Maximum-energy conjecture for integral weighted trees

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Let n≥5n\ge 5 and m≥nm\ge n. Write T(n,m){\mathcal T}(n,m) for the class of weighted trees on nn vertices with total edge weight mm, and let the energy of a weighted tree be the sum of the absolute values of its adjacency-matrix eigenvalues. A pendent edge is an edge incident with a leaf. Maximum-energy conjecture. The path in T(n,m){\mathcal T}(n,m) with weight sequence (m−n+2,1,…,1)(m-n+2,1,\ldots,1), where one of its pendent edges has weight m−n+2m-n+2, is the unique tree in T(n,m){\mathcal T}(n,m) with maximum energy.

The conjecture concerns the extremal energy of integral weighted trees and extends the preceding exact calculation for weighted paths on four vertices. The supplied text gives no resolution, so its status remains open.

References

Primary source

Richard A. Brualdi, Jia-Yu Shao, Shi-Cai Gong, Chang-Qing Xu and Guang-Hui Xu, “On the extremal energy of integral weighted trees”, arXiv:1106.5940 (2011).

Progress summary

Refreshed
Claimed progress

A reader-submitted argument claims the conjecture is solved, but no independent verification has been found.

The conjecture, stated by Brualdi, Shao, Gong, and Xu (2012), predicts that the path with one exceptional pendent edge uniquely maximizes energy among weighted trees with fixed order and total weight. The published source records this as Conjecture 10.

Known results

  • For the fixed weight sequence (a,1,…,1)(a,1,\ldots,1), the corresponding weighted path uniquely maximizes energy (2011 paper, Theorem 11 and Corollary 12).
  • Among weighted stars, the sequence (m−n+2,1,…,1)(m-n+2,1,\ldots,1) uniquely maximizes energy, with energy 2(m−n+2)2+n−22\sqrt{(m-n+2)^2+n-2} (2011 paper).

Community submission (unverified), August 25, 2026

A submitted proof argues that the conjecture extends even to real edge weights bounded below by one. Its approach uses convexity of the nuclear norm to reduce to one concentrated exceptional weight, then compares weighted matching coefficients and applies the Coulson integral to identify the pendent-edge path; the argument has not been independently checked.

Current status (as of August 2026): The full conjecture remains unverified; only the fixed-weight-sequence and weighted-star cases are established in the cited source, while a community-submitted complete proof is unconfirmed.

Sources

Solutions 1

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Full proof of the weighted-tree maximum-energy conjecture

We resolve the maximum-energy conjecture of R. A. Brualdi, J.-Y. Shao, S.-C. Gong, C.-Q. Xu, and G.-H. Xu, On the extremal energy of integral weighted graphs, Linear and Multilinear Algebra 60 (2012), 1255–1264, doi:10.1080/03081087.2011.624094. In fact, integrality is unnecessary: the same unique maximizer holds for arbitrary real edge weights bounded below by one.

Let TT be an nn-vertex tree with real edge weights we≥1w_e\geq1, and suppose

n≥5,∑e∈E(T)we=m>n−1,d=m−n+1>0,q=1+d=m−n+2.(1)n\geq5,\qquad \sum_{e\in E(T)}w_e=m>n-1,\qquad d=m-n+1>0,\qquad q=1+d=m-n+2. \tag{1}

Write A(T,w)A(T,w) for its weighted adjacency matrix. Since this matrix is real symmetric, its energy is its nuclear norm:

E(T,w)=∑i=1n∣λi(A(T,w))∣=∥A(T,w)∥∗.(2)\mathcal E(T,w)=\sum_{i=1}^{n}|\lambda_i(A(T,w))|=\|A(T,w)\|_*. \tag{2}

For each edge ee, let AeA_e be the adjacency matrix with weight qq on ee and weight one on every other edge. Setting pe=(we−1)/dp_e=(w_e-1)/d gives the exact convex decomposition

pe≥0,∑epe=1,A(T,w)=∑epeAe,E(T,w)≤∑epe∥Ae∥∗.(3)p_e\geq0,\qquad \sum_ep_e=1,\qquad A(T,w)=\sum_ep_eA_e, \qquad \mathcal E(T,w)\leq\sum_ep_e\|A_e\|_*. \tag{3}

We first identify the largest energy among these concentrated-weight trees. Let Mk(F)M_k(F) denote the number of kk-edge matchings of an unweighted forest FF on NN vertices. Deleting a leaf vv and its neighbor uu gives

Mk(F)=Mk(F−v)+Mk−1(F−{u,v}),Mk(F)≤(N−kk)=Mk(PN).(4)M_k(F)=M_k(F-v)+M_{k-1}(F-\{u,v\}), \qquad M_k(F)\leq\binom{N-k}{k}=M_k(P_N). \tag{4}

The inequality follows by induction and Pascal’s identity; isolated vertices are deleted separately. For a tree with a unique edge e=uve=uv of weight qq, its weighted matching coefficients are

bk(T,e)=Mk(T)+(q2−1)Mk−1(T−{u,v}).(5)b_k(T,e)=M_k(T)+(q^2-1)M_{k-1}(T-\{u,v\}). \tag{5}

Consequently, if Pn∗P_n^* denotes the path whose unique weight-qq edge is pendent, then (4) yields, for every kk,

bk(T,e)≤(n−kk)+(q2−1)(n−k−1k−1)=bk(Pn∗).(6)b_k(T,e) \leq\binom{n-k}{k}+(q^2-1)\binom{n-k-1}{k-1} =b_k(P_n^*). \tag{6}

The Coulson integral for a weighted tree is

E(T,e)=2π∫0∞1x2log⁡(∑k≥0bk(T,e)x2k) dx.(7)\mathcal E(T,e) =\frac{2}{\pi}\int_0^{\infty} \frac{1}{x^2}\log\left(\sum_{k\geq0}b_k(T,e)x^{2k}\right)\,dx. \tag{7}

Thus (6) implies E(T,e)≤E(Pn∗)\mathcal E(T,e)\leq\mathcal E(P_n^*), strictly whenever any coefficient inequality is strict. In fact,

M2(T)=(n−12)−∑v∈V(T)(deg⁡T(v)2)≤(n−22),(8)M_2(T)=\binom{n-1}{2}-\sum_{v\in V(T)}\binom{\deg_T(v)}2 \leq\binom{n-2}{2}, \tag{8}

with equality precisely when every vertex has degree at most two, that is, precisely when T=PnT=P_n. If T=PnT=P_n but ee is not pendent, then T−{u,v}T-\{u,v\} has n−4n-4 edges instead of the n−3n-3 edges of Pn−2P_{n-2}, making (6) strict at k=2k=2. Therefore

E(T,e)=E(Pn∗)⟺T=Pn and e is pendent.(9)\mathcal E(T,e)=\mathcal E(P_n^*) \quad\Longleftrightarrow\quad T=P_n\ \text{and }e\text{ is pendent}. \tag{9}

Combining (3) and (9) proves the claimed sharp upper bound. Moreover, equality in (3) forces T=PnT=P_n, all interior edges to have weight one, and the total excess dd to be supported on its two pendent edges. It remains to exclude a nontrivial split of this excess.

Let BB denote the bipartite adjacency block of a positively weighted path. It has full column rank, and

E(Pn,w)=2∥B∥∗.(10)\mathcal E(P_n,w)=2\|B\|_*. \tag{10}

For every full-column-rank real matrix BB, its nuclear norm has the unique orthogonal-column maximizer

∥B∥∗=max⁡QTQ=Itr⁡(QTB),U(B)=B(BTB)−1/2.(11)\|B\|_* =\max_{Q^{\mathsf T}Q=I}\operatorname{tr}(Q^{\mathsf T}B), \qquad U(B)=B(B^{\mathsf T}B)^{-1/2}. \tag{11}

Let BLB_L and BRB_R put the entire excess dd on the left or right pendent edge. If any nontrivial convex combination attains their common nuclear norm, then its maximizer in (11) also maximizes both endpoint matrices. Uniqueness therefore implies

U(BL)=U(BR)=U(BL+BR2).(12)U(B_L)=U(B_R)=U\left(\frac{B_L+B_R}{2}\right). \tag{12}

Suppose first that n=2r+1n=2r+1. The blocks BL,BRB_L,B_R have size (r+1)×r(r+1)\times r. A vector zz spanning the left kernel of a path block satisfies

w2j−1zj+w2jzj+1=0(1≤j≤r).(13)w_{2j-1}z_j+w_{2j}z_{j+1}=0 \qquad(1\leq j\leq r). \tag{13}

In particular, the ratio z2/z1z_2/z_1 equals −q-q for BLB_L and −1-1 for BRB_R. Their column spaces are therefore different, whereas (12) would give the same column space for both. Hence a nontrivial split cannot maximize the energy.

Now suppose n=2r≥6n=2r\geq6. The blocks are invertible r×rr\times r lower-bidiagonal matrices. At the midpoint put

B=BL+BR2,G=BTB,BL−BR=d(E11−Err).(14)B=\frac{B_L+B_R}{2},\qquad G=B^{\mathsf T}B,\qquad B_L-B_R=d(E_{11}-E_{rr}). \tag{14}

If (12) held, then UTBLU^{\mathsf T}B_L and UTBRU^{\mathsf T}B_R would both be symmetric positive definite. Therefore UT(E11−Err)U^{\mathsf T}(E_{11}-E_{rr}) would be symmetric. Since r≥3r\geq3, comparison of its (2,1)(2,1) and (1,2)(1,2) entries forces

U1,2=0.(15)U_{1,2}=0. \tag{15}

However, the first row of BB has its only nonzero entry B1,1=1+d/2>0B_{1,1}=1+d/2>0, so

U1,2=B1,1(G−1/2)1,2.(16)U_{1,2}=B_{1,1}(G^{-1/2})_{1,2}. \tag{16}

The matrix GG is positive definite tridiagonal with strictly positive off-diagonal entries. For every t>0t>0, the tridiagonal cofactor formula gives

[(G+tI)−1]1,2=−G1,2 det⁡((G+tI){3,…,r})det⁡(G+tI)<0.(17)[(G+tI)^{-1}]_{1,2} =-G_{1,2}\, \frac{\det((G+tI)_{\{3,\ldots,r\}})}{\det(G+tI)}<0. \tag{17}

The inverse-square-root integral consequently shows

(G−1/2)1,2=1π∫0∞t−1/2[(G+tI)−1]1,2 dt<0,(18)(G^{-1/2})_{1,2} =\frac1\pi\int_0^{\infty} t^{-1/2}[(G+tI)^{-1}]_{1,2}\,dt<0, \tag{18}

contradicting (15). Thus no nontrivial split is extremal for even n≥6n\geq6 either.

We have proved the stronger real-weight theorem

E(T,w)≤E(Pn;(m−n+2,1,…,1)),n≥5,we≥1,(19)\boxed{\displaystyle \mathcal E(T,w)\leq\mathcal E\big(P_n;(m-n+2,1,\ldots,1)\big), \qquad n\geq5,\quad w_e\geq1, } \tag{19}

with equality if and only if TT is a path and its unique edge of weight m−n+2m-n+2 is pendent, up to reflection. Restricting to positive integral weights proves the original conjecture for every n≥5n\geq5 and m≥nm\geq n.

The restriction n≥5n\geq5 is sharp for uniqueness. When n=4n=4, a path with consecutive weights a,b,ca,b,c has

E(P4;a,b,c)=2(a+c)2+b2.(20)\mathcal E(P_4;a,b,c)=2\sqrt{(a+c)^2+b^2}. \tag{20}

Thus every split of the excess between the two pendent edges, with b=1b=1, attains the same maximum; this is precisely the exceptional equality phenomenon ruled out by (15) when n≥6n\geq6.