type repair is an explicit test case, not a reduction of the general problem.