In a continuous space, a field is defined as a quantity present at any location in space. In a lattice as discrete space, the location consists of vertices where each vertex has a limited number of relations with other vertices. A field in a lattice needs to be expressed as a set of quantities related to the vertices. The field thus discretized limits the possibilities in the description of a field.

In a hypercubic lattice all vertices have the same coordination number. Assuming this also holds when fields are present, it means that there is a large number of vertices with edges having field characteristics in addition to the function of position determination in space. So there are field vertices of which at least two of the eight edges are needed to determine the position within the space and the rest can be field edges. Then, to allow for a diversity of field strengths, massive concentrations of field vertices are needed. Because large field strength must occur everywhere in space, the space would only consist of field vertices. If so, the vertices lose their function as the smallest entities of a fourth-dimensional space-time. This can be solved by a much larger coordination number or by positioning the field vertices in the boundaries of granules.

Another possibility is that interaction stems from the coincidence over time of three-dimensional regions with field action. Chapter 5 outlines how such an area could look like. The discrete field is then a coherent set of three-dimensional areas of various sizes L, expressed in the unit distance Δx of a lattice.

From a three-dimensional perspective, the three-dimensional area is a flat spatial plane that extends over time, called the active plane. A variety of field strengths is possible when the discrete field consists of a series of active planes at regular distance L. The spatial density of the field is then 1/L. The probability of two active planes of different fields with the same action coincide is 1/L².

With the active planes of size L² at mutual spatial distances L, the discrete field can be split into granules of size L³ having the action at the boundaries of the granule. This allows the discrete field to be divided into separate non-overlapping granules of size L³.

The likelihood of a granulated field also arises from the transformation of the usual units into the two units Δxand S of a hypercubic lattice with multiple directions [5], where Δx is the smallest distance of a lattice and S stands for the number of lattices in which a phenomenon is present. The conversion results in an expression of the field strength in one lattice or subspace:

E s u b = 1 / L d 2 1/Δt,

in which L_d is a quantity analogue to the discrete distance between two particles.

The inverse proportionality with an area indicates the existence of a field granule, or field granule of spatial size L d 3 . The conversion also results in a smallest field granule for the electron (electron radius) has the enormous local magnitude of about L d 0 = 3.38 × 10 19 Δ x , expressed in smallest lattice distance.

Three different types of field granules are required to describe the most common phenomena.

Still field granule;

The still field granule is immobile relative to the local discrete space. The field granule is regularly repeated every T_field. There can be different types of still field granules, each representing another type of action like electric or magnetic. It is assumed that the cause of the action is present in one of the side planes of the cubic field granule, making the presence frequency of an active plane 1/T_field. An example of a such plane with local deviation of the axis declination is described in Section 5.2. The inner space of the field granule is void, that is, a regular lattice.

Moving granule;

The moving granule, called moving space, is a cube with four moving side planes that ensures the regular interior space to move with relativistic effects. Section 5.5 describes the moving space in a lattice. This possibility is visually illustrated in Figure 1. The moving plane is a three-dimensional bounded area in R⁴, whose entire inner space is moving with speed v and the boundaries are such it forms the transition between the still outer space and the moving inner space. A more precise description of such a boundary is shown in Section 5.3 in the case of a lattice. The relativistic effects are showed in Section 5.4.

Jumping field granule moving at maximum speed;

A repeating space jump in time is another mode of movement of a field granule in a lattice. The field granule is present at one location during the time T before jumping to a successive location L (=T) in the direction of motion. In R⁴, the sequence of jumping field granules is located along the space-time diagonal. Seen from R³, the presence of the field granule moves with discrete speed v d = L / T = 1 . In Figure 2, the four-dimensional situation is roughly outlined, with the jumping field granule depicted as a three-dimensional cube.

To be in accordance with reality, it is supposed that the side faces of the cube to consist of two orthogonal planes with a E and B action.

The granular field is an ordered combination of various types of field granules forming constructions regularly distributed in space and time and interconnected via the corners. Next, it is investigated what the properties of granular fields will be if they are described as a combination of said granules.

Take the constructive combination of still and jumping field granules. The still E (or B) field is a time chain of still field granules. Let the moving field be a time chain of still E (or B) and jumping E, B field granules of the same size L, interconnected at the corner vertices, replacing one of a still field granules in the time

chain by a jumping field granule at each T jump = L / v . So, the time chain of field granules makes each T_jump a jump Lin the direction of movement. Because the jumping field granule consists of both E and B fields as presumed, the E field is present at all times. The jumping field granule is the cause of the presence of the B field during the short period T (=L) every T_jump.

It is obvious that the field strength is proportional to the time the field is present to perform its operation, i.e. has the probability of coinciding with another E or B field granule. Then the fraction B/E is equal to the ratio of the time periods in which the fields are present, so that B / E = T / T jump = v :

B = v E , (1)

or when B is the main field: E = v B .

Equation (1) is in accordance with the empirical expression of a moving electric or magnetic field, showing that the discrete field can be expressed in field granules.

The disadvantage of het above model is that it misses the reason for the repetition time T_jump, making the model incomplete.

Due to the spatial in homogeneity of the particle field, the motion of a granular particle field must be split into two of the above types of motion acting simultaneously. Described in granules, an endlessly extending particle field will consist of a series of concentric field granules of increasing size. A moving granulated particle field necessarily consists of the equal speed of all individual granules of different sizes. This makes that none of the three basic granules alone can describe the motion of the discrete particle field, the solution is a combined presence of a moving space (granule) and jumping granules. To this end, the motion of the particle field is split into an inner and outer sphere, the inner part is being moved by one moving granule with rib L_moving. The outer part by a series of combined still and jumping granules of suitable size moving in the manner of a homogeneous field as described in the previous paragraph.

The smallest part of the particle is present as a locally still field within the moving space and will, as part of the moving space, move gradually with discrete velocity v d = 1 / L moving relative to the surrounding space. Because the inner part is part of the moving space, it also has time dilation and length contraction.

Using the visualisations of Figure 1 and Figure 3, the moving granule of Figure 1 is implanted into the granule of the moving field of Figure 3. Many concentric granules a la Figure 3 of increasing size form the outer shell of the moving particle field.

The concentric field granules of the particle field have increasing discrete sizes L_di and the associated discrete repeat distances in time T_di. Let R_particle be the averaged effective spatial size of the many granules and T_particle the mean repeat distance of the granules, determined by:

1 / R particle = ∑ 1 / L d i 1/Δx, (2)

both provided with the corresponding discrete units. Remarkably, these two quantities have a significant difference in size, as can be seen from ref. [6]:

T particle = ( 2 π / α ) R particle . (3)

Wherein α is the fine structure constant. This means that in one subspace, the cube-shaped granules are only sporadically present over time. In the time in between, the field granules a represent in other subspaces. Call the particle mass in one subspace the average density of the still field granules at a given location, represented by:

m subspace = 1 / T particle 1/Δt. (4)

This is conform the particle mass in one subspace of reference [6].

Take a moving particle field. All particle granules with size L d i ≤ L moving are present within the moving space. It is reasonable that 1/T_particle is mainly determined by the field granules smaller than L_moving. Relative to the surroundings of the moving space, the density of the particle granules at successive positions in the surrounding space is given by multiplying 1/T_particle by the discrete velocity. This will be called the momentum per subspace:

p subspace = v d / T particle 1/Δt. (5)

In a lattice is Δ x = Δ t making v_d dimensionless.

EachT (=L_moving), the moving space makes a unit-step in the direction of motion so that after t = T 2 the total size L_moving of the cube has been covered. The outer part of the moving particle field must move in conjunction with the inner part, i.e. making a minimum jump L_moving every t = T 2 or a multiple thereof. This is possible if the outer particle field consists of a series of concentric shells of increasing discrete size L_di, with L d 1 = L moving . To be in motion, each shell consists of several still field granules and one jumping field granule, which makes every discrete t d i = L d i / v d a jump L_di in the direction of motion.

Implicitly, every jump L_di fits exactly into L_di+1, making L_di a plural of L_d1. This means that, seen in R³, the spatial distribution of the outer particle field is spaced by a multiple of L_moving. This means that during T² there is a still outer field, after which the still field is present at the next spatial location. Therefore there is a greater chance of interaction at mutual distances L_moving, which can be interpreted as the wavelengthλ_d. By doing that, the relation between the discrete wavelength λ_dof a moving particle in a discrete space and the discrete velocity becomes v d = 1 / λ d . Thus the number of outer field granules entering a new area, or the momentumof the particle field, is determined by

p subspace = 1 / L moving = 1 / λ d 1/Δx. (6)

This relation applies next to relation (5).

In one subspace, the wave length λ_d is expressed in units of one lattice. In the next chapter, relations (5) and (6) will be expanded to a space with multiple lattices. The interpretation λ d = L moving links the wavelength to the particle mass via Equation (9).

The jumping outer part of the moving particle resembles the jerking motion described in [7] [8] or [9]. The description of a moving particle given here is not only more extensive than in these references, it also enables a wide variety of velocities. To clarify this, take the situation where the moving particle consists of a series of concentric moving granules. Then, going from the outside in, there is an increase of velocity and time dilation caused by the successive moving spaces. According to the relativistic relations, the effect of one of the moving granules sized L_i on velocity and time dilation is determined by T i + 1 2 = T i 2 ( 1 − v i 2 ) with v i = 1 / L i . Withk moving spaces, the cumulative effect is T k + 1 2 = T 2 Π ( 1 − v i 2 ) | i = 1 , ⋯ , k . This makes that the velocity v_tot of the inner moving granule is determined by: T 2 ( 1 − v t o t 2 ) = T 2 Π ( 1 − v i 2 ) | i = 1 , ⋯ , k , making

v t o t 2 = 1 − Π ( 1 − 1 / L i 2 ) ≈ ∑ v i 2 − ⋯

With this expression any velocity can be obtained by a suitable combination of L_i.

When applying the mode of motion of a moving spherical symmetrical particle field from the previous chapter in a multidirectional space, the field is present in at least n_directions subspaces. Each subspace, if necessary, provided with a subspace with an axis in the direction of motion. The necessity for the outermost regions of the moving particle field to have a subspace with an axis in the direction of movement ensures that the number of these subspaces is also n_directions. Consequently, the moving particle field is present in n_directions subspaces with an axis in the direction of motion next to the n_directions subspaces with random axes. The different subspaces are interconnected via the space-point. The space-point of a multidirectional lattice is a time series of vertices connected in time, the vertices being part of subspaces with different spatial directions ref. [5].

In section 3.4 it has been determined that per subspace the densityof a field granule of the particle is m subspace = 1 / T particle . Multiplication of this particle mass per subspace by the number of subspaces n_particle gives the total densityof the particle field expressed in the two units of a multidirectional discrete space:

m discrete = n particle / T particle S/Δt. (7)

In reference [6] it has been shown that only the discrete units Δx and S are needed to express the physical quantities in a multidirectional lattice. Also in reference [6], the same mass expression (7) has been found.

With (5), the density of the particle granules in consecutive positions with respect to the particle’s surrounding space is

p discrete = v d n particle / T particle S/Δt.

By inserting the mass expression (7) herein, the momentum p_{d particle} expressed in discrete units is

p d particle = m discrete v d S/Δt, (8)

also in accordance with reference [6].

As explained in section 4.1, the outermost field of the moving particle is presented as a series of jump field grains in n_directions subspaces that all having an axis in the direction of motion. Equation (6) describes the momentum in one subspace, i.e. the frequency with which the outer field granules in one subspace enter new areas of space. For n_directions subspaces, the frequency is augmented by that number by which the momentum in the multi directional lattice becomes

p d particle = n directions / λ d S/Δx, (9)

λ_dis the discrete wavelength in the subspaces involved. Equation (9) links the wavelength to the particle mass.

In ref. [6] it is shown that the de Broglie relation in a multidirectional lattice is

p d = h d / λ d S/Δx, (10)

where in h_d is the discrete Planck’s constant,being the Planck’s constant expressed in the discrete units. With (9), the discrete Planck’s constant becomes:

h d = n directions S. (11)

Relation (11) has also been found in reference [6] by using the same reasoning as in section 3.6 to obtain the wavelength of the granulated photon field.

In case the number of edges per vertex is the same for every vertex of a hypercubic lattice, it is shown in section 5.4 that length contraction and time dilation (14) is present within the moving space, which is also true for the largest granule L_moving of the moving space. Because according to Equation (6) λ d = L moving , the wave length is subject to length contraction

λ ′ d = λ d 0 1 − v d 2 Δx. (12)

Using the equation (10), the relativistic momentum is

p ′ d = h d / λ ′ d

With p = m ⋅ v and considering that the v is the velocity in the surrounding space, makes the particle mass relativistic

m ′ d = m d 0 / 1 − v d 2 S/Δx. (13)

From the length contraction of the wave length follows the increase of the particle mass.Based on this, the following observations can be made.

According to Section 3.4, each granule of the outer paticle field L_di is a plural of L_moving. When the size of L_moving changes, the larger granules follow immediately. Apparently the successive particle granules are spatially interconnected.

Secondly, the densification by length contraction increases the presence of the outer field-units and therewith the likelihood of an encounter with another field (interaction). This is in line with the interpretation of the momentum of a granular field as the density of the particle granules at successive positions in space.

In a multidirectional discrete space, the endlessly extended particle field is present as a series of concentric granules of different sizes in each of the n_directions (>10²²) subspaces. To describe motion of an endlessly extended particle field with granules of limited sizes, it will consist of inner and outer granules. The inner field granules show a gradual displacement, represented mathematically by equation (8). The outer particle field shows step wise displacement represented by (9).

Because the largest granule within the moving space and the smallest granule of the outer part are somehow coupled, Equations (8) and (9) act simultaneously. This means that that in the case of granulated fields, the momentum of a particle is mathematically described in two ways, resembling the particle-wave duality.

To become familiar with structural deviations, an example of a very simple anomaly in the structure of a regular lattice is given in Figure 4(a).

Generally, a structural deviation in one vertex necessarily implies that the two adjacent vertices also have a structural deviation. A series of adjacent deviating

vertices constitutes a so-called anomaly-line. Note that an anomaly-line as in Figure 4(a) locally runs diagonally between two axes, and secondly that it has no beginning or end.

In R⁴, constructions of anomaly-lines can exist when several lines are combined to endlessly extending repetitive structures. Figure 4(b) illustrates such a construction. Herein four anomaly-lines merge at regular distances in space-time into one vertex. The sketched image is diagonal in space and time and is present in R⁴as a static column-like construction in four dimensions.

In the construction a recurring pattern can be recognized consisting of a cube-shaped assembly of eight anomaly-lines. Each cube consists of four pure spatial anomaly-lines and four lines diagonally in space-time. By focussing on the progression in the time of the cube-shaped pattern, the pattern makes each T a step L along the z-axis. The series of positions of the corner vertices of the cube can be expressed by the set { z , t } = { ( i Z , i T ) | i : integer , Z = T = L } .

Seen in R³ the cube moves with velocity v d = i Z / i T = 1 .

The assembly of anomaly lines can also be arranged so that the formed construction consists of a series of cube-like patterns extending endlessly in time. Seen from R³, these cubes stand still at one location.

With the possibility of the last section, no physics can be present. Namely, at two intersecting moving columns there is no conceivable transition in two fully different columns.

To provide for possible interactions, consider structural deviations whose anomalies are present on the boundaries of a three-dimensional region of R⁴. These anomalies affect the entire inner space-time region by tilting some axes of the region. These so-called tilted axes are not parallel to similar axes of the lattice surrounding the region. Because the organization of the internal axes is locally the same as in a hypercubic lattice, the space is regular within the said region.

Due to the tilting of the axes within an entire area, there is a chance that regions overlap cannot always occur, i.e. it has an interaction as result. These three-dimensional regions in R⁴ form an active plane within R³.

An active plane forms an endless corridor in time with, at the top and bottom of the corridor, the anomalies that cause the axes to tilt. Figure 5 shows an example of an active plane in the form of a time slice of the three-dimensional corridor.

The cohesion of slices along the y-axis is enhanced when a z-line is missing in the corridor at every T², caused by two open edges, i.e. an edge with a missing vertex, at the top and bottom. A missing z-axis means that there is a gap in time in the active plane. Then the organization of the anomalies along the y-axis in the top and bottom of the corridor can be such (for example in the manner of Appendix A) that every T (=L) the active plane has an open edge at the corner vertices.

Based on Figure 5, two distinct active planes can be distinguished, one with tilted z- and t-axes and the other with tilted y-axis and t-axis. This distinction makes that, apart from opposite spatial tilt direction, the active plane can have six different spatial orientations in R³.This is reminiscent of the six different E, B operating axes.

Active planes of opposite tilt cannot merge, which means that the merging of active planes is not possible in all cases. The said unconnected open edge at the corners each T allows to arrange several active planes into a cube, with which various field granulesof Section 3.1 can be formed.

By taking a small variation in the structure of Figure 5, an entire spatial plane is in motion. Figure 6 shows the structure of such plane, in which the time axis makes a spatial step Δz in the direction of motion each T. Herein, the anomalies at top and bottom are such that all time lines of the corridor and boundaries are relatively inclined in the direction of motion, where the tilted time axes having no beginning or end.

The time slice of the moving plane consists of the repeated occurrence of T segments in which one of the segments makes a jump in time due to a missing z-axis. The moving plane is formed by a series of L (=T) adjacent time slices in such a way that segments with missing z-axis are never present at the same time.

Seen in R⁴, the corridor with the moving plane looks static. In R³, the plane is in consecutive positions along the z-axis over time, which means it is in motion.

As can be seen in Figure 6, all axes with in the corridor are tilted in the same way so that the entire space of the corridor has a locally regular space structure that moves at local speed v d = 1 / T .

In the case of a moving space-point the set of subspaces must be such that one of them has an axis in the direction of motion. This subspace sets the space-point in motion.

An obvious definition for the distance between two vertices on an axis is the number of intermediate edges. Using this definition, the time distance within the moving plane is shorter than the comparable time distance in the surrounding space because of the missing z-axis in the moving plane. The time distance T² in surrounding space has a corresponding time interval T v 2 within the moving plane, which, due to the time gap, is one unit-distance less: T v 2 = T 2 – 1 . Seen from the surrounding space, combined with v = 1 / T , the time distance T_v within the moving plane becomes: T v = T 1 − v 2 .

As Figure 6 shows, the time axis within the moving plane is literally stretched relative to the time axis of the surroundings. Take the time distance Δt within the moving plane. In surrounding space, this time interval lasts longer, i.e. it comprises a larger number of Δt' vertices met: Δ t ′ / Δ t = T / T v . Using the above expression for T_v, the relation between the time intervals Δt' and Δt becomes

Δ t ′ = Δ t / 1 − v 2 ,

being the time dilation of events.

In the corridor the smaller number of vertices overtime is compensated by an increase in vertices in the direction of movement. To clarify this: The corridor extending indefinitely in time has, in addition to the boundary in upper and lower surfaces, also two side surfaces as boundaries. At the location of the side surfaces, the inner vertices are connected to the vertices outside of the corridor.

Take the side surface L. T expressed in distances of the surrounding space. The same side surface, expressed in distances of the corridor, comprises of L_vT_v vertices, where L_v is the mean number of vertices forming the height. At the surfaces, each vertex of the corridor is connected with a vertex of surrounding space, making L v T v = L T . As a result, the average number of vertices within the moving plane in the direction of the velocity is

Δ z ′ = Δ z 1 − v 2 .

Take a number of vertices Δz within the moving plane in the direction of motion. Seen from surrounding space, this distance comprises less intermediate edges Δz', making

Δ z ′ = Δ z 1 − v 2 , (14)

being the expression of the length contraction.

In a lattices-like discrete space, length contraction arises from the same coordination number of all vertices instead of the principle of relativity. In addition, it is based on a high regularity in the presence of anomalies in a hypercubic lattice as discrete space.

A moving field granule consists of a cube with four moving side planes. All these planes are moving with the same speed v in the same spatial direction. This caused all the vertices an edges of the cube’s interior also moves with speed v due to the interconnections with the side planes. Like the side planes, the entire space within the moving space will also have time dilation and length contraction as well as a regular space structure.

The consequence of the regular space structure is that each field granule positioned within the moving space has the same internal structure as placed in the non-moving situation, which is the subject of sections 3.3 and 4.2.