3. The primitive Projection Method

Projection of a regular lattice of higher dimension into the real physical space of lower dimension is a very useful method to construct a model structure of general lattices unifying usual lattices and quasilattices; the well-known examples are one-dimensional quasilattice as a projection from two-dimension, 2D-PT from five-dimension and three-dimensional quasilattice from six-dimension. Calculations with computer are easily carried out by this method. Sometimes they are done without recognizing the features of the structure. It is, at the same time, a merit and demerit of this method. The procedure to construct a d-dimensional general lattices from a D-dimensional simple lattice can be summarized as follows.

(1) Regard the D-dimensional original space W as direct sum of d-dimensional physical space W and d (= D - d ³ D/2)-dimensional pseudospace W = W1 Å W2

(2) Select the lattice points in W whose projection to the pseudospace lies in a certain region GC (the gazing crystal) which is defined as a projection of a D-dimensional hypercube. A general lattice G is the projection of them to the physical space. A quasilattice Q is a general lattice without periodicity. Let L be a D-dimensional vector from a lattice point to another lattice point.

L= L1Å  L2 ,   Li   Î Wi   (i= 1 and 2)                                           (3.1)

G ={L1; L2  Î  GC   Ì   W2Î    W1                                           (3.2)

(3) Now, the projection from W to W1can be regarded as a mapping from W2 to W1. When the mapping is an injection, the general lattice is a quasicrystal.

Therefore, all the informations of an infinite quasiperiodic arrangement in the GC in the whole universe of physical space W1 are concentrated in a small region GC in the pseudospace W2. A whole network is collapsed into the small area GC, keeping its connectivity. Some fortune teller decodes she informations contained in the inside of GC into everything in physical space by gazing it. It is the reason why the area is referred to as the gazing crystal (GC). In the projection from 2-dimension to one-­dimension, the point sequence {yn} in GC is very similar to a chaotic behaviour in point sequences in a dynamical mapping or a Poincare mapping of a dynamical process. General cases can be regarded as chaotic motion in multi-dimensional or branching time from this point of view.

From a conceptual point of view, the method is summarized as

 A d-dimensional general lattice is constructed by the projection of the D-dimensional lattice points whose Voronoi cells cross the d­dimensional space.

and

 Any information of the generalized crystal in the physical space, of which a quasicrystals included as special cases, contained in the gazing crystal in the pseudo space. A whole generalized lattice is collapsed into the gazing crystal keeping its connectivity.

It is noted that a gazing crystal is a compound of DCD-d  unit cells because it is a projection of  D-dimensional hypercube into (D-d)-dimensional space. It rigorously leads to an important conclusion that there are no simple repeat of any pair of the same unit cells in the primitive projection model. It is the most characteristic feature of the model.

Some examples of the gazing crystals are listed in Table 7. (see Appendix B)

Table 7: Examples of Gazing Crystals

In Example 2, the primitive projection model, being (..LMLSMLMLSMLLMSLMLMSL..) has no self-similarity. There are several transformations leading to a self-similar arrangement. For example, L ® LM, M ® LS, S ® M (LMLSLMMLMLSLSLMLSLMM..) and L ® LMS, M ® LM, S ® L (LMSLMLLMSLMLMSLMSLML..). These sequences can be regarded as either of symbol sequence or point sequence of relative separation lengths L : M : S = a : b : g (in the foot note of Table 7) = a : b : 1 (in Appendix B).

In Fig.1, the gazing crystal of the third example (4-dim. to 2-dim.) is shown. The closer the point in the gazing crystal, the higher the symmetry or the wider the ruling area of the local symmetry of the corresponding point in the physical space. It is noted that the primitive projection method exactly corresponds to the transformation method in this case. The corresponding Penrose transformation is shown in Fig.2. Fig.1 The Gazing Crystal of Example 3 in Table7
Numbers in the figure are the number of direct
neighbours of a point in the region. Fig.2 The corresponding Penrose Transformation.
The two kinds of tiles are square and rhombohedron
of 45o-135o. The similarity factor is 1 + Ö2. The
edges should be regarded as a single kind of arrows.

4. Three-Dimensional Tiling Obtained by the Primitive Projection

Suppose a 6-dimensional simple hypercubic lattice where the lattice vectors are {uk; k = 1,2,...,6}. Introduce another orthonormal set (x, y, z, X, Y, Z) in the six­dimensional original space W so that they are expressed in terms of uk's as. and The space is regarded as the direct sum of three-dimensional physical space W1 spanned by (x, y, z) and three-dimensional pseudospace W2 spanned by (X, Y, Z). Six renormalized quasilattice vectors are the renormalized physical-space­components of six bases of the original space. They are in the Cartesian coordinate system (x, y, z) above. Here a , b, g, x, h and z are given in Eq.(2.1). The arrangement of {±Vk; k = 1,2,...,6} has icosahedral symmetry. The renormalized pseudospace-components of six bases of the original space are three-dimensional vectors. in the Cartesian coordinate system (X, Y, Z) above. The arrangement of twelve {±Wk; k = 1,2,...,6} has icosahedral symmeetry too. The inner products among {Vk; k = 1,2,...,6} and among {Wk; k = 1,2,...,6} are summarized respectively in a matrix form. and Being a three-dimensional projection of a six-dimensional hypercubic domain, GC is a rhombic triacontahedron K30 whose edges are either of six unit vectors Wk's (see Chapter 2). Having icosahedral symmetry, K30 is rather spherical. The radii along three kinds of symmetry axes and to the edges are tabulated in Table 8. Table 8 Several Radii r of a Kepler 30-hedron K30 of Edge length 1

For a while, a tiling is regarded as a network composed of only unit vectors and its connectivity is mainly investigated. Never mind here that the body-diagonal length of O among extremely short ~0.963. A neighbour in this aspects may be referred to as a vectorial neighbour.

The variety of the vectorial environment of a point in physical space is nine types so long as the network structure concerns; the number of vectorial neighbours is either of 4, 5, 6 (two types), 7, 8, 9, 10 or 12. It is convenient to classify the 12-neighbour case into two cases as to be mentioned below. Then there are altogether ten types. These ten local structures as vectorial environment of a point have their associate domains in GC which are respectively denoted by 4, 5, 63, 65, 7, 8, 9, 10, 120 and l2* in Fig.3. Fig.3 The gazing crystal K30 for 6-dim, to 3-dim. projection. Only a quater
of a section at a plane containing two 2-fold, two 3-fold and two 5-fold axes
are drawn. Cut the pentagon ABCDE, fold along each of two dash lines and
attach the two sides AB horizontal and AE vertical. Then you will have a solid
object, whose solid angle at the vertex is n/15. it corresponds to a quater
section of a rhombohedral face or a sixtieth of the gazing crystal K30.

SELF-SIMILARITY

The domain 12* corresponding to the central point of Fl60 is exactly similar of factor t-3 to the whole G with the centre as the centre ot similarity. Suppose a similar domain of factor  t-2. Domain 120 is obtained by removing the domain 12* from it. The points in the domain correspond to the point in physical space with 12 vectorial neighbours but not the centre of Fl60. In other words, not only A6's but some O6's share the point.

The similar triacontahedral domain 120 of side length t-2 outside of 12* is for the points with twelve neighbours, which do not correspond to Fl60 but the compound of 2n O6's and (20 -n) A6's (n>0).

Let Sl (k)Vl be the summation over five unit vectors among twelve vectors {± Vk; k = 1,2,...,6} whose Vk-component is t = 5-1/2. Then the following relations hold for the mutually associated two vectors in the physical space and the pseudospace INSIDE OUT AND OUTSIDE IN

As mentioned above, the points in 12* sketch a rough structure in physical space in a scale of t3. More detailed structure in physical space is reflected in other region of  GC. Generally speaking, a rough structure are reflected in the central parts and the details or their internal structure are in the outer parts of  GC

The correspondence between a point in physical space and a point in pseudospace can be regarded as a mapping, since two spaces are correlated as the projection of a 6-dimensioiial vectors. A golden rhombus specified by two V's is mapped into a golden rhombus specified by the corresponding two W's where the angle of two V's and that of two W's are supplementary.

A6 « O6

An acute rhombohedron A6 specified by three V's is mapped into an O6 specified by the corresponding three W's where the principal diagonal is multiplied by t-3. An obtuse rhombohedron O6 specified by three V's is mapped into an A6 specified by the corresponding three W's where the principal diagonal is is multiplied by  -t3

Though each of rhombohedra is mapped into a rhombohedron, thus mapped rhombohedra are mutually overlapping in pseudospace. Then the mapping of a compound of some rhombohedra is complicated. Let us investigate the mapping of an F20 and K30.

F20 in physical space ® a 30-hedron with bottle neeck in pseudospace (Fig.4(a)

In Fig.4 points are connected so that the whole configuration of these points may be clearly seen than their point to point correspondence. As a connectivity of unit vectors, the points which correspond to the surface points in physical space construct a collapsed rhmbohedral 20-hedron with unit side length. As a three- dimensional point configuration, they are regardes as 22 vertices of a 30-hedron with bottleneck, among whose 30 faces 10 are equilateral triangles, the other 10 are another kind of equilateral triangles and the last 10 are trapezia.

A set of four internal points in physical space is mapped into the outside of the polyhedron ((1)-(4)) in Fig.4(a)) They must be in the gazing crystal. This requirement is rather strong. Thus the internal configuration of F20 in physical space is uniquely determined by the position of the polyhedron in tne gazing crystal in pseudospace.

K20 in physical space ® a concave 60-hedron with icosahedral symmetry in pseudospace (Fig.4(b))

The attitude in drawing Fig.4(b) is the same as in Fig.4(a) except that along and perpendicular to a 3-fold axis instead of a 5-fold axis. The 32 surface points of K30 in physical space are aranged with icosahedral symmetry. Then they are mapped so that the symmetry is kept. However their radii get smaller as given in Table 9. Table 9 Several Radii of a Concave 60-hedron in Pseudospace Fig. 4 (a) A bottle-neck 30-hedron in the pseudospace, which corresponds to F20
in the physical space. (1)-(4) correspond to the internal points in the physical space.

(b) A concave 60-hedron in the pseudospace,which corresponds to F20 in the physical space.
(1) - (10) correspond to the internal points in the physical space.

The whole distribution of these 32 points are regarded as a 60-hedron which is constructed by putting a triangular pyramid on each of 20 faces of an icosahedron whose circumradius is r5. As for the 10 internal points in physical space, they are mapped to the outside of the polygon as shown as (1)-(10) in Fig.4(b). Here an internal configuration with trigonal symmetry is chosen.

C ® an overlapping compound of two concave 60-hedron  (Fig.5

C is an overlapping of two K30's where an O6 ((2)-(3)), whose points are all on the surface of eithier of two K60's is shared in common. Among the points of two A6's (1)-(2) and (3)-(4), those but (1), (2), (3), and (4) are internal of either of the K30's. In the case of the maximum symmetry shown in Fig.5, the diameter of the sphere that contains all the mapped point is the maximum. In this case, some of the mapped points are inevitably on the edge of the gazing crystal.

Though all of the points (1)-(10) are outside of both 60-hedra ((1)-(3) and (2)-(4)) in the case of the maximum symmetry, the following should be noted. Points (2), (5), (6) and (7) are the internal of K30 ((2)-(4)) but not of K30 ((2)-(4)). Points (3), (8), (9) and (10) are outside of K30 ((2)-(4)) but not of K30 ((1)-(3)). Therefore in less symmetrical cases, two O6's are not necessarily at the both ends of the main axis (2)-(3) of the connected 60-hedra and point (3), for example, can be inside of 60­hedron ((2)-(4)). By this, the diameter is smaller and all the mapped points can be inside the gazing crystal. (see Fig. 3)

Fig. 5

In the gazing crystal, an available arrangement of two O6's and points (5)-(10) is uniquely determined for any position of the connected 60-hedron as easily seen from that the projection is deterministic. The arrangement of the internal points in a cage is uniquely determined according to the circumstance of a cage so that no simple repeat of the same unit cells. This is the most striking feature of the model. Its local symmetry is not so high as can be seen from the fact that A6* never be trigonal, but it is rather uniform.

From these investigations, the following can be concluded

 In the primitive projection model, the internal points of all the cages arange in rather bad symmetry. A cage with the internal points can not have trigonal symmetry.

5. Symmetry in the Transformation Model

In the transformation model, the hierarchy of symmetry can be designed by making use of its freedom. Start with a flower dodecahedron Fl60 which is the only configuration with full icosahedral symmetry among all the compound of A6's and O6's. Apply the Penrose transformation to this. The original Fl60 is kept unchanged and 20 F20's are put on the 20 flower faces. Fivefold symmetry and therefore icosahedral symmetry can not be kept since a F20 does not have 5-fold symmetry as easily seen from the fact that it has four internal points. However, there are some configurations with symmetry belonging to the symmetry group Th and T which are both subgroup of the group Ih. For the cage parts, trigonal symmetry can be kept. The same cage configuration can be always used. In such a case, system has a kind of chirality. By defining some rank for the centres of Fl60's, the hirarchical symmetry of Th or T is realizable.

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