Add Journal to My Library
International Mathematics Research Notices
, Volume 2018 (5) – Mar 1, 2018

21 pages

/lp/ou_press/flawlessness-of-h-vectors-of-broken-circuit-complexes-tiO0SDO010

- Publisher
- Oxford University Press
- Copyright
- © The Author 2016. Published by Oxford University Press. All rights reserved. For permissions, please e-mail: journals.permission@oup.com.
- ISSN
- 1073-7928
- eISSN
- 1687-0247
- D.O.I.
- 10.1093/imrn/rnw284
- Publisher site
- See Article on Publisher Site

Abstract One of the major open questions in matroid theory asks whether the $$h$$-vector $$(h_0,h_1,\ldots,h_s)$$ of the broken circuit complex of a matroid $$M$$ satisfies the following inequalities: h0≤h1≤⋯≤h⌊s/2⌋andhi≤hs−i for 0≤i≤⌊s/2⌋. This article affirmatively answers the question for matroids that are representable over a field of characteristic zero. 1 Introduction The notion of broken circuit complexes goes back to Whitney [39], who used his broken circuit idea to interpret the coefficients of the chromatic polynomial of a graph. This notion was later extended to matroids by Rota [27] and Brylawski [6]. Given a loopless matroid $$M$$ on ground set $$E$$, which is endowed with a linear ordering $$<$$, a broken circuit of $$(M,<)$$ is a circuit of $$M$$ with its least element removed. The broken circuit complex of $$(M,<)$$, denoted by $$BC_<(M)$$ (or briefly $$BC(M)$$ if no confusion may arise), is defined by BC(M):={F⊆E:F contains no broken circuit}. Broken circuit complexes have shown to be important in multiple ways. From the algebraic point of view, they play an interesting role in the study of hyperplane arrangements. In particular, the broken circuit idea was used to construct bases for two fundamental algebraic objects associated with a hyperplane arrangement, namely, the Orlik–Solomon algebra and the Orlik–Terao algebra [2, 25]. Through these constructions, broken circuit complexes have been an essential tool for studying important algebraic and homological properties of those algebras [11, 12, 17, 18, 21]. From the combinatorial point of view, $$f$$-vectors and $$h$$-vectors of broken circuit complexes encode very useful information about the underlying matroids. Recall that the characteristic polynomial of a matroid $$M$$ is defined as $$\chi(M;t):=\sum_{X\subseteq E}(-1)^{|X|}t^{r(M)-r(X)}$$, where $$r(\cdot)$$ denotes the rank function of $$M$$. This polynomial, which was introduced by Rota [27] as a generalization of the chromatic polynomial of a graph, plays a prominent role in the study of many combinatorial problems; see, for example, [8, 41]. A fascinating property of $$f$$-vectors of broken circuit complexes, which primarily makes these complexes important, is the following formula due to Whitney [39] and Rota [27]: χ(M;t)=∑i=0r(−1)ifitr−i, (1) where $$f_i$$ denotes the number of faces of $$BC(M)$$ of cardinality $$i$$. The $$h$$-vector of $$BC(M)$$, on the other hand, encodes the shelling polynomial of $$BC(M)$$ [2]. Furthermore, several properties of $$M$$ (such as connectivity [10] or being a series–parallel network [5]) and of $$BC(M)$$ (such as Gorensteinness or being a complete intersection [18]) are determined by the $$h$$-vector of $$BC(M)$$. For these reasons, $$f$$-vectors and $$h$$-vectors of broken circuit complexes are among the most interesting numerical invariants in matroid theory. Recently, great advances have been made in the study of $$f$$-vectors and $$h$$-vectors of broken circuit complexes. In particular, the long-standing conjectures of Rota–Heron [13, 28] and Welsh [38] on the unimodality and log-concavity of the $$f$$-vector of $$BC(M)$$ have been resolved by Adiprasito, Huh and Katz [1]. Additionally, Huh [16] proved that the $$h$$-vector of $$BC(M)$$ is log-concave if $$M$$ is representable over a field of characteristic zero. Recall that a sequence $$(a_0,a_1,\ldots,a_n)$$ of real numbers is said to be log-concave if $$a_j^2\ge a_{j-1}a_{j+1}$$ for all $$1\le j\le n-1$$. Also, this sequence is called unimodal if there exists $$0\leq p\leq n$$ such that $$a_0\leq a_1\leq \cdots \leq a_p\geq a_{p+1}\geq \cdots \geq a_n$$. Observe that if a sequence of positive numbers is log-concave, then it is unimodal. Despite the significant advances mentioned above, $$f$$-vectors and $$h$$-vectors of broken circuit complexes are still rather mysterious. In fact, the problem of characterizing these vectors is widely regarded as out of reach at the moment. A more realistic problem would be to find as many restrictions on these vectors as possible. Such restrictions are predicted by the following conjecture, which is in the focus of this article: Conjecture 1.1. Let $$M$$ be a loopless matroid. Let $$(h_0,h_1,\ldots,h_s)$$ be the $$h$$-vector of $$BC(M)$$, where $$s$$ is the largest index $$j$$ with $$h_j\ne0$$. Then the following inequalities hold: h0≤h1≤⋯≤h⌊s/2⌋andhi≤hs−i for 0≤i≤⌊s/2⌋. □ A sequence $$(h_0,h_1,\ldots,h_s)$$ of real numbers that satisfies the inequalities in the above conjecture is called strongly flawless, and it is called flawless if $$h_i\le h_{s-i}\ \text{ for }\ 0\leq i \leq \lfloor s/2\rfloor$$. Clearly, the strongly flawless condition can be rephrased as $$h_i\le h_j$$ for $$0\le i\le j\le s-i$$. Moreover, for a unimodal sequence, being flawless is equivalent to being strongly flawless. Conjecture 1.1 goes back to a still wide open conjecture of Stanley [32], which anticipates that the $$h$$-vector of the independence complex$$IN(M)$$ of a matroid $$M$$ is a pure $$O$$-sequence. The reader is referred to [3] for the definition of pure $$O$$-sequences as well as recent developments in the study of these interesting objects. Recall that $$IN(M)$$ is the collection of all independent sets in $$M$$, and that it contains $$BC(M)$$ as a subcomplex. In [14], Hibi showed that a pure $$O$$-sequence is strongly flawless. Inspired by this result, he proposed a weaker version of Stanley’s conjecture in [15], predicting that the $$h$$-vector of $$IN(M)$$ must be strongly flawless. This conjecture was resolved by Chari [9], who proved that $$IN(M)$$ has a convex ear decomposition. Subsequently, an algebraic version of Chari’s proof, which shows the existence of $$g$$-elements for a general Artinian reduction of the Stanley–Reisner ring of $$IN(M)$$, was given by Swartz in [34]. Therein, Conjecture 1.1 was also mentioned implicitly. As the set of $$h$$-vectors of independence complexes is strictly contained in the set of $$h$$-vectors of broken circuit complexes (see [6]), Conjecture 1.1 is stronger than and, in particular, implies Hibi’s conjecture. It is worth emphasizing that the techniques of Chari and Swartz for proving Hibi’s conjecture do not work in the case of broken circuit complexes, and thus cannot be used to establish Conjecture 1.1. Indeed, Swartz [34] provided examples of matroids whose broken circuit complexes do not admit $$g$$-elements and hence also fail to have a convex ear decomposition. The main goal of this article is to verify Conjecture 1.1 for matroids representable over a field of characteristic zero. In fact, we prove a somewhat stronger result. We say that a class of matroids $$\mathscr{M}$$ has a certain property (such as unimodal or strongly flawless) if the $$h$$-vector of the broken circuit complex of every matroid in $$\mathscr{M}$$ has that property. The main result of this article is as follows. Theorem 1.2. Let $$\mathscr{M}$$ be a minor-closed class of matroids. If $$\mathscr{M}$$ is unimodal, then it is strongly flawless. □ This theorem implies Conjecture 1.1 for matroids representable over a field of characteristic zero, by virtue of Huh’s log-concavity result [16] (see Corollary 3.5). Let us briefly outline how the proof of Theorem 1.2 proceeds. As mentioned before, a unimodal, flawless sequence is also strongly flawless. So it suffices to show that the $$h$$-vector of $$BC(M)$$ is flawless for every matroid $$M\in\mathscr{M}$$. To this end, we first reduce the proof to the case where $$M$$ is minimally connected (see Lemma 3.1). In this case, $$M$$ contains a removable series class $$S$$ (see Lemma 2.2). We then find two different ways to relate the $$h$$-vector of $$BC(M)$$ to the $$h$$-vector of $$BC(M/S)$$ (see Lemmas 3.2 and 3.3). Combining these comparisons, the flawlessness of the $$h$$-vector of $$BC(M)$$ will follow by induction and the unimodality of the $$h$$-vector of $$BC(M/S)$$. This article is organized as follows. In the next section, we review the basic notions of matroids and broken circuit complexes. Section 3 contains the proof of Theorem 1.2 and its immediate application to Orlik–Terao algebras. Finally, some questions related to our work are discussed in Section 4. 2 Preliminaries 2.1 Matroids The notion of matroids was introduced by Whitney [40] as a common generalization of dependence in linear algebra and graph theory. Since then a rich theory of matroids has been developed which provides a framework for approaching many combinatorial problems. In the following, we collect the needed facts and definitions from matroid theory, referring to the seminal book by Oxley [24] for more details. Definition 2.1. A matroid$$M=(E,\mathscr{I})$$ consists of a finite ground set $$E$$ and a nonempty collection $$\mathscr{I}$$ of subsets of $$E$$, called independent sets, satisfying the following conditions: (i) If $$I\in\mathscr{I}$$ and $$J\subseteq I$$, then $$J\in\mathscr{I}$$. (ii) If $$I,I'\in\mathscr{I}$$ and $$|I|<|I'|$$, then there exists $$e\in I'-I$$ such that $$I\cup e\in\mathscr{I}$$. □ In a matroid $$M=(E,\mathscr{I})$$, a basis is a maximal independent set. A subset of $$E$$ is called dependent if it is not a member of $$\mathscr{I}$$. A circuit is a minimal dependent set, and an $$m$$-circuit is a circuit of cardinality $$m$$. For any set $$X\subseteq E$$, all maximal independent subsets of $$X$$ have the same size, which is called the rank$$r(X)$$ of $$X$$. In particular, the rank of $$E$$, which is the common cardinality of all the bases of $$M$$, is also called the rank of $$M$$ and denoted by $$r(M)$$. A matroid can be specified by either its collection of bases, its collection of circuits, or its rank function. In fact, there are equivalent definitions of matroids in terms of bases, circuits, and rank functions. Two matroids $$M=(E,\mathscr{I})$$ and $$M'=(E',\mathscr{I}')$$ are isomorphic if there exists a bijection $$\varphi:E\to E'$$ such that for every subset $$X$$ of $$E$$, $$X\in\mathscr{I}$$ if and only if $$\varphi(X)\in\mathscr{I}'$$. The prototypical example of a matroid is the vector matroid$$M[A]$$ of a matrix $$A$$: the ground set $$E$$ of $$M[A]$$ is taken to be the set of columns of $$A$$, and a subset $$I\subseteq E$$ is independent if and only if the corresponding columns are linearly independent. A matroid is representable over a field $$K$$ if it is isomorphic to the vector matroid of a matrix over $$K$$. It should be noted, however, that not every matroid is representable over some field; see [24, Proposition 6.1.10]. Let $$M$$ be a matroid on the ground set $$E$$. Let $$\mathscr{B}$$ be the collection of bases of $$M$$. Then $$\mathscr{B}^*=\{E-B : B\in\mathscr{B}\}$$ is also the collection of bases of a matroid $$M^*$$. We call this matroid the dual of $$M$$. For example, $$M[A]^*\cong M[A^*]$$ for any matrix $$A$$, where $$A^*$$ is a matrix whose row space is the orthogonal space of the row space of $$A$$. An element $$e\in E$$ is called a loop if $$\{e\}$$ is a circuit of $$M$$. We say that $$M$$ is loopless if it has no loops. A loop of $$M^*$$ is called a coloop of $$M$$. More generally, circuits of $$M^*$$ are called cocircuits of $$M$$. A series class$$S$$ of $$M$$ is a maximal subset of $$E$$ such that $$S$$ contains no coloops and if $$e,f$$ are distinct elements of $$S$$, then $$\{e,f\}$$ is a cocircuit of $$M$$. A series class is non-trivial if it contains at least two elements. Notice that if $$S$$ is a series class and $$C$$ is a circuit of $$M$$, then either $$C\cap S=\emptyset$$ or $$S\subseteq C$$. This follows from the well-known fact that a circuit and a cocircuit of $$M$$ cannot have just a single element in common; see [24, Proposition 2.1.11]. Let $$X$$ be a subset of $$E$$. The deletion of $$X$$ from $$M$$, denoted $$M-X$$, is the matroid on ground set $$E-X$$ whose independent sets are the independent sets of $$M$$ that are contained in $$E-X$$. The contraction of $$X$$ from $$M$$ is defined to be $$M/X=(M^*-X)^*$$. Note that the operations of deletion and contraction commute, that is, $$(M-X)/Y=M/Y-X$$ for disjoint subsets $$X$$ and $$Y$$ of $$E$$. A minor of $$M$$ is a matroid which can be obtained from $$M$$ by a sequence of deletions and contractions. A class of matroids $$\mathscr{M}$$ is said to be minor-closed if for every $$M\in\mathscr{M}$$, all minors of $$M$$ are also members of $$\mathscr{M}$$. Let $$M_1$$ and $$M_2$$ be matroids on disjoint ground sets $$E_1$$ and $$E_2$$. Their direct sum$$M_1\oplus M_2$$ is the matroid on ground set $$E_1\cup E_2$$ whose independent sets are all possible unions of an independent set of $$M_1$$ with an independent set of $$M_2$$. The direct sum of a finite collection of matroids is then defined by iterating the previous construction. A matroid is called connected if it is not the direct sum of two smaller matroids. Otherwise, it is called disconnected. An arbitrary matroid $$M$$ can be decomposed uniquely (up to ordering) as a direct sum $$M=M_1\oplus\cdots\oplus M_k$$, where $$M_1,\ldots,M_k$$ are connected matroids. In that case, the matroids $$M_1,\ldots,M_k$$ are called the connected components of $$M$$. Let $$M$$ be a connected matroid on $$E$$. Then $$M$$ is called minimally connected if $$M-e$$ is disconnected for every $$e\in E$$. On the other hand, a series class $$S$$ of $$M$$ is said to be removable if $$M-S$$ is connected. Evidently, every removable series class of a minimally connected matroid is non-trivial. For the existence of removable series classes we will need the following result. Lemma 2.2. Let $$M$$ be a connected matroid on the ground set $$E$$ with at least two elements. Then $$M$$ contains a removable series class. In particular, if $$M$$ is minimally connected, then it contains a non-trivial removable series class. □ Proof. If $$M$$ has exactly one series class, then $$E$$ forms a circuit and hence $$E$$ itself is a removable series class of $$M$$. When $$M$$ contains at least two series classes, the result follows from [35, Proposition 5.3]. ■ Let $$M_1$$ and $$M_2$$ be matroids on ground sets $$E_1$$ and $$E_2$$ with $$E_1\cap E_2=\{e\}$$. Assume that $$e$$ is neither a loop nor a coloop of $$M_1$$ or $$M_2$$. Let $$\mathscr{C}(M_i)$$ denote the collection of circuits of $$M_i$$. The parallel connection$$P(M_1,M_2)$$ of $$M_1$$ and $$M_2$$ with respect to $$e$$ is the matroid on $$E_1\cup E_2$$ whose collection of circuits is given by C(P(M1,M2))=C(M1)∪C(M2)∪{C1∪C2−e:e∈Ci∈C(Mi) for i=1,2}. The deletion $$P(M_1,M_2)-e$$ is called the $$2$$-sum of $$M_1$$ and $$M_2$$, denoted by $$M_1\oplus_2M_2$$. Note that the circuits of $$M_1\oplus_2M_2$$ are the circuits of $$P(M_1,M_2)$$ not containing $$e$$; see [24, 3.1.14]. Thus C(M1⊕2M2)=C(M1−e)∪C(M2−e)∪{C1∪C2−e:e∈Ci∈C(Mi) for i=1,2}. (2) The following simple observation will be useful in Section 3. For brevity’s sake we call a matroid an $$m$$-circuit if its ground set is an $$m$$-circuit. Lemma 2.3. Let $$S$$ be a series class of a matroid $$M$$ with $$|S|=m$$. Set $$\widetilde{M}=M/(S-e)$$ for some $$e\in S$$. Then $$M\cong \widetilde{M}\oplus_2 C$$, where $$C$$ is an $$(m+1)$$-circuit containing $$e$$. □ Proof. By a slight abuse of notation we identify $$C$$ with its ground set. Then we may write $$C=S'\cup e$$, where $$|S'|=|S|$$. Notice that the collection $$\mathscr{C}(\widetilde{M})$$ of circuits of $$\widetilde{M}$$ consists of the minimal nonempty members of $$\mathscr{D}:=\{D-(S-e): D\in \mathscr{C}(M)\}$$; see [24, Proposition 3.1.11]. Since $$S$$ is a series class, either $$D\cap S=\emptyset$$ or $$S\subseteq D$$ for every $$D\in \mathscr{C}(M)$$. Hence, all members of $$\mathscr{D}$$ are minimal and nonempty. This yields C(M~)=D={D:D∈C(M),D∩S=∅}∪{D−(S−e):D∈C(M),S⊆D}. Now by (2), C(M~⊕2C) =C(M~−e)∪C(C−e)∪{C∪D−S:D∈C(M),S⊆D} ={D:D∈C(M),D∩S=∅}∪{S′∪(D−S):D∈C(M),S⊆D}. It then follows readily that $$M\cong \widetilde{M}\oplus_2 C$$, as desired. ■ Example 2.4. Let $$M$$ be the cycle matroid of the complete bipartite graph $$K_{2,3}$$, with the edges labelled as in Figure 1(a). Then $$S=\{1,2\}$$ is a series class of $$M$$. The 2-sum of $$\widetilde{M}=M/\{1\}$$ and the 3-circuit $$C=\{2,1',2'\}$$, which is the cycle matroid of the graph depicted in Figure 1(d), is clearly isomorphic to $$M$$. □ Fig. 1. View largeDownload slide $$M \cong \widetilde{M}\oplus_2 C$$. Fig. 1. View largeDownload slide $$M \cong \widetilde{M}\oplus_2 C$$. By iterating, the operation of parallel connection can be defined for special families of more than two matroids. Let $$M_1,\ldots,M_n$$ be matroids on ground sets $$E_1,\ldots,E_n$$ such that $$E_{i+1}\cap(\bigcup_{j=1}^i E_j)=\{e_i\}$$ for $$i=1,\ldots,n-1$$. Here, $$e_1,\ldots,e_{n-1}$$ need not be distinct. Assume further that each $$e_i$$ is neither a loop nor a coloop of the matroids containing it. Then we can form $$P(M_1,M_2)$$, $$P(P(M_1,M_2),M_3)$$, and so on. The last matroid obtained in this way, denoted by $$P(M_1,\ldots,M_n)$$, is called the parallel connection of $$M_1,\ldots,M_n$$ with respect to $$e_1,\ldots,e_{n-1}$$. Assume $$M$$ is a connected matroid on $$E$$. Then $$M$$ is called parallel irreducible at $$e\in E$$ if either $$|E|=1$$ or $$M$$ is not a parallel connection of two smaller matroids with respect to $$e$$. We say that $$M$$ is parallel irreducible if it is parallel irreducible at every element of $$E$$. The following result, which was essentially proved by Brylawski [5, Propositions 5.8, 5.9] (see also [19, Lemma 2.1]), indicates that in certain matroid arguments the general result can be obtained by restricting attention to the parallel irreducible case. Lemma 2.5. Let $$M$$ be a connected matroid on the ground set $$E$$. Then the following statements hold: (i) If $$M=P(M_1,M_2)$$ with respect to $$e$$, then $$M/e$$ is disconnected: M/e=M1/e⊕M2/e. Conversely, if $$M/e$$ is disconnected, then $$M$$ is a parallel connection of two smaller matroids with respect to $$e$$. Hence, $$M$$ is parallel irreducible if and only if $$M/e$$ is connected for every $$e\in E$$. (ii) $$M$$ admits a decomposition $$M=P(M_1,\ldots,M_n)$$, where each $$M_i$$ is connected and parallel irreducible. □ 2.2 Broken circuit complexes Let $$M$$ be a matroid, whose ground set $$E$$ is endowed with a linear order $$<$$. We further assume that $$M$$ is loopless, since otherwise $$BC(M)=\emptyset$$, which is not interesting for us here. Let $$r=r(M)$$. Then it is well-known that $$BC(M)$$ is an $$(r-1)$$-dimensional shellable simplicial complex; see [26] or [2, 7.4]. Let $$f(M)=(f_0(M),\ldots,f_r(M))$$ be the $$f$$-vector of $$BC(M)$$, where $$f_i(M)$$ is the number of faces of $$BC(M)$$ of cardinality $$i$$. Notice that $$f(M)$$ is independent of the chosen order $$<$$, as is easily seen from the Whitney–Rota formula (1). Define the $$h$$-vector$$h(M)=(h_0(M),\ldots,h_r(M))$$ and the $$h$$-polynomial (or shelling polynomial) $$h(M;t)=\sum_{i=0}^rh_i(M)t^{r-i}$$ of $$BC(M)$$ by the polynomial identity $$h(M;t)=(-1)^r\chi(M;1-t)$$. Thus, the $$f$$-vector and the $$h$$-vector of $$BC(M)$$ are correlated as follows fi(M)=∑j=0i(r−ji−j)hj(M) and hi(M)=∑j=0i(−1)i−j(r−ji−j)fj(M), i=0,…,r. In the sequel, for convenience, we make the convention that $$h_i(M)=0$$ for $$i<0$$ or $$i>r$$. Moreover, when it is clear from the context which matroid we are referring to, we will just write $$h_i$$ instead of $$h_i(M)$$. Both $$\chi(M;t)$$ and $$h(M;t)$$ are, up to sign, evaluations of the Tutte polynomial$$T(M;x,y)$$ of $$M$$, which is defined by T(M;x,y)=∑X⊆E(x−1)r(E)−r(X)(y−1)|X|−r(X). Evidently, $$\chi(M;t)=(-1)^rT(M;1-t,0)$$. Hence, $$h(M;t)=T(M;t,0)$$. For later usage we collect here several basis properties of the $$h$$-polynomial of $$BC(M)$$. They follow easily from the corresponding properties of the Tutte polynomial of $$M$$; see [8, 6.2] and [7, p. 182]. Lemma 2.6. Let $$M$$ be a loopless matroid of rank $$r$$ on the ground set $$E$$. Let $$h(M;t)=\sum_{i=0}^rh_it^{r-i}$$ be the $$h$$-polynomial of $$BC(M)$$. Then the following statements hold: (i) $$h_i\geq 0$$ for $$i=0,\ldots,r$$. Moreover, if $$M$$ has $$c$$ connected components, then $$r-c$$ is the largest index $$i$$ such that $$h_{i}\ne0$$. (ii) (Deletion-contraction) Suppose $$|E|\geq 2$$ and $$e\in E$$. Then h(M;t)={th(M−e;t) if e is a coloop of M,h(M−e;t)+h(M/e;t) otherwise. Thus, in particular, if $$M$$ is connected, then either $$M-e$$ or $$M/e$$ is connected. (iii) If $$M$$ is an $$(r+1)$$-circuit, then $$h(M;t)=t^r+t^{r-1}+\cdots+t$$ . (iv) Assume that $$M$$ is either the direct sum or the parallel connection of two matroids $$M_1$$ and $$M_2$$. Then h(M;t)={h(M1;t)h(M2;t) if M=M1⊕M2,t−1h(M1;t)h(M2;t) if M=P(M1,M2). □ As an important step in the proof of Theorem 1.2, we will relate the $$h$$-vector of $$BC(M)$$ to the $$h$$-vectors of broken circuit complexes of certain minors of $$M$$ which are obtained from $$M$$ by deleting or contracting elements in a series class. For this, the following simple facts will be necessary. Lemma 2.7. Let $$S=\{e_1,\ldots,e_m\}$$ be a series class of a loopless matroid $$M$$. For $$0\le j\le m-1$$, set $$M_j=M/\{e_1,\ldots,e_j\}$$ and $$S_j=\{e_{j+1},\ldots,e_m\}$$. Then the following statements hold: (i) $$r(M-S)=r(M)-m+1$$. (ii) $$r(M_j)=r(M)-j$$, and if $$M$$ is connected, so is $$M_j$$. (iii) $$S_j$$ is a series class of $$M_j$$ and $$M_j-S_j= M-S$$. (iv) For every $$e\in S$$ and $$e'\in S_j$$ the $$h$$-vectors of the broken circuit complexes of the matroids $$M-e,\ M-S$$ and $$M_j-e'$$ coincide. □ Proof. (i) Since, by definition, $$e_1$$ is not a coloop of $$M$$, we have that $$r(M-e_1)=r(M)$$; see, for example, [24, 3.1.5]. Now as every element of $$S_1$$ is a coloop of $$M-e_1$$, it holds that r(M−S)=r((M−e1)−S1)=r(M−e1)−|S1|=r(M)−m+1. (ii) As $$M_j=M_{j-1}/e_j$$ and $$e_j$$ is not a loop of $$M_{j-1}$$, we have $$r(M_j)=r(M_{j-1})-1$$; see for example, [24, 3.1.7]. In addition, $$M_{j-1}-e_j$$ is not connected since every element of $$S_j$$ is a coloop of this matroid. Hence, by Lemma 2.6(ii), $$M_j$$ is connected if $$M_{j-1}$$ is so. The assertion now follows by induction. (iii) By definition, it is easy to see that $$S_j$$ is a series class of $$M_j$$. Now since $$e_1,\ldots,e_j$$ are coloops of $$M-S_j$$, it follows from [24, Corollary 3.1.25] that Mj−Sj=(M−Sj)/{e1,…,ej}=(M−Sj)−{e1,…,ej}=M−S. (iv) Since the elements of $$S-e$$ are coloops of $$M-e$$, Lemma 2.6(ii) yields $$h(M-e;t)=t^{m-1}h(M-S;t)$$. Similarly, $$h(M_j-e';t)=t^{m-j-1}h(M_j-S_j;t)$$. As $$M-S=M_j-S_j$$ by (iii), the assertion follows. ■ 3 Flawlessness of $$h$$-vectors of broken circuit complexes This section is devoted to the proof of Theorem 1.2 and its applications. We begin with the following lemma, which is essential for reducing the proof of Theorem 1.2 to the case of minimally connected matroids. Recall that a sequence $$(a_0,a_1,\ldots,a_n)$$ is symmetric if $$a_i=a_{n-i}$$ for $$0\le i\le n$$. Let us say that a polynomial $$a_0t^{n+u}+a_1t^{n+u-1}+\cdots +a_nt^u$$ with $$a_0, a_n\ne 0$$ and $$u\ge0$$ has a certain property (such as symmetric, unimodal or strongly flawless) if its coefficient sequence $$(a_0,a_1,\ldots,a_n)$$ has that property. Lemma 3.1. If $$\varphi(t)$$ and $$\psi(t)$$ are strongly flawless polynomials with nonnegative coefficients, then so is their product. □ Proof. By definition, a polynomial is strongly flawless if and only if its product with any power $$t^u$$ ($$u\ge0$$) is so. Hence without loss of generality we may assume that $$\varphi(t)$$ and $$\psi(t)$$ have the following form: φ(t) =a0tn+a1tn−1+⋯+an−1t+an,ψ(t) =b0tm+b1tm−1+⋯+bm−1t+bm, where $$a_0,a_n,b_0,b_m> 0$$. We will argue by induction on dφ,ψ:=|{0≤i≤⌊n/2⌋:ai<an−i}|+|{0≤j≤⌊m/2⌋:bj<bm−j}|. If $$d_{\varphi, \psi}=0$$, then $$\varphi(t)$$ and $$\psi(t)$$ are symmetric polynomials. Observe that for a symmetric polynomial, being strongly flawless is equivalent to being unimodal. So $$\varphi(t)$$ and $$\psi(t)$$ are symmetric and unimodal. It follows that their product $$\varphi(t)\psi(t)$$ is also symmetric and unimodal (see, for example, [33, Proposition 1]). Thus, $$\varphi(t)\psi(t)$$ is strongly flawless, and we are done in this case. Now consider the case $$d_{\varphi, \psi}>0$$. We may suppose that $$a_i<a_{n-i}$$ for some $$0\le i\le \lfloor n/2\rfloor$$. Set $$k:=\min\{0\le i\le \lfloor n/2\rfloor: a_i<a_{n-i}\}$$. Let $$\overline{\varphi}(t)$$ be the polynomial obtained from $$\varphi(t)$$ by replacing the term $$a_{n-k}t^k$$ of $$\varphi(t)$$ with $$a_{k}t^k$$, that is, $$\overline{\varphi}(t)=\varphi(t)+(a_k-a_{n-k})t^{k}.$$ Then it is readily seen that $$\overline{\varphi}(t)$$ is strongly flawless. Moreover, $$d_{\overline{\varphi}, \psi}=d_{\varphi, \psi}-1$$. Writing $$\varphi(t)\psi(t)=\sum_{i=0}^{m+n}c_it^{m+n-i}$$ and $$\overline{\varphi}(t)\psi(t)=\sum_{i=0}^{m+n}c'_it^{m+n-i}$$, we get ci=∑u+v=iaubv={ci′if i<n−k or i>m+n−k,ci′+(an−k−ak)bi+k−notherwise. (3) Since $$a_{n-k}>a_k$$ and the coefficients of $$\psi(t)$$ are nonnegative, it holds that $$c_i\ge c'_i$$ for all $$i$$. Now let $$0\le i\le j\le m+n-i$$. We have to show that $$c_i\le c_j$$. Note that $$c'_i\le c'_j$$ by induction. So, if $$i<n-k$$, then it follows from (3) that $$c_i=c'_i\le c'_j\le c_j$$. Now suppose $$i\ge n-k$$. Then $$i\ge k$$ since $$k\le \lfloor n/2\rfloor$$. Hence $$j\le m+n-i \le m+n-k$$. Again by (3) we have cj−ci=cj′−ci′+(an−k−ak)(bj+k−n−bi+k−n)≥(an−k−ak)(bj+k−n−bi+k−n). Thus, the inequality $$c_i\le c_j$$ will be confirmed once we have shown that $$b_{i+k-n}\le b_{j+k-n}$$. But the last inequality holds since $$0\le i+k-n\le j+k-n\le m-(i+k-n)$$ (which follows easily from $$n-k\le i\le j\le m+n-i$$ and $$k\le \lfloor n/2\rfloor$$) and $$\psi(t)$$ is strongly flawless. This completes the proof. ■ In the sequel, for our purposes, it will be convenient to consider $$h$$-vectors with zero entries at the end removed. So, if we say that $$h(M)=(h_0(M),h_1(M),\ldots,h_s(M))$$ is the $$h$$-vector of $$BC(M)$$, then $$s$$ is the largest index $$i$$ with $$h_i(M)\ne 0$$. In this case, recall from Lemma 2.6(i) that $$s=r-c$$, where $$r=r(M)$$ and $$c$$ is the number of connected components of $$M$$. Now let $$M$$ be a loopless matroid and let $$h(M)=(h_0(M),h_1(M),\ldots,h_s(M))$$ be the $$h$$-vector of $$BC(M)$$. Define h¯i(M):={hs−i(M)−hi(M)for 0≤i≤⌊s/2⌋,0otherwise. Following Swartz [36], we call $$\bar h(M):=(\bar h_0(M),\bar h_1(M),\ldots,\bar h_{\lfloor s/2\rfloor}(M))$$ the complementary $$h$$-vector of $$BC(M)$$. For convenience we set $$\bar h(M)=(0)$$ if $$M$$ contains a loop. The next two lemmas present two different interpretations of the complementary $$h$$-vector of $$BC(M)$$ which involve the $$h$$-vector of $$BC(M/S)$$, where $$S$$ is a (removable) series class of $$M$$. Recall our convention that $$h_i(M/S)=0$$ for $$i<0$$ or $$i>r(M/S)$$. Lemma 3.2. Let $$M$$ be a connected matroid and $$S$$ a non-trivial removable series class of $$M$$ with $$|S|=m$$. Let $$h(M)=(h_0(M),h_1(M),\ldots,h_s(M))$$ be the $$h$$-vector of $$BC(M)$$. Then for every $$e\in S$$ and $$0\le i\le \lfloor s/2\rfloor$$, h¯i(M)=h¯i(M/e)+h¯i−m+1(M−S)+(hi−m+1(M/S)−hi−m(M/S)). □ Proof. If $$M$$ is a $$2$$-circuit, then the statement is easily seen to be true. So assume that $$M$$ is not a $$2$$-circuit. Suppose $$S=\{e_1,\ldots,e_m\}$$ with $$e=e_1$$. Set $$M_j=M/\{e_1,\ldots,e_j\}$$ for $$j=1,\ldots,m$$. We will show via induction that h¯i(M) =h¯i(M/e1)+h¯i−m+1(M−S)+(hi−j+1(Mj)−hi−j(Mj)) +(hi−m+1(M−S)−hi−j+1(M−S)) (4) for $$j=1,\ldots,m$$. The case $$j=m$$ then gives the desired assertion. Using the deletion-contraction formula (Lemma 2.6(ii)) and Lemma 2.7(iv), we have h¯i(M) =hs−i(M)−hi(M) =(hs−i(M−e1)+hs−i−1(M/e1))−(hi(M−e1)+hi−1(M/e1)) =(hs−i−1(M/e1)−hi(M/e1))+(hs−i(M−S)−hi−m+1(M−S)) +(hi(M/e1)−hi−1(M/e1))+(hi−m+1(M−S)−hi(M−S)). (5) By Lemma 2.7(ii), $$M/e_1$$ is connected and $$r(M/e_1)=r(M)-1$$. Thus, in particular, $$M/e_1$$ is loopless since $$M$$ is not a 2-circuit. So from Lemma 2.6(i) it follows that $$h_{s-1}(M/e_1)\ne 0$$, and hence $$\bar h_i(M/e_1)=h_{s-i-1}(M/e_1)-h_{i}(M/e_1)$$. Similarly, as $$M-S$$ is connected and $$r(M-S)=r(M)-m+1$$ (see Lemma 2.7(i)), it holds that $$h_{s-m+1}(M-S)\ne 0$$ and $$\bar h_{i-m+1}(M-S)=h_{s-i}(M-S)-h_{i-m+1}(M-S)$$. Thus (5) implies that (4) is true for $$j=1$$. To complete the induction argument, it suffices to show that (hi−j+1(Mj)−hi−j(Mj))+(hi−m+1(M−S)−hi−j+1(M−S)) =(hi−j(Mj+1)−hi−j−1(Mj+1))+(hi−m+1(M−S)−hi−j(M−S)), or equivalently, hi−j+1(Mj)−hi−j(Mj)= (hi−j(Mj+1)+hi−j+1(M−S)) −(hi−j−1(Mj+1)+hi−j(M−S)). But the last equality follows from the deletion-contraction formula, since $$M_{j+1}=M_j/e_{j+1}$$ and $$h_k(M-S)=h_k(M_j-e_{j+1})$$ (by Lemma 2.7(iv)). This finishes the proof. ■ Lemma 3.3. Let $$M$$ be a connected matroid and $$S$$ a series class of $$M$$ with $$|S|=m$$. Set $$\widetilde{M}=M/(S-e)$$ for some $$e\in S$$. Let $$h(M)=(h_0(M),h_1(M),\ldots,h_s(M))$$ be the $$h$$-vector of $$BC(M)$$. Then h¯i(M)={∑j=0min{i,s−m−i}h¯j(M~)+∑j=1i(hi−j(M/S)−hs−m+1−j(M/S)) if 0≤i≤min{m−1,s−m+1},∑j=i−m+1min{i,s−m−i}h¯j(M~)+∑j=1m−1(hi−j(M/S)−hs−i−j(M/S)) if m−1≤s−m+1 and m−1≤i≤⌊s/2⌋,0 if s−m+1≤m−1 and s−m+1≤i≤⌊s/2⌋. □ Proof. Note that $$\widetilde{M}$$ is connected by Lemma 2.7(ii). So $$\widetilde{M}$$ contains a loop if and only if it is itself a loop, which means that $$M$$ is a circuit. Since the lemma is clearly true in this case, we may henceforth assume that $$\widetilde{M}$$ is loopless. By Lemma 2.3, $$M\cong P(\widetilde{M}, C)-e$$, where $$C$$ is an $$(m+1)$$-circuit containing $$e$$. Thus, the deletion-contraction formula, Lemma 2.5(i) and Lemma 2.6(iv) yield h(M;t) =h(P(M~,C);t)−h(P(M~,C)/e;t) =h(P(M~,C);t)−h(M~/e⊕C/e;t) =h(M~;t)h(C;t)t−h(M/S;t)h(C/e;t). (6) Since $$r(\widetilde{M})=r(M)-m+1=s-m+2$$ (see Lemma 2.7(ii)) and $$r(M/S)=r(\widetilde{M})-1=s-m+1$$, we may write h(M~;t) =h0(M~)ts−m+2+h1(M~)ts−m+1+⋯+hs−m+1(M~)t and h(M/S;t) =h0(M/S)ts−m+1+h1(M/S)ts−m+⋯+hs−m(M/S)t. Plugging these polynomials into (6) and using Lemma 2.6(iii) we get h(M;t)=(∑j=0s−m+1hj(M~)ts−m+2−j)(∑k=0m−1tk)−(∑j=0s−mhj(M/S)ts−m+1−j)(∑k=1m−1tk). (7) From this formula we will derive formulas for the coefficients of $$h(M;t)$$, and thereby obtain the desired formula for the complementary $$h$$-vector. We distinguish two cases: $${\sf Case 1:}$$$$m-1\le s-m+1$$. Note that $$h_i(M)$$ is the coefficient of $$t^{s-i+1}$$ in $$h(M;t)$$. So from (7) we get hi(M)={∑j=0ihj(M~)−∑j=0i−1hj(M/S) for i≤m−1,∑j=i−m+1ihj(M~)−∑j=i−m+1i−1hj(M/S) for m−1≤i≤s−m+1,∑j=i−m+1s−m+1hj(M~)−∑j=i−m+1s−mhj(M/S) for s−m+1≤i≤s. (8) As $$\widetilde{M}$$ is loopless and connected, it follows from Lemma 2.6(i) that $$h_{s-m+1}(\widetilde{M})\ne 0$$. Thus $$\bar h_{j}(\widetilde{M})=h_{s-m+1-j}(\widetilde{M})-h_{j}(\widetilde{M})$$ for $$0\le j\le \lfloor \frac{s-m+1}{2}\rfloor$$. Now it is readily seen from (8) that h¯i(M)=hs−i(M)−hi(M)={∑j=0min{i,s−m−i}h¯j(M~)+∑j=1i(hi−j(M/S)−hs−m+1−j(M/S)) for 0≤i≤m−1,∑j=i−m+1min{i,s−m−i}h¯j(M~)+∑j=1m−1(hi−j(M/S)−hs−i−j(M/S)) for m−1≤i≤⌊s/2⌋. $${\sf Case 2:}$$$$s-m+1< m-1$$. In this case, (7) gives hi(M)={∑j=0ihj(M~)−∑j=0i−1hj(M/S) for i≤s−m+1,∑j=0s−m+1hj(M~)−∑j=0s−mhj(M/S) for s−m+1≤i≤m−1,∑j=i−m+1s−m+1hj(M~)−∑j=i−m+1s−mhj(M/S) for m−1≤i≤s. Hence h¯i(M)={∑j=0min{i,s−m−i}h¯j(M~)+∑j=1i(hi−j(M/S)−hs−m+1−j(M/S)) for 0≤i≤s−m+1,0 for s−m+1≤i≤⌊s/2⌋. The desired formula for $$\bar h_i(M)$$ is obtained by combining the two cases above. ■ Example 3.4. Let us revisit the cycle matroid $$M$$ of the complete bipartite graph $$K_{2,3}$$ discussed in Example 2.4. Notice that the series class $$S=\{1,2\}$$ of $$M$$ is removable. The graphs corresponding to the minors $$\widetilde{M}=M/\{1\},\ M-S,\ M/S$$ of $$M$$ are depicted in Figure 2. Using Lemma 2.6 one easily finds that $$h(M/S;t)=t^2,$$$$h(M-S;t)=t^3+t^2+t,$$$$h(\widetilde{M};t)=t^3+2t^2+t$$, and $$h(M;t)=t^4+2t^3+3t^2+t$$. Thus $$\bar h(M)=(1-1,3-2)=(0,1)$$. This agrees with the computation of $$\bar h(M)$$ using Lemma 3.2 or Lemma 3.3. For example, by Lemma 3.2, h¯1(M)=h¯1(M/{1})+h¯0(M−S)+(h0(M/S)−h−1(M/S))=0+0+(1−0)=1. On the other hand, by Lemma 3.3, h¯1(M)=h¯0(M~)+(h0(M/S)−h1(M/S))=0+(1−0)=1. □ Fig. 2. View largeDownload slide Minors of $$M$$ related to removable series class $$S=\{1,2\}$$. Fig. 2. View largeDownload slide Minors of $$M$$ related to removable series class $$S=\{1,2\}$$. We are now ready to prove our main result. Proof of Theorem 1.2. Let $$M\in\mathscr{M}$$ and let $$h(M)=(h_0(M),h_1(M),\ldots,h_s(M))$$ be the $$h$$-vector of $$BC(M)$$. Since $$h(M)$$ is unimodal by assumption, it suffices to prove that $$h(M)$$ is flawless, that is, the complementary $$h$$-vector of $$BC(M)$$ is nonnegative. We proceed by induction on the cardinality of the ground set $$E$$ of $$M$$. If $$|E|=1$$, then $$h(M)=(1)$$ and we have nothing to prove. So suppose $$|E|\ge2$$. We first show that we can reduce to the case where $$M$$ is minimally connected. By Lemmas 2.5(ii), 2.6(iv) and 3.1, we may assume that $$M$$ is connected, and furthermore, parallel irreducible. Thus, by Lemma 2.5(i), $$M/e$$ is connected for every $$e\in E$$. We will show that $$\bar h_i(M)\ge 0$$ for $$0\le i\le \lfloor s/2\rfloor$$ if there exists $$e\in E$$ with $$M-e$$ connected. Indeed, if $$s$$ is even and $$i=s/2$$, then $$\bar h_i(M)=0$$. Now assume that $$s$$ is odd or $$i<s/2$$. Then $$i\le \lfloor (s-1)/2\rfloor$$. Using the deletion-contraction formula we have h¯i(M) =hs−i(M)−hi(M) =(hs−i(M−e)+hs−i−1(M/e))−(hi(M−e)+hi−1(M/e)) =(hs−i(M−e)−hi(M−e))+(hs−i−1(M/e)−hi(M/e)) +(hi(M/e)−hi−1(M/e)) =h¯i(M−e)+h¯i(M/e)+(hi(M/e)−hi−1(M/e)). (9) The last equality follows since $$M-e$$ and $$M/e$$ are connected. By the induction hypothesis, the $$h$$-vectors of $$BC(M-e)$$ and $$BC(M/e)$$ are strongly flawless, implying that each summand of $$\bar h_i(M)$$ in the last row of (9) is nonnegative. Therefore, $$\bar h_i(M)$$ is nonnegative as well. Henceforth we may assume that $$M$$ is minimally connected. Then $$M$$ contains a non-trivial removable series class by Lemma 2.2. Let $$S$$ be such a series class of $$M$$ with $$|S|=m$$. Given $$0\le i\le \lfloor s/2\rfloor$$, let us verify that $$\bar h_i(M)\ge 0$$. If $$i\le m-1$$, then $$\bar h_i(M)\ge 0$$ by Lemma 3.2 and the induction hypothesis. Now consider the case $$i>m-1$$. Since $$i\le \lfloor s/2\rfloor$$, we must have $$m-1<s-m+1$$. It then follows from Lemmas 3.2, 3.3 and the induction hypothesis that h¯i(M)≥max{hi−m+1(M/S)−hi−m(M/S),∑j=1m−1(hi−j(M/S)−hs−i−j(M/S))}. Thus, if $$h_{i-m+1}(M/S)\ge h_{i-m}(M/S)$$, then $$\bar h_i(M)\ge 0$$. Suppose now that $$h_{i-m}(M/S)>h_{i-m+1}(M/S)$$. Then the unimodality of the $$h$$-vector of $$BC(M/S)$$ yields hi−m+1(M/S)≥⋯≥hi−1(M/S)≥⋯≥hs−i−1(M/S). It follows that for $$1\le j \le m-1$$, we have $$h_{i-j}(M/S)\ge h_{s-i-j}(M/S)$$, because $$i-m+1\le i-j\le s-i-j\le s-i-1$$. Hence ∑j=1m−1(hi−j(M/S)−hs−i−j(M/S))≥0, which also implies that $$\bar h_i(M)\ge 0$$. The proof is complete. ■ As a consequence of Theorem 1.2, we verify Conjecture 1.1 for matroids representable over a field of characteristic zero. Corollary 3.5. Let $$M$$ be a matroid representable over a field of characteristic zero. Then the $$h$$-vector of $$BC(M)$$ is strongly flawless. □ Proof. Let $$\mathscr{M}$$ be the class of matroids representable over a field of characteristic zero. Then it is well-known that $$\mathscr{M}$$ is minor-closed; see [24, Proposition 3.2.4]. Moreover, it follows from Huh’s log-concavity result [16, Theorem 3] that $$\mathscr{M}$$ is unimodal. So $$\mathscr{M}$$ is strongly flawless by Theorem 1.2. ■ Let us now derive an application of Corollary 3.5 to Orlik–Terao algebras. Recall that a (central) complex hyperplane arrangement$$\mathscr{A}=\{H_1,\ldots,H_n\}$$ is a collection of hyperplanes in $$\mathbb{C}^{r}$$, all of which contain the origin of $$\mathbb{C}^{r}$$. Suppose each hyperplane $$H_i$$ of $$\mathscr{A}$$ is given as the kernel of a linear form $$\alpha_i$$. Then the Orlik–Terao algebra of $$\mathscr{A}$$ is defined to be the $$\mathbb{C}$$-algebra generated by reciprocals of the $$\alpha_i$$’s: C(A):=C[1/α1,…,1/αn]. This algebra was introduced by Orlik and Terao in [23]. Since then it has appeared in different contexts and received considerable attention; see for example, [4, 11, 18, 20–22, 25, 29–31, 37]. An interesting property of $$C(\mathscr{A})$$ is that it degenerates flatly to the Stanley–Reisner ring of the broken circuit complex of the underlying matroid$$M(\mathscr{A})$$ of $$\mathscr{A}$$ [25, Theorem 4]. Thus, in particular, $$C(\mathscr{A})$$ is a Cohen–Macaulay ring and its $$h$$-vector coincides with the $$h$$-vector of $$BC(M(\mathscr{A}))$$. Recall that the underlying matroid $$M(\mathscr{A})$$ is defined to be the matroid on ground set $$\mathscr{A}$$ such that a subset $$B = \{H_{ i_ 1},\ldots , H _{i_ p}\}$$ of $$\mathscr{A}$$ is independent if and only if the corresponding linear forms $$\alpha_{i_1}, \ldots,\alpha_{i_p}$$ are linearly independent. Evidently, $$M(\mathscr{A})$$ is representable over $$\mathbb{C}$$. So from Corollary 3.5 we immediately get the following: Corollary 3.6. Let $$\mathscr{A}$$ be a complex hyperplane arrangement. Then the $$h$$-vector of the Orlik–Terao algebra of $$\mathscr{A}$$ is strongly flawless. □ It should be noted here that $$C(\mathscr{A})$$ has a canonical linear system of parameters [25, Proposition 7] and that, similar to Swartz’s examples mentioned in the introduction, the corresponding Artinian reduction of $$C(\mathscr{A})$$ needs not have $$g$$-elements [25, Remark 8]. It would therefore be difficult to provide an algebraic proof of the above corollary. 4 Concluding remarks In view of our main result (Theorem 1.2), Conjecture 1.1 would follow from the first one of the following successively stronger conjectured assertions: Conjecture 4.1. Let $$h(M)=(h_0,h_1,\ldots,h_s)$$ be the $$h$$-vector of the broken circuit complex of a matroid $$M$$. Set $$h'_i=h_i/\binom{h_1+i-1}{i}$$ for $$i=0,1,\ldots, s$$. Then (i) $$h(M)$$ is unimodal. (ii) $$h(M)$$ is log-concave. (iii) $$h(M)$$ is strongly log-concave, that is the sequence $$(h'_0,h'_1,\ldots,h'_s)$$ is log-concave. □ This still wide open conjecture was proposed by Brylawski [7, p. 232]. Therein, he also showed that Conjecture 4.1(ii) is stronger than Rota–Heron’s conjecture [13, 28] and Welsh’s conjecture [38]. As we mentioned before, significant progress towards proving Conjecture 4.1(ii) was made by Huh [16], who verified it for matroids representable over a field of characteristic zero. Concerning Conjecture 1.1 it is also worth noting the following question: Question 4.2. Let $$M$$ be a matroid and let $$h(M)=(h_0,h_1,\ldots,h_s)$$ be the $$h$$-vector of $$BC(M)$$, where $$h_s\neq 0$$. Define $$g(M)=(1,h_1-h_0,\ldots,h_{\lfloor s/2\rfloor}-h_{\lfloor s/2\rfloor -1})$$ to be the $$g$$-vector of $$BC(M)$$. Is it always true that $$g(M)$$ is an $$O$$-sequence? □ This question together with Conjecture 1.1 was posed by Swartz in [34], where he gave an affirmative answer to the question in the case of independence complexes. We believe that this question should also have an affirmative answer for broken circuit complexes in general. However, we would like to remark that it is not clear whether the question can be reduced to the case of parallel irreducible matroids. For this, one would, in analogy with Lemma 3.1, need that the property of the $$g$$-vector being an $$O$$-sequence is preserved under taking products. Currently, in joint work with Uwe Nagel, the first author is investigating this problem. Funding The first author was supported by the German Research Council DFG-GRK, 1916. Acknowledgments We wish to thank Ed Swartz for pointing out that Conjecture 4.1 is due to Brylawski. We are also grateful to the referees, whose thoughtful comments and useful suggestions led to several improvements in the article. References [1] Adiprasito K. Huh J. and Katz. E. Hodge theory for combinatorial geometries , arXiv:1511.02888 (accessed on November 11, 2016). [2] Björner A. The homology and shellability of matroids and geometric lattices. In Matroid Applications , vol. 40, 226– 83. Encyclopedia of Mathematics and its Applications. Edited by White. N. Cambridge: Cambridge University Press, 1992. Google Scholar CrossRef Search ADS [3] Boij M. Migliore J. Miró-Roig R. Nagel U. and Zanello. F. “On the shape of a pure O-sequence.” Memoirs of the American Mathematical Society 218, no. 1024. American Mathematical Society, 201 Charles Street, Providence, RI 02904-2294 USA, ( 2012). Google Scholar CrossRef Search ADS [4] Braden T. and Proudfoot. N. “The hypertoric intersection cohomology ring.” Inventiones mathematicae 177, no. 2 ( 2009): 337– 79. Google Scholar CrossRef Search ADS [5] Brylawski T. “A combinatorial model for series–parallel networks.” Transactions of the American Mathematical Society 154 ( 1971): 1– 22. Google Scholar CrossRef Search ADS [6] Brylawski T. “The broken-circuit complex.” Transactions of the American Mathematical Society 234 ( 1977): 417– 33. Google Scholar CrossRef Search ADS [7] Brylawski T. The Tutte polynomial. General. I. theory. In Matroid Theory and its Applications , edited by Barlotti A. 125– 275, Naples: Liguori, 1982. Google Scholar CrossRef Search ADS [8] Brylawski T. and Oxley. J. The Tutte polynomial and its applications. In Matroid Applications , edited by White. N. vol. 40, 123– 225, Encyclopedia of Mathematics and its Applications, Cambridge: Cambridge University Press, 1992. Google Scholar CrossRef Search ADS [9] Chari M. K. “Two decompositions in topological combinatorics with applications to matroid complexes.” Transactions of the American Mathematical Society 349 ( 1997): 3925– 943. Google Scholar CrossRef Search ADS [10] Crapo H. “A higher invariant for matroids.” Journal of Combinatorial Theory 2 ( 1967): 406– 17. Google Scholar CrossRef Search ADS [11] Denham G. Garrousian M. and Tohăneanu. S. “Modular decomposition of the Orlik–Terao algebra.” Annals of Combinatorics 18, no. 2 ( 2014): 289– 312. Google Scholar CrossRef Search ADS [12] Eisenbud D. Popescu S. and Yuzvinsky. S. “Hyperplane arrangement cohomology and monomials in the exterior algebra.” Transactions of the American Mathematical Society 355 ( 2003): 4365– 383. Google Scholar CrossRef Search ADS [13] Heron A. P. Matroid polynomials. In Combinatorics (Proceedings of the Conference on Combinatorial Mathematics, Mathematical Institute, Oxford, 1972), edited by Welsh D. Woodall D. 164– 202, Southend-on-Sea: The Institute of Mathematics and its Applications, 1972. [14] Hibi T. “What can be said about pure O-sequences?” Journal of Combinatorial Theory, Series A 50 ( 1989): 319– 22. Google Scholar CrossRef Search ADS [15] Hibi T. “Face number inequalities for matroid complexes and Cohen–Macaulay types of Stanley–Reisner rings of distributive lattices.” Pacific Journal of Mathematics 154 ( 1992): 253– 64. Google Scholar CrossRef Search ADS [16] Huh J. “h-vectors of matroids and logarithmic concavity.” Advances in Mathematics 270 ( 2015): 49– 59. Google Scholar CrossRef Search ADS [17] Kämpf G. and Römer. T. “Homological properties of Orlik–Solomon algebras.” Manuscripta Mathematica 129 ( 2009): 181– 210. Google Scholar CrossRef Search ADS [18] Le D. V. “On the Gorensteinness of broken circuit complexes and Orlik–Terao ideals.” Journal of Combinatorial Theory, Series A 123, no. 1 ( 2014): 169– 85. Google Scholar CrossRef Search ADS [19] Le D. V. “Broken circuit complexes of series–parallel networks.” European Journal of Combinatorics 51 ( 2016): 12– 36. Google Scholar CrossRef Search ADS [20] Le D. V. and Mohammadi. F. “On the Orlik–Terao ideal and the relation space of a hyperplane arrangement.” Advances in Applied Mathematics 71 ( 2015): 34– 51. Google Scholar CrossRef Search ADS [21] Le D. V. and Römer. T. “Broken circuit complexes and hyperplane arrangements.” Journal of Algebraic Combinatorics 38, no. 4 ( 2013): 989– 1016. Google Scholar CrossRef Search ADS [22] McBreen M. and Proudfoot. N. “Intersection cohomology and quantum cohomology of conical symplectic resolutions.” Algebraic Geometry 2, no. 5 ( 2015): 623– 41. Google Scholar CrossRef Search ADS [23] Orlik P. and Terao. H. “Commutative algebras for arrangements.” Nagoya Mathematical Journal 134 ( 1994): 65– 73. Google Scholar CrossRef Search ADS [24] Oxley J. Matroid Theory , vol. 21, 2nd ed., Oxford Graduate Texts in Mathematics. Oxford: Oxford University Press, 2011. [25] Proudfoot N. and Speyer. D. “A broken circuit ring.” Beiträge zur Algebra und Geometrie 47, no. 1 ( 2006): 161– 6. [26] Provan J. S. Decompositions, Shellings, and Diameters of Simplicial Complexes and Convex Polyhedra . Thesis, Cornell University, 1977. [27] Rota G.-C. “On the foundations of combinatorial theory. I. Theory of Möbius functions.” Zeitschrift für Wahrscheinlichkeitstheorie und verwandte Gebiete. 2 ( 1964): 340– 68. Google Scholar CrossRef Search ADS [28] Rota G.-C. “Combinatorial theory, old and new.” In: Proceedings of the International Congress of Mathematicians (Nice, 1970), 229– 233. Paris: Gauthier-Villars, 1971. [29] Sanyal R. Sturmfels B. and Vinzant. C. “The entropic discriminant.” Advances in Mathematics 244 ( 2013): 678– 707. Google Scholar CrossRef Search ADS [30] Schenck H. “Resonance varieties via blowups of $${\mathbb P}^2$$ and scrolls.” International Mathematics Research Notices 20 ( 2011): 4756– 778. [31] Schenck H. and Tohăneanu. Ş. “The Orlik–Terao algebra and 2-formality.” Mathematical Research Letters 16 ( 2009): 171– 82. Google Scholar CrossRef Search ADS [32] Stanley. R. P. “Cohen–Macaulay complexes. In Higher Combinatorics , edited by Aigner M. 51– 62. Dordrecht: Reidel, 1977. Google Scholar CrossRef Search ADS [33] Stanley R. P. “Log-concave and unimodal sequences in algebra, combinatorics, and geometry.” In Graph Theory and Its Applications, edited by Capobianco M. Guan M.G. Hsu D.F. and Tian F. 576, 500– 35, New York Academy of Sciences, New York, 1989. Google Scholar CrossRef Search ADS [34] Swartz E. “g-elements of matroid complexes.” Journal of Combinatorial Theory, Series B 88, no. 2 ( 2003): 369– 75. Google Scholar CrossRef Search ADS [35] Swartz E. “Lower bounds for h-vectors of k-CM, independence, and broken circuit complexes.” SIAM Journal on Discrete Mathematics 18, no. 3 ( 2004/05): 647– 61. Google Scholar CrossRef Search ADS [36] Swartz E. “g-Elements, finite buildings and higher Cohen–Macaulay connectivity.” Journal of Combinatorial Theory, Series A 113, no. 7 ( 2006): 1305– 20. Google Scholar CrossRef Search ADS [37] Terao H. “Algebras generated by reciprocals of linear forms.” Journal of Algebra 250 ( 2002): 549– 58. Google Scholar CrossRef Search ADS [38] Welsh D. Matroid Theory , London: Academic Press, 1976. [39] Whitney H. “A logical expansion in mathematics.” Bulletin of the American Mathematical Society 38 ( 1932): 572– 79. Google Scholar CrossRef Search ADS [40] Whitney H. “On the abstract properties of linear dependence.” American Journal of Mathematics 57, no. 3 ( 1935): 509– 33. Google Scholar CrossRef Search ADS [41] Zaslavsky T. The Möbius function and the characteristic polynomial. In Combinatorial Geometries , vol. 29, 114– 38, Encyclopedia of Mathematics and its Applications, edited by White N. Cambridge, Cambridge University Press, 1987. © The Author 2016. Published by Oxford University Press. All rights reserved. For permissions, please e-mail: journals.permission@oup.com. This article is published and distributed under the terms of the Oxford University Press, Standard Journals Publication Model (https://academic.oup.com/journals/pages/about_us/legal/notices) For permissions, please e-mail: journals. permissions@oup.com

International Mathematics Research Notices – Oxford University Press

**Published: ** Mar 1, 2018

Loading...

personal research library

It’s your single place to instantly

**discover** and **read** the research

that matters to you.

Enjoy **affordable access** to

over 18 million articles from more than

**15,000 peer-reviewed journals**.

All for just $49/month

Query the DeepDyve database, plus search all of PubMed and Google Scholar seamlessly

Save any article or search result from DeepDyve, PubMed, and Google Scholar... all in one place.

Get unlimited, online access to over 18 million full-text articles from more than 15,000 scientific journals.

Read from thousands of the leading scholarly journals from *SpringerNature*, *Elsevier*, *Wiley-Blackwell*, *Oxford University Press* and more.

All the latest content is available, no embargo periods.

## “Hi guys, I cannot tell you how much I love this resource. Incredible. I really believe you've hit the nail on the head with this site in regards to solving the research-purchase issue.”

Daniel C.

## “Whoa! It’s like Spotify but for academic articles.”

@Phil_Robichaud

## “I must say, @deepdyve is a fabulous solution to the independent researcher's problem of #access to #information.”

@deepthiw

## “My last article couldn't be possible without the platform @deepdyve that makes journal papers cheaper.”

@JoseServera

DeepDyve ## Freelancer | DeepDyve ## Pro | |
---|---|---|

Price | FREE | $49/month |

Save searches from | ||

Create lists to | ||

Export lists, citations | ||

Read DeepDyve articles | Abstract access only | Unlimited access to over |

20 pages / month | ||

PDF Discount | 20% off | |

Read and print from thousands of top scholarly journals.

System error. Please try again!

or

By signing up, you agree to DeepDyve’s Terms of Service and Privacy Policy.

Already have an account? Log in

Bookmark this article. You can see your Bookmarks on your DeepDyve Library.

To save an article, **log in** first, or **sign up** for a DeepDyve account if you don’t already have one.