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Lagrangian Cobordism and Shadow Distance
in Tamarkin Category

Tomohiro Asano    Yuichi Ike    Wenyuan Li
Abstract

We study exact Lagrangian cobordisms between exact Lagrangians in a cotangent bundle in the sense of Arnol’d, using microlocal theory of sheaves. We construct a sheaf quantization for an exact Lagrangian cobordism between Lagrangians with conical ends, prove an iterated cone decomposition of the sheaf quantization for cobordisms with multiple ends, and show that the interleaving distance of sheaves is bounded by the shadow distance of the cobordism. Using the result, we prove a rigidity result on Lagrangian intersection by estimating the energy cost of splitting and connecting Lagrangians through cobordisms.

1 Introduction

Lagrangian cobordisms between Lagrangian submanifolds was first introduced by Arnol’d [Arnold80I, Arnold80II]. Recently, Biran–Cornea [BC13, BC14] discovered the deep relation between Lagrangian cobordisms and Fukaya categories, and Cornea–Shelukhin [CS19] introduced the shadow distance of Lagrangian cobordisms, which was then used by Biran–Cornea–Shelukhin [BCS18] to show rigidity results of Lagrangian intersections.

On the other hand, the microlocal theory of sheaves developed by Kashiwara–Schapira [KS90] has been shown to be a powerful tool in symplectic geometry following the pioneering work of Nadler–Zaslow [NZ, Nad] and Tamarkin [Tamarkin]. Sheaf-theoretic methods have been effectively applied to symplectic geometry, for example, [GKS, Chiu17, Gu23, Shende19conormal, GPS20microlocal, zhang2021capacities], and have advantage in the studies of for example degenerate intersections of Lagrangians [Ike19, AISQ] and non-smooth limits of Lagrangians [AI22Complete, GV22].

In this paper, we apply sheaf theory to the study of Lagrangian cobordisms, explore the algebraic relations of sheaves induced by Lagrangian cobordisms, and compare the interleaving distance introduced by the first two authors [AI20] with the shadow distance of Lagrangian cobordisms [CS19], which leads to rigidity results of Lagrangian intersections.

1.1 Main results

Let MM be a closed manifold. Let L0,,L_{0},\dots, Lm1L_{m-1} and L0,,Ln1TML^{\prime}_{0},\dots,L^{\prime}_{n-1}\subset T^{*}M be exact Lagrangian submanifolds with conical ends. An exact Lagrangian cobordism with conical ends VT(M×)V\subset T^{*}(M\times\mathbb{R}) between (L0,,Lm1)(L_{0},\dots,L_{m-1}) and (L0,,Ln1)(L^{\prime}_{0},\dots,L^{\prime}_{n-1}) is an exact Lagrangian with conical end VV_{\infty} such that VT,(M×[1,1])V_{\infty}\cap T^{*,\infty}(M\times[-1,1]) is compact and

VT(M×(,1])\displaystyle V\cap T^{*}(M\times(-\infty,-1]) =i=0m1Li×(,1]×{i},\displaystyle=\bigcup_{i=0}^{m-1}L_{i}\times(-\infty,-1]\times\{i\}, (1.1)
VT(M×[+1,+))\displaystyle V\cap T^{*}(M\times[+1,+\infty)) =j=0n1Lj×[+1,+)×{j}.\displaystyle=\bigcup_{j=0}^{n-1}L^{\prime}_{j}\times[+1,+\infty)\times\{j\}. (1.2)

In this study, we use the Tamarkin category 𝒟(M)\mathcal{D}(M), which is a localization of the sheaf category Sh(M×)\operatorname{\mathrm{Sh}}(M\times\mathbb{R}). We can equip 𝒟(M)\mathcal{D}(M) with an interleaving distance d𝒟(M)d^{\prime}_{\mathcal{D}(M)} that is stable under Hamiltonian isotopies [AI20]. See Subsection 2.2 for details. For any exact Lagrangian LTML\subset T^{*}M, we can construct a simple sheaf FL𝒟(M)F_{L}\in\mathcal{D}(M) with reduced microsupport on LL [Gu12, JT17, Vi19, Gu23]. They are called sheaf quantizations of LL.

Our first result is the following existence theorem of a sheaf quantization of a Lagrangian cobordism, namely, that there exists a simple sheaf with reduced microsupport in the given exact Lagrangian cobordism.

Theorem 1.1 (see LABEL:thm:sheaf-quan-cob-filling).

Let VT(M×)V\subset T^{*}(M\times\mathbb{R}) be an exact Lagrangian cobordism with conical ends between (L0,,Lm1)(L_{0},\dots,L_{m-1}) and (L0,,Ln1)(L^{\prime}_{0},\dots,L^{\prime}_{n-1}) with vanishing Maslov class and relative second Stiefel–Whitney class. Then there is a simple sheaf quantization F𝒟(M×)F\in\mathcal{D}(M\times\mathbb{R}).

Remark 1.2 (see LABEL:rem:quan-jintreumann).

Jin–Treumann [JT17, Subsection 1.11.4] have mentioned that such a theorem should be true after deforming the Lagrangian cobordism so that it becomes lower exact and satisfies [JT17, Assumption 3.7], which requires an extra proof as VV is not eventually conical in T(M×)T^{*}(M\times\mathbb{R}). Our approach avoids that assumption.

Our second result is the following iterated cone decomposition theorem of a sheaf quantization of a Lagrangian cobordism. We write

[\displaystyle[ G0G1Gk1Gk]\displaystyle G_{0}\to G_{1}\to\dots\to G_{k-1}\to G_{k}]\coloneqq
Cone(Cone(Cone(G0[k]G1[1k])Gk1[1])Gk).\displaystyle\operatorname{Cone}(\operatorname{Cone}(\dots\operatorname{Cone}(G_{0}[-k]\to G_{1}[1-k])\to\dots\to G_{k-1}[-1])\to G_{k}). (1.3)
Theorem 1.3 (see LABEL:theorem:iterated_cone).

Let FF be a simple sheaf quantization of Lagrangian cobordism VV between (L0,,Lm1)(L_{0},\dots,L_{m-1}) and (L0,,Ln1)(L^{\prime}_{0},\dots,L^{\prime}_{n-1}). Set FsF|M×t×{s}F_{s}\coloneqq F|_{M\times\mathbb{R}_{t}\times\{s\}}. Then one has iterated decompositions

F1\displaystyle F_{-1} =[FL0FL1FLm2FLm1],\displaystyle=\left[F_{L_{0}}\to F_{L_{1}}\to\dots\to F_{L_{m-2}}\to F_{L_{m-1}}\right], (1.4)
F+1\displaystyle F_{+1} =[FLn1FLn2FL1FL0],\displaystyle=\left[F_{L^{\prime}_{n-1}}\to F_{L^{\prime}_{n-2}}\to\dots\to F_{L^{\prime}_{1}}\to F_{L^{\prime}_{0}}\right], (1.5)

where FLiF_{L_{i}} (resp. FLjF_{L^{\prime}_{j}}) is a simple sheaf quantization of LiL_{i} (resp. Lj)L^{\prime}_{j}).

Our third result is the following inequality for the interleaving distance by the shadow distance of a Lagrangian cobordism. For a Lagrangian cobordism VT(M×)V\subset T^{*}(M\times\mathbb{R}), the shadow 𝒮(V)\mathcal{S}(V) of VV is defined as the area of T𝒰(V)T^{*}\mathbb{R}\setminus\mathcal{U}(V), where 𝒰(V)\mathcal{U}(V) is the union of unbounded regions of Tp(V)T^{*}\mathbb{R}\setminus p(V) with p:T(M×)Tp\colon T^{*}(M\times\mathbb{R})\to T^{*}\mathbb{R} being the projection map. It is known that in the exact setting, the Lagrangian shadow induces a metric on all Lagrangian submanifolds [CS19]. Our result in particular implies an isomorphism of the sheaves in the Tamarkin category modulo torsion objects 𝒯(M)=𝒟(M)/Tor\mathcal{T}(M)=\mathcal{D}(M)/\mathrm{Tor} where sheaves related by Hamiltonian isotopies become isomorphic.

Theorem 1.4 (see LABEL:theorem:inequality_multiple_ends).

Let FF be a simple sheaf quantization of Lagrangian cobordism VV and consider iterated cone decompositions as in Theorem 1.3. Then there exist real numbers ci,cj(i=1,,m1,j=0,,n1)c_{i},c^{\prime}_{j}\in\mathbb{R}\ (i=1,\dots,m-1,j=0,\dots,n-1) such that

d𝒟(M)(F~1,F~+1)𝒮(V),d^{\prime}_{\mathcal{D}(M)}(\tilde{F}_{-1},\tilde{F}_{+1})\leq\mathcal{S}(V), (1.6)

where

F~1\displaystyle\tilde{F}_{-1} [FL0Tc1FL1Tcm2FLm2Tcm1FLm1],\displaystyle\coloneqq\left[F_{L_{0}}\to T_{c_{1}}F_{L_{1}}\to\dots\to T_{c_{m-2}}F_{L_{m-2}}\to T_{c_{m-1}}F_{L_{m-1}}\right], (1.7)
F~+1\displaystyle\tilde{F}_{+1} [Tcn1FLn1Tcn2FLn2Tc1FL1Tc0FL0].\displaystyle\coloneqq\left[T_{c^{\prime}_{n-1}}F_{L^{\prime}_{n-1}}\to T_{c^{\prime}_{n-2}}F_{L^{\prime}_{n-2}}\to\dots\to T_{c^{\prime}_{1}}F_{L^{\prime}_{1}}\to T_{c^{\prime}_{0}}F_{L^{\prime}_{0}}\right]. (1.8)

In particular, one has F~1F~+1\tilde{F}_{-1}\simeq\tilde{F}_{+1} in 𝒯(M)\mathcal{T}(M).

In fact, we prove Theorems 1.3 and 1.4 in more general setting, without assuming the cobordism is a Lagrangian submanifold. See the main body of the paper.

We apply the theorems above to Lagrangian intersection, recovering [BCS18, Thm. C] in the cotangent bundle case, which shows that there is an energy cost to separate or connect Lagrangians through cobordisms.

Theorem 1.5 (see LABEL:theorem:intersection).

Let VT(M×)V\subset T^{*}(M\times\mathbb{R}) be an exact Lagrangian cobordism with conical ends between (L0,,Lm1)(L_{0},\dots,L_{m-1}) and LL^{\prime}. Moreover, let NN be a Lagrangian and assume that the Lagrangians are in general position so that each pair of N,L0,,Lm1N,L_{0},\dots,L_{m-1}, and LL^{\prime} intersect transversally and there are no point in the intersection any triple of them. Then there exists a constant δ>0\delta>0 that depends only on L0,,Lm1L_{0},\dots,L_{m-1}, and NN satisfying the following. If 𝒮(V)<δ\mathcal{S}(V)<\delta then

#(NL)i=0m1#(NLi).\#(N\cap L^{\prime})\geq\sum_{i=0}^{m-1}\#(N\cap L_{i}). (1.9)
Remark 1.6 (see LABEL:rem:morse-bott-intersect).

Our methods can be immediately generalized to clean intersections of Lagrangian submanifolds. When L0L_{0} and L1L_{1} intersect cleanly along DD, one can define the surgery L0#DL1L_{0}\#_{D}L_{1} along DD and build a Lagrangian cobordism from L0,L1L_{0},L_{1} to L0#DL1L_{0}\#_{D}L_{1} [MakWu, Lem. 6.1].

Comparing to previous Lagrangian intersection results using sheaf theoretic methods [Ike19, AISQ], we need to estimate the energy of higher homotopies in the iterated cone decomposition, which, in Lagrangian Floer theory, come from pseudo-holomorphic polygons instead of just pseudo-holomorphic strips. See the main body of the paper.

1.2 Related work

The relation between Lagrangian cobordisms and Fukaya categories and their filtrations has been studied in many previous works. Biran–Cornea [BC13, BC14] showed that (monotone) Lagrangian cobordisms induce iterated cone decompositions in the Fukaya categories. Cornea–Shelukhin [CS19] introduced the shadow distance of Lagrangian cobordisms, and later Biran–Cornea–Shelukhin [BCS18] used the shadow distance to prove results on Lagrangian intersection using the theory of weakly filtered AA_{\infty}-categories. More recently, motivated by the geometry, Biran–Cornea–Zhang [BCZ23] developed the theory of persistence triangulated categories and showed that the Tamarkin category and the Fukaya category are persistence triangulated categories.

It is well known that the Hofer distance of C1C^{1}-close Lagrangians is related to the shadow of Lagrangian movie under Hamiltonian isotopies [Milinkovic]. Since its introduction, the Lagrangian shadow has become a standard tool in the study of quantitative aspects of Lagrangian submanifolds. See [Hicks21, HicksMak22] for interesting geometric constructions that involve the Lagrangian shadows.

The algebraic results above can also be enhanced to a categorical level. Biran–Cornea [BC14] defined a category that with a functor into the cone resolution category of the Fukaya category, while Nadler–Tanaka [NadTanaka] defined a stable \infty-category of Lagrangian cobordisms with an exact functor into the wrapped Fukaya category [Tanaka16, Tanaka16Exact]. We expect that the sheaf quantization result here provides a way to define a functor from that category to the sheaf categories.

Finally, it is expected that the relation between Lagrangian cobordisms and Fukaya categories passes through the Waldhausen ss-construction in algebraic KK-theory. In particular, Biran–Cornea [BC14] conjectured an isomorphism between the Lagrangian cobordism group and the Grothendieck group of the Fukaya category. See [BCZ23-2] for the relation between the Grothendieck group and persistence of the Fukaya category. It would be interesting to study the question for the sheaf categories.

Acknowledgment

TA thanks Kaoru Ono for the helpful discussions. TA was partially supported by Innovative Areas Discrete Geometric Analysis for Materials Design (Grant No. 17H06461). YI thanks Alexandru Oancea for the fruitful discussions. He also thanks Paul Biran, Octav Cornea, and Jun Zhang for helpful discussions and clarifications. YI was partially supported by JSPS KAKENHI Grant Numbers 21K13801 and 22H05107. WL thanks Xin Jin and David Treumann for helpful discussions and clarifications and Bingyu Zhang for helpful discussions.

2 Preliminaries

In this section, we recall some basics of the microlocal sheaf theory due to Kashiwara and Schapira [KS90]. Throughout this paper, all manifolds are assumed to be of class CC^{\infty} without boundary. Let 𝐤\mathbf{k} be a field until the end of this paper.

Until the end of this section, let XX be a CC^{\infty}-manifold. For a locally closed subset AA of XX, we denote by A¯\overline{A} its closure and by Int(A)\operatorname{\operatorname{Int}}(A) its interior. We also denote by ΔX\Delta_{X} or simply Δ\Delta the diagonal of X×XX\times X. We denote by πX:TXX\pi_{X}\colon T^{*}X\to X the cotangent bundle of XX. We write 0X0_{X} for the zero-section of TXT^{*}X and set T̊XTX0X\mathring{T}^{*}X\coloneqq T^{*}X\setminus 0_{X}. We denote by (x;ξ)(x;\xi) a local homogeneous coordinate system of TXT^{*}X. The cotangent bundle TXT^{*}X is an exact symplectic manifold with the Liouville 1-form λTX=ξ,dx\lambda_{T^{*}X}=\langle\xi,dx\rangle.

2.1 Microsupports of sheaves

For a manifold XX, we write 𝐤X\mathbf{k}_{X} for the constant sheaf with stalk 𝐤\mathbf{k} and let Sh(X)=Sh(𝐤X)\operatorname{\mathrm{Sh}}(X)=\operatorname{\mathrm{Sh}}(\mathbf{k}_{X}) denote the dg-derived category of sheaves of 𝐤\mathbf{k}-vector spaces on XX. One can define Grothendieck’s six operations between dg-derived categories of sheaves om,,f,f1,f!,f!\mathop{{\mathcal{H}}om}\nolimits,\allowbreak\otimes,\allowbreak f_{*},\allowbreak f^{-1},\allowbreak f_{!},\allowbreak f^{!} for a morphism of manifolds f:XYf\colon X\to Y [Spaltenstein, Schn18]. For a locally closed subset ZZ of XX, we denote by 𝐤ZSh(X)\mathbf{k}_{Z}\in\operatorname{\mathrm{Sh}}(X) the constant sheaf with stalk 𝐤\mathbf{k} on ZZ, extended by 0 on XZX\setminus Z. Moreover, for a locally closed subset ZZ of XX and FSh(X)F\in\operatorname{\mathrm{Sh}}(X), we define

FZF𝐤Z,ΓZ(F)om(𝐤Z,F).F_{Z}\coloneqq F\otimes\mathbf{k}_{Z},\quad\Gamma_{Z}(F)\coloneqq\mathop{{\mathcal{H}}om}\nolimits(\mathbf{k}_{Z},F). (2.1)

Let X1,X2,X3X_{1},X_{2},X_{3} be manifolds and πij:X1×X2×X3Xi×Xj\pi_{ij}\colon X_{1}\times X_{2}\times X_{3}\to X_{i}\times X_{j} for ij{1,2,3}i\neq j\in\{1,2,3\}. For K12Sh(X1×X2)K_{12}\in\operatorname{\mathrm{Sh}}(X_{1}\times X_{2}) and K23Sh(X2×X3)K_{23}\in\operatorname{\mathrm{Sh}}(X_{2}\times X_{3}), their composition is defined by

K12K23=π13!(π121K12π231K23).K_{12}\circ K_{23}=\pi_{13!}(\pi_{12}^{-1}K_{12}\otimes\pi_{23}^{-1}K_{23}). (2.2)

Following [KS90, robalo2018lemma], for FSh(X)F\in\operatorname{\mathrm{Sh}}(X), we let SS(F)\operatorname{{\operatorname{SS}}}(F) denote the microsupport of FF, which is a conical (i.e., invariant under the action of >0\mathbb{R}_{>0}) closed subset of TXT^{*}X. The set SS(F)\operatorname{{\operatorname{SS}}}(F) describes the singular codirections of FF, in which FF does not propagate. We also use the notation SS̊(F)SS(F)T̊X=SS(F)0X\mathring{\operatorname{{\operatorname{SS}}}}(F)\coloneqq\operatorname{{\operatorname{SS}}}(F)\cap\mathring{T}^{*}X=\operatorname{{\operatorname{SS}}}(F)\setminus 0_{X}.

By using microsupports, we can microlocalize the category Sh(X)\operatorname{\mathrm{Sh}}(X). Let ATXA\subset T^{*}X be a subset and set Ω=TXA\Omega=T^{*}X\setminus A. We denote by ShA(X)\operatorname{\mathrm{Sh}}_{A}(X) the full dg-subcategory of Sh(X)\operatorname{\mathrm{Sh}}(X) consisting of sheaves whose microsupports are contained in AA. By the triangle inequality, the subcategory ShA(X)\operatorname{\mathrm{Sh}}_{A}(X) is a pretriangulated subcategory. We set

Sh(X;Ω)Sh(X)/ShA(X),\operatorname{\mathrm{Sh}}(X;\Omega)\coloneqq\operatorname{\mathrm{Sh}}(X)/\operatorname{\mathrm{Sh}}_{A}(X), (2.3)

the dg-quotient of Sh(X)\operatorname{\mathrm{Sh}}(X) by ShA(X)\operatorname{\mathrm{Sh}}_{A}(X). A morphism u:FGu\colon F\to G in Sh(X)\operatorname{\mathrm{Sh}}(X) becomes a quasi-isomorphism in Sh(X;Ω)\operatorname{\mathrm{Sh}}(X;\Omega) if uu is embedded in an exact triangle FuGH+1F\overset{u}{\to}G\to H\overset{+1}{\to} with SS(H)Ω=\operatorname{{\operatorname{SS}}}(H)\cap\Omega=\varnothing. We also denote by Sh(A)(X)\operatorname{\mathrm{Sh}}_{(A)}(X) the full dg-subcategory of Sh(X)\operatorname{\mathrm{Sh}}(X) formed by FF for which there exists a neighborhood UU of AA satisfying SS(F)UA\operatorname{{\operatorname{SS}}}(F)\cap U\subset A.

2.2 Tamarkin category and interleaving distance

Here, we recall the Tamarkin category 𝒟(X)\mathcal{D}(X) and the interleaving distance.

We write (x;ξ)(x;\xi) for a local homogeneous coordinate system on TXT^{*}X and (t;τ)(t;\tau) for the homogeneous coordinate system on TtT^{*}\mathbb{R}_{t}. Define the maps

π1,π2,m:X××X×t,\displaystyle\qquad\pi_{1},\pi_{2},m\colon X\times\mathbb{R}\times\mathbb{R}\to X\times\mathbb{R}_{t}, (2.4)
π1(x,t1,t2)\displaystyle\pi_{1}(x,t_{1},t_{2}) =(x,t1),π2(x,t1,t2)=(x,t2),m(x,t1,t2)=(x,t1+t2).\displaystyle=(x,t_{1}),\ \pi_{2}(x,t_{1},t_{2})=(x,t_{2}),\ m(x,t_{1},t_{2})=(x,t_{1}+t_{2}).

For F,GSh(X×t)F,G\in\operatorname{\mathrm{Sh}}(X\times\mathbb{R}_{t}), one sets

FG\displaystyle F\star G m!(π11Fπ21G),\displaystyle\coloneqq m_{!}(\pi_{1}^{-1}F\otimes\pi_{2}^{-1}G), (2.5)
om(F,G)\displaystyle\mathop{{\mathcal{H}}om}\nolimits^{\star}(F,G) π1om(π21F,m!G).\displaystyle\coloneqq\pi_{1*}\mathop{{\mathcal{H}}om}\nolimits(\pi_{2}^{-1}F,m^{!}G). (2.6)

Note that the functor \star is a left adjoint to om\mathop{{\mathcal{H}}om}\nolimits^{\star}.

Tamarkin proved that the localized category Sh(X×t;{τ>0})\operatorname{\mathrm{Sh}}(X\times\mathbb{R}_{t};\{\tau>0\}) is equivalent to both the left orthogonal Sh{τ0}(X×t){}^{\perp}\operatorname{\mathrm{Sh}}_{\{\tau\leq 0\}}(X\times\mathbb{R}_{t}) and the right orthogonal Sh{τ0}(X×t)\operatorname{\mathrm{Sh}}_{\{\tau\leq 0\}}(X\times\mathbb{R}_{t})^{\perp}:

Pl𝐤X×[0,+)():Sh(X×t;{τ>0})Sh{τ0}(X×t),\displaystyle P_{l}\coloneqq\mathbf{k}_{X\times[0,+\infty)}\star(\ast)\colon\operatorname{\mathrm{Sh}}(X\times\mathbb{R}_{t};\{\tau>0\})\xrightarrow{\sim}{}^{\perp}\operatorname{\mathrm{Sh}}_{\{\tau\leq 0\}}(X\times\mathbb{R}_{t}), (2.7)
Prom(𝐤X×[0,+),):Sh(X×t;{τ>0})Sh{τ0}(X×t).\displaystyle P_{r}\coloneqq\mathop{{\mathcal{H}}om}\nolimits^{\star}(\mathbf{k}_{X\times[0,+\infty)},\ast)\colon\operatorname{\mathrm{Sh}}(X\times\mathbb{R}_{t};\{\tau>0\})\xrightarrow{\sim}\operatorname{\mathrm{Sh}}_{\{\tau\leq 0\}}(X\times\mathbb{R}_{t})^{\perp}.

We set Ω+{τ>0}T(X×t)\Omega_{+}\coloneqq\{\tau>0\}\subset T^{*}(X\times\mathbb{R}_{t}) and define a map ρ:Ω+TX\rho\colon\Omega_{+}\to T^{*}X as (x,t;ξ,τ)(x;ξ/τ)(x,t;\xi,\tau)\mapsto(x;\xi/\tau).

Definition 2.1.

One defines

𝒟(X)Sh(X×t;Ω+)Sh{τ0}(X×t)Sh{τ0}(X×t).\mathcal{D}(X)\coloneqq\operatorname{\mathrm{Sh}}(X\times\mathbb{R}_{t};\Omega_{+})\simeq{}^{\perp}\operatorname{\mathrm{Sh}}_{\{\tau\leq 0\}}(X\times\mathbb{R}_{t})\simeq\operatorname{\mathrm{Sh}}_{\{\tau\leq 0\}}(X\times\mathbb{R}_{t})^{\perp}. (2.8)

For F𝒟(X)F\in\mathcal{D}(X), one defines its reduced microsupport by

RS(F)ρ(SS(F)Ω+)¯TX.\operatorname{RS}(F)\coloneqq\overline{\rho(\operatorname{{\operatorname{SS}}}(F)\cap\Omega_{+})}\subset T^{*}X. (2.9)

For a closed subset AA of TXT^{*}X, one also defines a full subcategory 𝒟A(X)\mathcal{D}_{A}(X) of 𝒟(X)\mathcal{D}(X) by

𝒟A(X){F𝒟(X)RS(F)A}.\mathcal{D}_{A}(X)\coloneqq\{F\in\mathcal{D}(X)\mid\operatorname{RS}(F)\subset A\}. (2.10)

For F𝒟(X)F\in\mathcal{D}(X), we take the canonical representative Pl(F)Sh{τ0}(X×t)P_{l}(F)\in{}^{\perp}\operatorname{\mathrm{Sh}}_{\{\tau\leq 0\}}(X\times\mathbb{R}_{t}) unless otherwise specified. Note that if FSh{τ0}(X×t)F\in{}^{\perp}\operatorname{\mathrm{Sh}}_{\{\tau\leq 0\}}(X\times\mathbb{R}_{t}), then om(F,G)Sh{τ0}(X×t)\mathop{{\mathcal{H}}om}\nolimits^{\star}(F,G)\in\operatorname{\mathrm{Sh}}_{\{\tau\leq 0\}}(X\times\mathbb{R}_{t})^{\perp}. Thus om\mathop{{\mathcal{H}}om}\nolimits^{\star} induces an internal Hom functor om:𝒟(X)op×𝒟(X)𝒟(X)\mathop{{\mathcal{H}}om}\nolimits^{\star}\colon\mathcal{D}(X)^{\mathrm{op}}\times\mathcal{D}(X)\to\mathcal{D}(X). We also often regard om(F,G)\mathop{{\mathcal{H}}om}\nolimits^{\star}(F,G) as in Sh{τ0}(X×t){}^{\perp}\operatorname{\mathrm{Sh}}_{\{\tau\leq 0\}}(X\times\mathbb{R}_{t}) by applying the projector PlP_{l}.

Proposition 2.2 (cf. [GS14, Lem. 4.18]).

For F,G𝒟(X)F,G\in\mathcal{D}(X), one has

Hom𝒟(X)(F,G)ΓX×[0,+)(X×t;om(F,G)).\operatorname{Hom}_{\mathcal{D}(X)}(F,G)\simeq\Gamma_{X\times[0,+\infty)}(X\times\mathbb{R}_{t};\mathop{{\mathcal{H}}om}\nolimits^{\star}(F,G)). (2.11)

Now we introduce a pseudo-distance d𝒟(X)d^{\prime}_{\mathcal{D}(X)} on the Tamarkin category 𝒟(X)\mathcal{D}(X). Note that our distance d𝒟(X)d^{\prime}_{\mathcal{D}(X)} here is different from the distances used in [AI20, AISQ, AI22Complete]. Here we use weakly (a,b)(a,b)-isomorphic to obtain an isomorphism in 𝒯(X)\mathcal{T}(X) (see Remark 2.4 below), while in [AI20, AISQ] the authors only use (a,b)(a,b)-interleaving in the definition. Nevertheless, all the results in [AI20, AISQ] hold for this stronger notion [AI20, Remark 4.5]. For cc\in\mathbb{R}, consider the translation map Tc:X×X×,Tc(x,t)=(x,t+c)T_{c}\colon X\times\mathbb{R}\to X\times\mathbb{R},\,T_{c}(x,t)=(x,t+c). By abuse of notation, we write TcTc:Sh(X×t)Sh(X×t)T_{c}\coloneqq{T_{c}}_{*}\colon\operatorname{\mathrm{Sh}}(X\times\mathbb{R}_{t})\to\operatorname{\mathrm{Sh}}(X\times\mathbb{R}_{t}) and the induced functor Tc:𝒟(X)𝒟(X){T_{c}}_{*}\colon\mathcal{D}(X)\to\mathcal{D}(X). For cdc\leq d, there exists a natural transformation τc,d:TcTd\tau_{c,d}\colon T_{c}\to T_{d} between the functors on 𝒟(X)\mathcal{D}(X).

Definition 2.3.

Let F,G𝒟(X)F,G\in\mathcal{D}(X) and a,b0a,b\in\mathbb{R}_{\geq 0}.

  1. (i)\mathrm{(i)}

    The pair (F,G)(F,G) is said to be said to be weakly (a,b)(a,b)-isomorphic if there exist morphisms α,δ:FTaG\alpha,\delta\colon F\to{T_{a}}G and β,γ:GTbF\beta,\gamma\colon G\to{T_{b}}F such that

    1. (1)\mathrm{(1)}

      FαTaGTaβTa+bFF\xrightarrow{\alpha}{T_{a}}G\xrightarrow{{T_{a}}\beta}{T_{a+b}}F is homotopic to τ0,a+b(F):FTa+bF\tau_{0,a+b}(F)\colon F\to{T_{a+b}}F,

    2. (2)\mathrm{(2)}

      GγTbFTbδTa+bGG\xrightarrow{\gamma}{T_{b}}F\xrightarrow{{T_{b}}\delta}{T_{a+b}}G is homotopic to τ0,a+b(G):GTa+bG\tau_{0,a+b}(G)\colon G\to{T_{a+b}}G, and

    3. (3)\mathrm{(3)}

      τa,2a(G)ατa,2a(G)δ\tau_{a,2a}(G)\circ\alpha\simeq\tau_{a,2a}(G)\circ\delta and τb,2b(F)βτb,2b(F)γ\tau_{b,2b}(F)\circ\beta\simeq\tau_{b,2b}(F)\circ\gamma.

  2. (ii)\mathrm{(ii)}

    One defines

    d𝒟(X)(F,G)inf{a+b0|a,b0,(F,G) is weakly (a,b)-isomorphic}.d^{\prime}_{\mathcal{D}(X)}(F,G)\coloneqq\inf\left\{a+b\in\mathbb{R}_{\geq 0}\mathrel{}\middle|\mathrel{}\begin{aligned} &a,b\in\mathbb{R}_{\geq 0},\\ &\text{$(F,G)$ is weakly $(a,b)$-isomorphic}\end{aligned}\right\}. (2.12)
Remark 2.4.

We can define a new category 𝒯(X)\mathcal{T}(X) as the quotient category 𝒟(X)/Tor\mathcal{D}(X)/\operatorname{Tor}, where Tor\operatorname{Tor} is the null system consisting of objects whose distance with the zero object are finite. Then it is shown in [GS14] that

Hom𝒯(X)(F,G)hoUNKNOWN (2.13)