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Realizations of planar graphs as Poincaré-Reeb graphs of refined algebraic domains

Naoki kitazawa Institute of Mathematics for Industry, Kyushu University, 744 Motooka, Nishi-ku Fukuoka 819-0395, Japan
TEL (Office): +81-92-802-4402
FAX (Office): +81-92-802-4405
n-kitazawa@imi.kyushu-u.ac.jp, naokikitazawa.formath@gmail.com https://naokikitazawa.github.io/NaokiKitazawa.html
Abstract.

Algebraic domains are regions in the plane surrounded by mutually disjoint non-singular real algebraic curves. Poincaré-Reeb Graphs of them are graphs they naturally collapse: such graphs are formally formulated by Sorea, for example, around 2020. Their studies found that nicely embedded planar graphs are Poincaré-Reeb graphs of some algebraic domains. These graphs are generic with respect to the projection to the horizontal axis. Problems, methods and results are elementary and natural and they apply natural approximations nicely for example.

We present our new approach to extension of the result to a non-generic case and an answer. We first formulate generalized algebraic domains, surrounded by non-singular real algebraic curves which may intersect with normal crossings. Such domains and certain classes of them appear in related studies of graphs and regions surrounded by algebraic curves explicitly.

Key words and phrases:
(Non-singular) real algebraic manifolds and real algebraic maps. Algebraic domains. Poincaré-Reeb Graphs. Singularity theory of Morse(-Bott) functions.2020 Mathematics Subject Classification: Primary 14P05, 14P10, 52C15, 57R45. Secondary  58C05.

1. Introduction.

In real algebraic geometry, regions in the plane surrounded by (so-called) non-singular real algebraic curves are fundamental spaces and objects. [2, 24, 25] show a kind of studies which are also elementary, natural and surprisingly, developing recently. They try to understand the shapes, especially, convexity, of the regions. They are defined as algebraic domains. Graphs they naturally collapse to respecting the projection to the horizontal axis {(t,0)t}\{(t,0)\mid t\in\mathbb{R}\} are introduced and shown to be important: hereafter let n{\mathbb{R}}^{n} denote the nn-dimensional Euclidean space, which is also a smooth manifold equipped with the standard Euclidean metric, and x0||x||\geq 0 the distance between xnx\in{\mathbb{R}}^{n} and the origin 0n0\in{\mathbb{R}}^{n} under the metric as usual (:=1\mathbb{R}:={\mathbb{R}}^{1}). They have shown that for a naturally embedded planar graph being generic with respect to the projection, we can find an algebraic domain collapsing naturally to the graph. There classical and strong arguments such as approximation by real polynomials are essential. Such a graph is also named a Poincaré-Reeb graph of the algebraic domain. Our study extends their result to graphs which may not be generic in the sense above.

1.1. Our notation on topological spaces, manifolds and graphs.

Let πm,n:mn{\pi}_{m,n}:{\mathbb{R}}^{m}\rightarrow{\mathbb{R}}^{n} with m>n1m>n\geq 1 denote the so-called canonical projection πm,n(x)=x1{\pi}_{m,n}(x)=x_{1} where x=(x1,x2)n×mn=mx=(x_{1},x_{2})\in{\mathbb{R}}^{n}\times{\mathbb{R}}^{m-n}={\mathbb{R}}^{m}. We also use Dk:={xkx1}D^{k}:=\{x\in{\mathbb{R}}^{k}\mid||x||\leq 1\}, for the kk-dimensional unit disk, and Sk:={xk+1x=1}S^{k}:=\{x\in{\mathbb{R}}^{k+1}\mid||x||=1\}, for the kk-dimensional unit sphere, for example.

For a topological space XX and its subspace YXY\subset X, we use Y¯\overline{Y} for its closure and YY^{\circ} for its interior: we omit information on the outer space XX unless otherwise stated: we can guess from our arguments. For a topological space XX decomposed into a so-called cell complex, we can define the dimension dimX\dim X uniquely as the dimension of the cell of the maximal dimension (only depending on the topology of XX): topological manifolds, polyhedra, and graphs, which are regarded as 11-dimensional CW complexes, are of such a class. For a topological manifold XX whose boundary is non-empty, we use X\partial X for its boundary and IntX:=XX{\rm Int}\ X:=X-\partial X. For a smooth manifold XX and xXx\in X, we use TxXT_{x}X for the tangent vector space of XX at xx. For smooth manifolds XX and YY and a smooth map c:XYc:X\rightarrow Y, a point xXx\in X is its singular point if the rank of the differential dcx:TxXTc(x)Y{dc}_{x}:T_{x}X\rightarrow T_{c(x)}Y is smaller than both the dimensions dimX\dim X and dimY\dim Y: note that dcx{dc}_{x} is a linear map. The zero set SS of a real polynomial map or more generally, a union SS of its connected components is non-singular if the polynomial map has no singular point in the set SS: remember the implicit function theorem.

A graph is a CW complex where an edge is a 11-cell and a vertex is a 0-cell. The set of all edges (vertices) of the graph is the edge set (vertex set) of the graph. Two graphs G1G_{1} and G2G_{2} are isomorphic if there exists a (piecewise smooth) homeomorphism ϕ:G1G2\phi:G_{1}\rightarrow G_{2} mapping the vertex set of G1G_{1} onto that of G2G_{2}: such a homeomorphism is called an isomorphism of the graphs. A digraph is a graph all of whose edges are oriented and two digraphs are isomorphic if there exists an isomorphism of graphs between them preserving the orientations, which is defined as an isomorphism of the digraphs.

1.2. Refined algebraic domains.

Definition 1.

A pair of a family 𝒮={Sj2}\mathcal{S}=\{S_{j}\subset{\mathbb{R}}^{2}\} each SjS_{j} of which is the zero set of a real polynomial fjf_{j} and non-singular and to each of which fjf_{j} is associated and a region D𝒮2D_{\mathcal{S}}\subset{\mathbb{R}}^{2} satisfying the following conditions is called a refined algebraic domain.

  1. (1)

    The region satisfies D𝒮=Sj𝒮{xfj(x)>0}2D_{\mathcal{S}}={\bigcap}_{S_{j}\in\mathcal{S}}\{x\mid f_{j}(x)>0\}\subset{\mathbb{R}}^{2} and a bounded connected component of 2Sj𝒮Sj{\mathbb{R}}^{2}-{\bigcup}_{S_{j}\in\mathcal{S}}S_{j} and the intersection D𝒮¯Sj\overline{D_{\mathcal{S}}}\bigcap S_{j} is non-empty for any curve Sj𝒮S_{j}\in\mathcal{S}.

  2. (2)

    At points in D𝒮¯\overline{D_{\mathcal{S}}}, at most two distinct curves Sj1,Sj2𝒮S_{j_{1}},S_{j_{2}}\in\mathcal{S} intersect and the following are satisfied: for each point pj1,j2p_{j_{1},j_{2}} in such an intersection, the sum of the tangent vector spaces of them at pj1,j2p_{j_{1},j_{2}} coincides with the tangent vector space of 2{\mathbb{R}}^{2} at pj1,j2p_{j_{1},j_{2}}.

This also respects [13] for example. We discuss the restriction of π2,1{\pi}_{2,1} to D𝒮¯\overline{D_{\mathcal{S}}}. We consider the set FD𝒮F_{D_{\mathcal{S}}} of all points in the following. This is finite thanks to the real algebraic situation.

  • Points in D𝒮¯\overline{D_{\mathcal{S}}} which are also in exactly two distinct curves Sj1S_{j_{1}} and Sj2S_{j_{2}}.

  • If we remove the finite set before from the set D𝒮¯D𝒮\overline{D_{\mathcal{S}}}-D_{\mathcal{S}} of dimension 11, then we have a smooth manifold of dimension 11 (a curve which is not necessarily connected) and which has no boundary. Points which are singular points of the restriction of π2,1{\pi}_{2,1} to the obtained smooth curve in D𝒮¯D𝒮\overline{D_{\mathcal{S}}}-D_{\mathcal{S}}.

We can define the following equivalence relation D𝒮{\sim}_{D_{\mathcal{S}}} on D𝒮¯\overline{D_{\mathcal{S}}}: two points are equivalent if and only if they belong to a same component of the preimage of a single point for the restriction of π2,1{\pi}_{2,1} to D𝒮¯\overline{D_{\mathcal{S}}}. Let qD𝒮q_{D_{\mathcal{S}}} denote the quotient map and VD𝒮V_{D_{\mathcal{S}}} the function uniquely defined by the relation π2,1=VD𝒮qD𝒮{\pi}_{2,1}=V_{D_{\mathcal{S}}}\circ q_{D_{\mathcal{S}}}. The quotient space WD𝒮:=D𝒮¯/D𝒮W_{D_{\mathcal{S}}}:=\overline{D_{\mathcal{S}}}/{\sim}_{D_{\mathcal{S}}} is a digraph by the following. We can check this from general theory [21, 22] or see [12] for example: we do not need to understand this theory.

  1. (1)

    The vertex set is the set of all points vv whose preimage qD𝒮1(v){q_{D_{\mathcal{S}}}}^{-1}(v) contains at least one point of the finite set FD𝒮F_{D_{\mathcal{S}}} above.

  2. (2)

    The edge connecting v1v_{1} and v2v_{2} are oriented as one departing from v1v_{1} and entering v2v_{2} according to VD𝒮(v1)<VD𝒮(v2)V_{D_{\mathcal{S}}}(v_{1})<V_{D_{\mathcal{S}}}(v_{2}).

Definition 2.

We call the (di)graph above a Poincaré-Reeb (di)graph of D𝒮D_{\mathcal{S}}.

As this graph, we can consider a situation where for a graph GG, a nice map VGV_{G} on its vertex set onto a partially ordered set PP is given and orients the graph according to the values. More precisely, each edge ee of the graph connects two distinct vertices ve,1v_{e,1} and ve,2v_{e,2} and it is oriented. Furthermore, it is oriented according to the rule: the edge ee departs from ve,1v_{e,1} and enters ve,2v_{e,2} if VG(ve,1)<VG(ve,2)V_{G}(v_{e,1})<V_{G}(v_{e,2}): let << denote the order on PP. We call a pair of such a graph GG and a map VGV_{G} a V-digraph. For V-graphs, isomorphisms between two V-digraphs and the notion that two V-digraphs are isomorphic can be defined, based on the property of preserving the orders of the values of the maps VGV_{G}. We can also define the Poincaré-Reeb V-digraph of D𝒮D_{\mathcal{S}} by associating the function VD𝒮V_{D_{\mathcal{S}}}.

1.3. Our main result.

Two graphs, digraphs, and V-digraphs are weakly isomorphic if there exists a homeomorphism regarded as an isomorphism after suitable addition of finitely many vertices: the edge sets of the graphs also change.

Theorem 1.

For any graph GG and a piecewise smooth function cG:Gc_{G}:G\rightarrow\mathbb{R} such that the restriction cGe{c_{G}}{\mid}_{e} is injective for each edge ee of GG, we can canonically give GG the structure of a V-digraph by the function cGc_{G}. We also assume the following.

  1. (1)

    The function cGc_{G} is the composition of some piecewise smooth embedding eG:G2e_{G}:G\rightarrow{\mathbb{R}}^{2} with π2,1{\pi}_{2,1}.

  2. (2)

    The degree of each vertex of GG is not 22. The local extremum of cGc_{G} must be achieved at a vertex of degree 11.

Then we have a refined algebraic domain DGD_{G} and its Poincaré-Reeb V-digraph of DGD_{G} and the V-digraph GG are weakly isomorphic.

Note that [2] has shown a generic case: the degrees of vertices are always 11 or 33 with the values of cGc_{G} at distinct vertices being always distinct. They only consider real algebraic domains: curves are mutually disjoint. On the other hand, the resulting V-digraphs have been shown to be isomorphic in the case. The constraint that curves are the zero sets of some real polynomials is not considered there and the author has commented first in [11]: in the original study the curves are only unions of some connected components of the zero sets.

1.4. Organization of our paper and our main work.

In the next section, we show Theorem 1. In the third section, we introduce that our graph is regarded as the so-called Reeb graph of a nice real algebraic function. The Reeb graph of a smooth function is a classical and fundamental object ([20]). This is defined as the quotient space of the manifold similarly to Poincaré-Reeb graphs. This represents the manifold compactly. This also gives a new answer to the following: can we reconstruct a real algebraic function whose Reeb graph is isomorphic to the given graph? We also present related studies since the birth of the study by Sharko ([23]), in 2006, reconstructing nice differentiable (smooth) functions on closed surfaces.

2. A proof of Theorem 1.

In this section, we prove Theorem 1, our main new result.

We use fundamental arguments from singularity theory and real algebraic geometry. Especially, approximations.

See [6] for singularity theory of differentiable maps. For example, we mainly consider the Hesse matrix of a differentiable maps of the class C2C^{2}, the symmetric matrix canonically defined as the matrix of the second derivatives. Smooth functions such that the determinant of the Hesse matrix, or the Hessian, at each point of the space of the domain is not 0, are important. Such a function is also a so-called Morse function. A Morse-Bott function is a smooth function whose singular point is represented as the composition of a smooth map with no singular point with a Morse function for suitable local coordinates.

See [1, 14, 15] for real algebraic geometry, for example. See also [3] for approximations by real polynomials.

Last, our present approximation mainly respects [2] as an explicit and important case and revises some. We respect these arguments from singularity theory and approximations implicitly.

Related to this, see also [11] where we do not assume the arguments from the preprint.

Hereafter, an ellipsoid of 2{\mathbb{R}}^{2} centered at a point x0=(x0,1,x0,2)x_{0}=(x_{0,1},x_{0,2}) means a set of the form {x=(x1,x2)2a1(x1x0,1)2+a2(x2x0,2)2r}\{x=(x_{1},x_{2})\in{\mathbb{R}}^{2}\mid a_{1}{(x_{1}-x_{0,1})}^{2}+a_{2}{(x_{2}-x_{0,2})}^{2}\leq r\} where a1,a2,r>0a_{1},a_{2},r>0. Sets of this type are also important.

A proof of Theorem 1.

We consider the graph eG(G)2e_{G}(G)\subset{\mathbb{R}}^{2}. We can change the graph eG(G)e_{G}(G) which is also a CW complex as follows.

Here, we choose sufficiently small positive numbers ϵ1,ϵ2>0{\epsilon}_{1},{\epsilon}_{2}>0. We can choose them so that we can argue with no problem. We can see this by following our arguments.

First we consider a point pp\in\mathbb{R} where the preimage π2,11(p){{\pi}_{2,1}}^{-1}(p) contains at least one vertex of eG(G)e_{G}(G). We can choose vertices vp,m=(p,pm)v_{p,{\rm m}}=(p,p_{{\rm m}}) and (p,pM)(p,p_{{\rm M}}) contained in the preimage in such a way that the value pmp_{{\rm m}} is the minimum of the values of the second components among such vertices in the preimage and that the value pMp_{{\rm M}} is the maximum of the values of the second components among such vertices in the preimage. We first add a segment Sp:={(p,y)pmϵ2ypM+ϵ2}S_{p}:=\{(p,y)\mid p_{{\rm m}}-{\epsilon}_{2}\leq y\leq p_{{\rm M}}+{\epsilon}_{2}\}.

We have a new CW complex eG(G)Spe_{G}(G)\bigcup S_{p}. Let vp:=(p,pv)eG(G)2v_{p}:=(p,p_{v})\in e_{G}(G)\subset{\mathbb{R}}^{2} be a vertex such that cGc_{G} does not have a local extremum at eG1(vp)G{e_{G}}^{-1}(v_{p})\in G, which is also regarded as a vertex of GG.

Let NvN_{v} be a neighborhood represented as Nv:={x=(x1,x2)pϵ1<x1<p+ϵ1,pvϵ2<x2<pv+ϵ2}N_{v}:=\{x=(x_{1},x_{2})\mid p-{\epsilon}_{1}<x_{1}<p+{\epsilon}_{1},p_{v}-{\epsilon}_{2}<x_{2}<p_{v}+{\epsilon}_{2}\}.

We define Sp,ϵ:={(p,y)pm+ϵypMϵ}S_{p,{\epsilon}^{\prime}}:=\{(p,y)\mid p_{{\rm m}}+{\epsilon}^{\prime}\leq y\leq p_{{\rm M}}-{\epsilon}^{\prime}\} and Sp±ϵ12,ϵ:={(p±ϵ12,y)pm+ϵypMϵ}S_{p\pm\frac{{\epsilon}_{1}}{2},{\epsilon}^{\prime}}:=\{(p\pm\frac{{\epsilon}_{1}}{2},y)\mid p_{{\rm m}}+{\epsilon}^{\prime}\leq y\leq p_{{\rm M}}-{\epsilon}^{\prime}\} where another sufficiently small positive number ϵ>0{\epsilon}^{\prime}>0 is chosen.

The set π2,11(p±ϵ1)eG(G){{\pi}_{2,1}}^{-1}(p\pm{\epsilon}_{1})\bigcap e_{G}(G) is finite. There exists a curve in eG(G)e_{G}(G) and an edge departing from each point p±ϵ1,jp_{\pm{\epsilon}_{1},j} there to the vertex vpv_{p}. We change each of these curves to a union of two segments intersecting in a one-point set. More precisely, we can change and change the curves as follows.

For each curve in eG(G)e_{G}(G), the first segment is a straight segment departing from the point p±ϵ1,jp_{\pm{\epsilon}_{1},j} and entering another point p±ϵ12,jp_{\pm\frac{{\epsilon}_{1}}{2},j}, which is a point in NvSp±ϵ12,ϵN_{v}\bigcap S_{p\pm\frac{{\epsilon}_{1}}{2},{\epsilon}^{\prime}}. We also choose these segments as mutually disjoint ones.

Next, for each curve, the second segment is chosen as the unique horizontal segment connecting p±ϵ12,jp_{\pm\frac{{\epsilon}_{1}}{2},j} and a point in the segment Sp,ϵS_{p,{\epsilon}^{\prime}}, which can be uniquely chosen. We also construct the segments in such a way that the horizontal segments from points pϵ12,jp_{-\frac{{\epsilon}_{1}}{2},j}, the values of whose first components are pϵ12p-\frac{{\epsilon}_{1}}{2}, are beyond the horizontal segments from points p+ϵ12,jp_{+\frac{{\epsilon}_{1}}{2},j}, the values of whose first components are p+ϵ12p+\frac{{\epsilon}_{1}}{2}. Thus Nv(eG(G)Sp)N_{v}\bigcap(e_{G}(G)\bigcup S_{p}) is changed.

For all of such vertices vpv_{p} and values pp\in\mathbb{R} with the preimages π2,11(p){{\pi}_{2,1}}^{-1}(p) containing some vertices in the graph eG(G)e_{G}(G), we can do similarly and do. We also remove SpvpNv¯S_{p}-{\bigcup}_{v_{p}}\overline{N_{v}} for all the values pp here. Thus we have a new 1-dimensional CW complex GϵG_{\epsilon} from eG(G)e_{G}(G).

For GϵG_{\epsilon}, we can consider a sufficiently small regular neighborhood [7] as a 22-dimensional smooth compact submanifold MDM_{D} in 2{\mathbb{R}}^{2}. We can also choose MDM_{D} in such a way that the boundary MSM_{S} is the zero set of some real polynomial and a non-singular set according to the presented theory on approximation. More precisely, we can do so that the restriction of π2,1{\pi}_{2,1} to the boundary MSM_{S} satisfies the following.

  • The restriction is a Morse function.

  • All of singular points of the restriction is as follows.

    • Each singular point of the function is corresponded to either a vertex of eG(G)e_{G}(G) of degree 11 which is also sufficiently close or a connected component of NvGϵN_{v}-G_{\epsilon} whose closure contains no point of the form (x,pv±ϵ2)(x,p_{v}\pm{\epsilon}_{2}) where all vertices vpv_{p} as argued above are considered.

    • In addition, the correspondence is a one-to-one correspondence. We name the singular point of the function of the first (second) type a definite (resp. indefinite) type.

    • At a definite type singular point svMSs_{v}\in M_{S} of the function the value is greater (resp. smaller) than the value cG(π2,1(v))c_{G}({\pi}_{2,1}(v)) at the corresponding vertex vv of eG(G)e_{G}(G) if cGc_{G} has a local maximum (resp. minimum). Note that the values are also sufficiently close.

    • Each indefinite type singular point sv,jMSs_{v,j}\in M_{S} of the function is in the corresponding connected component of NvGϵN_{v}-G_{\epsilon} whose closure contains no point of the form (x,pv±ϵ2)(x,p_{v}\pm{\epsilon}_{2}) and sv,js_{v,j} is sufficiently close to the segments SpS_{p} and Sp,ϵS_{p,{\epsilon}^{\prime}}.

We can put a sufficiently small suitable ellipsoid centered at an indefinite type singular point si:=(si,1,si,2)s_{{\rm i}}:=(s_{{\rm i},1},s_{{\rm i},2}) of the function in 2{\mathbb{R}}^{2} in such a way that the boundary of the ellipsoid contains a point (p,si,2)(p,s_{{\rm i},2}). At a definite type singular point sd:=(sd,1,sd,2)s_{{\rm d}}:=(s_{{\rm d},1},s_{{\rm d},2}) of the function, we can put a sufficiently small circle containing exactly two points in MSM_{S} in such a way that one of the points is of the form (p,sd,p)(p,s_{{\rm d},p}) and sufficiently close to sds_{{\rm d}} and that the restriction of the projection π2,1{\pi}_{2,1} to the intersection of the small circle and MDM_{D} is injective.

We have a new set by removing the intersection of MDM_{D} and each ellipsoid and the disk bounded by each new small circle from MDM_{D}. We naturally have a new refined algebraic domain DGD_{G} and we can check that this is our desired refined algebraic domain.

For arguments here, see also FIGUREs 13.

Refer to caption
Figure 1. Around a vertex vpeG(G)v_{p}\in e_{G}(G) and NvN_{v}. The set Nv(eG(G)Sp)N_{v}\bigcap(e_{G}(G)\bigcup S_{p}) (, in the upper part,) is changed.
Refer to caption
Figure 2. Around a connected component of NvGϵN_{v}-G_{\epsilon} whose closure contains no point of the form (x,pv±ϵ2)(x,p_{v}\pm{\epsilon}_{2}). The blue region shows (the interior of) MDM_{D} partially and the red ellipsoid is added.
Refer to caption
Figure 3. Around a vertex of degree 11 of eG(G)e_{G}(G). The blue region shows (the interior of) MDM_{D}, containing the graph eG(G)e_{G}(G), partially. The red circle (with the disk bounded by this) is added.

This completes the proof. ∎

3. Relations with Reeb graphs of real algebraic functions.

This section presents a kind of applications to construction of examples in real algebraic geometry and singularity theory of differentiable (smooth) maps. We assume several arguments from the published article [9] and our preprints [10, 11, 12].

We can define the Reeb (V-di)graph of a smooth function c:Xc:X\rightarrow\mathbb{R} on a closed manifold as follows. These graphs have been classical and strong tools in understanding the manifolds ([20]).

Two points of XX are equivalent if and only if they are in a same connected component of the preimage c1(y)c^{-1}(y). Let c{\sim}_{c} denote the equivalence relation and Wc:=X/cW_{c}:=X/{\sim}_{c} the quotient space. Let qc:XWcq_{c}:X\rightarrow W_{c} denote the quotient map associated with the unique continuous function c¯:Wc\bar{c}:W_{c}\rightarrow\mathbb{R} satisfying c=c¯qcc=\bar{c}\circ q_{c}. The vertex set of WcW_{c} can be defined as the set of all elements vv such that the preimage qc1(v){q_{c}}^{-1}(v) contains at least one singular point of cc in the case where the image of the set of all singular points of cc is a finite set ([21, 22]). The graph is the Reeb graph of cc and the pair of the graph with (the restriction of) the function c¯\bar{c} (to the vertex set) is the Reeb V-digraph of cc.

We define a surjective map m𝒮,A:𝒮Am_{\mathcal{S},A}:\mathcal{S}\rightarrow A onto some finite set AA. We also pose the constraint that for two distinct curves Sj1,Sj2𝒮S_{j_{1}},S_{j_{2}}\in\mathcal{S} which intersect in D𝒮¯\overline{D_{\mathcal{S}}}, the values of the map are distinct. We also define another positive integer valued function m𝒮,A,0m_{\mathcal{S},A,0} on AA. Let S:={(x,(ya)aA)2×aAm𝒮,A,0(a)+1jm𝒮,A1(a)(fj(x))Σj=1m𝒮,A,0(a)+1ya,j2=0,aA}S:=\{(x,(y_{a})_{a\in A})\in{\mathbb{R}}^{2}\times{\prod}_{a\in A}{\mathbb{R}}^{m_{\mathcal{S},A,0}(a)+1}\mid{\prod}_{j\in{m_{\mathcal{S},A}}^{-1}(a)}(f_{j}(x))-{\Sigma}_{j=1}^{m_{\mathcal{S},A,0}(a)+1}{y_{a,j}}^{2}=0,a\in A\}: here for the notation ya,jy_{a,j} is the jj-th component of yam𝒮,A,0(a)+1y_{a}\in{\mathbb{R}}^{m_{\mathcal{S},A,0}(a)+1} for example. This is the zero set of a real polynomial map in 2×aAm𝒮,A,0(a)+1{\mathbb{R}}^{2}\times{\prod}_{a\in A}{\mathbb{R}}^{m_{\mathcal{S},A,0}(a)+1} and non-singular. We omit precise arguments. See [10]. [12] also presents this. We consider the restriction of πΣaA(m𝒮,A,0(a)+1)+2,1{\pi}_{{\Sigma}_{a\in A}(m_{\mathcal{S},A,0}(a)+1)+2,1} to SS. The Reeb V-digraph of the resulting function is isomorphic to the Poincaré-Reeb V-digraph of D𝒮D_{\mathcal{S}}. See [10, 12] again and see also [9] and the preprint [11]. By our construction, we can check that the resulting function is a Morse-Bott function.

Related to this we explain history of reconstruction of nice smooth functions and the manifolds from given graphs.

[23] is a pioneering study, constructing nice smooth functions whose Reeb graphs are isomorphic to given finite graphs of a certain nice class. The functions are locally elementary polynomials. This is extended in [17] to the case of all finite graphs. [18] studies the Morse function case mainly the case of functions on closed surfaces. [16, 19] study a kind of general theory of Morse functions and their Reeb graphs. [19] mainly studies deformations of Morse functions via deformations of Reeb graphs. Following [19], [16] studies classifications of Morse functions on manifolds of general dimensions via systems of hypersurfaces, represented as preimages of the functions, for example. [4, 5] study the Morse-Bott function case, mainly the case of functions on closed surfaces. [8] studies cases of functions of certain classes naturally generalizing the classes of Morse-Bott functions on 33-dimensional closed manifolds where surfaces of preimages of points are prescribed. This is regarded as a pioneering study considering cases where preimages of single points are prescribed before reconstruction of functions.

The case of globally real algebraic functions is pioneered in [9].

Our theorem gives a kind of new answers to the real algebraic case. We can reconstruct real algebraic functions whose Reeb graphs are only homeomorphic to the given graphs. Related to this, [4] is for reconstruction of Morse-Bott functions in the differentiable (smooth) situation whose Reeb graphs are only homeomorphic to the given graphs.

4. Conflict of interest and Data availability.

Conflict of interest. The author works at Institute of Mathematics for Industry (https://www.jgmi.kyushu-u.ac.jp/en/about/young-mentors/). This is closely related to our study. We thank them for supports and encouragement. The author is also a researcher at Osaka Central Advanced Mathematical Institute (OCAMI researcher), which is supported by MEXT Promotion of Distinctive Joint Research Center Program JPMXP0723833165. He is not employed there. We also thank them. The author would also like to thank the conference ”Singularity theory of differentiable maps and its applications” (https://www.fit.ac.jp/\simfukunaga/conf/sing202412.html) for an opportunity to present [9, 10, 11]. Comments presented there have motivated the author to study further including the present study. This conference is also supported by the Research Institute for Mathematical Sciences, an International Joint Usage/Research Center located in Kyoto University.
 
Data availability.
Data essentially related to our present study are all in the present file.

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