Deleting or adding arrows of a bound quiver algebra and Hochschild (co)homology
Claude Cibils, Marcelo Lanzilotta, Eduardo N. Marcos, Andrea Solotar

TL;DR
This paper investigates how the Hochschild (co)homology of bound quiver algebras varies with modifications to the quiver, such as adding or deleting arrows, using advanced homological tools.
Contribution
It provides a detailed description of the changes in Hochschild (co)homology under quiver modifications employing relative Hochschild (co)homology and the Jacobi-Zariski sequence.
Findings
Describes the impact of arrow modifications on Hochschild (co)homology.
Utilizes the Jacobi-Zariski long exact sequence for analysis.
Employs a one-step relative projective resolution of tensor algebras.
Abstract
We describe how the Hochschild (co)homology of a bound quiver algebra changes when adding or deleting arrows to the quiver. The main tools are relative Hochschild (co)homology, the Jacobi-Zariski long exact sequence obtained by A. Kaygun and a one step relative projective resolution of a tensor algebra.
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Deleting or adding arrows of a bound quiver algebra and Hochschild (co)homology
Claude Cibils, Marcelo Lanzilotta, Eduardo N. Marcos,
and Andrea Solotar This work has been supported by the projects UBACYT 20020130100533BA, PIP-CONICET 11220150100483CO, USP-COFECUB. The third mentioned author was supported by the thematic project of FAPESP 2014/09310-5 and acknowledges support from the ”Brazilian-French Network in Mathematics”. The fourth mentioned author is a research member of CONICET (Argentina) and a Senior Associate at ICTP.
Abstract
We describe how the Hochschild (co)homology of a bound quiver algebra changes when deleting or adding arrows to the quiver. The main tools are relative Hochschild (co)homology, the Jacobi-Zariski long exact sequence obtained by A. Kaygun and a length one relative projective resolution of tensor algebras.
2010 MSC: 18G25, 16E40, 16E30, 18G15
Keywords: Hochschild, cohomology, homology, relative, quiver, arrow
1 Introduction
Hochschild (co)homology has been widely studied for algebras presented by quivers and relations, that is for bound quiver algebras. The main purpose of this work is to make precise how the Hochschild (co)homology changes when deleting or adding arrows.
In 1956 G. Hochschild [24] introduced a relative (co)homological theory, which amounts to consider an exact category, see [29, 7]. This theory has been used rarely, in part because of a lack of relation with the usual (co)homological theory given in [23]. Nevertheless, for an extension of algebras such that is a projective -bimodule, A. Kaygun has established in 2012 [25, 26] a Jacobi-Zariski long exact sequence connecting both theories. Note that M. Auslander and Ø. Solberg have considered relative homological algebra, see [4] and [33].
In Section 2 we provide an account of the relative (co)homological theory and we show that for a tensor algebra there is a relative projective resolution of length one.
An inert arrow of a bound quiver algebra is an arrow of the quiver which is not involved in a minimal set of relations of . Our main result in Section 3 is that deleting a set of inert arrows does not change the Hochschild homology in degrees greater or equal than .
On the other hand in Section 4 we provide formulas for Hochschild cohomology, also when deleting inert arrows of a bound quiver algebra. For degrees greater or equal than , the change of dimension is expressed in terms of the dimensions of vector spaces between indecomposable injective and projective modules, with multiplicities given by the dimensions of some relative paths that we introduce in Section 4.
The proofs rely on the reverse procedure, that is on adding arrows. This way we obtain a tensor algebra over the original algebra for a suitable projective bimodule. This algebra is finite dimensional if and only if adding arrows does not create relative cycles. In case of adding just one arrow, which does not leads to a relative cycle, the tensor algebra is a trivial extension which has been already considered in [17]. In this paper E.L. Green, C. Psaroudakis and Ø. Solberg study this operation in relation to the finitistic dimension conjecture.
In Section 5 we apply our results to the amalgamation of a bound quiver algebra with a quiver without oriented cycles. In this section we also consider Hochschild cohomology of Gorenstein algebras, by adding arrows to its quiver.
The results that we obtain in this paper are in the framework of replacing an algebra by a closely related algebra, towards producing algorithmic ways for computing Hochschild (co)homology. Other work in this direction can be found for instance in [5, 6, 9, 10, 15, 16, 18, 22, 27, 28]. Hochschild (co)homology has been also considered for bound quiver algebras in relation to their representations and their deformations, see for instance [19, 21, 22, 32].
Hochschild (co)homology is a derived invariant, see for instance [30]. M. Gerstenhaber has shown in [14] that Hochschild (co)homology affords additional structure: cup and cap products, and the Gerstenhaber bracket. Together with Connes’ differential this constitutes the differential calculus, or Tamarkin-Tsygan calculus of an algebra, see for instance [34, 11]. This theory is also a derived invariant, see [1, 2]. It should be interesting to describe the effect of deleting an inert arrow of a bound quiver algebra on its differential calculus.
2 Relative Hochschild (co)homology and tensor algebras
Let be a field and let be an extension of -algebras. Modules are left modules.
An -module is relative projective if for any -morphism with a -section, and any -morphism , there exists an -morphism such that . The category of -modules is an exact category with respect to the short exact sequences which are -split, see [7]. As mentioned in [7], these notions are commonly attributed to D. Quillen [29]. The projective objects of this exact category (see [7, Definition 11.1]) are the relative projective modules.
An -module is induced if it is isomorphic to , where is a -module. As proved by Hochschild in [24], a module is relative projective if and only if it is isomorphic to a direct summand of an induced module.
Definition 2.1
[24]** A relative projective resolution of an -module is a complex
[TABLE]
where is relative projective for all and there exists a -contracting homotopy, that is there exist -maps of degree such that .
It can be easily shown that relative projective resolutions are the projective resolutions in the exact category with respect to -split short exact sequences, see [7, Definition 12.1]. The usual comparison theorem holds for relative projective resolutions, see [24, p. 250] and [7, Theorem 12.4]. Hence the following definitions do not depend, up to isomorphism, on the choice of a relative projective resolution.
Definition 2.2
Let and be -modules and let be a relative projective resolution. The cohomology of the cochain complex
[TABLE]
is .
Let be a left -module and let be a right -module. Let be a relative projective resolution. The homology of the chain complex
[TABLE]
is .
Next we recall the relative theory provided by Hochschild in [24] for bimodules.
Let and be -algebras. The category of -bimodules is identified with the category of -modules. A projective -bimodule is a projective -module.
Definition 2.3
Let be an -bimodule. The relative Hochschild cohomology and homology of respect to with coefficients in are respectively the graded vector spaces
[TABLE]
[TABLE]
There is a relative bar resolution of which provides the subsequent way of computing relative Hochschild (co)homology, see [24]. As mentioned in the Introduction, Kaygun obtained long exact sequences relating the usual Hochschild (co)homology with the relative one, see [25, 26].
Let be a -algebra and let be a -bimodule. The *tensor algebra *
[TABLE]
is a non negatively graded algebra with and for . Its positive part is .
Example 2.4
Let be a finite quiver, with set of vertices , set of arrows , and the maps which associate to each arrow respectively its source and target vertices. The path algebra is the tensor algebra over the semisimple commutative algebra of the -bimodule . We denote by the set of paths of length , note that .
A bound quiver algebra is an algebra , where is an admissible ideal, that is for some .
Let be an algebraically closed field. By results of P. Gabriel in [12, 13], see also for instance [3, Theorem 3.7] or [31], a finite dimensional -algebra is Morita equivalent to a bound quiver algebra.
We recall the universal property of a tensor algebra . Let be a -algebra. An algebra morphism is uniquely determined by an algebra morphism - which turns into a -bimodule - and a -bimodule morphism .
Theorem 2.5
Let be the tensor algebra over a -algebra of a -bimodule . Let be a -bimodule. For ,
[TABLE]
[TABLE]
Proof. We will show that the following is a relative projective resolution of :
[TABLE]
where is the product of and We obtain the results of the statement by using this relative resolution to compute Hochschild (co)homology.
It is straightforward to verify that . Clearly the involved -bimodules are induced, hence they are relative projective.
In order to define a -contracting homotopy, we introduce notation. Firstly, instead of we will write . Secondly observe that the tensor element can be considered in different ways: for any decomposition with and , it can be viewed as an element of
[TABLE]
In this case we write this element as For and we remark that the notation is:
[TABLE]
[TABLE]
Finally for with and , the tensor can also be considered as an element of
[TABLE]
In this case we denote it by . For and we write:
[TABLE]
[TABLE]
With these notations the morphisms and are as follows:
[TABLE]
[TABLE]
The sequence (2.1) is graded, it is the direct sum of the following sequences of -bimodules:
[TABLE]
Next we define and and we prove that these maps verify the following:
- •
and are -bimodule maps,
- •
and ,
- •
providing this way the required contracting homotopy, see Definition 2.1.
The morphism is defined by , note that it is well defined. Moreover is easily seen to be a -section of .
In order to define , let , with . Let
[TABLE]
be given by
[TABLE]
Observe that . Each is a well defined -morphism. We put . Next we verify that .
[TABLE]
Finally we verify that .
[TABLE]
[TABLE]
In particular
3 Homology
Let be a bound quiver algebra, and let be a minimal finite subset of the path algebra such that . Note that elements are possibly linear combination of parallel paths, that is of paths with the same source and the same target vertices, see for instance [3].
Definition 3.1
Let be a bound quiver algebra. An arrow of is inert if does not appear in any of the paths which provide the elements of .
Let be a set of inert arrows, let be the quiver where the arrows of are deleted. We set
[TABLE]
where the denominator is the two sided ideal generated by in . Note that is a bound quiver algebra. Moreover is a subalgebra of .
Theorem 3.2
Let be a bound quiver algebra and let be a set of inert arrows of . For
[TABLE]
The proof will rely on the reverse procedure, namely adding new arrows.
Definition 3.3
Let be a quiver and let be a finite set of new arrows, that is is a finite set with maps . The new quiver is given by and , where the source and target maps are provided by the corresponding maps of and .
Let be a bound quiver algebra, and let be a set of new arrows. We set
[TABLE]
Remark 3.4
Suppose that is finite dimensional. Obviously the set of arrows is inert and .
If is a bound quiver algebra and is a set of inert arrows, then .
Given a bound quiver algebra and a set of new arrows , consider the projective -bimodule
[TABLE]
The following result is clear by using the universal property of tensor algebras.
Theorem 3.5
Let be a bound quiver algebra, and let be a set of new arrows. The algebra is isomorphic to the tensor algebra .
Theorem 3.6
Let be a bound quiver algebra, and let be a set of new arrows. For
[TABLE]
Proof. By the previous result, . The -bimodule is projective, hence the Jacobi-Zariski long exact sequence for Hochschild homology obtained by Kaygun holds, see [25, 26]. On the other hand, by Theorem 2.5 we have that for . Then for . Moreover . The second summand is zero since the -bimodule of coefficients is projective.
4 Cohomology
In case of deleting one inert arrow we will obtain the following result. Note that for a right module, we denote by the left module .
Theorem 4.1
Let be a bound quiver algebra, let be an inert arrow from to and let . For we have
[TABLE]
See Remark 4.3 for a proof of the previous result.
Next we state a result for a set of deleted arrows. As in the previous section, the proof will be by the reverse procedure of adding arrows. However the Jacobi-Zariski long exact sequence for cohomology requires that the bimodule of coefficients is finite dimensional. To ensure this, and to state the result, we introduce the following.
Let be a bound quiver algebra, let be a set of inert arrows and let , see (3.1).
A pair of arrows of is linked if .
- -
A relative -path is a sequence of arrows of such that is linked for . The source and the target of are respectively and .
- -
The set of relative -paths is denoted , while the set of all relative paths is denoted .
- -
The relative path is a relative cycle if is linked. This way an arrow is a relative cycle if is linked, that is if .
- -
We set
[TABLE]
If , then .
We will prove the following as a consequence of Theorem 4.6.
Theorem 4.2
Let be a bound quiver algebra, let be a set of inert arrows and let . For we have
[TABLE]
Remark 4.3
The proof of Theorem 4.1 follows: if , then there is only one relative path . The formula above gives
[TABLE]
Moreover, at the end of this section we will prove that
[TABLE]
We first prove the following.
Proposition 4.4
Let be a bound quiver algebra, let be a set of new arrows and let be the associated projective -bimodule, see (3.2). We have
[TABLE]
The algebra is finite dimensional if and only if the length of the relative paths is bounded, that is there are no relative cycles.
Proof. We sketch the proof in case , where is from to and from to , hence . One of the four direct summands of is
[TABLE]
which is isomorphic as a -bimodule to If is linked, then this direct summand is non zero and it corresponds to the relative path in the formula. The rest of the proof is along the same lines.
Lemma 4.5
Let be a bound quiver algebra, and let . We have
[TABLE]
Proof. First we recall that if and are left -modules, then
[TABLE]
see for instance [8, p. 170, 4.4]).
Let and be respectively left and right finite dimensional -modules, so that the -bimodules and are isomorphic. Then
[TABLE]
Theorem 4.6
Let be a bound quiver algebra, let be a set of new arrows and let . Suppose that there are no relative cycles, that is is finite dimensional. For
[TABLE]
Proof. We infer from the Jacobi-Zariski long exact sequence obtained by Kaygun in [25, 26] and from Theorem 2.5 that for we have Moreover By Proposition 4.4
[TABLE]
Lemma 4.5 provides the result.
Theorem 4.2 is inferred from the previous result by adding as new arrows the deleted ones.
Lemma 4.7
Let be a bound quiver algebra. Let be a new arrow from to which does not provides a relative oriented cycle, and let . For
[TABLE]
Proof. The Kaygun’s Jacobi-Zariski long exact sequence and Theorem 2.5, show that for
[TABLE]
We have that because is not a relative oriented cycle, that is . Hence , where . A simple computation shows that . Hence
[TABLE]
Lemma 4.5 provides the result.
We record the following result as a consequence of Theorem 4.1.
Corollary 4.8
Let be a bound quiver algebra, let be an inert arrow from to and let . If is an injective module, and/or if is a projective module, we have for
[TABLE]
In order to use the previous result, we recall the well known criterion for a projective indecomposable module to be injective.
Proposition 4.9
Let be a bound quiver algebra and let . The indecomposable projective left module is injective if and only if is a simple module for a vertex , and . In that case .
5 Examples
5.1 Amalgamation with a quiver without oriented cycles
Let be a bound quiver algebra, and let be a finite quiver without oriented cycles. We will construct a quiver where some vertices of and are identified.
Let and , with a bijective map . Let be the equivalence relation on given by . We extend it to an equivalence relation on in the obvious manner, each other vertex is just equivalent to itself.
Definition 5.1
The amalgamated quiver is given by
- •
,
- •
.
The amalgamated algebra is .
Theorem 5.2
Let be a bound quiver algebra, let be a finite quiver without oriented cycles and let be as above. Suppose that for each path of positive length of , one of its extremities is not in . For
[TABLE]
Proof. Let be the quiver with the set of new vertices added - each one is a connected component of . Consider the algebra B=\Lambda\times\mbox{{\Large\times}}_{|S_{0}\setminus Y|}k. Hochschild cohomology is additive on the product of algebras, and for , hence for .
Recall that is the quiver with the set of new arrows added, we have . The hypotheses on the paths of imply that there are no relative oriented cycles, hence is finite dimensional. Moreover, for each relative path at least one of its extremities is an isolated vertex . We have that , which is a simple module. The corresponding ’s in Theorem 4.6 vanish.
5.2 Gorenstein algebras
A finite dimensional -algebra is Gorenstein if is of finite injective dimension as a left module, and the injective left module is of finite projective dimension , see for instance [20]. The algebra is called -Gorenstein for the maximum of these numbers.
Let be a bound quiver algebra. If is -Gorenstein, then for any the projective dimension of and the injective dimension of is at most . For instance selfinjective algebras are [math]-Gorenstein algebras. The following result is a consequence of Theorem 4.6.
Proposition 5.3
Let be a bound quiver algebra which is -Gorenstein. Let be the quiver obtained from by adding a finite number of new arrows, and suppose is finite dimensional. For and ,
[TABLE]
while for - that is if is selfinjective- the isomorphism holds for .
Example 5.4
For , let be the following cyclic connected quiver:
s_{0}$$s_{1}$$s_{i}$$s_{m-1}$$a_{0}$$a_{1}$$a_{m-2}$$a_{m-1}$$a_{i}
For , let , which is a selfinjective algebra. Let be the quiver obtained from by adding a finite number of arrows at pairs of vertices. Suppose that is finite dimensional, that is there are no relative oriented cycles. For
[TABLE]
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