Rep-tiles
Abstract.
An -dimensional rep-tile is a compact, connected submanifold of with non-empty interior which can be decomposed into pairwise isometric rescaled copies of itself whose interiors are disjoint. We show that every smooth compact -dimensional submanifold of with connected boundary is topologically isotopic to a polycube that tiles the -cube, and hence is topologically isotopic to a rep-tile. Consequently, there is a rep-tile in the homotopy type of any finite CW complex. In addition to classifying rep-tiles in all dimensions up to isotopy, we also give new explicit constructions of rep-tiles in all dimensions, including examples in the homotopy type of any finite bouquet of spheres.
1. Manifolds which are rep-tiles
We prove that every compact codimension- smooth submanifold of with connected boundary can be topologically isotoped to a polycube which tiles the cube . As a consequence, any such manifold is topologically isotopic to a rep-tile, defined next. A rep-tile is a codimension-0 subset of with non-empty interior which can be written as a finite union of pairwise isometric sets each of which is similar to ; and such that have non-intersecting interiors whenever . A rep-tile in which is also homeomorphic to a compact smooth manifold will be called a -dimensional rep-tile.
Since every -dimensional rep-tile has connected boundary (Lemma 3.2), as does every -dimensional manifold that tiles the -cube, our result proves that any submanifold of which could potentially be homeomorphic to an -dimensional rep-tile is in fact isotopic to one. Thus, our work completes the isotopy classification of manifolds that tile the cube, and of -dimensional rep-tiles, in all dimensions.
Early sightings of rep-tiles were recorded in [Gar63, Gol64]. Because -dimensional rep-tiles tile , rep-tiles have been studied not only for their intrinsic beauty but also in connection with tilings of Eucidean space; see [Gar77] or [Rad21] for a discussion of the case . A notable achievement was a non-periodic tiling of the plane by a rep-tile, due to Conway, which was later used to create the first example of a pinwheel tiling, i.e. one in which the tile occurs in infinitely many orientations [Rad94]. The elegant 2-dimensional rep-tile portrayed in Figure 1 was the building block in one of Goodman-Strauss’s constructions of a hierarchical tiling of [Goo98] and is also found in [Thu89].

The first planar rep-tile with non-trivial fundamental group was discovered by Grünbaum, settling a question of Conway [Cro91, C17]. In 1998, Gerrit van Ophuysen found the first example of a rep-tile homeomorphic to a solid torus, answering a question by Goodman-Strauss [vOp97]. Tilings of of higher genus were also constructed in [Sch94]. Tilings of by mutually isometric knots were constructed by [Oh96]. Adams proved that any compact submanifold of with connected boundary tiles it [Ada95]. Building on the above work, in 2021 came the homeomorphism classification of 3-dimensional rep-tiles.
Theorem 1.1.
[Bla21] A submanifold of is homeomorphic to a 3-dimensional rep-tile if and only if it is homeomorphic to the exterior of a finite connected graph in .
The above implies that any 3-manifold which could potentially be homeomorphic to a rep-tile is indeed homeomorphic to one. This follows from Fox’s re-embedding theorem [Fox48], which classifies compact 3-manifolds that embed in , together with Lemma 3.2, which shows that a rep-tile has connected boundary.
Our main result is Theorem 1.2, which completes the isotopy classification of manifold rep-tiles in all dimensions, without relying on a classification of codimension-0 submanifolds of .
Theorem 1.2.
Let be a compact smooth -manifold with connected boundary. Then, is topologically isotopic to a rep-tile.
Corollary 1.2.1.
Let be a compact connected CW complex of dimension . Then is homotopy equivalent to a -dimensional rep-tile.
Proof.
Suppose that is a compact connected CW complex of dimension . Then, embeds in , by the Nöbeling-Pontryagin Theorem [Den90, p. 125, Theorem 9]. Let be a closed regular neighborhood of in . Then is a compact -manifold embedded in . Moreover, has a single boundary component. Indeed, suppose has two or more connected components Since is a closed manifold embedded in , it is orientable, so . Moreover, since , we have that for each Therefore, we see from the long exact sequence of the pair that the inclusion-induced map is injective. But has the homotopy type of an -complex, which is a contradiction. Therefore, by Theorem 1.2, is isotopic to a rep-tile. ∎
The proof of Theorem 1.2 describes a procedure for isotoping any codimension-0 smooth submanifold of with connected boundary to a rep-tile. While the proof is constructive, in effect it is done without writing down any new rep-tiles. In Section 2 we therefore also give, for any , an explicit construction of a rep-tile homeomorphic to . This leads to an almost equally explicit construction of a rep-tile in the homotopy type of any finite bouquet of spheres. In particular, we can build explicit rep-tiles with non-vanishing homotopy groups in arbitrarily many dimensions.
The paper is organized as follows: in Section 2 we construct a rep-tile homeomorphic to , presented explicitly as a union of cubes in , introduce the technique of ball swapping, show how to construct rep-tiles homotopy equivalent to wedges of spheres, investigate suspensions of rep-tiles, and construct rep-tiles with arbitrary footprints. Section 3 is where we prove the main theorem.
1.1. Rep-tiles and tilings of Euclidean space
Rep-tiles induce self-similar tilings of Euclidean space. Thus, they can potentially be used to construct non-periodic and aperiodic tilings of the plane and higher-dimensional Euclidean spaces. Self-similar tilings have connections to combinatorial group theory [Con90], propositional logic [Wan60, Ber66, Rob71] (where some of the questions in the field originated), and dynamical systems [Thu89], among others. Our rep-tiles give new self-similar tilings of by tiles with interesting topology. Additionally, in our proof of Theorem 1.2 we show that every compact smooth -manifold with connected boundary in is topologically isotopic to a polycube that tiles a cube. In [Gol66], Golomb developed a hierarchy for polycubes that tile , and tiling a cube is the most restrictive level of his hierarchy. Hence all compact smooth -manifolds with connected boundary lie in the most restrictive level of Golomb’s hierarchy, up to isotopy.
2. Explicit rep-tiles in all dimensions
In this section, an -dimensional polycube is a union of unit -cubes whose vertices lie on the integer lattice in . We will be repeatedly using the fact that a polycube that tiles a cube is a rep-tile (see Lemma 3.1). In this section we will realize the homotopy type of certain -manifolds as rep-tiles by the following procedure. We will construct a polycube such that (where denotes homotopy equivalence) and such that two copies of , related by a rotation, tile the -dimensional cube. In the case where has the homotopy type of a sphere, , the rep-tile we build is homeomorphic to a trivial 2-dimensional disk bundle on the sphere, . (This demonstrates that rep-tiles can have non-trivial for all answering Conway’s and Goodman-Strauss’s question in dimensions three and higher.) It is a fairly straightforward consequence that finite wedges of spheres of different dimensions can be built similarly.
2.1. Stacks of cubes
A stack of -cubes with stacking direction is an -dimensional polycube such that: (1) All -cubes in lie above the hyperplane (that is, every point in has non-negative coordinate), and (2) for every -cube in that does not have a face contained in , there is another -cube of directly below it (where height is measured by the -axis).
Let the subspace of determined by have the standard tiling by -cubes induced by the integer lattice in . Given , a stack of -cubes with stacking direction , we consider its projection to the hyperplane , which we call its footprint. By the definition of a stack of cubes, we can think of as consisting of columns of -cubes lying above each -cube in its footprint , which is itself an -dimensional polycube. In other words, the homotopy type of is determined by ; and itself is determined by , together with integer labels in each -cube of , specifying the height of the column of -cubes which lie above it. Therefore, we can describe by such a labeled footprint. Figure 2 illustrates a 2-dimensional stack of cubes (left) and its description via a labeling on its 1-dimensional footprint (right).
The image of such a stack of cubes under an isometry of is also called a stack of cubes, with the image of under the isometry being the stacking direction.

2.2. Rep-tiles homotopy equivalent to .
We use cube-stacking notation as above to describe a rep-tile homeomorphic to for all . This description is a simplification, suggested by Richard Schwartz [Sch25], of the construction given in [Bla24]. We define a stack of cubes as follows. The footprint is a polycube in .

Throughout the following discussion, the reader should refer to Figure 3. Define the core, denoted , of to be the union of unit cubes in the standard integer-lattice tiling of containing the point . The shell of is To create the labeled footprint of our stack of cubes , we first partition into two halves: , those containing cubes with -coordinate at least 2; and , those containing cubes with -coordinate less than 2. Finally, we label each cube in with a 4, and each cube in with a 0. All cubes in the shell are labeled 2. (We recall that the label of each -cube in the footprint indicates the height of the column of -cubes stacked on top of it.) Observe that , which consists of all unit cubes in with nonzero label, is homeomorphic to the shell, which is in turn homeomorphic to . Similarly, the stack of cubes determined by this labeling is homeomorphic to .
Next we show that is a rep-tile. Let denote rotation by about the -plane which is the intersection of and . Observe that the closure of the complement of in is also a stack of cubes, with stacking direction , is isometric to , and in particular, is the image of under As and tile the cube , and since is a union of cubes, is a rep-tile.
2.3. Ball swapping.
We note that there is a lot of flexibility regarding the heights of columns in the construction of a rep-tile given above. Consider any column in of height . Let denote the column of which shares a footprint with . Since form a column of height 4, the heights of and add up to 4. Moreover, unit cubes can be traded between and while preserving the property that the resulting polycube and its image under tile . As long as both columns remain of height strictly between 0 and 4 and their heights add up to 4, this swap preserves both the homeomorphism type of and the property that two copies of tile a cube.
More generally, let be any non-empty -dimensional polycube in . Let be a group of isometries of such that the orbit of under tiles a cube . (As before, this implies that is a rep-tile.) Let denote any unit cube contained in and let be an arbitrary element of . Denote by the image of under . We note that is also a polycube whose orbit under is . Hence, is also a rep-tile. We will refer to this move as a ball swap. (Aside: the fact that performing a ball swap on a polycube that tiles an -cube produces another polycube that tiles an -cube does not depend in an essential way on the fact that is a -cube. More complicated pieces could be swapped as well, preserving the tiling property.) Ball swapping, which was inspired by work of Adams [Ada95, Ada97], turns out to be a powerful tool for building rep-tiles, as we will see in Section 3. To be precise, a version of the ball swap – one which involves an action of a group of order on and trading multiple balls simultaneously across their individual orbits – is the key idea in the Proof of Theorem 1.2. The second main ingredient in the proof is this: a priori, might not have a clear relationship to ; to guarantee that is homeomorphic to or isotopic to , care must be taken in the choice of group action and the choice of .
2.4. Rep-tilean bouquets
Let . The construction in Section 2.2 has produced stacks of -dimensional cubes in with the following useful properties:
-
(1)
Each polycube intersects in an -ball equal to and intersects in an -ball equal to ;
-
(2)
the polycube and its image under rotation by about tile .
Note that any two such polycubes of the same dimension and can be placed side-by-side in the direction so that is contained in and is contained in . For example, place two copies of the stack of cubes in the top of Figure 3 back-to-back. In this configuration . Thus, has the homotopy type of the wedge ; and, after rescaling in the direction and subdividing the integer lattice, it too satisfies the conditions (1) and (2) above.
Now consider and , two of the rep-tiles constructed in Section 2.2 of dimension and respectively. If , then can be embedded in so that conditions (1) and (2) hold. By stacking and this embedding of as in the previous paragraph, we construct a rep-tile in the homotopy type of , itself capable of becoming part of a further rep-tilean wedge. By iterating this process, rep-tiles in the homotopy type of any finite wedge of spheres can be constructed.
2.5. Suspending Rep-Tiles
Let be an order 2 rotation about some -subspace in . We note that if is any connected -dimensional stack of cubes such that two copies of , related by , tile an -cube, then can be used to construct an -dimensional rep-tile in the homotopy type of the suspension of . We sketch this construction with a specific choice of coordinates below. For clarity, we assume that tile the cube .
Let denote any -dimensional stack of unit cubes which has the property that and its image under under tile . (For instance, could be one of the rep-tiles in the homotopy type of a wedge of spheres that we previously constructed.) Because we know that takes cubes at height 4 (with respect to the stacking direction) to holes at height zero; and vice-versa. In particular, contains as many cubes at height 4 as it has unit-cube-sized holes at height 0. Therefore, we may suspend as by the following steps
-
(1)
embed into ;
-
(2)
cubify in the natural way, writing as a union of unit -cubes of the form ;
-
(3)
move all height-4 cubes in to fill all holes at height zero in that slice;
-
(4)
repeat the last step in .
Crucially, steps 3 and 4 constitute ball swaps (see Section 2.3). This guarantees that the resulting polycube is still a rep-tile. Moreover, since the slice is a stack of cubes, filling all cubes that correspond to “height-0 holes” in (that is, those holes in which are height-0 holes in crossed with ) turns into a ball. Therefore, as before, ball swapping in the first and last slices of has the effect, up to homotopy, of contracting each of the ends of to a point. This completes the suspension of . Figures 4 and 5 illustrate the suspensions of rep-tiles homeomorphic to and , respectively.
Let and denote any pair of columns in Figures 4 or 5 which trade a cube during the ball-swapping operations. Specifically, say is height 0 and the top cube of is moved to during the ball swapping. Now suppose next highest cube of (now at height 3) is also moved to column . This would constitute a ball swap, since the unit cube remains within its orbit under the rotation. Executing this additional swap between all such pairs has the effect that all columns of heights 3 and 1 become columns of height 2. The result would be the rep-tile constructed in Section 2.2. Put differently, rep-tiles homeomorphic to can also be obtained from the rep-tile in Figure 2 inductively, via a sequence of suspensions and ball swaps. For details on this approach, see Section 2 of [Bla24].


Left column: four layers of , combining to form . Middle column: ball swapping occurs in the first and fourth slices. Right column: bottom slice: , second slice: ; third slice: ; fourth slice: . The union of the four slices is the suspended rep-tile.
Note that by a further ball swap we could replace all 3’s and all 1’s by 2’s. This would produce another rep-tile homeomorphic to , namely the one described in Section 2.2.
2.6. Rep-tiles with arbitrary footprints
The following was observed by Richard Schwartz [Sch25] while perusing the first version of our article.
Proposition 2.1.
[Sch25] There is an -dimensional rep-tile in the homotopy type of any compact polycube in .
This result, together with the existence of cubifications for smooth codimension-0 submanifolds of (see Section 3.5) can be used to prove a version of Corollary 1.2.1. Specifically, we see that it is possible to realize the homotopy type of any compact -dimensional CW complex as a -dimensional rep-tile , without appealing to Theorem 1.2. The present approach uses an extra dimension; but it is rather explicit (given a polycube footprint to start with) and has the advantage that just 2 copies of can tile the -cube.
Proof of Proposition 2.1.
We first observe that for any compact -polycube there is a positive even integer such that is isotopic to an -polycube in such that contains all unit cubes in whose smallest -coordinate is equal to . (To see this, begin by translating so that it is contained in . Then, apply the following sequence of isotopies: shift at least two units away from the hyperplane in the positive direction; then grow a (cubical) finger out of until it touches ; then add the cubes whose union is to .)
Next create an -dimensional stack of cubes whose footprint is a polycube in , namely the boundary connected sum of with . We shall label the -cubes contained in to indicate the height of the corresponding column. In this manner, we will obtain the desired stack of -cubes in the homotopy type of . The -cubes in are labeled . All -cubes which are contained in but not in are labeled 0. Let denote reflection in about the plane . Cubes in that are contained in are labeled . Remaining cubes are labeled . See Figure 6.
Let be rotation about the -plane in determined by and . Next we observe that the sum of the labels of each unit cube in and its reflection about sum to . It follows that the stack of cubes determined by this labeling, together with , tile . Then, after rescaling, two isometric copies of tile an -cube. This produces a rep-tile in the homotopy type of the original footprint, , as desired. ∎

3. All is rep-tile
We will denote the standard integer lattice in , consisting of all points in with integer coordinates, by . This lattice induces a cell structure on , whose -cells are the -facets of unit cubes with vertices in .
We will also work with subdivisions of this lattice, and refer to the closed -cells in any such decomposition as atomic cubes. The size of an atomic cube will depend on the subdivision used. Precisely, suppose and let denote the scaling function given by . Let , and let denote the corresponding cell structure.
Definition 3.1.
An -dimensional polycube is a submanifold of that is isometric to a finite union of atomic cubes in for some .
Definition 3.2.
A compact -manifold is said to -tile a subset if such that is isometric to for all and , and for all .
Lemma 3.1.
Let be an -dimensional polycube that tiles a cube . Then, is a rep-tile.
Proof.
By identifying each atomic cube in the polycube decomposition of with , we can tile each cube in with a finite number of pairwise isometric manifolds, each of which is similar to . We have thus tiled by rescaled copies of . ∎
In particular, a polycube that tiles the cube must have connected boundary, which follows from the following Lemma.
Lemma 3.2.
Let be a manifold which is homeomorphic to an -dimensional rep-tile. Then is non-empty and connected.
Proof.
Since is a homeomorphic to a rep-tile, we have that embeds in . Hence, . The proof that is connected when is given in [Bla21, Theorem 4.2] and works without modification in all dimensions. ∎
We recall our main theorem below.
Theorem 1.2.
Let be a compact smooth -manifold with connected boundary. Then, is topologically isotopic to a rep-tile.
Our main theorem is a consequence of the following.
Theorem 3.3.
Let be a compact smooth -manifold with connected boundary. Then, is topologically isotopic to a -dimensional polycube which -tiles a cube.
A key step in the proof that any satisfying the hypotheses of Theorem 1.2 is isotopic to a rep-tile is to decompose , the closure of the complement of in an -cube, into a union of closed -balls with non-overlapping interiors. Given a manifold , the smallest number of -balls in such a decomposition of is called the ball number of , denoted . Upper bounds on the ball number of a manifold in terms of its algebraic topology have been found by Zeeman [Zee63] and others [Luf69, Kob76, Sin79]. We rely on the following.
Theorem 3.4.
[2.11 of [Kob76]] Let be a connected compact PL -manifold with non-empty boundary. Then .

3.1. Overview of the proof of Theorem 1.2
The main ingredient is Theorem 3.3, which we prove using a strategy we refer to as a ball swap. To start, is smoothly embedded in so that . In turn, the unit cube sits inside the cube . Since is disjoint from and has a single boundary component, is connected. By Theorem 3.4, we may decompose into -dimensional balls .111If , one could use fewer balls here and tile the cube with fewer copies of , but we use balls for simplicity in the proof of the main theorem. After a homotopy of which restricts to an isotopy on each piece of the decomposition of , we ensure that the pieces of this decomposition intersect an -disk on as shown in Figure 8, in what we call a taloned pattern. The defining features of taloned patterns include: there is an -disk on such that and each of intersect that disk in an -ball and intersect the boundary of the disk in an -ball; the -balls are disjoint inside this disk; and is adjacent to each ball in this disk. (See Section 3.2 for the formal definition.) The homotopy used to create the taloned pattern is achieved in Lemmas 3.5 and 3.6 below. We then isotope so that the -disk which constitutes the taloned pattern of Figure 8 is identified with the union of faces of whose interiors lie in the interior of , with certain additional restrictions. These restrictions guarantee that certain rotated copies of the contained in cubes adjacent to in are disjoint, allowing us to form the boundary connected sum of with these balls without changing the isotopy class of . Indeed, we give a family of rotations , , together with one additional rotation if is odd, such that the orbit of under these rotations tiles . By taking the boundary sum of with the image of each under an appropriate choice of rotation above, we obtain the desired manifold . By construction, is isotopic to and, moreover, the orbit of under the above set of rotations gives a tiling of . A 2-dimensional tile created via ball swapping is shown in Figure 7. A sketch of in dimension is shown in Figure 14. Finally, we show that this construction can be “cubified”, so that is a polycube tiling , completing the proof of Theorem 3.3. Once this is established, Theorem 1.2 follows from Lemma 3.1.
3.2. Taloned Patterns
We define the desired boundary pattern described above. A -claw is a tree which consists of one central vertex and leaves, each connected to by a single edge. See Figure 8.

Our goal is to construct a boundary pattern on such that there exists an embedded disk with the following properties:
-
•
is a single -disk, for all ;
-
•
is an -disk, for all ;
-
•
.
-
•
for .
We regard the boundary pattern as the regular neighborhood of a -claw, with the following decomposition: contains a neighborhood of the central vertex; and each containing a neighborhood of a leaf. See Figure 8. We call this a taloned pattern of intersections.
We begin by proving Lemma 3.5, which ensures that, in the interior of , the union of the boundaries of the pieces in the interior of our decomposition of can be assumed to be connected.
Lemma 3.5.
Let be a compact -manifold with a single boundary component embedded in the -cube such that , where each is an -ball, and such that the interiors of and the are pairwise disjoint. Then after a homotopy of which restricts to isotopies on the interiors of and the , is a connected -complex.
Proof.
Let . We partition into layers as follows (see Figure 9). Define the first layer as . We will use the notation . Next choose a minimal collection of disjoint, embedded paths on such that
-
•
is connected,
-
•
the interior of is contained in a single element of ; and
-
•
no has both endpoints on the same connected component of .


Note that any given element of the decomposition may contain the interior of more than one of the paths , i.e., it is possible to have for . For each , we let denote the set of all such that .
Since the are disjoint, for each , we can choose a disjoint regular neighborhood in of such that intersects the boundary of exactly two other elements and of , one at each of the endpoints and , respectively. For each , let denote the set of all such that . Next, modify the decomposition of as follows (see Figure 10).
-
•
For each , delete all the whose interiors intersect , replacing each by
-
•
Then, attach each to , replacing each (which may coincide with , if did not intersect the interior of any ) by
This process can be achieved by a homotopy of which restricts to isotopies on the interiors of the elements of . We imagine elements of as growing fingers along the . From now on, we will simply call these finger moves and will not describe them explicitly.
After performing finger moves on the elements of along the , we can assume is connected. Then inductively define , where is defined analogously to . Since is connected for each and meets , we have that is connected. Continue inductively for each , where is the number of layers. By construction, is connected for each and intersects non-trivially. Therefore is connected, so is connected as well. ∎
Lemma 3.6.
Let be a compact -manifold with connected boundary embedded in the -cube such that , with , where each is a -ball and such that the interiors of and the are pairwise disjoint. After applying a self-homotopy of that restricts to an isotopy on the interior of each component in the above decomposition, we can find an -claw embedded in such that its regular neighborhood in is a taloned pattern.
Proof.
By Lemma 3.5, we can assume is connected, so we can perform a finger move on along a path in to ensure that meets . Since has a single boundary component and , we can assume there exists a point on the interior of an face of that lies on for some . Relabeling the if necessary, we assume .
Without loss of generality, assume lies on the face defined by , and let . After an isotopy of , we can assume some -ball satisfies the following:
We can further assume that and .
Choose distinct points on the disk , as in Figure 11. We claim that one can choose disjoint paths from a point in to the point for each .
To produce the , we again apply Lemma 3.5. In dimensions 4 and higher, we can achieve disjointness of the by a perturbation. In dimension 3, we perform an oriented resolution at each point of intersection of the ’s which can not be removed by perturbation inside . In dimension 2, there is only one such path, , since
Once the paths are disjoint, we perform a finger move which pushes a neighborhood of in along to a neighborhood of in . As a result, the balls intersect in the boundary pattern shown in Figure 11 (middle). We then choose a claw as shown in Figure 11 (bottom). The regular neighborhood of this claw in is isotopic to a taloned pattern (Figure 8), as desired. ∎

3.3. Proof of main theorem.
We begin by setting up the necessary notation. For each , let be the -dimensional face of the -cube contained in the hyperplane . For the moment, we will assume that is even. The case of odd requires an extra step, which we leave until the end of the proof.
Let be the rotation by about the -plane that carries the axis to the axis. Note that each has order four and that these rotations commute, generating a group isomorphic to . Given a vector , we define the rotation as follows:
We set
We claim that the orbit of a unit sub-cube under this group action is the entire -dimensional cube . In other words, is tiled by the distinct unit cubes
To see this, first decompose into unit sub-cubes of the form , where each is either or . Fixing , for each choice of and from the set , the product is a unit square in the plane, which we denote by Let , i.e is the unit square in the first quadrant of . Then for some . Hence, each of the unit cubes above can be expressed as
for some . Moreover, for each , the such that is unique. To see this, note that each has exactly one corner with all nonzero coordinates (and therefore with all coordinates ). On the other hand, the cube also has exactly one corner with all (namely, the image of the point ), and its coordinates satisfy the formula In other words, the coordinates uniquely determine each component and therefore itself.
Observe that the cube intersects along its face , and the cube intersects along its face . Thus, each rotation gives a pairing of the faces of . We use this pairing to carry out a ball swap as previously described. This will allow us to build the rep-tile .
3.4. Realizing the taloned pattern on
We will now describe a homotopy of which restricts to an isotopy on the interiors of and the balls . Our goal is to use Lemma 3.6 to position and so that their intersections with the boundary of satisfy:
-
(1)
For each , the only ball meeting the face is (and thus ),
-
(2)
is disjoint from , and
-
(3)
is disjoint from .
In what follows, we refer the reader to a schematic in Figure 12. Figure 13 illustrates this configuration in dimension 4.
For each , let be the -facet in equal to the intersection of with the -plane given by setting and . Likewise, let be the -facet in equal to the intersection of with the -plane given by setting and . Note that this pair of facets are exactly those that are simultaneously parallel to the intersection and contained in .


Now, we fix points and by setting
and
where the and entries are taken to be in the and coordinates.
Let be the -balls whose existence is guaranteed by Theorem 3.4. By Lemma 3.6, after an isotopy of and the , there is an -claw embedded in such that its regular neighborhood in is a taloned pattern as shown in Figure 8. Moreover, after an isotopy of supported near its boundary, we can assume that the taloned pattern is mapped homeomorphically to such that the intersection is a closed regular neighborhood of radius of the point in , and also that if , then . We do not assume any restrictions on the intersections of and the with the remaining faces of .
Note that this set-up has several convenient consequences. First, the union intersects in a single -ball, since meets the taloned pattern in a single -ball. Furthermore, the center and radius of were chosen to guarantee that the ball is disjoint from the neighborhood , and therefore contained in . Similarly, the ball is contained in .
3.5. Cubification of the decomposition
Recall that for any positive integer , by we denote the lattice in whose unit cubes have side length .
Let . Since and each can be assumed piecewise-smooth, has a closed regular neighborhood . Being a codimension-0 compact submanifold of it is isotopic to a polycube, also denoted , in a sufficiently fine lattice . (In the course of cubification, we shall increase as needed without further comment.) We also assume that all cubes in which intersect form a regular neighborhood of . Similarly for each ; and for each double intersection, or ; and each triple intersection, etc.
The closure is then also a polycube; similarly for each . To complete the cubification of the ensemble we assign cubes in back to the constituent pieces in an iterative fashion. Specifically, all cubes in which intersect are assigned to , and their union is denoted ; of the remaining cubes, all that intersect are assigned to , and the resulting polycube is denoted ; and so on. By the above assumptions, each of the pieces is isotopic to the corresponding polycube since we are only adding or removing small cubes intersecting the boundary. In addition, the union of the interiors of is isotopic to the union of the interiors of .
Furthermore, by selecting a sufficiently fine lattice, we can ensure that the isotopies performed, taking each of to a polycube, are arbitrarily small. Thus, they preserve properties (1), (2) and (3) from Section 3.4.
Recycling notation, we will from now on refer to , , , as , , , respectively.
3.6. Construction of the rep-tile.
Finally we construct our rep-tile :
We claim that (1) is isotopic to , and (2) isometric copies of tile the cube . A schematic of in dimension is shown in Figure 14 (for intuition in the case of even, simply ignore and its rotated copy in the figure).

Proof of (1). The images of the cube under the rotations give a family of distinct unit cubes in , each of which shares a unique face with . More specifically, the cube intersects along its face , and the cube intersects along its face Refer to Figure 12.
It follows that the intersections of each ball and with the cube are disjoint -balls contained in . (Recall that the center and radius of the were chosen carefully so that this is the case.) Therefore, is a boundary connected sum of with a collection of -balls, one in each neighboring cube. An isotopy therefore brings to the initial embedding of , as desired. This concludes the proof of (1).
Proof of (2). Let , , and . Note that, since , we have that and . In addition, the first equality on the next line clearly implies the second:
We now show that
Since decomposes into the cubes , it is sufficient to show that every point is contained in for some . This is a consequence of the fact that is the union of and one ball from the orbit of for each . However, this fact may not be self-evident, so we provide an explicit proof.
Consider a point . If is in the orbit of , then , so . Now, suppose for some . To find which rotation of contains , consider the isometric ball . There are two cases: if , then , and if , .
Let be the vector with equal to if and if . In other words, the vector is equal to the vector modified only by shifting its coordinate by . Observe that . This shows that indeed is equal to the union of the .
To show that is tiled by isometric copies of , we need to check that the have non-overlapping interiors. First observe that has -volume 1, and that has -volume . Since exactly isometric copies of make up , they must have disjoint interiors. This concludes the proof of (2).
3.7. Constructing the rep-tile in odd dimensions
We have yet to handle the case where is odd, i.e. for some integer . As before, let denote the face of intersecting the -plane where . In this case, in addition to the rotations defined above, we require an additional rotation by an angle of about the -plane where . Note that by definition, , and so carries to its neighboring cube in .
For , choose points as before. Choose the point on the -facet of where intersects the -plane . More specifically, we let
and be a neighborhood of in the face with radius . This guarantees that is disjoint from . Therefore, we can again define the boundary sum:
which is isotopic to and tiles as before. To complete our proof that is a rep-tile for any , we appeal to Lemma 3.1. ∎
Acknowledgments:
This paper is the product of a SQuaRE. We are indebted to AIM, whose generous support and hospitality made this work possible. AK is partially supported by NSF grant DMS-2204349, PC by NSF grant DMS-2145384, RB by NSF grant DMS-2424734, and HS by NSF grant DMS-1502525. We thank Kent Orr for many helpful discussions. We are grateful to Richard Schwartz for his feedback on the first version of this paper; and for numerous valuable suggestions, notably a simplification of our original construction of spherical rep-tiles.
Ball Number
Let be a frog with a cube for a bride
Place in a box with some balls beside
Set free, the balls
Dance through walls
Out plops a Rep-tile with frogs inside
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