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Research article Special Issues

Connected surfaces with boundary minimizing the Willmore energy

  • Received: 02 October 2019 Accepted: 17 March 2020 Published: 23 March 2020
  • For a given family of smooth closed curves γ1,...,γαR3 we consider the problem of finding an elastic connected compact surface M with boundary γ=γ1...γα. This is realized by minimizing the Willmore energy W on a suitable class of competitors. While the direct minimization of the Area functional may lead to limits that are disconnected, we prove that, if the infimum of the problem is <4π, there exists a connected compact minimizer of W in the class of integer rectifiable curvature varifolds with the assigned boundary conditions. This is done by proving that varifold convergence of bounded varifolds with boundary with uniformly bounded Willmore energy implies the convergence of their supports in Hausdorff distance. Hence, in the cases in which a small perturbation of the boundary conditions causes the non-existence of Area-minimizing connected surfaces, our minimization process models the existence of optimal elastic connected compact generalized surfaces with such boundary data. We also study the asymptotic regime in which the diameter of the optimal connected surfaces is arbitrarily large. Under suitable boundedness assumptions, we show that rescalings of such surfaces converge to round spheres. The study of both the perturbative and the asymptotic regime is motivated by the remarkable case of elastic surfaces connecting two parallel circles located at any possible distance one from the other. The main tool we use is the monotonicity formula for curvature varifolds ([15,31]) that we extend to varifolds with boundary, together with its consequences on the structure of varifolds with bounded Willmore energy.

    Citation: Matteo Novaga, Marco Pozzetta. Connected surfaces with boundary minimizing the Willmore energy[J]. Mathematics in Engineering, 2020, 2(3): 527-556. doi: 10.3934/mine.2020024

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  • For a given family of smooth closed curves γ1,...,γαR3 we consider the problem of finding an elastic connected compact surface M with boundary γ=γ1...γα. This is realized by minimizing the Willmore energy W on a suitable class of competitors. While the direct minimization of the Area functional may lead to limits that are disconnected, we prove that, if the infimum of the problem is <4π, there exists a connected compact minimizer of W in the class of integer rectifiable curvature varifolds with the assigned boundary conditions. This is done by proving that varifold convergence of bounded varifolds with boundary with uniformly bounded Willmore energy implies the convergence of their supports in Hausdorff distance. Hence, in the cases in which a small perturbation of the boundary conditions causes the non-existence of Area-minimizing connected surfaces, our minimization process models the existence of optimal elastic connected compact generalized surfaces with such boundary data. We also study the asymptotic regime in which the diameter of the optimal connected surfaces is arbitrarily large. Under suitable boundedness assumptions, we show that rescalings of such surfaces converge to round spheres. The study of both the perturbative and the asymptotic regime is motivated by the remarkable case of elastic surfaces connecting two parallel circles located at any possible distance one from the other. The main tool we use is the monotonicity formula for curvature varifolds ([15,31]) that we extend to varifolds with boundary, together with its consequences on the structure of varifolds with bounded Willmore energy.


    The theory of pictures and picture groups comes from topology and goes back to the first author's PhD thesis [17] where pictures were used to represent elements in the higher algebraic K-theory group K3Z[π] and these were used to obtain obstructions to the 1-parameter "pseudoisotopy implies isotopy" problem, extending work of Allen Hatcher and John Wagoner who showed the relation between K2Z[π] and pseudoisotopy [16]. The salient fact is that pictures for a group G represent elements of H3(G) and, by an observation of S.M. Gersten [15], K3R=H3(St(R)) for any ring R (and K2R is the center of the Steinberg group St(R)). Pictures are also known as "spherical diagrams" in some text books on combinatorial group theory [33]. They are also called "Peiffer diagrams" and generally attributed to Renée Peiffer who gave the algebraic definition of pictures in [34]. (See Theorem 4.) "Partial pictures" were used by John Wagoner [37] to describe the boundary map in the long exact K-theory sequence of an ideal. Later, in [22], John Klein and the first author used Morse theory to construct a picture representing nontrivial elements of K3Z[ζ] where ζn=1. In the case n=2,ζ=1, this picture was shown in [18] to give a generator of K3Z=Z/48. Later, in joint work with Kent Orr [23], the first author used pictures to obtain new results on Milnor's ¯μ link invariants.

    Pictures also appeared in representation theory and combinatorics. Harm Derksen and Jerzy Weyman used what we now call "semi-invariant pictures" for acyclic quivers to give a new proof of the saturation conjecture for Littlewood-Richardson coefficients [10]. This was based on the seminal work of Alastair King [29] using geometric invariant theory to study representations of quivers. Around this time, Sergey Fomin and Andrei Zelevinsky invented cluster algebras [13], [14]. Soon after that, Aslak Bakke Buan, Robert Marsh, Markus Reineke, Idun Reiten and the second author in [8] associated to any acyclic cluster algebra a "cluster category" whose rigid indecomposable objects correspond to the cluster variables. Following this breakthrough, a large body of knowledge has been accumulated [7], [11], [12], [2]. This includes work of the authors, together with Kent Orr and Jerzy Weyman giving the connection between cluster theory of acyclic quivers and semi-invariant pictures in [24], [25], [27].

    Later, Takahide Adachi, Osamu Iyama, and Idun Reiten [1] extended cluster theory to arbitrary finite dimensional algebras using τ-rigid objects in place of cluster variables. In [25] the real Schur roots of an acyclic valued quiver are shown to be c-vectors for the associated cluster algebra and labels for the "walls" D(β) for the "wall-and-chamber" structure for hereditary algebras (given by the semi-invariant pictures) in [25], [27]. In [6], Thomas Brüstle, David Smith and Hipolito Treffinger extend the "wall-and-chamber" structure to arbitrary finite dimensional algebras using τ-tilting theory and the space of stability conditions following Tom Bridgeland [3].

    Maximal green sequences were invented by Bernhard Keller to study Kontsevich-Soebelman's version [30], [31] of the Donaldson-Thomas invariants. What we call "linear" maximal green sequences in [20] were earlier used by Markus Reineke for similar formulas in [35]. Originally, a maximal green sequence was defined to be a sequence of "green" mutations of an initial "seed" for a cluster algebra, a mutation in the k-direction being "green" if the k-th c-vector is positive. However, here we use the representation theoretic version where c-vectors βi are replaced with "wall-crossing" through the walls D(βi). See [20], [21] for a detailed explanation of how these and other versions of the definition of maximal green sequences are related.

    One of the big questions which we would like to understand is the conjecture that there are only finitely many maximal green sequences (possibly none) for any exchange matrix. In particular, this is still not known for arbitrary acyclic exchange matrices. These correspond to maximal wall crossing sequences in the wall-and-chamber structure for a hereditary algebra. This version of the conjecture has been verified for tame hereditary algebras by Thomas Brüstle, Gregoire Dupont and Matthieu Pérotin [4] and extended to cluster-tilted algebras of tame type by Thomas Brüstle, Stephen Hermes and the authors in [5].

    In the present paper we have two objectives. The first is to devise a method for attacking hereditary algebras of infinite type by looking at a finite "admissible" set of exceptional modules Mβ where βS, an admissible sequence of roots. (We recall in the Appendix the definition of exceptional modules and the fact that they are uniquely determined by their dimension vectors which are real Schur roots β.) The idea is to study maximal green sequences, which are given by sequences of wall crossing, by looking only at the subsequence of those walls D(β) where βS. Such subsequences are examples of "maximal S-green sequences" (Definition 1.16) that we consider in greater generality in this paper. Since a maximal green sequence cannot cross the same wall twice [5], these subsequences will be bounded in length by the size of S. The same holds for more general maximal S-green sequences by Remark 1.23.

    The second objective is to determine exactly which such sequences will occur using the "picture group". The main theorem of this paper, Theorem A, is that, for admissible S, maximal S-green sequences are in bijection with positive expressions for the "Coxeter element" cS in the "picture group" G(S) (Definition 1.9). We observe that there is at least one maximal S-green sequence given by the "Coxeter green sequence" (Remark 1.17). Also, there are only finitely many maximal S-green sequences by Remark 1.23.

    Section 1 has the definitions of "admissible" and "weakly admissible" sets of real Schur roots which are "laterally" and "vertically ordered" and "weakly vertically ordered" sets of roots. These are concepts introduced in this paper for the purpose of using finite methods to study infinite sets of representations.

    Subsection 1.2 has a statement of the main results Theorem A and Corollary B. In subsection 1.3 an outline of the proof of Theorem A is given using three lemmas C, D, E.

    Section 2 contains a discussion of "compartments". Whereas the union of all the walls D(β) divides Euclidean space Rn into possibly infinitely many "chambers", since we consider only finitely many walls, D(β) for βS, the complement of these walls has only finitely many regions which we call "compartments". In subsection 2.3 we prove Lemma D which describes the sequence of compartments in a maximal S-green sequence.

    The theory of pictures and picture groups is explained in Section 3. The main theorem for pictures is the "Atomic Deformation Theorem" (Theorem 3.18) which says that every picture for the picture group G(S) has an "atomic deformation" to the empty picture, equivalently, any picture is equivalent to a disjoint union of "atoms". This idea comes from [23] where a similar theorem is proved leading to results in topology. The Atomic Deformation Theorem is used to prove the last two lemmas C and E completing the proof of the main result.

    Section 4 is the Appendix which reviews the well-known properties of exceptional sequences, real Schur roots and wide subcategories used in this paper.

    In this section we give the basic definitions used in this paper which are the concepts of "vertical" (Def. 1.4) and "lateral" orderings (Def. 1.2) of real Schur roots and "admissible" sequences of such roots (Def. 1.6). We define "pictures" (Fig. 1) for the "picture group" G(S) for S (Def. 1.9) and we define "maximal S-green sequences" (Def. 1.16). We also give the statements of the main theorems A, B and an outline of the proofs using three lemmas about pictures C, D, E. Corollary B is the special case of Theorem A for a hereditary algebra of finite representation type with the admissible set of roots being all positive roots of the root system. In this special case, we obtain a group theoretic description of all maximal green sequences. We believe that, using τ-tilting theory, analogous statements can be obtained for any finite dimensional algebra in particular those which are τ-tilting finite. However, in this paper, all quivers will be valued quivers without oriented cycles, possibly of infinite type. See the Appendix for basic background material on exceptional modules and real Schur roots.

    Figure 1.  On the left is the semi-invariant picture L(S0) for the admissible subsequences S0=(α1,α2,α4) of S from Example 1.13. L(S0) is a subset of S2R3. Thus, e.g., D(αi) are actually coordinate hyperplanes. The S0-compartments are the components of the complement of L(S0). For example, U++0=U++ is the region on the positive side of the two hyperplanes D(α1),D(α2). U++ is the set of point in U+ on the positive side of D(α4). On the right, the wall D(α3) cuts all five S0-compartments in half giving the semi-invariant picture for S=(α1,α2,α4,α3) with ten compartments.

    We assume that Q is a valued acyclic quiver and we always consider subsets S of the set of positive real Schur roots of Q. The positive real Schur roots are precisely the dimension vectors of the exceptional modules over any modulated quiver with underlying valued quiver Q [25]. We need to order the roots, in these subsets S, in two different ways which we call "lateral" and "vertical" ordering.

    Notation 1.1. Let Q be a modulated quiver and β a positive real Schur root.

    1. We will denote by Mβ the unique exceptional module with dimension vector equal to β. Exceptional modules are always indecomposable.

    2. A positive real Schur root β will be called a subroot of β if the exceptional module Mβ is isomorphic to a submodule of Mβ. This is denoted by ββ.

    3. A positive real Schur root β" will be called a quotient root of β if the exceptional module Mβ" is isomorphic to a quotient of Mβ. This is denoted by ββ".

    Definition 1.2. By a lateral ordering on a set of real Schur roots S we mean a total ordering on S satisfying the following for any α,βS.

    1. If hom(α,β)0 then αβ, where hom(α,β)=dimKHomΛ(Mα,Mβ).

    2. If ext(α,β)0 then α>β, where ext(α,β)=dimKExtΛ(Mα,Mβ).

    Remark 1.3. We now state several basic facts and some examples of S with lateral ordering and some S which do not admit such ordering.

    1. If S has lateral ordering then for all α,βS, either hom(α,β)=0 or ext(α,β)=0.

    2. The left-to-right order of preprojective roots as they occur in the Auslander-Reiten quiver, together with any ordering on the summands of the middle term of each almost split sequence, is a lateral ordering. (This is any total ordering on this set of roots so that α<β whenever there is a irreducible map MαMβ.)

    3. The set af all regular roots does not admit a lateral ordering.

    4. The simple roots can always be laterally ordered by taking αi<αj whenever there is an arrow ji in the quiver.

    5. If ω is a rightmost root in S in lateral order then ext(β,ω)=0 for all βS and hom(ω,β)=0 for all βωS.

    6. Any subset of a laterally ordered set of roots is laterally ordered with the same ordering.

    Definition 1.4. A sequence of real Schur roots S=(β1,,βm) is said to be vertically ordered if the following two conditions are satisfied for each βkS.

    1. Let ββk be any (positive real Schur) subroot of βk. Then β=βj for some jk.

    2. Let β"βk be a (positive real Schur) quotient-root of βk. Then β"=βj for some jk.

    The sequence S is weakly vertically ordered if, for each βkS, at least one of the above two conditions is satisfied.

    Remark 1.5. A finite set of positive real Schur roots which is closed under subroots and quotient roots can be vertically ordered if the roots are ordered by length, and the roots of the same length are ordered in any way.

    Definition 1.6. Let S be a finite set of positive real Schur roots.

    1. S is called admissible if it has a lateral and a vertical ordering

    2. S is called weakly admissible if it has a lateral ordering and a weakly vertical ordering

    3. an admissible sequence is an admissible set listed in its vertical ordering

    4. a weakly admissible sequence is a weakly admissible set listed in its weakly vertical ordering

    Remark 1.7. Let (β1,,βm) be an admissible sequence (of positive real Schur roots). The following will be crucial for the induction steps in the proofs.

    1. If one of the βi's is removed, the sequence (β1,^βi,βm) is a weakly admissible sequence (not necessarily admissible sequence).

    2. If the last element βm is removed then the resulting sequence will still be an admissible sequence.

    "Semi-invariant pictures". These groups were defined using all positive roots (the algebras were of finite representation type). We now give a more general definition of "picture groups", using admissible subsets of positive real Schur roots for all finite dimensional hereditary algebras.

    Definition 1.8. Let S be an admissible set of (positive real Schur) roots. We will call a subset RS relatively closed if R is closed under extensions in S.

    Relatively closed subsets RS of admissible sets, have "picture groups", which we now define.

    Definition 1.9. For any relatively closed subset RS of an admissible set of roots S, we define the picture group G(R) as follows. There is one generator x(β) for each βR. There is the following relation for each pair βi,βj of hom-orthogonal roots with ext(βi,βj)=0:

    x(βi)x(βj)=x(γk) (1)

    where γk runs over all roots in R which are linear combinations γk=akβi+bkβj,ak,bkZ0 in increasing order of the ratio ak/bk (going from 0/1 where γ1=βj to 1/0 where γk=βi). In particular, x(α),x(β) commute when α,β are both hom-orthogonal and ext-orthogonal. For any gG(R), we define a positive expression for g to be any word in the generators x(β) (with no x(β)1 terms) whose product is g.

    Remark 1.10. (a) Note that G(R) is independent of the choice of S. However, the existence of an admissible S containing R is important. Also, by the well-known Theorem 4.8, each γk=akβi+bkβj has βi as a subroot and βj as a quotient root if βi,βj are hom-orthogonal with ext(βi,βj)=0.

    (b) Whenever RR are relatively closed subsets of an admissible set S we get a homomorphism of groups G(R)G(R) since any relation among the generators of G(R) is also a relation among the corresponding generators of G(R).

    (c) Definition 1.9 is a generalization of the notion of "picture groups" for hereditary artin algebras of finite representation type as defined in [27]. Indeed, the picture group G(Λ) for such an algebra is, by definition, equal to the picture group G(Φ+(Λ)) for the set Φ+(Λ) of all positive roots of Λ. These roots are vertically ordered by dimension and laterally ordered by their position in the Auslander-Reiten quiver of Λ, i.e., there exists a lateral ordering so that, for any irreducible map MαMβ, α<β in lateral order.

    Definition 1.11. Given S admissible, we define the Coxeter element cS of G(S) to be the product of the generators x(αi) for all simple roots αiS in lateral order, i.e., so that αi<αj whenever there is an arrow ij in the quiver of the algebra.

    Remark 1.12. As an element of the picture group G(S), this product cS=x(αi) is independent of the choice of the lateral ordering. This is because one can pass from any lateral ordering to any other by transposing consecutive generators x(αi),x(αj) when there is no arrow between them in the quiver. But in that case, x(αi),x(αj) commute. So, the product remains invariant.

    Example 1.13. Consider the quiver of type A3 with straight orientation: 123. The Auslander-Reiten quiver, with modules on the left and corresponding roots on the right is:

    x(βi)x(βj)=x(γk) (1)

    The set S=(α1,α2,α4,α3) is vertically ordered since the subroot α1 and quotient root α2 of α4 come before it. The set S is admissible since it also has a lateral ordering α1<α4<α2<α3. The subsequence S=(α1,α4,α3) is weakly admissible. Also, S is relatively closed in S since the missing element is simple.

    The picture group G(S) has four generators x(α1),x(α2),x(α3),x(α4) and four relations given by the four pairs of hom-orthogonal roots:

    1. x(α1)x(α2)=x(α2)x(α4)x(α1) from the extension α1α4α2.

    2. x(α2)x(α3)=x(α3)x(α2) since the extension α5 of α2 by α3 is not in S.

    3. x(α1)x(α3)=x(α3)x(α1) since α1,α3 do not extend each other.

    4. x(α4)x(α3)=x(α3)x(α4) since α6S.

    Thus x(α3) is central. (This follows from the fact that α3 is last in both vertical and lateral orderings.) The picture group G(S) has generators x(α1),x(α3),x(α4) modulo the relation that x(α3) is central. The Coxeter element of G(S) is

    cS=x(α1)x(α2)x(α3).

    Remark 1.14. If βi,βj are hom-orthogonal and βi<βj in lateral order then

    x(βi)x(βj)=x(βj)w

    where w is a positive expression in letters γ where βiγ<βj in lateral order since hom(βi,γ)0 and hom(γ,βj)0 when γβi.

    An important case is when j=m, the size of S. For βi,βm hom-orthogonal we get

    x(βi)x(βm)=x(βm)x(βi).

    since the other roots γk in the formula above would come after βm so do not lie in S.

    We recall that, for all roots β, there is a unique exceptional module Mβ with dimension vector β. The subset D(β)Rn is given by

    D(β)={xRn:x,β=0 and x,β0 ββ}

    where ββ means that Mβ contains an exceptional submodule isomorphic to Mβ. The inner product x,β is the weighted dot product x,β=xibifi where xi,bi are the ith coordinates of x,β and fi=dimKEnd(Si) where Si is the ith simple module. So, D(β) does not contain points in Rn all of whose coordinates are positive (or negative). For more details see Appendix 4.

    Theorem 4.1 in the Appendix proves that D(β) has the following equivalent description.

    D(β)={xRn:x,β=0 and x,β"0 β"↞β}

    where β"↞β means that Mβ has an exceptional quotient module isomorphic to Mβ".

    Given S a weakly admissible sequence of roots, let CL(S)Rn denote the union of D(β) for all βS. Since this set is invariant under scaling in the sense that λCL(S)=CL(S) for all λ>0, we usually consider just the intersection L(S):=CL(S)Sn1. The semi-invariant picture for G(S) is defined to be this set L(S)Sn1 together with the labels of its walls by positive roots and the normal orientation of each wall D(β) telling on which side the vector β lies. When n=3, we draw the stereographic projection of this set onto the plane. (Projecting away from the negative octant. See Figures 1 and 2.)

    Figure 2.  Semi-invariant picture L(S) for the weakly admissible sequence S=(α1,α4,α3) from Example 1.13. The solid green arrow indicates an S-green path giving the maximal S-green sequence U,U+0,U+0+. Note that the dashed green arrow indicates another S-green path giving the maximal S-green sequence U,U+, U+0,U+0+. So, "maximal" is a misnomer when S is only weakly admissible. Also, L(S) is not a "planar picture" for G(S) as defined in Section 3 since S is not admissible.

    Definition 1.15. Given S=(β1,,βm) weakly admissible and ϵ=(ϵ1,,ϵm){0,+,}m.

    1. Define Uϵ to be the convex open set given by

    Uϵ={xRn:x,βi>0 if ϵi=+ and x,βj<0 if ϵj=}.

    2. ϵ will be called admissible (with respect to S) if for all 1km we have:

    ϵk=0D(βk)Uϵ1,,ϵk1=.

    3. When ϵ is admissible the open set Uϵ will be called an S_-compartment. See Fig. 1, 2.

    In Proposition 2.1 below we show that, for S weakly admissible, each compartment Uϵ is open and convex and these regions form the components of the complement of CL(S) in Rn.

    Definition 1.16. For any weakly admissible S, we define a maximal S_-green sequence (of length s) to be a sequence of S-compartments Uϵ(0),,Uϵ(s) satisfying the following.

    1. Every pair of consecutive compartments Uϵ(i1),Uϵ(i) is separated by a wall D(βki) so that ϵ(i1)ki= and ϵ(i)ki=+ and ϵ(i1)j=ϵ(i)j for all j<ki.

    2. Uϵ(0) is the compartment containing vectors all of whose coordinates are negative.

    3. Uϵ(s) is the compartment containing vectors all of whose coordinates are positive.

    We say that (Uϵ) is an S_-green sequence if only the first condition is satisfied. We define an S_-green path representing the S-green sequence (Uϵ) to be a continuous path, γ:RRn, so that, for some t1<t2<<ts we have the following

    1. γ(t)Uϵ(0) when t<t1

    2. γ(t)Uϵ(s) when t>ts

    3. γ(t)Uϵ(i) for 0<i<s whenever ti<t<ti+1

    4. For 1is, γ(t) goes from the negative side to the positive side of D(βki) for some βkiS when t crosses the value ti.

    The word "maximal" may be misleading. (See Figure 2.)

    Remark 1.17. The green arrow in Figure 2 is an example of a "Coxeter path" which is given more generally as follows. Let S be an admissible set of roots. Let α1,,αk be the simple roots in S in any lateral order. In other words, any arrow between the corresponding vertices in the quiver go from αj to αi only when i<j. Also, all roots in S have support at these vertices by definition of an admissible set. The corresponding Coxeter path is defined to be the linear path γ:RRn

    γ(t)=(t,t,,t)jαj.

    This path crosses the hyperplanes D(αi) at time t=i (in the order α1,α2,) and it passes from the negative to the positive side of each hyperplane.

    Also, this path is disjoint from all other walls D(β) for βS not simple. To see this, suppose γ(t0)D(β). Then

    γ(t0),β=0=(t0j)fjbj.

    So, some of the coefficients t0j are positive and some are negative with the positive ones coming first, say t01,t02,,t0p positive and the rest negative. In that case β=b1α1+b2α2++bpαp is a sum of subroots of β, but γ(t0),β>0 which contradicts the assumption that γ(t0)D(β). So, the Coxeter path does not meet any D(β) for βS not simple. Thus, the Coxeter path is an S-green path. Since the coordinates of γ(t) are all negative for t<<0 and all positive for t>>0, this green path gives a maximal S-green sequence which we call the Coxeter green sequence. The product of the group labels on the walls crossed by this green sequence form the Coxeter element cS=x(α1)x(α2)x(αk)G(S).

    The main property of UϵRn is that it is convex and nonempty when S is weakly admissible and ϵ is admissible with respect to S (Proposition 2.1). Furthermore, when S is admissible, the complement of the union of these regions forms a "picture" for the picture group G(S). The precise statement is as follows.

    Theorem 1.18. When S is admissible, each S-compartment Uϵ can be labelled with an element of the picture group g(ϵ)G(S) so that, if Uϵ and Uϵ are separated by a wall D(β), βS, with Uϵ on the positive side of D(β), then

    g(ϵ)x(β)=g(ϵ). (2)

    Note that, given any system of compartment labels g(ϵ) satisfying (2), left multiplication of all labels by a fixed element of G(S) will preserve the condition. Therefore, we may, without loss of generality, assume that g(ϵ)=1 on the negative S-compartment Uϵ where all ϵi are negative or zero. Theorem 1.18 follows from the following lemma.

    Lemma 1.19. For S weakly admissible, every S-compartment Uϵ lies in a maximal S-green sequence given by an S-green path.

    Proof. Given any S-compartment Uϵ, choose a general point vUϵ and consider the straight line f(t)=v+(t,t,,t), tR. This line passes though walls D(β) only in the positive direction since

    (1,1,,1),β>0

    for all positive roots β. Thus f(t) is an S-green path giving an S-green sequence. For t>>0, the coordinates of f(t) are all positive. For t<<0, they are all negative. Therefore f(t) gives a maximal S-green sequence passing through the S-compartment Uϵ at t=0.

    Proof of Theorem 1.18. Given an S-compartment Uϵ choose an S-green path through Uϵ as in the lemma above. Let g(ϵ) be the product of labels x(βi) for the walls crossed by this path on the way to Uϵ. Condition (2) will be satisfied. We only need to show that g(ϵ) is well defined. To do this suppose we have two S-green paths γ,γ from the negative compartment to Uϵ. Since Rn is contractible these paths are homotopic. The homotopy gives a mapping of h:[0,1]2Rn. Make this a smooth mapping transverse to CL(S).

    Since each wall D(β) is contained in the hyperplane H(β), CL(S) is contained in the union of these hyperplanes. The intersection of two hyperplanes has codimension 2. Since S is finite, there are only finitely many such subspaces. We ignore the other intersections which have higher codimension. By transversality, the homotopy h will only meet these codimension 2 subspaces at a finite number of points. Let x0Rn be one these points and let B be the set of all βS so that x0D(β). Let A be the set of minimal elements of B, i.e., the set of all αB so that no subroot of α lies in B.

    Then A has at most two elements since, otherwise, by Proposition 4.3, the intersection of D(α) for αA has codimension 3. If A has only one element then A=B. In that case, the wall crossing sequence is unchanged when the path is deformed past x0. The remaining case is when A has two elements: A={α1,α2}. By Corollary 4.9, the other elements of B are positive linear combinations β=xα1+yα2 and D(β) lies on the negative side of D(α1) and the positive side of D(α2) since α1β implies v,α10 for all vD(β). This means that, on one side of x0, the S-green path goes through D(α1) followed by D(α2) and on the other side, it goes through D(α2), then, being on the positive side of D(α2) and on the negative side of D(α1) it goes through D(β) for βB. (See Figure 3.) This sequence of wall crossings gives the same element of the picture group. So, the group label g(ϵ) is independent of the path. This proves the theorem.

    Figure 3.  A typical intersection of two walls D(α1) and D(α2) producing walls D(βi). In this drawing there is only β=α1+α2. The green path γ crosses D(α1),D(α2) and γ crosses D(α2),D(β),D(α1). The homotopy h:γγ passes through x0.

    Lemma 1.20. Take any maximal S-green sequence for S admissible and consider the sequence of walls D(βk1), ,D(βks) which are crossed by the sequence. Then the product of the corresponding generators x(βki)G(S) is equal to the Coxeter element cSG(S):

    x(βk1)x(βks)=x(αi).

    Proof. Use Theorem 1.18 with the group element g(ϵ)=1 on the negative S-compartment. Then the group label on the positive S-compartment is equal to the product of the positive expression associated to any maximal S-green sequence. By Remark 1.17, any Coxeter path gives the Coxeter element. Therefore, every maximal S-green sequence gives a positive expression for the Coxeter element of G(S).

    Lemma 1.20 can be rephrased as follows. Any maximal S-green sequence gives a positive expression for cS by reading the labels of the walls which are crossed by the sequence. The main theorem of this paper is the following theorem and its corollary.

    Theorem A. Suppose that S is an admissible set of roots. Then, the operation described above gives a bijection:

    {maximalSgreensequences}{positiveexpressionsforcSinG(S)}

    It is clear that distinct maximal S-green sequences give distinct positive expressions. Therefore, it suffices to show that every positive expression for cS can be realized as a maximal S-green sequence.

    Recall from Remark 1.10(c) that, for Λ a hereditary artin algebra of finite representation type, the set Φ+(Λ) of positive roots of Λ forms an admissible set and that the picture group of Λ is equal to the picture group of S=Φ+(Λ). This leads to the following corollary.

    Corollary B. For Λ any hereditary artin algebra of finite representation type, there is a bijection between the set of maximal green sequences for Λ and the set of positive expressions for the Coxeter element cQ=x(α1)x(αn) in G(Λ)=G(Φ+(Λ)).

    The proof is by induction on m, the size of the finite set S. If m=1, the root β1 must be simple. So, the group G(S) is infinite cyclic with generator x(β1) which is equal to cS. There are two compartments U1,U1 separated by the single hyperplane D(β1)=H(β1). And U,U+ is the unique S-green sequence. The associated positive expression is x(β1) which is the unique positive expression for cS. So, the result holds for m=1. Thus, we may assume that m2 and the theorem holds for the admissible sequence of roots S0=(β1,,βm1).

    Remark 1.21. One key property of the last element βm in an admissible sequence S is that, for ββm in S, x(β) commutes with x(βm) if and only if β is hom-orthogonal to βm. The reason is that there is a formula for the commutator of two roots if and only if they are hom-orthogonal and, in that case, the commutator is a product of extensions of these roots. But any extension comes afterwards in admissible (vertical) order, so any extension of βm will not be in the set S.

    Lemma 1.22. There is a surjective group homomorphism

    π:G(S)G(S0)

    given by sending each x(βi)G(S) to the generator in G(S0) with the same name when i<m and sending x(βm) to 1.

    Proof. By Remark 1.21 there are only two kinds of relations in G(S) involving x(βm):

    1. Commutation relations: [x(βm),x(βj)]=1 when βm,βj are hom-orthogonal.

    2. Relations in which x(βm) occurs only once:

    x(βi)x(βj)=x(βj)x(βm)x(βi).

    In both cases, when x(βm) is deleted, the relation in G(S) reduces to a relation in G(S0) (or to the trivial relation x(βj)=x(βj) in Case 1). Thus, G(S0) is given by G(S) modulo the relation x(βm)=1.

    Suppose m2 and βm is simple, say βm=αk the kth simple root. Then, since S is admissible, all previous roots βj,j<m have support disjoint from αk. Then x(βm) is central and G(S) is the product G(S)=G(S0)×Z where the Z factor is generated by x(βm). Thus a positive expression for cS is given by any positive expression for xS0 with the letter x(βm) inserted at any point.

    Each S0-compartment Uϵ is the inverse image in Rn of a compartment for S0 in Rn1. Thus, any S-maximal green sequence will pass through these walls giving a maximal S0-green sequence and must, at some point, pass from the negative side of the hyperplane D(βm) to its positive side. (See Figure 1 for an example.) By induction on m, this S0-maximal green sequence is any positive word for cS0 and the crossing of D(βm) inserts x(βm) at any point. This describes all words for cS. So, the theorem holds in this case.

    Now suppose βm is not simple. Then S,S0 have the same set of simple roots. So, π(cS)=cS0. Suppose that w is a positive expression for cS in G(S). Let π(w)=w0 be the positive expression for cS0 in G(S0) given by deleting every instance of the generator x(βm) from w. By induction on m, there exists a unique maximal S0-green sequence Uϵ(0),,Uϵ(s) which realizes the positive expression w0. These fall into two classes.

    Class 1. Each S0-compartment Uϵ(i) in the maximal S0-green sequence is disjoint from D(βm).

    For maximal S0-green sequences in this class, each Uϵ(i)=Uϵ(i) where ϵ(i)=(ϵ1,,ϵm) with ϵm=0 and ϵ(i)=(ϵ1,,ϵm1). Therefore, the maximal S0-green sequence Uϵ(i) is also a maximal S-green sequence and w0=w by the following lemma proved in subsection 3.5. So, the positive expression w is realized by a maximal S-green sequence.

    Lemma C. Let w,w be two positive expressions for the same element of the group G(S). Suppose π(w)=π(w), i.e., the two expressions are identical modulo the generator x(βm). Then x(βm) occurs the same number of times in w,w. In particular, x(βm)1 in G(S).

    In the case at hand, w=w0 does not contain the letter x(βm). So, neither does w and we must have w=w0 as claimed. So, by Lemma C, the theorem hold when w0=π(w) corresponds to a maximal S0-green sequence of Class 1.

    Class 2. At least one S0-compartment in the S0-green sequence meets D(βm).

    For green sequences in this class, the S0-compartments which intersect D(βm) are consecutive:

    Lemma D. Let Uϵ(0),,Uϵ(s) be a maximal S0-green sequence. Then

    1. The S0-compartments Uϵ(i) which meet D(βm) are consecutive, say Uϵ(p),,Uϵ(q).

    2. Let D(βki) be the wall between Uϵ(i1) and Uϵ(i) so that w0=x(βk1)x(βks). Then βm is hom-orthogonal to βki for p<iq but not hom-orthogonal to βkp, βkq+1.

    3. For p<iq and δ{+,}, D(βki) is also the wall separating Uϵ(i1),δ and Uϵ(i),δ.

    Lemma D tells us: (1) The S0-compartments Uϵ(r) for prq are divided into two S-compartments by the wall D(βm). (3) The wall separating consecutive S0-compartments Uϵ(r),Uϵ(r+1) for pr<q also separate the pairs of S-compartments Uϵ(r),,Uϵ(r+1), and Uϵ(r),+,Uϵ(r+1),+. (See Figure 4.)

    Figure 4.  The green path γ1 is in Class 1 since it is disjoint from D(βm). The green path γ2 is in Class 2 and passes through three S0-compartments Uϵ(p),Uϵ(r),Uϵ(q) in V0=int(V(βm)W(βm)). Each of these is divided into two S-compartments by the wall D(βm) and γ2 passes through four of these S-compartments in V0. D(βm) is the part of the hyperplane H(βm) inside the oval region V(βm) and outside of W(βm).

    So, we can refine the maximal S0-green sequence to a maximal S-green sequence, by staying on the negative side of D(βm) until we reach the S-compartment Uϵ(r), for some prq, then cross through D(βm) into Uϵ(r),+ and continue in the given S0-compartments but on the positive side of D(βm). This gives the maximal S-green sequence

    Uϵ(0),0,,Uϵ(p1),0,Uϵ(p),,,Uϵ(r),,Uϵ(r),+,,Uϵ(q),+,Uϵ(q+1),0,,Uϵ(s),0

    of length s+1 giving the positive expression

    wr=x(βk1)x(βkp)x(βkr)x(βm)x(βkr+1)x(βkq)x(βks).

    By the defining relations in the group G(S), the generators x(β) and x(βm) commute if β is hom-orthogonal to βm. By (3) in the lemma this implies that wr is a positive expression for cS if prq. We have just shown that each such wr is realizable by a maximal S-green sequence. So, it remains to show that the positive expression w that we started with is equal to one of these wr.

    By Lemma C, x(βm) occurs exactly once in the expression w. We need to show that, if the generator x(βm) occurs in the "wrong place" then w is not a positive expression for cS, in other words, the product of the elements of w is not equal to cS. This follows from the following lemma proved in subsection 3.5.

    Lemma E. Let

    R(βm)={βiS0:hom(βi,βm)=0=hom(βm,βi)}.

    Let βj1,,βjs be elements of S0 which do not all lie in R(βm). Then x(βm), x(βji) do not commute in the group G(S).

    By part (2) of Lemma D, βkrR(βm) if p<rq and βkp,βkq+1R(βm). So, this lemma implies that wr is a positive expression for cS if and only if prq. So, we must have w=wr for one such r and w is realizable. This concludes the outline of the proof of the main theorem. It remains only to prove the three lemmas C, D, E invoked in the proof.

    Remark 1.23. The number of times a maximal S-green sequences crosses D(βm) is at most one. In Class 1, the number is zero by definition. In Class 2, the number is one as explained in detail above assuming Lemmas C, D, E. It follows that any maximal S-green sequence crosses any wall D(βk) for βkS at most once since βk will be the last element of the subsequence R=(β1,,βk) of S (which is admissible by Remark 1.7) and any maximal S-green sequence gives a maximal R-green sequence which crosses D(βk) the same number of times. It follows that any maximal S-green sequence has length at most equal to the size of S. Since S is finite, it follows that there are only finitely maximal S-green sequences.

    We derive the basic properties of the compartments Uϵ and prove Lemma D. The basic property is the following.

    Proposition 2.1. For all weakly admissible S and all admissible ϵ the S-compart-ment Uϵ is convex and nonempty. When ϵm0, or equivalently, when D(βm)Uϵ1,,ϵm1 is nonempty, the boundary of D(βm) does not meet Uϵ1,,ϵm1. Equivalently,

    D(βm)Uϵ1,,ϵm1=H(βm)Uϵ1,,ϵm1.

    Consequently, the S-compartments form the components of the complement of CL(S) in Rn.

    Proof. When m=1, β1 is simple and D(β1)=H(β1) is a hyperplane whose complement has two convex components U+,U. So, the proposition holds for m=1. Now, suppose m2 and all statements hold for m1. Let S0=Sβm. This a weakly admissible sequence of roots. So, the S0-components Uϵ are convex and open and their union is the complement of CL(S0).

    Since S is weakly admissible, it either contains all subroots of βm or it contains all quotient roots of βm. By symmetry we assume the first condition. Let ϵ=(ϵ1,,ϵm1) be admissible of length m1. If (ϵ,0) is admissible for S then Uϵ,0=Uϵ. Otherwise, Uϵ meets D(βm). In that case UϵD(βm) must be empty since any element x0D(βm) must be an element of D(β) for some proper subroot β. By assumption, \beta'\in\mathcal{S}_0 . So, x_0\in CL(\mathcal{S}_0) . This gives a contradiction since \mathcal{U}_\epsilon is disjoint from CL(\mathcal{S}_0) by induction on m . Therefore, \mathcal{U}_\epsilon is divided into two convex open sets \mathcal{U}_{\epsilon,+} and \mathcal{U}_{\epsilon,-} separated by D(\beta_m) . So the \mathcal{S} -compartments fill up the complement of CL(\mathcal{S}_0)\cup D(\beta_m) = CL(\mathcal{S}) .

    For \mathcal{S}_0 weakly admissible, let \mathcal{V} be the closure of the union of some set of \mathcal{S}_0 -compartments \mathcal{U}_\epsilon . Then \mathcal{V} has internal and external walls. The internal walls of \mathcal{V} are the ones between two of the compartments \mathcal{U}_\epsilon,\mathcal{U}_{\epsilon'} in \mathcal{V} . \mathcal{V} has points on both sides of the internal walls. The external walls of \mathcal{V} are the ones which separate \mathcal{V} from its complement. The region \mathcal{V} will be called inescapable if it is on the positive side of all of its external walls. I.e., they are all red on the inside. Once an \mathcal{S}_0 -green sequence enters such a region, it can never leave. Since \mathcal{V} is closed, it contains all of its internal and external walls. We also consider open regions \mathcal{W} which are inescapable regions minus their external walls. Then \mathcal{W} is the complement of the closure of the union of all compartments not in \mathcal{W} .

    Given an admissible sequence \mathcal{S} with last object \beta_m which we assume to be nonsimple, let \mathcal{S}_0 = (\beta_1,\cdots,\beta_{m-1}) . Recall that this is also admissible. We will construct two inescapable regions \mathcal{W}(\beta_m),\mathcal{V}(\beta_m) where the first is open and the second is closed. All maximal \mathcal{S}_0 -green sequences start outside both regions, end inside both regions and fall into two classes: those that enter \mathcal{W}(\beta_m) before they enter \mathcal{V}(\beta_m) and those that enter \mathcal{V}(\beta_m) before they enter \mathcal{W}(\beta_m) . And these coincide with the two classes of maximal \mathcal{S}_0 -green sequences discussed in the outline of the main theorem (Corollary 2.5 below).

    The first inescapable region is the open set

    \mathcal{W}(\beta_m): = \{x\in\mathbb{R}^n: \left < {x,\alpha}\right > > 0\text{ for some }\alpha\subsetneq\beta_m\}.

    For example, on the left side of Figure 1, m = 3 and \mathcal{W}(\beta_3) is the interior of D(\alpha_1) .

    Proposition 2.2. The complement of \mathcal{W}(\beta_m) in \mathbb{R}^n is closed and convex. Furthermore:

    \begin{equation} \mathcal{W}(\beta_m)\cap H(\beta_m) = H(\beta_m)-D(\beta_m). \end{equation} (3)

    Proof. The complement of \mathcal{W}(\beta_m) is

    \mathbb{R}^n\backslash\mathcal{W}(\beta_m) = \{x\in\mathbb{R}^n: \left < {x,\alpha}\right > \le0\text{ for all }\alpha\subsetneq\beta_m\}

    which is closed and convex since it is given by closed convex conditions \left<{x,\alpha}\right>\le0 .

    For the second statement, suppose that v\in H(\beta_m) . Then \left<{v,\beta_m}\right> = 0 . By the stability conditions which we are using to define D(\beta_m) , v\in D(\beta_m) if and only if \left<{v,\alpha}\right>\le0 for all \alpha\subset\beta_m , in other words,

    D(\beta_m) = H(\beta_m)\cap(\mathbb{R}^n\backslash\mathcal{W}(\beta_m))

    which is equivalent to (3).

    Proposition 2.3. The region \mathcal{W}(\beta_m) is inescapable. I.e., all external walls are red. Furthermore, each external walls of \mathcal{W}(\beta_m) has the form D(\alpha) for some \alpha\subsetneq \beta_m . Consequently, every \mathcal{S}_0 -compartment is contained either in \mathcal{W}(\beta_m) or in its complement.

    Proof. Take any external wall D(\alpha) of \mathcal{W}(\beta_m) . Let v_t be a continuous path which goes through that wall from inside to outside. In other words, v_t\in\mathcal{W}(\beta_m) for t<0 and v_t\notin \mathcal{W}(\beta_m) for t\ge0 . By definition of \mathcal{W}(\beta_m) this means that there is some \alpha'\subsetneq \beta_m so that \left<{v_t,\beta}\right> changes sign from positive to nonpositive at t goes from negative to nonnegative.

    By choosing v_t in general position, v_0 will not lie in H(\alpha') for any \alpha'\neq\alpha . So, we must have \alpha\subsetneq\beta_m . And \left<{v_t,\alpha}\right>>0 for t<0 and \left<{v_t,\alpha}\right><0 for t>0 . Therefore, \mathcal{W}(\beta_m) is on the positive (red) side of the external wall D(\alpha) . So, \mathcal{W}(\beta_m) is inescapable.

    Since each part of the boundary lies in D(\alpha) for some \alpha\in \mathcal{S}_0 , the boundary of \mathcal{W}(\beta_m) is contained in the union of the boundaries of the \mathcal{S}_0 -compartments. So, all such compartments are either entirely insider or entirely outside \mathcal{W}(\beta_m) .

    The second inescapable region is the closed set

    \mathcal{V}(\beta_m) = \{y\in\mathbb{R}^n: \left < {y,\gamma}\right > \ge 0\text{ for all quotient roots $\gamma$ of $\beta_m$}\}.

    For example, on the left side of Figure 1, m = 3 and \mathcal{V}(\beta_3) is the closure of the interior of D(\alpha_2) . In Figure 4, \mathcal{V}(\beta_m) is the region enclosed by the large oval. By arguments analogous to the ones above, we get the following.

    Proposition 2.4. \mathcal{V}(\beta_m) is a closed convex inescapable region whose external walls all have the form D(\gamma) where \gamma is a quotient root of \beta_m . So, every \mathcal{S}_0 -compartment is contained in \mathcal{V}(\beta_m) or its complement. Furthermore,

    \mathcal{V}(\beta_m)\cap H(\beta_m) = D(\beta_m).

    Recall that a maximal \mathcal{S}_0 -green sequence with \mathcal{S}_0 = (\beta_1,\cdots,\beta_{m-1}) is in:

    1. Class 1 if each \mathcal{S}_0 -compartment \mathcal{U}_{\epsilon(i)} in the green sequence is disjoint from D(\beta_m) .

    2. Class 2 if at least one \mathcal{S}_0 -compartment, say \mathcal{U}_{\epsilon(j)} , in the \mathcal{S}_0 -green sequence meets D(\beta_m) . So, \mathcal{U}_{\epsilon(j)} is divided into two \mathcal{S} -compartments \mathcal{U}_{\epsilon(j),-} and \mathcal{U}_{\epsilon(j),+} . See Figure 4.

    Corollary 2.5. A maximal \mathcal{S}_0 -green sequence is in Class 1 if and only if it passes through \mathcal{W}(\beta_m)\backslash \mathcal{V}(\beta_m) . It is in Class 2 if and only if it contains a compartment in

    \mathcal{V}(\beta_m)\backslash \mathcal{W}(\beta_m) = \{x\in \mathbb{R}^n: \left < {x,\alpha}\right > \le 0\;\mathit{\text{for all}}\;\alpha\subsetneq \beta_m\;\mathit{\text{and}}\;\left < {x,\gamma}\right > \ge0\;\mathit{\text{for all}}\;\beta_m\twoheadrightarrow\gamma\}.

    Proof. Every maximal green sequence starts on the negative side of the hyperplane H(\beta_m) and ends on its positive side. Therefore the maximal \mathcal{S}_0 -green sequence must cross the hyperplane at some point. Since \beta_m\notin \mathcal{S}_0 , none of the \mathcal{S}_0 -compartments has H(\beta_m) as a wall. So, there must be one compartment in the \mathcal{S}_0 -green sequences which meets the hyperplane H(\beta_m) . Let \mathcal{U}_\epsilon be the first such compartment. Then, either \mathcal{U}_\epsilon\cap D(\beta_m) is empty or nonempty. In the first case, \mathcal{U}_\epsilon is in \mathcal{W}(\beta_m) and it is outside \mathcal{V}(\beta_m) . Since \mathcal{W}(\beta_m) is inescapable and does not meet D(\beta_m) , the green sequence is in Class 1. In the second case, \mathcal{U}_\epsilon is in \mathcal{V}(\beta_m) and not in \mathcal{W}(\beta_m) and the green sequence is in Class 2. So, these two cases correspond to Class 1 and Class 2 proving the corollary.

    Recall that \mathcal{R}(\beta_m) is the set of all \alpha\in\mathcal{S}_0 which are hom-orthogonal to \beta_m . Let \mathcal{V}_0 be the interior of the closed region \mathcal{V}(\beta_m)\backslash \mathcal{W}(\beta_m) . Thus

    \begin{align*} \mathcal{V}_0 &: = {\rm int}(\mathcal{V}(\beta_m)\backslash \mathcal{W}(\beta_m))\\ & = \{x\in \mathbb{R}^n: \forall\alpha\subsetneq \beta_m\left < {x,\alpha}\right > < 0\text{ and }\left < {x,\gamma}\right > > 0\,\forall\beta_m\twoheadrightarrow\gamma, \gamma\neq\beta_m\}. \end{align*}

    Proposition 2.6. For all \alpha\in\mathcal{S}_0 , \alpha\in\mathcal{R}(\beta_m) if and only if D(\alpha)\cap \mathcal{V}_0\neq\emptyset .

    Proof. Suppose that x\in D(\alpha)\cap \mathcal{V}_0 and hom(\beta_m,\alpha)\neq0 . Then there is a subroot \alpha' of \alpha which is also a quotient root of \beta_m : \beta_m\twoheadrightarrow \alpha'\subset \alpha . Since \alpha\in\mathcal{S}_0 we cannot have \beta_m\subset \alpha . Therefore \alpha' is a proper quotient of \beta_m . Then \left<{x,\alpha'}\right>>0 since x\in\mathcal{V}_0 and \left<{x,\alpha'}\right>\le0 since x\in D(\alpha) and \alpha'\subset\alpha . This is a contradiction. So, hom(\beta_m,\alpha) = 0 . A similar argument shows that hom(\alpha,\beta_m) = 0 . So, \alpha\in\mathcal{R}(\beta_m) .

    Conversely, if \alpha\in\mathcal{R}(\beta_m) then \alpha,\beta_m span a rank 2 wide subcategory \mathcal{A}(\alpha,\beta_m) of mod\text-\Lambda . Choose any tilting object T in the left perpendicular category ^\perp\mathcal{A}(\alpha,\beta_m) (for example the sum of the projective objects). Then the g -vector g(\underline\dim\, T) lies in the interior of both D(\alpha) and D(\beta_m) by Proposition 4.6 since M_\alpha,M_{\beta_m} are the minimal objects in T^\perp = \mathcal{A}(\alpha,\beta_m) . So, g(\underline\dim\, T)\in \mathcal{V}_0 . So, D(\alpha) meets \mathcal{V}_0 .

    Corollary 2.7. The open region \mathcal{V}_0 contains no vertices of the semi-invariant picture L(\mathcal{S}_0) .

    Proof. Suppose that x_0\in \mathcal{V}_0 is a vertex of L(\mathcal{S}_0) . By Theorem 4.5, we have a wide subcategory \mathcal{W}(x_0) of all modules V so that x_0\in D(V) . Since x_0 is a vertex of L(\mathcal{S}_0) , the wide subcategory \mathcal{W}(x_0) must have rank n-1 and its minimal objects must lie in \mathcal{S}_0 , i.e., \mathcal{W}(x_0) = \mathcal{A}(\alpha_1,\cdots,\alpha_{n-1}) where \alpha_i\in\mathcal{S}_0 .

    By Proposition 2.6, each \alpha_i is hom-orthogonal to \beta_m . This implies that \alpha_1,\cdots, \alpha_{n-1} together with \beta_m form the minimal roots of a wide subcategory of rank n . By Theorem 4.7 this must be all of mod\text-\Lambda . So, \beta_m must be a simple root contrary to our initial assumption. Therefore \mathcal{V}_0 contains no vertices of L(\mathcal{S}_0) .

    Corollary 2.8. Let \alpha_1,\cdots,\alpha_k be pairwise hom-orthogonal elements of \mathcal{R}(\beta_m) then the intersection D(\alpha_1)\cap \cdots\cap D(\alpha_k)\cap D(\beta_m)\cap\mathcal{V}_0 is nonempty.

    Proof. More precisely, let \mathcal{A}(\alpha_1,\cdots,\alpha_k,\beta_m) be the rank k+1 wide subcategory of mod\text-\Lambda with simple objects M_{\alpha_i},M_{\beta_m} . Let T = T_1\oplus \cdots\oplus T_{n-k-1} be any cluster tilting object of the cluster category of ^\perp\mathcal{A}(\alpha_1,\cdots,\alpha_k,\beta_m) . Then the g -vector g(\underline\dim\, T) is a point in D(\alpha_1)\cap\cdots\cap D(\alpha_k)\cap D(\beta_m) which lies in the interior of D(\beta_m) . This can be proved by induction on k using the argument in the proof of Proposition 2.6.

    We will show that maximal \mathcal{S}_0 -green sequences satisfy the three properties listed in Lemma D.

    Proposition 2.9. An \mathcal{S}_0 -compartment \mathcal{U}_\epsilon meets D(\beta_m) if and only if \mathcal{U}_\epsilon\subseteq\mathcal{V}_0 .

    Before proving this we show that this implies the first property in Lemma D. Recall that this states:

    D(1) In every maximal \mathcal{S}_0 -green sequence in Class 2, the compartments which meet D(\beta_m) are consecutive.

    Proof of D(1). Let \mathcal{U}_{\epsilon(i)} be a maximal \mathcal{S}_0 -green sequence. Let p,q be minimal so that \mathcal{U}_{\epsilon(p)}\subseteq\mathcal{V}(\beta_m) and \mathcal{U}_{\epsilon(q)}\subseteq\mathcal{W}(\beta_m) . When the green sequence is in Class 2, p<q . Since \mathcal{V}(\beta_m) is inescapable, \mathcal{U}_{\epsilon(i)}\subseteq\mathcal{V}(\beta_m) iff p\le i . Since \mathcal{W}(\beta_m) is inescapable, \mathcal{U}_{\epsilon(i)}\subseteq\mathcal{V}_0 iff p\le i<q . So, the compartments of the green sequence which lie in \mathcal{V}_0 are consecutive. By the proposition these are the compartments which meet D(\beta_m) .

    Proof of Proposition 2.9. Let \mathcal{U}_\epsilon be an \mathcal{S}_0 -compartment in \mathcal{V}_0 . Let x\in \mathcal{U}_\epsilon . If \left<{x,\beta_m}\right> = 0 then x\in H(\beta_m)\cap \mathcal{V}_0\subset D(\beta_m) and we are done. So, suppose \left<{x,\beta_m}\right>\neq0 . Pick a point y\in D(\beta_m)\cap \mathcal{V}_0 and take the straight line from x to y . Since \mathcal{V}_0 is convex, this line is entirely contained in \mathcal{V}_0 . If the line is not in \mathcal{U}_\epsilon then it must meet an internal wall D(\alpha) on the boundary of \mathcal{U}_\epsilon . By Proposition 2.6, \alpha\in\mathcal{R}(\beta_m) .

    Let k be maximal so that the closure of \mathcal{U}_\epsilon contains a point z\in D(\alpha_\ast) = D(\alpha_1)\cap\cdots\cap D(\alpha_k) where \alpha_1,\cdots,\alpha_k\in \mathcal{R}(\beta_m) are pairwise hom-orthogonal. Then, by Corollary 2.8, D(\alpha_\ast)\cap D(\beta_m)\cap \mathcal{V}_0 is nonempty. Let w be an element. Since D(\alpha_\ast) and \mathcal{V}_0 are both convex, D(\alpha_\ast)\cap \mathcal{V}_0 contains the straight line \gamma(t) = (1-t)z+tw , 0\le t\le 1 .

    Let \delta be a very small vector so that \left<{\delta,\beta_m}\right> = 0 and z+\delta\in\mathcal{U}_\epsilon . Consider the line \gamma(t)+\delta . This is in \mathcal{U}_\epsilon for t = 0 and lies in D(\beta_m) when t = 1 . This proves the proposition if \gamma(t)+\delta\in \mathcal{U}_\epsilon for all 0\le t\le1 . So, suppose not. Let t_0 be minimal so that this open condition fails. Then the line \gamma(t) meets another wall at t = t_0 and \gamma(t_0) will be a point in the closure of \mathcal{U}_\epsilon which meets a codimension k+1 set D(\alpha_0)\cap D(\alpha_1)\cap\cdots\cap D(\alpha_k) where \alpha_0\in \mathcal{S}_0 is hom-orthogonal to the other roots \alpha_i . (Take \alpha_0 of minimal length among the new roots so that \gamma(t_0)\in D(\alpha_0) .) This contradicts the maximality of k . So, there is no point t_0 and \gamma(1)+\delta\in \mathcal{U}_\epsilon\cap D(\beta_m) as claimed.

    We have already shown property (2) in Lemma D: Any maximal \mathcal{S}_0 -green sequence of Class 2 crosses a wall D(\gamma) at some point to enter region \mathcal{V}_0 , passes through several internal walls of \mathcal{V}_0 , then exists \mathcal{V}_0 by a wall D(\alpha) of \mathcal{W}(\beta_m) . By Propositions 2.4, 2.3 \gamma is a quotient root of \beta_m and \alpha is a subroot of \beta_m , both not hom-orthogonal to \beta_m . By Proposition 2.6 the internal walls of \mathcal{V}_0 are D(\beta) where \beta\in\mathcal{R}(\beta_m) . So, property (2) in Lemma D holds.

    The last property we need to verify in Lemma D is the following.

    D(3) Suppose that the two \mathcal{S}_0 -compartments \mathcal{U}_{\epsilon(1)} and \mathcal{U}_{\epsilon(2)} meet along a common internal wall D(\beta_j) . Then the \mathcal{S} -compartments \mathcal{U}_{\epsilon(1),+},\mathcal{U}_{\epsilon(2),+} meet along the common internal wall D(\beta_j) and the \mathcal{S} -compartments \mathcal{U}_{\epsilon(1),-},\mathcal{U}_{\epsilon(2),-} also meet along D(\beta_j) .

    Proof. Let \mathcal{S}' , \mathcal{S}_0' be \mathcal{S},\mathcal{S}_0 with \beta_j deleted. Then \mathcal{S}',\mathcal{S}_0' are weakly admissible. Since \beta_j\notin\mathcal{S}_0' , the two \mathcal{S}_0 -compartments \mathcal{U}_{\epsilon(1)} and \mathcal{U}_{\epsilon(2)} merge to form one \mathcal{S}_0' -compartment \mathcal{U}_\epsilon . This compartment meets D(\beta_m) so it breaks up into two \mathcal{S}' -compartments \mathcal{U}_{\epsilon,+} and \mathcal{U}_{\epsilon,-} . We know that D(\beta_j) must divide these two \mathcal{S}' -compartments into four \mathcal{S} -compartments since \mathcal{U}_{\epsilon(1)} , \mathcal{U}_{\epsilon(2)} are both divided into two parts by D(\beta_m) . Since \mathcal{S}' -compartments are convex by Proposition 2.1, this can happen only if D(\beta_j) meets both \mathcal{S}' -compartments and forms the common wall separating the two halves of each.

    In this section we will use planar pictures to prove the two properties of the group G(\mathcal{S}) that we are using: Lemmas C and E. The key tool will be the "sliding lemma" (Lemma 3.17) which comes from the first author's PhD thesis [17]. Unless otherwise stated, all pictures in this section will be planar. We begin with a review of the topological definition of a (planar) picture with special language coming from the fact that all relations in our group G(\mathcal{S}) are commutator relations. Since this section uses only planar diagrams, we feel that theorems can be proven using diagrams and topological arguments. Algebraic versions of these arguments using HNN extensions, geometric realizations of categories and cubical CAT(0) categories can be found in other papers which prove similar results for pictures of arbitrary dimension ([26], [19], [27]). The first example of a picture group for a picture group of a Dynkin quiver appears in a paper by Jean-Louis Loday [32] where the picture group for the quiver of type A_n with straight orientation is constructed and the picture space (the K(\pi,1) for the picture group) is also constructed.

    Suppose that the group G has a presentation G = \left<\mathcal{X}\,|\,\mathcal{Y}\right> . This means there is an exact sequence

    R_\mathcal{Y}\hookrightarrow F_\mathcal{X}\twoheadrightarrow G

    where F_\mathcal{X} is the free group generated by the set \mathcal{X} and R_\mathcal{Y}\subseteq F_\mathcal{X} is the normal subgroup generated by the subset \mathcal{Y}\subseteq F_\mathcal{X} . Then G is the fundamental group of a 2-dimensional CW-complex X^2 given as follows. Let X^1 denote the 1-dimensional CW-complex having a single 0-cell e^0 , one 1-cell e^1(x) for every generator x\in\mathcal{X} attached on e^0 . Then \pi_1X^1 = F_\mathcal{X} and any f\in F_\mathcal{X} gives a continuous mapping \eta_f:S^1\to X^1 given by composing the loops corresponding to each letter in the unique reduced expression for f . Here S^1 = \{z\in\mathbb{C}:||z|| = 1\} , 1\in S^1 is the basepoint and S^1 is oriented counterclockwise.

    Let X^2 denote the 2-dimensional CW-complex given by attaching one 2-cell e^2(r) for every relations r\in\mathcal{Y} using an attaching map

    \eta_r:S^1\to X^1

    homotopic to the one described above. We choose each mapping \eta_r so that it is transverse to the centers of the 1-cells of X^1 . So, the inverse images of these center points are fixed finite subsets of S^1 . The relation r is given by the union of these finite sets, call it E_r\subset S^1 , together with a mapping \lambda:E_r\to \mathcal{X}\cup \mathcal{X}^{-1} indicating which 1-cell the point goes to and in which direction the image of \eta_r traverses that 1-cell. Then we have:

    r = \prod\limits_{x\in E_r}\lambda(x)\in F_\mathcal{X}.

    The circle S^1 is the boundary of the unit disk D^2 = \{x\in \mathbb{C}: ||x||\le 1\} . Let CE_r\subset D^2 denote the cone of the set E_r :

    CE_r: = \bigcup\limits_{x\in E_r}\{ax\in D^2: 0\le a\le 1\}.

    This is the union of the straight lines from all x\in E_r to 0\in D^2 .

    Figure 5.  The cone of E_r in D^2 is the part inside the circle S^1 . The asterisks \ast indicates the position of the basepoint 1\in S^1 . The labels are drawn on the negative side of each edge.

    A picture is a geometric representation of a continuous pointed mapping \theta:S^2\to X^2 where pointed means preserving the base point. A (pointed) deformation of a picture represents a homotopy of such a mapping. Deformation classes of pictures form a module over the group ring {\mathbb Z} G .

    Definition 3.1. Given a group G with presentation G = \left<\mathcal{X}\,|\,\mathcal{Y}\right> and fixed choices of E_r\subset S^1 , \lambda:E^4\to \mathcal{X}\cup\mathcal{X}^{-1} , a picture for G is defined to be a graph L embedded in the plane \mathbb{R}^2 with circular edges allowed, together with:

    1. a label x\in \mathcal{X} for every edge in L ,

    2. a normal orientation for each edge in L ,

    3. a label r\in \mathcal{Y}\cup \mathcal{Y}^{-1} for each vertex in L ,

    4. for each vertex v , a smooth ( C^\infty ) embedding \theta_v:D^2\to \mathbb{R}^2 sending 0 to v

    satisfying the following where E(x) denotes the union of edges labeled x .

    (a) Each E(x) is a smoothly embedded 1-manifold in \mathbb{R}^2 except possibly at the vertices.

    (b) For each vertex v\in L , \theta_v^{-1}(E(x))\subseteq CE_r is equal to the cone of \lambda^{-1}(\{x,x^{-1}\}) \subset E_r .

    The image of 1\in S^1 under \theta_v:D^2\to \mathbb{R}^2 will be called the basepoint direction of v and will be indicated with \ast when necessary.

    The embedding \theta_v has positive, negative orientation when r\in\mathcal{Y} , r\in\mathcal{Y}^{-1} , respectively.

    One easy consequence of this definition is the following.

    Proposition 3.2. Given a picture L for G , there is a unique label g(U)\in G for each component U of the complement of L in \mathbb{R}^2 having the following properties.

    1. g(U_\infty) = 1 for the unique unbounded component U_\infty .

    2. g(V) = g(U)x if the regions U,V are separated by an edge labeled x and oriented towards V .

    Proof. For any region U , choose a smooth path from \infty to any point in U . Make the path transverse to all edge sets. Then let g(U) = x_1^{\epsilon_1}\cdots x_m^{\epsilon_m} if the path crosses m edges labeled x_1,\cdots,x_m with orientations given by \epsilon_i . This is well defined since any deformation of the path which fixes the endpoints and which pushes it through a vertex will not change the product g(U) since the paths on either side of the vertex have edge labels giving a relation in the group and therefore give the same product of labels in the group G .

    Remark 3.3. Any particular smooth path \gamma from U_\infty to U gives a lifting f_\gamma(U) of g(U) to the free group F_\mathcal{X} .

    It is well-known that the set of deformation classes of pictures for any group G is a {\mathbb Z} G -module P(G) . (See Theorem 3.5 and Corollary 3.7 below.)

    The action of the group G is very easy to describe. Given any picture L and any generator x\in \mathcal{X} , the pictures xL, x^{-1}L are given by enclosing the set L with a large circle, labeling the circle with x and orienting it inward or outward, respectively. Addition of pictures is given by disjoint union of translates of the pictures.

    To define the equivalence relation which we call "deformation equivalence" of pictures, it is helpful to associate to each picture L an element \psi(L)\in {\mathbb Z} G\!\left<\mathcal{Y}\right> where {\mathbb Z} G\!\left<{\mathcal{Y}}\right> is the free {\mathbb Z} G module generated by the set of relations \mathcal{Y} . This is given by

    \psi(L) = \sum\limits_{v_i} g(v_i) \left < {r_i}\right >

    where the sum is over all vertices v_i of L , r_i\in \mathcal{Y}\cup\mathcal{Y}^{-1} is the relation at v_i , g(v_i)\in G is the group label at the basepoint direction of v_i and \left<{r^{-1}}\right> = -\left<r\right> by definition.

    Definition 3.4. A deformation L_0\simeq L_1 of pictures for G is defined to be a sequence of allowable moves given as follows.

    1. Isotopy. L_0\simeq L_1 if there is an orientation preserving diffeomorphism \varphi:\mathbb{R}^2\to \mathbb{R}^2 so that L_1 = \varphi(L_0) with corresponding labels. By isotopy we can make the images of the embeddings \theta_v:D^2\to\mathbb{R}^2 disjoint and arbitrarily small.

    2.Smooth concordance of edge sets. There are two concordance moves:

    (a) If L_0 contains a circular edge E with no vertices and L_0 does not have any point in the region enclosed by E then L_0\simeq L_1 where L_1 is obtained from L_0 by deleting E .

    (b) If U is a connected component of \mathbb{R}^2-L_0 and two of the walls of U have the same label x oriented in the same way (inward towards U or outward) then, choose a path \gamma in U connecting points on these two edges then perform the following modification of L_0 in a neighborhood of \gamma to obtain L_1\simeq L_0 .

    \psi(L) = \sum\limits_{v_i} g(v_i) \left < {r_i}\right >

    3. Cancellation of vertices. Suppose that two vertices v_0,v_1 of L_0 have inverse labels r,r^{-1} . Suppose that there is a path \gamma disjoint from L_0 connecting the basepoint directions of v_0,v_1 . Let V be the union of the \theta_{v_0}(D^2),\theta_{v_1}(D^2) and a small neighborhood of the path \gamma . We can choose V to be diffeomorphic to D^2 . Then L_0\simeq L_1 if L_0,L_1 are identical outside of the region V and L_1 has no vertices in V . (The two vertices in V\cap L_0 cancel.)

    \psi(L) = \sum\limits_{v_i} g(v_i) \left < {r_i}\right >

    Concordance means L_0,L_1 have the same vertex sets and are equal in a neighborhood of each vertex and that f_{\gamma_i}\in F_\mathcal{X} are equal for L_0 , L_1 for some (and thus every) choice of paths \gamma_i disjoint from vertices from \infty to the basepoint direction of each vertex of L_0 . The same paths work for L_1 since L_0,L_1 have the same vertex set.

    Theorem 3.5. [37][18, Prop 7.4] L_0,L_1 are deformation equivalent if and only if \psi(L_0) = \psi(L_1) . Furthermore, the set of possible values of \psi(L) for all pictures L is equal to the kernel of the mapping

    {\mathbb Z} G\!\left < {\mathcal{Y}}\right > \xrightarrow{d_2} {\mathbb Z} G\!\left < {\mathcal{X}}\right >

    where d_2\left<r\right> = \sum \partial_x r\!\left<x\right> , where \partial_x is the Fox derivative of r with respect to x .

    The Fox derivative of w\in F_\mathcal{X} is given recursively on the reduced length of w by

    1. \partial_x(x) = 1 , \partial_x(x^{-1}) = -x^{-1} .

    2. \partial_x(y) = 0 if y\in\mathcal{X}\cup \mathcal{X}^{-1} is not equal to x,x^{-1} .

    3. \partial_x(ab) = \partial_x a+a\partial_xb for any a,b\in F_\mathcal{X} .

    Definition 3.6. The group of pictures P(G) is defined to be the group of deformation classes of pictures for G .

    Corollary 3.7. There is an exact sequence of {\mathbb Z} G -modules

    0\to P(G)\to {\mathbb Z} G\!\left < {\mathcal{Y}}\right > \xrightarrow{d_2} {\mathbb Z} G\!\left < {\mathcal{X} }\right > \xrightarrow{d_1} {\mathbb Z} G\xrightarrow\epsilon {\mathbb Z}\to 0

    where d_1\sum a_i\left<{x_i}\right> = \sum a_i(x_i-1) , \epsilon:{\mathbb Z} G\to {\mathbb Z} is the augmentation map and d_2 is as above.

    Remark 3.8. The chain complex {\mathbb Z} G\!\left<{\mathcal{Y}}\right>\xrightarrow{d_2} {\mathbb Z} G\!\left<{\mathcal{X}}\right> \xrightarrow{d_1} {\mathbb Z} G is the cellular chain complex of the universal covering \widetilde{X^2} of the 2-dimensional CW complex X^2 constructed above. Since \widetilde{X^2} is simply connected, we have

    P(G) = H_2(\widetilde{X^2}) = \pi_2(\widetilde{X^2}) = \pi_2(X^2).

    Therefore, P(G) = \pi_2(X^2) as claimed at the beginning of this subsection.

    We also use "partial pictures". These are given by cutting a picture in half using a straight line transverse to the picture.

    Definition 3.9. Let w be a word in \mathcal{X}\cup \mathcal{X}^{-1} given by a finite subset W of the x -axis in \mathbb{R}^2 together with a mapping W\to \mathcal{X}\cup\mathcal{X}^{-1} . A partial picture with boundary \partial L = w is defined to be a closed subset L of the upper half plane so that the intersection of L with the x -axis is equal to W together with labels on L so that the union of L and its mirror image L_- in the lower half plane is a picture for G and so that the labels on the edges which cross the x -axis agree with the given mapping W\to \mathcal{X}\cup\mathcal{X}^{-1} . We call L\cup L_- the double of L .

    Figure 6.  On the left, L_1 is a partial picture with \partial L_1 = abr_1b^{-1}a^{-1}cr_2c^{-1} where r_1 = x^{-1}y^{-1}z and r_2 are relations (or inverse relations). L_1 is the "standard partial picture" for q(L_1) = (ab,r_1)(c,r_2)\in Q(G) . On the right is L_2 , a deformation of L_1 with \partial L_2 = cc^{-1}\partial L_1 . q(L_2) = (c,r_2)(cr_2^{-1}c^{-1}ab,r_1) since the vertex for r_2 is on the left and cr_2^{-1}c^{-1}ab is given by reading the labels on the dotted path \ell_1' . Then q(L_1) = q(L_2) by (4)..

    A deformation of a partial picture L is defined to be any deformation of its double in which vertices do not cross the x -axis and which are transverse to the x -axis at the beginning and end of the deformation. (See Figure 6 for an example where the deformation pushes the c curve through the x -axis producing the cancelling pair cc^{-1} in the word for \partial L_2 .) It is clear that deformation of partial pictures preserves its boundary \partial L = w as an element of the free group F_\mathcal{X} and that w lies in the relation group R_\mathcal{Y}\subseteq F_\mathcal{X} . The main theorem about partial pictures is the following.

    Theorem 3.10. The set of deformation classes of partial pictures forms a (nonabelian) group Q(G) given by generators and relations as follows.

    1. The generators of Q(G) are pairs (f,r) where f\in F_\mathcal{X} and r\in\mathcal{Y} .

    2. The relations in Q(G) are given by

    (f,r)(f',r')(f,r)^{-1} = (frf^{-1}f',r')

    Note that there is a well defined group homomorphism

    \varphi:Q(G)\to F_\mathcal{X}

    given by \varphi(f,r) = frf^{-1} . Then relation (2) can be written as

    \begin{equation} (f,r)(f',r') = (\varphi(f,r)f',r')(f,r). \end{equation} (4)

    The image of \varphi is R_\mathcal{Y} , the normal subgroup generated by all r\in\mathcal{Y} . We use the notation

    \begin{equation} (f,r^{-1}): = (f,r)^{-1}. \end{equation} (5)

    This is compatible with the relations in Q(G) and with the homomorphism \varphi since

    (f,r^{-1})(f',r')(f,r) = (fr^{-1}f^{-1}f',r')

    and \varphi(f,r^{-1}) = fr^{-1}f^{-1} = \varphi(f,r)^{-1}. We assume that the relations are irredundant. So, \mathcal{Y} , \mathcal{Y}^{-1} will be disjoint.

    The generators and relations for Q(G) first appeared in a paper by Renée Peiffer [34]. For this reason, the relations (4) and (5), or rather the equivalent equation (f,r)(f,r^{-1}) = 1 are called Peiffer transformations of the first and second kind, respectively [33].

    Proof. Given a partial picture L for G = \left<\mathcal{X}|\mathcal{Y}\right> , e.g. L_1 in Figure 6, the corresponding element q(L_1)\in Q(G) is given as follows.

    First, by a small deformation of the partial picture, we may assume that the x -coordinates of the vertices of L are all distinct. Label the vertices v_1,\cdots,v_n from left to right (in order of increasing x -coordinates). From the basepoint direction of vertex v_i , draw a lines \ell_i straight up. By a small deformation we can make the green lines transverse to L . (These are dotted arrow \ell_1,\ell_2 in Figure 6.) At each vertex v_i left r_i\in \mathcal{Y}\coprod \mathcal{Y}^{-1} be the relation at v_i and let f_i\in F be given by reading the labels of the edges in L traversed by \ell_i oriented towards v_i . The resulting element of Q(G) is

    q(L) = (f_1,r_1)\cdots(f_n,v_n).

    In Figure 6, on the left, we have r_1 = x^{-1}y^{-1}z ( r_2 is not given) f_1 = ab , f_2 = c . This gives

    q(L_1) = (ab, x^{-1}y^{-1}z)(c,r_2)

    On the right the vertices are in the reverse order. So, (c,r_2) comes first. The new line \ell_1' traverses six edges of L_2 giving (cr_2^{-1}c^{-1}ab,r_1) . So, the element of Q(G) associated to L_2 is

    q(L_2) = (c,r_2)(cr_2^{-1}c^{-1}ab,r_1).

    By (4) we see that q(L_1) = q(L_2)\in Q(G) .

    Claim 1. q(L)\in Q(G) is invariant under deformations of L and therefore well-defined.

    Proof. First, consider deformations which keep the vertices v_1,\cdots,v_n in the same order. Then the lines \ell_1,\cdots,\ell_n will cross edges whose labels give the same elements f_1,\cdots,f_n\in F since the only changes will be to add or delete cancelling pairs of edges labeled x,x^{-1} . So, q(L) remains the same.

    Next, consider deformations in which the order of the vertices changes. This happens when, at some point in the deformation, one vertex, say v_i , passes above the next, v_{i+1} (or the previous one v_{i-1} as in Figure 6). In that case, the line \ell_i will cross the same edges as before, but the line \ell_{i+1} will cross edges f_{i+1} before and \varphi(f_i,r_i)f_{i+1} after the deformation. This will change (f_i,r_i)(f_{i+1},r_{i+1}) to (\varphi(f_i,r_i)f_{i+1},r_{i+1})(f_i,r_i) which are equal by (4). Thus q(L)\in Q(G) is unchanged.

    Finally, consider a deformation in which two vertices are cancelled. In that case, they must be consecutive, say v_i,v_{i+1} , the relations r_i,r_{i+1} must be inverse to each other and the paths \ell_i,\ell_{i+1} must cross the same edges making f_i = f_{i+1} , since otherwise, the vertices are not allowed to cancel. So, (f_{i+1},r_{i+1}) = (f_i,r_i^{-1}) which cancels (f_i,r_i) in Q(G) by (5). So, q(L) is unchanged in all deformations.

    Conversely, let Q = (f_1, r_1) \cdots(f_n,r_n)\in Q(G) . We will construct the "standard partial picture" L_Q satisfying q(L_Q) = Q . An example of a standard picture is L_1 in Figure 6.

    1. Let w_i be the unique reduced word in the letters \mathcal{X}\coprod \mathcal{X}^{-1} represents f_i . Each r_i is already given as a (cyclically) reduced word. Let

    w(Q) = w_1r_1w_1^{-1}\cdots w_nr_n w_n^{-1}.

    2. Along the x -axis choose a sequence of points one for each letter in w(Q) and label these points with the letters of w(Q) .

    3. Connect the points labeled with the letters in r_i to a point v_i above these points with line segments labeled with the letters of r_i . Place a base point direction \ast above v_i . Then the word given by reading the edge labels counterclockwise around v_i staring at \ast will be r_i .

    4. From the points labeled with the letters in w_i , w_i^{-1} draw vertical lines going up labeled with the letters of w_i , w_i^{-1} . Above vertex v_i connect the lines from w_i to ones from w_i^{-1} with semicircles centered at v_i . Since all the loose edges in the upper half-plane have been closed off, this gives a partial picture L . We denote this L_Q and call it the standard partial picture corresponding to Q .

    Claim 2. q(L_Q) = Q .

    Claim 3. L_{q(L)}\simeq L .

    These two claims imply that Q\mapsto L_Q , L\mapsto q(L) give a 1-1 correspondence between deformation classes of partial pictures and the elements of Q(G) .

    Proof of Claim 2. This follows directly from the construction of L_Q . The straight line going up from each vertex v_i will cross the picture through semicircular edges labelled with the letters of w_i . The relation at v_i is r_i by construction. So q(L_Q) = (w_1,r_1)\cdots(w_n,r_n) = Q .

    Proof of Claim 3. Given a partial picture L with q(L) = Q , for example L_2 in Figure 6, a deformation of L to the standard picture L_Q is given by "pushing down" to the x -axis all edges outside a small nbd of the lines \ell_i . Since there are no vertices of L outside these neighborhoods, this deformation is allowed. The result is a standard partial picture for Q = q(L) . See Figure 7.

    Thus Q\leftrightarrow L_Q is a bijection as claimed.

    Figure 7.  Dotted lines \ell_1,\ell_2 are given by definition of q(L_2) . Take dashed lines parallel to \ell_1,\ell_2 and connected with small semicircles below vertices v_1,v_2 . Push the dashed line down to the x -axis. This gives an admissible deformation of L_2 (on the left) to L_{q(L_2)} (on the night). The dotted lines \ell_1,\ell_2 cross the same edges in both partial pictures.

    If the same letter, say x , occurs more than twice in a relation r , then, at the vertex v , the edge set E(x) cannot be a manifold. (For example, if G = \left<x\,|\, x^3\right> then E(x) will not be a manifold.) However, this does not happen in our case because our relations are "good".

    We define a good commutator relation to be a relation of the form

    r(a,b): = ab(bc_1,\cdots,c_ka)^{-1}

    where a,b,c_1,\cdots,c_k are distinct elements of \mathcal{X} and k\ge0 . The letters a,b will be called X-letters and the letters c_j will be called Y-letters in the relation. In the picture, the two X-letters in any commutator relation form the shape of the letter "X" since the lines labeled with these letters go all the way through the vertex. Call theses X-edges at the vertex. The edges labeled with the Y-letters go only half way and stop at the vertex. Call these Y-edges at the vertex. (See Figure 8.) In the definition of a picture we can choose the sets E_r\subset S^1 so that the points labeled a,a^{-1} (and b,b^{-1} ) are negatives of each other. Then the edge sets E(a),E(b) will be manifolds. (Since a,b,c_j are all distinct there are no other coincidences of labels at the vertices.)

    Figure 8.  The X-letters a,b have edge sets which are smooth at the vertex. The basepoint direction is on the negative side of both X-edges E(a),E(b) .

    We have the following trivial observation.

    Proposition 3.11. Suppose that G = \left<\mathcal{X}\,|\,\mathcal{Y}\right> is a group having only good commutator relations. Then, given any label x , the edge set E(x) in L is a disjoint union of smooth simple closed curves and smooth paths. At both endpoints of each path, x occurs as a Y-letter. It occurs as x at one end and x^{-1} at the other.

    Corollary 3.12. Suppose that G has only good commutator relations. Then, for any picture L for G and any label x , the number of vertices of L having x as Y-letter is equal to the number of vertices of L having x^{-1} as Y-letter.

    Let \mathcal{S} = (\beta_1,\cdots,\beta_m) be an admissible sequence of real Schur roots for a hereditary algebra \Lambda . Then G(\mathcal{S}) has only good commutator relations. We need the Atomic Deformation Theorem which says that every picture in G(\mathcal{S}) is a linear combination of "atoms". In other words atoms generate P(G) . The definition comes from [27] and [26] but is based on [23] where similar generators of P(G) are constructed for a torsion-free nilpotent group G .

    Suppose that \mathcal{S} is admissible and \alpha_\ast = (\alpha_1,\alpha_2,\alpha_3) is a sequence of three hom-orthogonal roots in \mathcal{S} ordered in such a way that ext(\alpha_i,\alpha_j) = 0 for i<j . Let \mathcal{A}(\alpha_\ast) be the rank 3 wide subcategory of mod\text-\Lambda with simple objects \alpha_\ast . One easy way to describe this category is

    \mathcal{A}(\alpha_\ast) = (^\perp M_{\alpha_\ast})^\perp

    where M_{\alpha_\ast} = M_{\alpha_1}\oplus M_{\alpha_2}\oplus M_{\alpha_3} . In other words, \mathcal{A}(\alpha_\ast) is the full subcategory of mod\text-\Lambda of all modules X having the property that {\rm Hom}(X,Y) = 0 = {\rm Ext}(X,Y) for all Y having the property that {\rm Hom}(M_{\alpha_\ast},Y) = 0 = {\rm Ext}(M_{\alpha_\ast},Y) . The objects of \mathcal{A}(\alpha_\ast) are modules M having filtrations where the subquotients are M_{\alpha_i} . Since ext(\alpha_i,\alpha_j) = 0 for i<j , the modules M_{\alpha_1} occur at the bottom of the filtration and M_{\alpha_3} occurs at the top of the filtration. Let wide(\alpha_\ast) denote the set of all dimension vectors of the objects of \mathcal{A}(\alpha_\ast) . The elements of wide(\alpha_\ast) are all nonnegative integer linear combinations of the roots \alpha_i . These are elements of the 3-dimensional vector space \mathbb{R}\alpha_\ast spanned by the roots \alpha_\ast .

    Let L(\alpha_\ast)\subseteq S^2 be the semi-invariant picture for the category \mathcal{A}(\alpha_\ast) . We recall ([27], [26], [19]) that L(\alpha_\ast) is the intersection with the unit sphere S^2\subseteq\mathbb{R}\alpha_\ast\cong \mathbb{R}^3 with the union of the 2-dimensional subset D(\beta) of \mathbb{R}\alpha_\ast where \beta\in wide(\alpha_\ast) given by the stability conditions:

    D(\beta): = \left\{x\in\mathbb{R}\alpha_\ast: \left < {x,\beta}\right > = 0, \left < {x,\beta'}\right > \ge 0\text{ for all $\beta'\subset \beta$, $\beta'\in wide(\alpha_\ast)$}\right\}

    When we stereographically project L(\alpha_\ast)\subset S^2 into the plane \mathbb{R}^2 we get a planar picture for the group G(wide(\alpha_\ast)) according to the definitions in this section.

    Definition 3.13. Let \mathcal{S},\alpha_\ast be as above. Then the atom A_\mathcal{S}(\alpha_\ast)\subset \mathbb{R}^2 is defined to be the picture for G(\mathcal{S}) given by taking the semi-invariant picture L(\alpha_\ast)\subset S^2 , stereographically projecting it away from the point -\sum \underline\dim\, P_i\in\mathbb{R}\alpha_\ast where P_i are the projective objects of \mathcal{A}(\alpha_\ast) and deleting all edges having labels x(\gamma) where \gamma\notin\mathcal{S} .

    Figure 9 gives an example of an atom. We need to prove that certain aspects of the shape are universal.

    Figure 9.  The atom A_\mathcal{A}(\alpha, \beta, \omega). There are three circles labeled \alpha, \beta, \omega. There is only one vertex (black dot) outside the brown circle labeled \omega. There is only one vertex inside the \alpha circle. The faint gray line is deleted since, in this example, its label is not in the set \mathcal{S}.

    Proposition 3.14. Any atom A_\mathcal{S}(\alpha_1,\alpha_2,\alpha_3) has three circles E(\alpha_i) = D(\alpha_i) with labels x(\alpha_i)\in G and all other edge sets have two endpoints. There is exactly one vertex v outside the \alpha_3 circle. This vertex has the relation r(\alpha_1,\alpha_2) . Dually, there is exactly one vertex inside the \alpha_1 circle with relation r(\alpha_2,\alpha_3)^{-1} .

    We use the notation r(\alpha,\beta) for r(x(\alpha),x(\beta)) For example, the blue lines in Figure 8 meet at two vertices giving the relations

    r(\alpha,\beta) = x(\alpha)x(\beta)\left(x(\beta)x(\gamma_1) x(\gamma_2)x(\alpha)\right)^{-1}

    at the top and r(\alpha,\beta)^{-1} in the middle of the brown x(\omega) circle.

    Proof. The only objects of \mathcal{A}(\alpha_\ast) which do not map onto M_{\alpha_3} are the objects of \mathcal{A}(\alpha_1,\alpha_2) which are the objects M_{\alpha_1},M_{\alpha_2} and their extensions M_{\gamma_j} . These give the terms in the commutator relation r(\alpha_1,\alpha_2) and these lines meet at only two vertices in the atom. All other edges of the atom have at least one abutting edge with a label \gamma where \gamma\twoheadrightarrow \alpha_3 . By the stability condition defining D(\gamma) , these points must be inside or on the \alpha_3 circle as claimed.

    We will prove the Sliding Lemma 3.17 and derive some consequences such as the Atomic Deformation Theorem 3.18 which says that every picture for G(\mathcal{S}) is a linear combination of atoms. First, some terminology. We say that L' is an atomic deformation of L if L' is a deformation of L plus a linear combination of atoms. Thus the Atomic Deformation Theorem states that every picture has an atomic deformation to the empty picture.

    Suppose that \mathcal{S} is an admissible set of roots with a fixed lateral ordering and let \omega\in \mathcal{S} . Recall that \mathcal{S}_-(\omega) is the set of all \beta\le \omega in lateral order in \mathcal{S} . In particular, either \beta = \omega or hom(\omega,\beta) = 0 and ext(\beta,\omega) = 0 . Also, \mathcal{R}_-(\omega) is the set of all \beta\in\mathcal{S}_-(\omega) which are hom-orthogonal to \omega . Since these are relatively closed subsets of \mathcal{S} , the picture groups G(\mathcal{S}_-(\omega)) and G(\mathcal{R}_-(\omega)) are defined. (See Remark 1.10.)

    \begin{align*} \mathcal{S}_-(\omega)&: = \{ \beta\in\mathcal{S}\,:\, \beta\le \omega\text{ in lateral order }\}\\ \mathcal{R}_-(\omega)&: = \{\beta\in\mathcal{S}_-(\omega)\,:\, hom(\beta,\omega) = 0\} \end{align*}

    for any \omega\in\mathcal{S} .

    Lemma 3.15 (Monomorphism Lemma). The homomorphism G(\mathcal{R}_-(\omega))\to G(\mathcal{S}_-(\omega)) induced by the inclusion \mathcal{R}_-(\omega)\hookrightarrow \mathcal{S}_-(\omega) has a retraction \rho given on generators by

    \rho(x(\beta)) = \begin{cases} x(\beta) & \mathit{\text{if}}\; \beta\in \mathcal{R}_-(\omega)\\ 1 & \mathit{\text{otherwise}} \end{cases}

    Furthermore, \rho takes pictures and partial pictures L for G(\mathcal{S}_-(\omega)) and gives a picture or partial picture \rho(L) for G(\mathcal{R}_-(\omega)) by simply deleting all edges with labels x(\beta) where \beta\notin \mathcal{R}_-(\omega) .

    Figure 11 gives an example of how this lemma is used. The proof is analogous to the proof of the dual statement which goes as follows. Recall that, for any \alpha in an admissible set of roots \mathcal{S} , \mathcal{S}_+(\alpha) is the set of all \beta\ge \alpha in \mathcal{S} and \mathcal{R}_+(\alpha) is the set of all \beta\in \mathcal{S}_+(\alpha) which are hom-orthogonal to \alpha . As in the case of \mathcal{S}_-(\omega),\mathcal{R}_-(\omega) these are relatively closed subsets of \mathcal{S} .

    Figure 11.  Illustrating proof of Atomic Deformation Theorem 3.18: \Sigma' (in red) is on the negative side of an innermost E(\omega) curve \Sigma (in blue). The picture L = L_0\cup L_1 , on the left, is deformation equivalent to the disjoint union of two pictures: L" = L_0\cup \rho(L_0') , in the middle, and L' = \rho(L_0)\cup L_1 on the right. The E(\omega) component \Sigma lies either in L' or L" . (Here it is in L" in the middle.) In either case, it can be removed by the Sliding Lemma 3.17.

    Lemma 3.16. The homomorphism G(\mathcal{R}_+(\alpha))\to G(\mathcal{S}_+(\alpha)) induced by the inclusion \mathcal{R}_+(\alpha)\hookrightarrow \mathcal{S}_+(\alpha) has a retraction \rho given on generators by

    \rho(x(\beta)) = \begin{cases} x(\beta) & \mathit{\text{if}} \;\beta\in \mathcal{R}_+(\alpha)\\ 1 & \mathit{\text{otherwise}} \end{cases}

    Furthermore, \rho takes pictures and partial pictures L for G(\mathcal{S}_+(\alpha)) and gives a picture or partial picture \rho(L) for G(\mathcal{R}_+(\alpha)) by simply deleting all edges with labels x(\beta) where \beta\notin \mathcal{R}_+(\alpha) .

    Proof. The key is that \mathcal{R}_+(\alpha) is given by a linear condition. Since ext(\alpha,\beta) = 0 for all \beta\in \mathcal{S}_+(\alpha) (and hom(\beta,\alpha) = 0 for all \beta\neq \alpha in \mathcal{S}_+(\alpha) ) we have:

    \mathcal{R}_+(\alpha) = \{\beta\in\mathcal{S}_+(\alpha)\,:\, \left < {g(\alpha),\beta}\right > = hom(\alpha,\beta)-ext(\alpha,\beta) = 0\}.

    Since any two letters in any relation in are linearly independent, if two letters in any relation in G(\mathcal{S}_+(\alpha)) lie in \mathcal{R}_+(\alpha) then all the letters in the relation lie in \mathcal{R}_+(\alpha) . Thus, if only part of the relation survives under the retraction it must be a single letter. This letter, say \gamma , cannot be a Y-letter: If it were and \gamma_1,\gamma_2 are the X-letters in that relation then hom(\alpha,\gamma_1) and hom(\alpha,\gamma_2) would both be nonzero. Since one of these is a subroot of \gamma , this would also make hom(\alpha,\gamma)\neq0 and \gamma\notin \mathcal{R}_+(\alpha) . So, none of the letters in such a relation will lie in \mathcal{R}_+(\alpha) . Therefore, the retraction \mathcal{S}_+(\alpha)\to \mathcal{R}_+(\alpha) sends relations to relations and induces a retraction of groups \rho:G(\mathcal{S}_+(\alpha))\to G(\mathcal{R}_+(\alpha)) .

    Given any picture or partial picture L for G(\mathcal{S}_+(\alpha)) , each vertex has a relation r which has the property that either \rho(r) = r or \rho(r) is an unreduced relation of the form xx^{-1} or \rho(r) is empty. In the second case \rho(r) = xx^{-1} we consider the vertex as part of the smooth curve E(x) . Removal of all edges with labels not in \mathcal{R}_+(\alpha) therefore keeps L looking locally like a picture for \mathcal{R}_+(\alpha) . But pictures and partial pictures are defined by local conditions.

    Using the Monomorphism Lemma 3.15, we can now state and prove the key lemma about pictures for G(\mathcal{S}) . Recall that E(\omega) is the union of the set of edges with label x(\omega) and that, for any root \beta\in\mathcal{R}_-(\omega) , any vertex with relation r(\beta,\omega) or r(\beta,\omega)^{-1} has Y-edges on the positive side of the X-line E(\omega) . (For example, in Figure 9, \alpha,\beta and all letters \gamma_i in r(\alpha,\beta) lie in \mathcal{R}_-(\omega) . So the edges corresponding to the commutator relations r(\gamma_i,\omega) for all letters \gamma_i in r(\alpha,\beta) lie in the interior of the brown circle E(\omega) = D(\omega) . Since Figure 9 is an atom, the edges are curved in the positive direction.) We also note that the base point direction is on the negative side of both X-lines at each crossing.

    Lemma 3.17 (Sliding Lemma). Suppose that L is a picture for G(\mathcal{S}) so that E(\omega) is a disjoint union of simple closed curves. Let U be one of the components of the complement of E(\omega) and let \Sigma = \overline U\cap E(\omega) be the boundary of the closure \overline U of U . Suppose that U is on the negative side of \Sigma and that all edges in L\cap U have labels x(\beta) for \beta\in\mathcal{R}_-(\omega) . Then there is an atomic deformation L\sim L' which alters L only in an arbitrarily small neighborhood V of \overline U so that L'\cap V contains no edges with labels \ge \omega in lateral order.

    Proof. By assumption, every edge which crosses \Sigma has a label x(\beta) where \beta\in\mathcal{R}_-(\omega) . This implies that all Y-edges at all vertices on \Sigma lie outside the region U . So, at each vertex of \Sigma , only one edge E(\beta) goes into the region U . Also, all basepoint directions of all vertices on \Sigma lie inside U .

    The proof of the lemma is by induction on the number of vertices in the region V containing \Sigma . Suppose first that this number is zero. Then \Sigma has no vertices and L\cap U is a union of disjoint simple closed curves which can be eliminated by concordance one at a times starting with the innermost simple closed curve. This includes \Sigma . The result has no edges with labels \ge\omega .

    Suppose next that L has vertices on the set \Sigma but no vertices in the region U enclosed by \Sigma . Then every edge of L in U is an arc connecting two vertices on \Sigma and the negative side of each arc has a path connecting the two basepoint directions at these two vertices. So, we can cancel all pair of vertices and we will be left with no vertices in V . As before, we can then eliminate all closed curves in V including \Sigma which has now become a union of simple closed curves.

    Finally, suppose that U contains a vectex v having relation r(\alpha,\beta)^\pm . So, v contributes \pm g\left<{r(\alpha,\beta)}\right> to the algebraic expression for L . Then \alpha,\beta\in\mathcal{R}_-(\omega) by assumption. Now add the atom \mp A(\alpha,\beta,\omega) (which resembles Figure 9) in the region containing the basepoint direction of v . (See the left side of Figure 10.) This adds \mp gA(\alpha,\beta,\omega) to the algebraic expression for L . The atom has a circle labeled x(\omega) oriented inward with exactly one vertex outside this circle with relation r(\alpha,\beta)^\mp (the mirror image of the relation at v ) by Proposition 3.14. The new vertex cancels the vertex v . (See the right side of Figure 10.) Repeating this process eliminates all vertices in the new region U' .

    Figure 10.  Illustrating proof of Sliding Lemma 3.17: \Sigma in blue is a disjoint union of E(\omega) closed curves which encloses a region \overline U = \Sigma\cup U . All Y-edges for vertices on \Sigma lie outside U . The atom \mathcal{A}(\alpha,\beta,\omega) in the proof has already been added on the left. The new region U' is the complement of the new \omega oval in U . The vertex v has been cancelled with the vertex in the atom on the right.

    After that, all edges in \overline U' , the closure of U' can be eliminated. This eliminates all edges with label \omega from V . However, it also introduces new edge sets (the interior of the \omega oval in the atom). However, these all have labels <\omega . So, we are done.

    Since the entire process was a sequence of picture deformations and addition of {\mathbb Z} G(\mathcal{S}) multiples of atoms, it is an atomic deformation.

    Theorem 3.18 (Atomic Deformation Theorem). Suppose that \mathcal{S} is an admissible set of real Schur roots. Then any picture for G(\mathcal{S}) has a null atomic deformation. I.e., it is deformation equivalent to a {\mathbb Z} G linear combination of atoms. Equivalently, the {\mathbb Z} G(\mathcal{S}) -module P(G(\mathcal{S})) is generated by atoms.

    This theorem follows from the Sliding Lemma and we will see that it implies Lemma C.

    Proof. Let \mathcal{S} = (\beta_1,\cdots,\beta_m) be an admissible set of roots. Let \beta^1,\cdots,\beta^m be the same set rearranged in lateral order. Let \mathcal{R}^k be the set of all elements of \mathcal{S} which are \le \beta^k in lateral order. Thus, \mathcal{R}^k = \mathcal{S}_-(\beta^k) . Take k minimal so that the labels which occurs in L all lie in \mathcal{R}^k . If k = 1 then L has no vertices and is a disjoint union of simple closed curves which are null homotopic. By induction, it suffices to eliminate \omega = \beta^k as a label from the picture L by picture deformations and addition of atoms without introducing labels \beta^j for j>k .

    Since \omega is a rightmost element in the set \mathcal{R}^k , x(\omega) does not occur as a Y-letter at any vertex of L . Therefore the edge set E(\omega) is a disjoint union of simple closed curves. Let \Sigma be innermost such curve and \Sigma' be a curve parallel to \Sigma on the negative side. (See Figure 11.) Then \Sigma' crosses on those edges E(\beta) where \beta\in \mathcal{S}_-(\omega) are hom-orthogonal to \omega . In other words, \beta\in \mathcal{R}_-(\omega) .

    Let L_0' be the mirror image of L_0 through \Sigma' . Then L_0\cup L_0' is null deformable, i.e., L_0+L_0' = 0 in the group of partial pictures Q(\mathcal{R}^k) . Since \Sigma' meets only edges with labels in \mathcal{R}_-(\omega) , we can apply the retraction \rho from the Monomorphism Lemma 3.15 to just one side of \Sigma' and still have a well-defined picture. This construction gives us two pictures: L' = \rho(L_0)\cup L_1 and L" = L_0\cup \rho(L_0') .

    Claim L is deformation equivalent to L'\coprod L" , i.e., L = L'+L" in the group \mathcal{P}(\mathcal{R}^k) .

    Pf: The group of pictures \mathcal{P}(\mathcal{R}^k) is a a subgroup of the group of partial pictures \mathcal{Q}(\mathcal{R}^k) and in that group we have:

    L = L_0+L_1 = L_0+\rho(L_0')+\rho(L_0)+L_1 = L"+L'

    since \rho(L_0')+\rho(L_0) = \rho(L_0+L_0') = \rho(0) = 0 .

    The simple closed curve \Sigma lies either in L' or L" . If \Sigma\subset L' then \Sigma can be removed by L' by an atomic deformation by the Sliding Lemma 3.17 since the edges inside \Sigma are in \mathcal{R}_-(\omega) , bing in \rho(L_0) . If \Sigma\subset L" (as drawn in Figure 11), the region outside \Sigma has all labels in \mathcal{R}_-(\omega) . So, it can be removed by Lemma 3.17. In both cases, the number of E(\omega) components in L'\coprod L" (the same as the number of components in L ) has been reduced by one by an atomic deformation without introducing any new labels \ge\omega . By induction on the number of components of E(\omega) , this set can be removed and k can be reduced by one. So, by induction on k , we are done. The entire picture can be deformed into nothing by atomic deformation.

    The proofs of Lemmas C and E are very similar.

    Proof of Lemma C. Suppose that w,w' are expressions for the same element of G(\mathcal{S}) and \pi(w) , \pi(w') are equal as words in the generators of G(\mathcal{S}_0) . This means that \pi(w^{-1}w') reduces to the trivial (empty) word in G(\mathcal{S}_0) .

    Let L be a partial picture giving the proof that w^{-1}w' is trivial in G(\mathcal{S}) . Then \pi(L) can be completed to a true picture L_0 for the group G(\mathcal{S}_0) by joining together cancelling letters in \pi(w^{-1}w') . By the Atomic Deformation Theorem 3.18, L_0 is equivalent to a sum of atoms. However, each atom A for G(\mathcal{S}_0) can be lifted to an atom \tilde A for G(\mathcal{S}) by definition of the atoms. Therefore, up to deformation equivalence, L can be lifted to a picture \tilde L for G(\mathcal{S}) . By Corollary 3.12, the number of vertices of \tilde L having x(\beta_m) as Y-letter is equal to the number of vertices having x(\beta_m)^{-1} as Y-letter. This implies that the number of vertices in L_0 lifting to ones in \tilde L having x(\beta_m)^{-1} as Y-letter is equal to the number of vertices in L_0 lifting to ones in \tilde L having x(\beta_m)^{-1} as Y-letter are equal. So, the number of times x(\beta_m),x(\beta_m)^{-1} occur as Y-letters in L are equal. So, the number of times that x(\beta_m),x(\beta_m)^{-1} occur in the word w^{-1}w' are equal. So, x(\beta_m) occurs the same number of times in the words w,w' as claimed.

    Proof of Lemma E. Recall that \beta_m is the last element of an admissible set \mathcal{S} . Lemma E says that if w_0 is a positive expression for some element of G(\mathcal{S}) which commutes with x(\beta_m) then every letter of w_0 commutes with \beta_m . To prove this, suppose not and let w_0 be a minimal length positive expression in the letters \mathcal{S} satisfying the following.

    1. As an element of G(\mathcal{S}) , w_0 commutes with x(\beta_m) .

    2.One of the letters of w_0 , say x(\beta) , does not commute with x(\beta_m) . Equivalently, \beta,\beta_m are not hom-orthogonal (Remark 1.21).

    Clearly, w_0 has at least 2 letters and the first and last letter of w_0 do not commute with x(\beta_m) .

    In the group G(\mathcal{S}) we have the relation

    W = w_0 x(\beta_m) w_0^{-1}x(\beta_m)^{-1} = 1.

    A proof of the relation W = 1 gives a partial picture L for G(\mathcal{S}) having the word W as it boundary. Let \beta^1,\cdots,\beta^m be the letters in \mathcal{S} in lateral order. Then \beta_m = \beta^k for some k . Let \beta^i,\beta^j be the letters which occurs in the partial picture L with i minimal and j maximal. Then i<j and i\le k\le j . In particular, either i< k or k<j . By symmetry we may assume that k<j . Then we will use the Monomorphism Lemma 3.15 for \omega = \beta^j\neq \beta_m . (For k = j the argument is the same using the dual lemma 3.16 with \alpha = \beta^i .)

    There are two cases. Either \lambda = \beta^j is a letter in W or not.

    Case 1. \lambda is not a letter in W . Then the edge set E(\lambda) is a disjoint union of simple closed curves. We claim that these can all be eliminated by Lemmas 3.15 and 3.17. Let \Sigma be any component of E(\lambda) . Let \Sigma' be a parallel curve on the negatives side of \Sigma . Then \Sigma' crosses only edges E(\beta) where \beta is hom-orthogonal to \lambda . Therefore, we can apply the retraction \rho:G(\mathcal{S}_-(\lambda))\to G(\mathcal{R}_-(\lambda)) to the region enclosed by \Sigma' to eliminate all edges in that region which are not hom-orthogonal to \lambda . By the Sliding Lemma 3.17 we can then eliminate \Sigma if it is still there. Repeating this process produces a new partial picture L' with boundary W so that the laterally rightmost letter in L' is a letter in W , i.e., we are reduced to Case 2.

    Case 2. \lambda = \beta^j is a letter in W . Since j>k , \lambda is then a letter in w_0 . The generator x(\lambda) may occur several times in w_0 and x(\lambda)^{-1} occurs in w_0^{-1} . Taking the first occurrence of x(\lambda) in w_0 we can write w_0 = w_1x(\lambda)w_2 there x(\lambda) is not a letter in w_1 . Then

    W = w_1x(\lambda)w_2 x(\beta_m)w_2^{-1}x(\lambda)^{-1}w_1^{-1}x(\beta_m)^{-1}

    is the boundary of L which is a partial picture for G(\mathcal{S}_-(\lambda)) . Since \lambda is rightmost in later order, x(\lambda) does not occur as a Y-letter at any of the vertices of L . Therefore, the edge set E(\lambda) is a disjoint union of simple closed curves and disjoint arcs connecting the x(\lambda) in w_0 to the x(\lambda)^{-1} in w_0^{-1} . Since these arc are disjoint, the outermost such arc \Sigma connects the first occurrence of x(\lambda) in w_0 to the last occurrence of x(\lambda)^{-1} in w_0^{-1} . Let \Sigma' be an arc parallel to \Sigma on its negative side. Thus L = L_0\cup L_1 where L_0 is the portion of L enclosed by \Sigma' . Since x(\lambda) is to the left of x(\lambda)^{-1} , \Sigma\subset L_0 . (See the left side of Figure 12.)

    Figure 12.  (Proof of Lemma E) The partial picture L for G(\mathcal{S}_-(\lambda)) is divided into two parts L = L_0\cup L_1 by \Sigma' . Applying \rho:G(\mathcal{S}_-(\lambda))\to G(\mathcal{R}_-(\lambda)) to L_0 eliminates x(\lambda) from the word w_0 = w_1x(\lambda)x_2 but does not eliminage x(\beta_m) . Then w_1\rho(w_2) commutes with x(\beta_m) contradicting the minimality of w_0 .

    Using the Monomorphism Lemma 3.15, we apply the retraction \rho to L_0 . This will eliminate \Sigma and all occurrences of the letter x(\lambda) in W giving a new relation:

    w_1\rho(w_2) \rho(x(\beta_m)) \rho(w_2)^{-1}w_1^{-1} x(\beta_m)^{-1} = 1

    or, equivalently, w_1\rho(w_2) \rho(x(\beta_m)) = x(\beta_m)w_1\rho(w_2) . By Lemma C proved above, x(\beta_m) occurs the same number of times in these two expressions. So, \rho(x(\beta_m)) = x(\beta_m) . In particular, \lambda is hom-orthogonal to \beta_m . Equivalently x(\lambda) commutes with x(\beta_m) . So, x(\lambda) is not the first letter of w_0 which means w_1 is a nontrivial word.

    This gives a new word w_0' = w_1 \rho(w_2) which is shorter than w_0 , commutes with x(\beta_m) and has at least one letter (the first letter of w_1 ) which does not commute with x(\beta_m) . This contradicts the minimality of w_0 and completes the proof of Lemma E.

    This Appendix contains basic background material for this paper. Details can be found in [25] and [20]

    We assume throughout the paper that Q is a quiver without loops, oriented cycles or multiple edges i\to j (since multiplicity of edges is included in the valuation). We recall briefly that a valuation on a quiver Q is given by assigning positive integers f_i to each vertex i and pairs of positive integers (d_{ij},d_{ji}) to every arrow i\to j in Q having the property that f_id_{ij} = f_jd_{ji} . For example, the Kronecker quiver is \bullet\xrightarrow{(2,2)} \bullet . A \underline{K} -modulation of a valued quiver is given by assigning a division algebra F_i of dimension f_i at each vertex and an F_i\text-F_j -bimodule M_{ij} on each arrow i\to j with \dim_KM_{ij} = f_id_{ij} = f_jd_{ji} . A representation of a modulated quiver consists of a right F_i -vector space V_i at each vertex and an F_j -linear map V_i\otimes M_{ij}\to V_j on each arrow i\to j . A representation V is called a brick if its endomorphism ring is a division algebra. An exceptional module is a brick having no self-extensions. For hereditary algebras of finite type, all bricks are exceptional.

    Given any module X we denote by X^\perp the full subcategory of mod\text-\Lambda with all objects Y so that

    {\rm Hom}_\Lambda(X,Y) = 0 = {\rm Ext}_\Lambda(X,Y)

    Similarly, ^\perp X is the category of all \Lambda -modules Y so that X\in Y^\perp . An exceptional sequence of length k is defined to be a sequence of exceptional modules E_1,E_2,\cdots, E_k so that E_i\in E_j^\perp for all i<j .

    The dimension vector \underline\dim\, V of a representation of a modulated quiver is defined to be (d_1,d_2,\cdots,d_n) where d_i is the dimension of V_i as a vector space over F_i . A real Schur root of the valued quiver Q is defined to be the dimension vector of an exceptional module for any modulation of Q . This concept is known to be independent of the choice of modulation. See [25] for details. In this paper we assume a modulation is given.

    The semi-stability set D(V) of any module V is defined by

    D(V): = \{x\in\mathbb{R}^n\,:\, \left < {x,\underline\dim\, V}\right > = 0\text{ and } \left < {x,\underline\dim\, V'}\right > \le 0\text{ for all submodules } V'\subset V\}

    where we use the bilinear pairing:

    \left < {x,y}\right > = \sum x_iy_if_i.

    For any real Schur root \beta let D(\beta) = D(M_\beta) where M_\beta is the unique exceptional module with dimension vector \beta . In this paper we use the following refinement of the definition of D(\beta) which is essentially proved in [25].

    Theorem 4.1. For \beta a real Schur root and x\in \mathbb{R}^n so that \left<x,\beta\right> = 0 , the following are equivalent.

    1. \left<{x,\beta'}\right>\le 0 for all real Schur subroots \beta' of \beta .

    2. \left<{x,\underline\dim\, V'}\right>\le0 for all submodules V\subseteq M_\beta .

    3. \left<{x,\underline\dim\, V"}\right>\ge0 for all quotient modules V" of M_\beta .

    4. \left<{x,\beta"}\right>\ge0 for all real Schur quotient roots of \beta .

    Proof. It is shown in [25] that (1) is equivalent to (2) for x\in {\mathbb Z}^n . This easily implies that (1) and (2) are equivalent for x\in \mathbb{Q}^n . Taking the closure we get that (1) and (2) are equivalent for all x\in\mathbb{R}^n .

    The equivalence (2)\Leftrightarrow (3) is obvious. The equivalence (3)\Leftrightarrow(4) follows from the equivalence (1)\Leftrightarrow(2) . Indeed, applying the duality functor D = {\rm Hom}(-,K) , the exceptional \Lambda -module M_\beta and quotient module M_{\beta"} become exceptional D\Lambda modules with the same dimension vectors, but DM_{\beta"}\subset DM_\beta . So, x\in \mathbb{R}^n satisfies (4) for \Lambda if and only if \left<{-x,\beta"}\right>\le 0 for \beta"\subset \beta (as D\Lambda -roots). Equivalently, x\in D_\Lambda(\beta) using the criteria (1), (2) if and only if -x\in D_{D\Lambda}(\beta) using the quotient root criteria (4), (3) respectively. So (3)\Leftrightarrow(4) .

    Following [20], we use g -vectors and modified dot product in this paper instead of the Euler product used in [25]. and we define the \underline{g} -vector of a module X to be

    g(X): = \underline\dim\, P_0/rad\,P_0-\underline\dim\, P_1/rad\,P_1

    where

    0\to P_1\to P_0\to X\to 0

    is the minimal projective presentation of X . Equivalently, g(X) = C_\Lambda^{-1}\underline\dim\, X where C_\Lambda is the Cartan matrix of \Lambda .

    Lemma 4.2. The g -vector of X satisfies the following for any representation V .

    \left < {g(X),\underline\dim\, V}\right > = \dim_K{\rm Hom}_\Lambda(X,V)-\dim_K{\rm Ext}_\Lambda(X,V).

    In particular, \left<{g(X),\underline\dim\, V}\right> = 0 when X\in\,^\perp V .

    Proof. This follows from the exact sequence:

    0\to {\rm Hom}_\Lambda(X,V)\to {\rm Hom}_\Lambda(P_0,V) \to {\rm Hom}_\Lambda(P_1,V)\to {\rm Ext}_\Lambda(X,V)\to 0

    and the evident fact that \dim_K{\rm Hom}_\Lambda(P,V) = \left<{g(P),\underline\dim\, V}\right> .

    This immediately gives the following.

    Proposition 4.3. The dimension vectors of modules in an exceptional sequence are linearly independent.

    Proof. Suppose that E_1,\cdots,E_k is an exceptional sequence. Lemma 4.2 implies

    \left < {g(E_j),\underline\dim\, E_i}\right > = 0

    for all i<j . But \left<{g(E_j),\underline\dim\, E_j}\right> = \dim_K {\rm End}_\Lambda(E_j)\neq0 . So, \underline\dim\, E_j cannot be a linear combination of \underline\dim\, E_i for I<j .

    The g -vector of a shifted projective module P[1] is define by g(P[1]): = -g(P) .

    We have the following "Virtual Stability Theorem" from [25].

    Theorem 4.4. If X\in\,^\perp M_\beta then g(X)\in D(\beta) . If P\in\,^\perp M_\beta is projective then g(P[1]) = -g(P)\in D(\beta) . Conversely, for any x\in D(\beta)\cap {\mathbb Z}^n there is a module X and a projective module P so that

    1. x = g(X\oplus P[1]) = g(X)-g(P) .

    2. X,P\in\,^\perp M_\beta , i.e., {\rm Hom}(X\oplus P,M_\beta) = 0 = {\rm Ext}(X,M_\beta) .

    Recall that a full subcategory \mathcal{W} of an abelian category \mathcal{A} is wide if it is closed under extension and kernels and cokernels of morphism between objects. This implies in particular that \mathcal{W} is closed under taking direct summands.

    Returning to the case of mod\text-\Lambda for a hereditary algebra \Lambda , we note that X^\perp is a wide subcategories for any object X . To see this, look at the following six term exact sequence for any short exact sequence 0\to A\to B\to C\to 0 .

    \begin{equation*} \begin{split} 0\to{\rm Hom}(X,A)\to\ & {\rm Hom}(X,B)\to {\rm Hom}(X,C)\to \\ &{\rm Ext}(X,A)\to{\rm Ext}(X,B)\to{\rm Ext}(X,C)\to0 \end{split} \end{equation*}

    If A,C\in X^\perp then we see that B\in X^\perp . If B\in X^\perp then {\rm Hom}(X,A) = 0 = {\rm Ext}(X,C) . So, any object which is both a subobject and quotient object of an object of X^\perp is also in X^\perp . So, X^\perp is a wide subcategory of mod\text-\Lambda . Similarly, ^\perp X is a wide subcategory.

    Closely related to this example is the following well-known fact. (See [20] for a short proof.)

    Theorem 4.5. Let R be any subset of \mathbb{R}^n . Then the set \mathcal{W}(R) of all representation V so that R\subset D(V) is a wide subcategory of mod\text-\Lambda .

    Consider the case when R = \{x_0\} is a single point x_0\neq0\in \mathbb{R}^n . Suppose that \mathcal{S} is an admissible set of real Schur roots. Recall our notation that D(\beta) = D(M_{\beta}) where M_{\beta} is the unique exceptional module with dimension vector \beta .

    What can we say about the set of \beta \in \mathcal{S} so that x_0\in D(\beta) ?

    Proposition 4.6. Let \alpha\in \mathcal{S} . Then x_0 is in the interior of D(\alpha) if and only if M_{\alpha} is a minimal object of the wide subcategory \mathcal{W}(x_0) .

    Proof. If x_0 lies in the interior of D(\alpha) , \left<{x_0,\gamma}\right><0 for all subroots \gamma\subsetneq \alpha . So, x_0\notin D(\gamma) . So, \alpha is minimal. The converse follows in the same way.

    A wide subcategory \mathcal{W}\subset mod\text-\Lambda has rank \underline{k} if it is isomorphic to the module category of an hereditary algebra with k simple modules. More concretely, such a wide subcategory contains k {\rm Hom} -orthogonal exceptional modules forming an exceptional sequence: X_1,X_2,\cdots,X_k . In other words, {\rm Ext}(X_j,X_i) = 0 for j\ge i . And all other objects of \mathcal{W} are iterated extensions of the X_i with each other. From this description we see that the X_i are objects of \mathcal{W} of minimal length, i.e., proper subobjects and proper quotient objects of the X_i do not lie in \mathcal{W} . In particular, the X_i are uniquely determined by \mathcal{W} . In general, not every wide subcategory of mod\text-\Lambda has finite rank. For example, when \Lambda has infinite representation type, the subcategory of regular modules is a wide subcategory of infinite rank since the Auslander-Reiten translation functor \tau is an automorphism on this subcategory.

    One special case of a finite rank wide subcategory which we need in this paper is the case k = n .

    Theorem 4.7. Let (E_1,\cdots,E_n) be an exceptional sequence of {\rm Hom} -orthogonal objects in mod\text-\Lambda . Then all E_i are simple. In particular, mod\text-\Lambda is the only wide subcategory of rank n .

    Proof. This follows from the theory of exceptional sequences. By [9] and [36], the action of the braid group on n strands acts transitively on the set of exceptional sequences of length n . However, by definition, braid moves keep objects in the same wide subcategory which is the category of all objects which are iterated extensions of the E_i with each other. By the theorem of [9] and [36], this includes all exceptional sequences. But the sequence of simple modules of mod\text-\Lambda forms an exceptional sequence. So, every simple \Lambda -module is in our wide subcategory. So, the wide subcategory is all of mod\text-\Lambda . Since the E_i are minimal objects, they must all be simple.

    Let \alpha_1,\cdots,\alpha_k be real Schur roots so that (M_{\alpha_1},\cdots,M_{\alpha_k}) is a sequence of {\rm Hom} -orthogonal sequence of modules forming an exceptional sequence. Then we denote by \mathcal{A}(\alpha_1,\cdots,\alpha_k) , or \mathcal{A}(\alpha_\ast) for short, the wide subcategory of mod\text-\Lambda generated by the modules M_{\alpha_i} . As remarked above, this is a rank k wide subcategory whose objects have a filtration with subquotients M_{\alpha_i} . Another description is:

    \mathcal{A}(\alpha_1,\cdots,\alpha_k) = \,^\perp\left( (M_{\alpha_1}\oplus\cdots\oplus M_{\alpha_k})^\perp\right)

    In other words, \mathcal{A}(\alpha_\ast) = \,^\perp (E_1\oplus\cdots\oplus E_{n-k}) for any choice of a complete exceptional sequence (E_1,\cdots,E_{n-k},M_{\alpha_1},\cdots,M_{\alpha_k}) ending in the M_{\alpha_i} .

    Here is another well-known fact that we need.

    Theorem 4.8. The wide subcategory \mathcal{W} = \mathcal{A}(\alpha_1,\cdots,\alpha_k) described above contains the exceptional module M_\beta if and only if \beta is a nonnegative linear combination of the \alpha_i .

    Proof. Necessity of this condition is clear since all objects of \mathcal{W} are iterated extensions of the modules M_{\alpha_i} . For the converse, we choose an extension of this sequence to a complete exceptional sequence (E_1,\cdots,E_{n-k},M_{\alpha_1},\cdots,M_{\alpha_k}) . Then \mathcal{W} = \,^\perp(E_1\oplus\cdots\oplus E_{n-k}) . By Theorem 4.4, an exceptional module M_\beta lies in \mathcal{W} if and only if g(\beta)\in \bigcap_jD(E_j) . But this is a convex set. Since this condition holds for the roots \alpha_i , it holds for any nonnegative linear combination of the \alpha_i .

    For an admissible set of roots \mathcal{S} , this theorem and Proposition 4.6 imply the following.

    Corollary 4.9. For x_0\neq0\in\mathbb{R}^n , let \alpha_1,\cdots,\alpha_k be the elements of \mathcal{S} for which M_{\alpha_i} is minimal in \mathcal{W}(x_0) = \{M\,:\,x_0\in D(M)\} . Then, \mathcal{S}\cap \mathcal{W}(x_0) is the set of elements of \mathcal{S} which are sums of these roots ( \beta = \sum n_i\alpha_i for n_i\ge0 ).

    Proof. Let \beta\in \mathcal{S}\cap \mathcal{W}(x_0) . So, x_0\in D(\beta) . If \beta is not one of the \alpha_i then, by Proposition 4.6, x_0\in \partial D(\beta) . This implies that x_0\in D(\gamma) for a subroot \gamma\subsetneq \beta . It follows that x_0\in D(\gamma') for all components \gamma' of the quotient root \beta-\gamma . These subroots and quotient roots of \beta all lie in \mathcal{S} since \mathcal{S} is admissible. By induction on the length of \beta we conclude that each \gamma,\gamma' is a nonnegative linear combination of the \alpha_i . So, the same holds for their sum \beta .

    Conversely, suppose \beta\in\mathcal{S} has the form \beta = \sum n_i\alpha_i for n_i\ge0 . Since \mathcal{S} is admissible, the modules M_{\alpha_1},\cdots,M_{\alpha_k} are {\rm Hom} -orthogonal and form an exceptional sequence (being in lateral order). By Theorem 4.8, M_\beta lies in the wide subcategory \mathcal{W}(x_0) as claimed.

    The authors thank Thomas Brüstle, Eric Hanson, Steve Hermes, Moses Kim, Kent Orr and Jerzy Weyman for numerous discussions about "pictures" and their relation to maximal green sequences. The first author acknowledges support of the Simons Foundation. Both authors are grateful to the referees for numerous very helpful comments and also for their interest in the history of this subject.



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