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CONTINUOUS QUIVERS OF TYPE A (III) EMBEDDINGS OF CLUSTER THEORIES

Published online by Cambridge University Press:  11 February 2022

KIYOSHI IGUSA
Affiliation:
Mathematics Department Brandeis University Waltham, Massachusetts 02453, USA igusa@brandeis.edu
JOB D. ROCK
Affiliation:
Hausdorff Research Institute for Mathematics Poppelsdorfer Alle 45 Bonn 53115, Germany jobrock@brandeis.edu
GORDANA TODOROV
Affiliation:
Mathematics Department Northeastern University Boston, Massachusetts 02115, USA g.todorov@northeastern.edu
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Abstract

We continue the work started in parts (I) and (II) of this series. In this paper, we classify which continuous quivers of type A are derived equivalent. Next, we define the new ${\mathcal {C}(A_{{\mathbb {R}},S})}$, which we call weak continuous cluster category. It is a triangulated category, it does not have cluster structure but it has a new weaker notion of “cluster theory.” We show that the original continuous cluster category of [15] is a localization of this new weak continuous cluster category. We define cluster theories to be appropriate groupoids and we show that cluster structures satisfy the conditions for cluster theories. We describe the relationship between different cluster theories: some new and some obtained from cluster structures. The notion of continuous mutation which appears in cluster theories (but not in cluster structures) appears in the next paper [20].

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© (2022) The Authors. The publishing rights in this article are licenced to Foundation Nagoya Mathematical Journal under an exclusive license
Figure 0

Figure 1 A visual depiction of a continuous quiver of type A.

Figure 1

Figure 2 Supports for some indecomposable projectives described in Theorem 1.1.7.

Figure 2

Figure 3 An example of a continuous quiver of type A and the image of $\mathop {\boldsymbol {\Gamma }}$.

Figure 3

Figure 4 Part of the AR-space of the bounded derived category ${\mathcal {D}^b(A_{{\mathbb {R}}})}$.

Figure 4

Figure 5 Depiction of Example 2.2.8, where V is indecomposable and W has four indecomposable summands.

Figure 5

Figure 6 Constructing the cone object from Example 2.2.8 and Figure 5.

Figure 6

Figure 7 A visual depiction of the obstruction to a derived equivalence $\mathcal G:\mathcal D^b(A_{{\mathbb {R}}})\to {\mathcal {D}^b(A_{{\mathbb {R}},S})}$ for $S={\mathbb {N}}$ and $S={\mathbb {Z}}$ in the proof of Theorem 2.3.5.

Figure 7

Figure 8 In this example, $Y=Y_1\oplus Y_2$ where $Y_1$ has the same y-coordinate as X. Then $Z^\varepsilon =I_1^\varepsilon \oplus Z_1\oplus Z_2^\varepsilon $. As $\varepsilon \to 0$, $I_1^\varepsilon $ moves to the right until it becomes $0$, $Z_2^\varepsilon $ moves up to $Z_2$, $Z_1$ stays where it is. Also, $T^\varepsilon X$ goes to $ TX$. Thus the distinguished triangle is $X\to Y_1\oplus Y_2\to Z_1\oplus Z_2\to TX$. The support of $\operatorname {\mathrm {Hom}}_{\mathcal D_r}(X,-)$ is shaded.

Figure 8

Figure 9 A visual aide to compute Example 4.2.6.

Figure 9

Figure 10 Schematics of Case (1)(ii) and Case (1)(iii) on the left and right, respectively, in the proof of Lemma 4.3.7.

Figure 10

Figure 11 Schematics of Case (2)(i) and Case (2)(ii) on the left and right, respectively, in the proof of Lemma 4.3.7.