pleiadian technology | book 3
- METOL
- GEODESIC CRYSTAL
- GEOPLANET
- USC TORROID
- SEMICONDUCTING PROPERTIES
- CRYSTAL TYPES, GEOMETRIES, AND DOPANT RATIOS
- METOL GROWTH
1. METOL
In the diagram [sic] for the “expanded lattice geodesic,” the individual geodesics are Bucky Fullerenes that have been grown into a much more compressed form than any of the ones that have been grown to date. Usually, a quadrivalent atom is selected as the framework atom of the geodesic crystal.
The individual geodesics are so compressed that their atoms are bonded to each other in an inner electron orbital, where they produce frequencies of visible light when electrons are conducted across their surfaces.
The individual geodesics are then grown into the expanded lattice structure with cubic symmetry. There are many spaces in this lattice. These hold the dopant atoms which are added in the second growth process. If these are diamagnetic atoms then superconductivity is the result, and if they are magnetic atoms, then it is supermagnetism.
There is also a crystal that is completely unknown that I call “superluminal.” These are dodecahedron quasicrystals. This crystal has groups of diamagnetic/magnetic cations that alternate with anions at the vertex points of the decagons and pentagons, which are the basic geometrical units of the crystal. The electric fields between these groups is very high, and this strongly rotates the light that is put through them. The anions in these crystals are geodesics with a strong magnetic field. This field attracts and holds large numbers of electrons when they move through the superconducting geodesic crystal, and this is the basis for their being anionic, that is, of holding a negative charge.
The light is bent with a high index of refraction as it transmits through the quasicrystalline lattice, but it is also rotated on the inner surfaces of this lattice by a new type of crystalline configuration, the Unit Spiral Cell. USCs are areas where the pentagon symmetry of the quasicrystal is rotated into a square symmetry. This rotation is depicted in the diagram.
[DIAGRAM][sic]
When electrons are accelerated through a superconducting lattice with diamagnetic dopants, the magnetic atoms that are in the body-centered lattice produce photons through luminescence excitation. These photons radiate into and through the quasicrystal lattice, where their electromagnetic fields are rotated by the circular lattice structure. The highly charged metal cations and anions in the lattice bend the light through an almost 90-degree angle (an “R” value of infinity), producing a nonlinear optical rotation that is unheard of in any known crystals.
This rotation breaks the light down into DeBroglie Quanta, which are a different form of energy from the known Plank Quanta. The DeBroglie Wave Quanta have momentum, and when this changes with a rate of time (d/dt), a force field is produced. The photon momenta change by virtue of a constantly modulating and changing photon energy field, i.e., with many different wavelengths, energy densities, and coherence lengths. This force field then becomes the basis of a new lifting force, if it can be given coherence by the symmetry of the crystalline matrix that is producing it.
There are still some puzzling questions about the nature of the physical effects and fields that are produced when these materials operate. They are composed of metals and should be opaque, but they have optical properties which indicate transparency. How is this accomplished? Do they transmit energy initially in the infrared, and then increase it into the visible and ultraviolet? This is what happens in sonoluminescence. Do they operate with a valence-to-conduction frequency shift, or a harmonic doubling, as occurs in nonlinear crystals?
The overall structure of the metols is an integrated complex of cubic and quasicrystalline geodesics. They are merged into a single crystalline form with a 4-5-4 symmetry by virtue of the fact that the cubic string of geodesics actually grows as side chains to the geodesic-cation quasicrystals. The latter have their cations at vertex points in the crystalline structure, and are much more rigidly bonded for this reason. The stronger bonds of the quasicrystals means that their individual cation and anion groups can hold higher levels of charge and still remain in the structure. This is not true in the cubic crystals, where the cation groups are loosely bonded into the space positions between the individual geodesics, and in the centers of the geodesic hexagons. If these atoms are energized to too high a level, their kinetic energy will cause them to leave the crystalline structure entirely.
The 4-5-4 crystalline complex is the true metol cholesterol. The main body molecules are held in the quasicrystalline pentagons and decagons. These consist of groups that are both anionic and cationic. However, when electrons are put through the superconducting crystal, an overall or net negative charge develops as the anions become overcharged with electrons. This conforms to the charge structure of cholesterols, which have negative hydroxyls in their main bodies.
The side chains of the cholesterols are positively charged hydrocarbon molecules that are sugars. The positive charges of this group of molecules is provided by the hydrogen ion. In the metols, the side chains are positively charge geodesics that are combined with diamagnetic atoms that also have a positive valence. The geodesics in the superconducting lattice also attract electrons, but they are incapable of holding them, as the pressure of the SC current keeps them moving through the structure. They can be regarded as having a permanent positive charge, which is in conformity to the charge structure of the cholesterol molecules of animals.
The side chain geodesics can also grow with a rotation that is similar to the rotation of the side chains of cholesterol. The top and bottom pentagons (or hexagons) on one geodesic are rotated through an angle of 36 degrees with respect to one another. If two adjacent geodesics bond with these structures facing one another, they will have this angle of rotation between them. If the rotation continues down the length of the string of geodesics, each one in the string will be rotated through this angle with respect to the previous one in the string.
The rotational conformation of the geodesics in the superconducting cubes is probably caused by the rotational action of the magnetic field during the magnetic arc growth process. The torque of the magnetic field as it acts upon the ions in the field could rotate the geodesics, or perhaps this is a naturally occurring growth process that would develop regardless of the growth technique that is used. It is possible, too, that the successive geodesics may be rotated through angles that are greater or less than the 36-degree angle between the top and bottom pentagon-hexagon faces of one geodesic.
It is difficult to imagine the structure of a crystal that is yet to be grown, and then to relate that structure to the laws of electrogravitation that are yet to be defined.
The quasicrystal has anions at all of its vertices. The cations in this crystal are in the more weakly bonded positions between the anions. This structure mimics that of the anion framework radicals that make up cholesterol. In cholesterol, these are hydroxyl radicals, which are the negative ions on the water molecule. In the quasicrystal, this is the quadrivalent anion metal. [sic: metol?]
The quasicrystal is grown under heat and pressure in a process that is similar to the ones that are used to grow the known quasicrystals. However, when the surface layers of the crystal are rotated into the superconducting layer of the metol lattice, a different technique is used. The cations in the quasicrystal are pulled out of their positions by a strong magnetic field that is acting in a high-pressure inert gas environment.
The high-pressure environment prevents the cations from leaving the quasicrystalline surface entirely. The inert gases are highly ionized, and they, too, are rotated in the magnetic field. The rotation of these gases acts to hold the less energetic cations in place as they begin to loosen themselves from the surface of the quasicrystal. The inert gases guide these cations into their spiral positions according to the relative ratio of their masses to their magnetic fields. The magnetic ones are most vigorously rotated into the USCs, while the diamagnetic ones are pushed into the centers of the spiraling planes, which appear as augers. Transcendental equations can be used to describe the auger.
While the cations move into the spiral planes, the anions remain in their pentagons, and the USC is a series of spirals encased in anions with pentagon structures.
Toward the end of the layer of USCs, the geodesics that are used to construct the superconducting layer begin to occur in the lattice. This is the transition zone between the 5 and 4 symmetry layers. The geodesics are composed of quadrivalents that have a “multivalent” charge distribution. This is the same as the carbon-carbon bond of hydrocarbon molecules. On the surface of the geodesic, each atom is surrounded by three other atoms in a tetrahedron bonding pattern. All of the framework atoms in a geodesic share electrons with their three nearest neighbors.
In the transition zone, the pure anion pentagons merge into the pentagons and hexagons that are composed of anion-cation groups. In the 4-symmetry superconducting layer, the bonds connecting the pentagons are broken and reattached to the diamagnetic atoms that bond into the centers of the hexagons.
The basic purpose of the 4-5-4 metol is to convert light energy into light force. Electricity is used to do this. Electrons are driven initially into the copper wires of the magnetic induction coils, which have geodesic iron cores. The magnetic field strength develops, through hysteresis, to a high Gauss level, and then suddenly the electrical current goes into its “off” cycle, and the magnetic field collapses, and the electrons rush out to ground, which is in the direction of the perimeter of the ship.
The superconducting current moves in this direction because the metol is doped with “n” and “p” (negative and positive) in the same manner as a semiconductor is doped. The “p” atoms are concentrated toward the outside of the craft, and the “n” atoms towards the inside. The electrons are negatively charged, and they will always be attracted to the positive atoms, so they naturally want to move toward the outside of the hull of the craft.
The superconducting current is enormous‒over five million amperes. Many of its electrons jump off the superconductor’s diamagnetic atoms and strike the rare earth atoms that have been doped into the metol’s lattice structure. These atoms are tightly bonded into the lattice, as are the other atoms, which become transparent to light. They become the color centers of the crystal, similar to the color centers that are found in many of the crystals that are known to science.
An electron that is moving freely through space is an x-ray. When one of them strikes a dopant atom, the atom’s electrons absorb some of its energy and re-emit it at a much lower energy level in the visible or ultraviolet frequency bands in a process that is known as luminescence. The photons that are emitted during this process are then used to power the craft.
The photons are broken down by an optical rotation that is far more severe than any that is known to occur in any of the nonlinear optical crystals that are used in our modern-day lasers. This rotation is so severe because only metal [sic: metol?] atoms are used in the metol. These atoms develop the highest density electric and magnetic fields that can occur in any of the known elements. If they were not used, the nonlinear effects of the material would not be as severe, and the light would not break down into its force field components.
2. GEODESIC CRYSTALS
The exchange of positive and negative charges occurs in the 4-5-4 crystal structure. These numbers refer to the symmetry of the basic crystalline layers that make up the metol. The four layers are positive geodesics that have a quasicrystal structure. This polarizes the individual charge centers of the crystal and makes it very alive electrically with many dipole fields.
In the Fullerene Geodesic Crystals that have been grown, the framework atoms have a net charge that is positive, this as a result of their growth conditions. This means that they will attract small numbers of electrons. This is important for superconduction, as these crystals must act as the negative valence portion of the superconducting plane. They are, in effect, the equivalent of the oxygen atoms in the superconducting copper-oxygen square planes in Perovskites.
The valence of the copper atoms in the Perovskites is critical to superconduction. They must have at least a charge of +2.2 for superconduction to occur. If there are copper voids in the lattice, the valence of the remaining copper atoms will be increased, and this is one way to achieve the desired valence.
There are about twice as many oxygen atoms as copper atoms in a Perovskite. This means that their average valence only is half that of the coppers, or about +1.1. If a similar ratio must occur in a geodesic superconductor, then the positive framework atoms must have this same average charge. Currently, this is not the case, as the Fullerenes that have been grown have a net charge per atom of only one tenth of this value.
Obviously, in the growth of the metols, the first step will have to be the growth of Fullerenes that have a considerably more compressed structure than do the existing ones. This compression will decrease their size considerably and, in the process, squeeze the framework atoms’ electrons out of their outer orbits and ionize the entire structure with a positive charge. This charge, in turn, will attract enough electrons for them to act as the negative valence member of the superconducting planes.
The structure of the metol geodesics is not only different from the structure of the known Fullerenes in their size and charge, but in the distribution of the individual atoms as well. In the Metol Geodesics, the framework atoms are augmented diamagnetic atoms. In addition, one of these atoms is located at the center of the geodesic. The diamagnetic atoms will not substitute for framework atoms in the structure of the geodesic, this because of their inappropriate valences, but they will bond loosely onto their surfaces in the center of the hexagons. The number of diamagnetics depends upon the number of hexagons, and this, in turn, upon the number of framework atoms in the lattice structure.
When a diamagnetic atom bonds into the center of the hexagon in a geodesic crystal, it interrupts the framework bonds of the hexagons. These are the bonds that form three of the hexagon sides. These sides normally connect the 12 pentagons of the geodesic to each other, holding the structure together. When the diamagnetic atoms attach themselves to the surface of a geodesic, they form tetrahedron bonds with its framework atoms. Three framework atoms are forced to break one of their framework bonds to an adjacent framework atom when one dopant atom locates in the center of a hexagon. These three bonds are then reattached to a single dopant atom, and the resulting crystallographic structure is a tetrahedron.
The tetrahedral bonding patterns and symmetries of the hexagon-centered dopant atoms is such that as many as two atoms can bond into this location. When this happens, the 12 pentagons in the geodesic are only connected to each other by the tetrahedron bonds of the dopants. In a group of three pentagons, a single dopant atom can connect two pentagons together, but it cannot connect the third pentagon, something that would occur naturally in an undoped geodesic.
When dopant atoms bond onto the surface of a geodesic crystal during its second growth cycle, an entirely new structure is created, one that is much more loosely bonded than the original one, and as such is capable of absorbing and emitting a wide range of molecular vibrational frequencies.
There are 20 hexagons in a 60-member geodesic crystal, and there can be either one or two dopant atoms in the middle of each hexagon. This makes a possible total of 100 atoms for the new geodesic crystal. If a single atom also locates at the center of the geodesic, which is the corner of the cube in the superconducting lattice structure, then there are 101 atoms per crystal.
A single dopant atom can locate easily, with plenty of space to spare, in the center of a hexagon. Two dopant atoms, however, are another case. These must locate on top of each other in the center position, or at slight angles from one another, depending upon their relative sizes in comparison to the size of the framework atoms.
The one hundred possible atoms for the new geodesic metol crystal is the same basic number of atoms that are found in a quasicrystal. This symmetry is not coincidental, as the quasicrystal must grow naturally out from the geodesic crystals in the 4-5-4 metol complex.
When the living geodesic forms, it mimics another feature of biological conformation and structure. The new form of the crystal is similar to the form that occurs in chains of biological molecules. These are a series of pentagons and hexagons that are connected to each other in their forward and backward directions. If these molecular chains were connected in three directions instead of two, then they would curve over into the spherical shape of the geodesic crystal.
Any geodesic crystal that can be inscribed completely into a sphere can only have 12 pentagons, as this is all that is required to fold these structures into a spherical conformation. However, they can have almost any number of hexagons, as these only elongate the structures, making them ellipsoidal instead of spherical. The spherical Fullerene has 60 framework atoms, and this one occurs with the greatest frequency in the growth populations of these crystals. The growth populations can be varied by changing the growth conditions, and then geodesics with more than 60 framework atoms will become common.
In a 60-member geodesic, the ratio of framework atoms to hexagons (and dopant atoms) is: 60/20, or: 3/1. In a 90-member structure, the ratio decreases to: 90:35, or: 18/7. The larger the geodesic, the smaller the ratio is between the framework and dopant atoms??? [sic: hexagons???]
The diamagnetic atoms make the structure a much better superconductor. The existing Fuller Geodesics will superconduct without having any diamagnetic atoms in their structures, so if these types of atoms can be added into their structures, they would superconduct at much higher temperatures.
These diamagnetic atoms in the metols mimic the actions of the mineral salts in biological membranes, and in clusters of water molecules. In many types of biological activities, ions, such as sodium or calcium, are pumped through the holes in membranes or water clusters. Whether the ion will move through a given hole or not is dependent upon its diameter in comparison to that of the hole. If it is too large, it will not move through the hole and will remain on the outside.
In the Metol Geodesics, the diamagnetic atoms are drawn into the center positions of the hexagons. When this happens, they are mimicking the actions of ionic salts, such as sodium and calcium, in the membranes of living things. They can only bond loosely into these positions, and are likely to move into other positions when electromagnetic energy is oscillated through the material.
The diamagnetic atoms that bond into the tetrahedrons in the geodesic crystals also occupy the face and edge-centered positions in the cubic lattice structure of the superconductor. Their location, however, is only approximate to these positions, as there is some freedom to move around inside the lattice structure of the superconductors. The tetrahedral bonds can have any number of angular orientations inside the lattice, and their coordination in the larger cubic lattice is secondary to their coordination within the geodesic’s framework atoms.
If all of the 20 hexagons in a 60-member geodesic crystal have a dopant ion attached to their centers, another geodesic will be formed by the diamagnetic atoms. This will be the dodecahedron, which has 20 points and 12 faces. In this case, a diamagnetic atom is located at each point. This polyhedron is the smallest true geodesic, as the regular polyhedrons that are smaller, the cube, octagon, and tetrahedron, are not based upon the pentagons and hexagons of the Fullerene.
The close packing of the geodesics in the cubic lattice structure of the metols does not allow for dopant atoms at all of the hexagon locations. [DIAGRAM] [sic]
Because this lattice is body-centered, there is no room for other atoms (or ions) along the diagonals that run between the cubes. In contrast, however, there is a great deal of room along the edges of the cubes, and in the centers of the faces of the cubes. The dopant atoms will locate in these positions. This type of structure in a cube is referred to as “face-centered” and “body-centered” symmetry. It has been observed to occur in the Fullerenes that have been grown by the modern material sciences, the difference being that these crystals have alkaline metal cations in these locations instead of magnetic or diamagnetic atoms.
There are a total of 7 or 8 diagonal locations where it is not possible to have a dopant atom in the structure of the cubic geodesic crystal. If all of these positions are vacant, then there would be a total of 12 or 13 possible hexagon positions where dopant atoms might locate. If another dopant atom is also located at the center of the geodesic, at the corner of the cube, then the total for each geodesic would be 13 or 14 atoms. This would be the case if the atoms were large cations, such as potassium, but they are not. Instead, they are the much smaller diamagnetic and magnetic atoms, and it is possible to have more than 13 or 14 of them per geodesic.
It is not certain how many dopants can squeeze into the face and edge centered positions of the cubic lattice of the metols. This would depend upon their degree of intrinsic ionization, as the greater their positive charge, the smaller is their radius. It is likely that there are at least three atoms per location, but there may be as many as four or five. If there are three, then the total for one 60-member geodesic is 37-40 atoms; for four atoms the total is 49-53 atoms, and for five, 61-66 atoms. The symmetry of the cubic arrangement is such that the dopant atoms for one geodesic are shared by all of the surrounding ones. Since there are 14 surrounding geodesics, six in the 90-degree lattice group of one cube, and eight in the diagonal lattice of the second cube group, the total number of dopant atoms per geodesic is lowered.
The diamagnetic atoms in the metols form what could be referred to as “strings” of atoms. These have the shape of a standing wave in a fluid medium, with the compression node of the wave occurring in the spaces between the geodesics (where the diamagnetic atoms locate), and the rarefaction part in between the geodesics (where there are no dopants). These strings will superconduct electrons at any temperature, and are the physical basis for this phenomenon in the metols.
When electrons move onto the diamagnetic strings and superconduct, they do so as a plasma that has fluid qualities. This plasma is cohered by a standing photon wave pattern with a wavelength that is equal to the length of one of the sides of the square or cubic lattice. Superconduction does not occur inside the actual geodesic. Instead, this structure acts as a mold or shape that organizes the diamagnetic atoms so that they occur in a continuous string.
The other portion of the 4-symmetry metol is the magnetic geodesic array. This, too, plays a vital role in the production of the force field. The magnetic geodesic sheets are similar to the diamagnetic sheets except that the dopant atoms are magnetic instead of diamagnetic. Because of the presence of these materials, this portion of the 4-5-4 metol structure develops very strong magnetic fields. These fields are induced from the craft’s main generator unit.
Because the diamagnetic layers shield the magnetic layers from magnetic penetration, the magnetic layers must be magnetized from one of their ends. When this happens, magnetic lines-of-force run parallel to the electric lines-of-force of the superconducting current. This is similar to the charging of the superconductor with electrons which are superconducted to the other end of the material. When the magnetic layer is magnetized by the large induction coils of the generator unit, the field lines run parallel to the direction of the superconducting current. These lines are forced into the five symmetry superluminal layers which occur between the four symmetry layers, and they excite the cations there into a high degree of luminescence. This occurs because the magnetic field produces a high level of spin in the orbital electrons, and this, in turn, produces photons of light at many frequencies. This phenomenon has been observed in modern physics and is known as the Zeemann and Stark Effect.
The structure of the Metol Geodesic has now evolved into a far different realm than that of the known Fuller Geodesics. The surface of the framework is now much tighter and more compressed than in the normal geodesic crystals. This leads toward a more highly charged structure. In addition, magnetic and diamagnetic atoms occur instead of the random cations that occur in the known Fullerenes. These enhance the magnetic and diamagnetic effects of the metol crystals until superconductivity and supermagnetism are achieved at much higher temperatures than for the known compounds.
The metol geodesics are arranged into a cubic-square plane lattice. It is cubic in its broadest terms, but the planes that make up the surfaces of the cubes are so irregular that the cubic structure disappears over the long-range order of the crystal, and it is actually more accurate to describe it as a series of “stacked planes.” This property of the metols is identical to the structure of the Perovskite superconductors, which are variously described as having either a cubic or a stacked planar geometry.
The four symmetry of the metol occurs in two groups of geodesics, one which has magnetic dopants and the other which has diamagnetic dopants. These form the “bread” of the sandwich that is the completed form of the metol.
3. GEOPLANET
The earth must have a magnetic core and a diamagnetic-crystalline mantle if the geodesic is to be a model for its internal structure. The magnetic core of the earth includes many heavy elements that are paramagnetic, such as the rare earths. Only small numbers of these atoms find their way up into the mantle and crust of the earth, something that is borne out by geological surveys, which shows that these are the rarest of elements at the surface (and in the crust) of the earth.
The crust of the earth contains small amounts of the diamagnetic elements, such as copper, silver, gold, and lead.
The magma between the crust and the mantle could be compared to the heat that the electron common cloud produces as it orbits the geodesic crystal.
The core of the earth is so compressed that most of its electrons have been squeezed out of their orbits. They then migrate to the crust-mantle interface of the earth on convection currents, where they find new homes in the very hot materials that make up the earth’s magma.
The dynamo action of the core produces convection currents that are highly charged with electrons. These currents carry the free ionized electrons of the core atoms that move towards the surface of the earth. The magma zone of the earth occurs at the interface of its mantle and crust. The magma is actually the lower section of the crust. This section has been heated to its melting point by the convection currents that are coming up from the center of the earth, and when it melts, it forms a thin zone of fluid that the crust of the earth then rests upon.
This picture of the earth can be used as a model for the electrical functioning of the geodesic crystals. In both cases, the pressures in the structures (earth and crystal) are so great that the atom’s outer electrons have been removed (ionized). These electrons orbit around the outside of the geodesic structure, in orbits where they are free from the high pressures that they would be subjected to if they were inside the earth geodesic.
The magma of the earth can be likened to the infrared band of energies that some of the electrons that are in the common cloud produce as they orbit the geodesic crystals. The crust that lies outside of the geodesic is the thin layer where individual geodesic crystals can bond to adjacent crystals or to other types of structures, either molecular or crystal ionic. This is the zone of life on the earth, and the zone where a single geodesic can make life by coming together with other forms of matter.
The boundary between the core and the mantle is not distinct. It is only a transition zone where the temperature and pressures cause a phase change in the material from a plastic state to one that is solid. This also occurs in geodesic crystals, where the cations are tightly bonded with the framework atoms of the structure.
The core of the earth holds a large net positive charge, this because its electrons have migrated to the surface of the earth. The surface, in turn, holds a large negative charge. This separation of charges produces an electric [sic: field] that acts from the center of the earth to its surface.
This single geodesic crystal mimics the earth most closely in its electronic structure. The cation at its center is ionized, holding a positive charge. The electrons of the cation and framework atoms are orbiting outside the crystal, and the same electric field develops from the center of the cation to the surface of the geodesic.
4. USC TOROID
The unit spiral cell toroid is a more complex variation of the USC that has been described. This cell begins with the normal USC, which is then spun while it is still in a semi-molten or plastic state. This spinning motion produces cavitation along a central axis, producing an elongated cylinder. When magnetic and diamagnetic atoms are added during this growth process, they fall into the cylinder and arrange themselves in a perfect spiral pattern according to their masses, the heavier ones moving to the outside of the cylinder and the lighter ones to the inside.
This cell combines many geodesics into a toroid-shaped crystal. The USC is grown by combining the individual geodesics with a thin substrate of dopant atoms that is only one or two atoms in thickness. Small electrical currents are put through the substrates as the geodesics are distributed on the substrate’s surface. The geodesics will attach to the substrate at one of its hexagon faces as the current moves through it. This current produces a toroidal distribution pattern on the surface. Currents of different potentials produce different geometrical shapes. Some look like flowers with either three, four, or five petals. (Japan Tech).
The USC toroids are elliptical in shape. They are developed during a substrate growth process. When the substrate-geodesic growth process occurs, a current is put through the substrate as the geodesics are moved onto its surface. As the current moves through the conductive substrate, flows in undulating sine wave patterns around the individual geodesics. This sine wave pattern is shown in the diagram here [DIAGRAM: 9 TOROIDS][sic]. When the growth process has been completed for several layers of geodesic toroids and diamagnetic substrate atoms, this sine wave pattern becomes a wave guide for the superconducting electron currents which is put through the metol material.
The toroid develops naturally in each layer of material that is grown in this phase of the growth process of the metol material. When another layer of diamagnetic atoms and geodesic crystals are grown together, the diamagnetic atoms fill in the spaces between the geodesics. But they also cling to the top surfaces of the geodesics, creating an irregular diamagnetic surface over the toroid collection of individual geodesic crystals. This surface must be ground down until it is perfectly flat before it can be used as a the substrate for the next layer of geodesics.
When the second layer of geodesics is depositioned onto the first layer, the crystals are drawn into locations that are directly over the ones that are below. Repetitions of this procedure build up the geodesic toroid into the third dimension. This third dimensional form is the final form of the USC.
As the USC toroids are being grown, each layer of geodesics bonds to the one below at the site of one of its hexagons. This bonding site is always a hexagon, because these structures have a center space that is capable of holding an atom. (covered under dopants and geodesics).
When geodesic layers bond together at surface hexagon sites, they usually assume a position that gives them an angular rotation with respect to each other. Each successive geodesic in the vertical chain that runs through the toroidal layers is rotated with respect to the one that lies below it.
This rotational conformation of the geodesic toroids mimics the side chain rotation of the cholesterol molecules that occurs in the bodies of animals. This rotation causes light to shine through these liquid crystals that are to be rotated. This, too, is the effect of the rotation of successive geodesics in the vertical toroid chains. This rotation occurs in parallel with the direction of the toroid’s center hole.
During the substrate-geodesic growth process, the hollow toroid of the USC fills with dopant atoms that are drawn up into it by electrical eddy currents. These currents move from the outside of the toroid to the inside of its hollow center, and then back to the outside again in a repetitive pattern. These currents pick up dopant atoms one at a time and distribute them in a spiral pattern around the circumference of the hole in the center of the toroid.
The spiral distribution of atoms inside the toroid ring is the heart of the USC. This is the optical component of the crystal. Inside the toroid hole, atoms align themselves into patterns that are based upon the five-fold symmetry of the quasicrystal. The spiral cell portion of the USC has the same atoms as the geodesic crystal that make up the larger structure, but it does not have the same symmetry. The new symmetry is instead that of the rotated quasicrystal, identical to the known quasicrystals, except that the parallel layers of atoms have been grown into a slip lattice, rotational symmetry.
The rotational growth process of the USC quasicrystal distributes the atoms inside the toroid hole according to their mass, with the heavier ones moving toward the outside and the lighter ones towards the inside of the hole. This means that “like” atoms will occur together at specific distances from the axis or center line of the spiral.
During the growth process for the USCs, the individual crystals are continually washed in acid baths that remove the excess dopant atoms that have clung to the surfaces of the individual geodesics. Although these atoms are diamagnetic and conductive, and will conduct electrons very well, their presence on the surface makes it irregular, decreases its structural strength, and produces eddy currents which will interfere with the superconducting wave guides that will accompany the electrons through the material when the power is turned on.
When the USC has completed its growth cycle, it has its surface washed clean in an x-ray beam that knocks most of the remaining dopant atoms off its surface. This is necessary to prepare these cells for their final assembly into the largest unit cell, that of the light cell crystal.
Light cell crystals have approximately the dimensions of the light waves that are produced when the electrical current is oscillated through the metols in the hull of the craft. To fabricate a light cell, many thousands of USCs have their optical axes placed into a common alignment by applying a magnetic field. The USCs have previously been given a common magnetic alignment during the deposition growth process, and the application of this field produces a common alignment in the second growth process.
The USCs are combined with a vapor of diamagnetic dopant atoms which coats them evenly. This is done in a vacuum, so the dopant atoms are strongly bonded onto the surface of the USCs. This is the final growth process, and the metol now consists of trillions of USCs that are aligned both optically and magnetically. The metol is ready for its assembly into the structural sections of the spacecraft.
The baths must use very strong acids to remove these loosely bonded dopant atoms. This is a slow, careful, and painstaking process that must be monitored constantly for material defects. This is where the basic unit cells for the craft are fabricated, and each cell must be grown to as high a degree of perfection as is possible.
If the USCs were stacked in a single line, there would be 20 million of them per lineal meter, and 20 million times 20 million (400 trillion) per square meter. One small spacecraft has a hull surface area of about 35 square meters, which would contain about 14 quadrillion USCs. One can imagine how long it must take, and how difficult it must be, to build one of these spacecraft.
All of the USCs in the metol material must have a common rotational direction, either clockwise or counterclockwise. When electrons become trapped in the spiral centers of these cells, they must orbit and rotate in the same direction, if the force field is to be coherent. The primary light that is produced in the cells must rotate in one direction only, or its force field effects will cancel, as two different rotational directions will produce gravity waves that are 180 degrees out-of-phase with each other, cancelling each other out. These USCs are given a common rotational direction by giving them a common magnetic polarization, that is, one end of the USC is always given the same magnetic pole charge, either North or South. When the light cells are fabricated, the applied magnetic field will pull all of the USCs into a common magnetic (and hence optical) alignment.
Electrons, photons, and primary light have the same rotational direction in the metol material. When electrons move through the USC layers, they can take a variety of paths. The inside of the toroid has a diameter that is about the same as that of the DNA molecule, about 50 Angstroms. When electrons spiral around this hole, they emit x-rays that have wavelengths that are close to the center hole’s size. If these wavelengths can be tuned to the natural wavelength spectra of the atoms that make up the USC, then the conversion of the electron’s kinetic energy into x-ray energies will occur without the emission of any infrared energy, which is normally caused by the violent collisions of electrons with other electrons or atomic nuclei. This means that electron energies can be transduced into the lower frequency energies of the visible and ultraviolet spectrum without any heating effects.
This is another important property of the metols and the USCs. Electrons are the basic fuel of the electrogravitational spacecraft. Their energies are used to produce photons, which then are broken down into a coherent stream of light force photons which ultimately, after amplification and coordination, produce the force field. Electrons are also used to charge up the hull structure with an electric field, which in turn produces the nonlinear optical effects in the USCs.
The USCs are micro cells that coordinate the momenta of electrons. When enough micro cells have been combined to equal the size of a wavelength of light, the next unit cell, the “light cell,” has been created. This cell is a cell in name only. It is used only to describe a cell that has the proportions of a light wave. A flat disk of USCs with a diameter that is equal to L/2pi (the wavelength of light divided by two times pi), is one light cell.
The most favorable conduction paths lead the electrons into the centers of the toroids, where they are run up through the spiral chains of diamagnetic atoms. The magnetic spirals occur in parallel with the diamagnetic spirals, and the electrons spin as if they were trapped in extremely small microwave cavities. These cavities, however, are much smaller than any that have ever been fabricated, and they cause the electrons to spin with frequencies which are in the range of their own inherent magnetic spin frequencies. This tunes the spin frequency through the spiral coils to the orbital spin frequency of the electron. This produces a resonance which traps the electron in a small plasma field, where all of its energy is drained out of it and radiated away in space.
If the electron spin radiation process that has just been described is re-energized by additional photon energies, the electric field of the electrons will interact with the photons and produce SNO effects. These effects break down the photons into the primary light energy that then becomes the light force field for the craft. The primary light moves out of the toroids in the direction of the center of the craft. This energy is able to radiate through any material without being absorbed or encountering resistance. It is closer to neutrino energy than electron or photon energies.
The metol USC combines optical and superconducting effects to produce the craft’s force field. These cells are grown on substrates that lie flat in the planetary gravitational field, but when they are assembled into the hull of the ship, they must be turned up on their sides and pressed together.
The USCs bond together into long chains. These chains cross over one another to produce a metallic fiber that is very strong.
5. SEMICONDUCTING PROPERTIES
The material is somewhat different from the known semiconductors in that it also has optical and dielectric properties as well. These allow the material to convert electrical to photon energies over the entire sweep of a valence-to-conduction band. At the bound or valence energy level, the material emits only small amounts of light, but in the highly excited conduction states, large number of photons are emitted. In addition, there is the doubling of conduction frequencies from the visible band into the ultraviolet band. The emissions of this band occur as white light.
The semiconductor material is grown with the same “n-p” (negative-positive) dopants as the known semiconductor materials that are used in so many different electronic devices.
In the craft, the negative dopants occur in the material that is closest to the center of the ship. This material attracts positive charge and repels negative charge, and so the current is naturally away from this portion of the material and drawn toward the positive doped material, which is toward the outside of the craft.
The semiconducting material has the structure of a quasicrystal and the conformation of biological molecules. It is grown initially into sheets that are a series of parallel layers. This, too, is common to the known semiconducting materials, such as silicon or germanium. But there layers must undergo an additional structural transformation before they can successfully convert light energy into force (times a distance). This involves their growth into a three-dimensional lattice configuration, also known as a “slip lattice.” This lattice occurs in natural crystals, but it is difficult to grow into synthetic crystals.
Once the three-dimension slip lattice has been grown into the semiconductor metol, the final biological conformation is achieved by folding over the slip lattice and compressing it into a series of cylinders. These cylinders will rotate light as they compress it, and it this combined action that converts it into a force field that is able to act through the distance of the folded lattice. It is the distance through the lattice that is required to transform it into a force. When it is multiplied by the force, it is equal to the energy of the photons that are moving through the semiconducting material.
The semiconducting material allows electrons to flow through it in a direction that is always pointed towards the outside of the craft. These electrons flow parallel to the photons that have been emitted by the luminescence dopants that are located in planes that are between the superconductor and the semiconductor, and in random locations inside of the semiconductor. These dopant materials are strongly magnetic, and their magnetic fields cause the semiconducting electrons to spin with a great deal of energy inside the material. This spin occurs at microwave frequencies of energy, and so this type of radiation is a by-product of the array of materials. This field is strongly interactive with the rotated light’s magnetic and electric fields, and plays an important role in stabilizing the force field as it is produced by the decay of the photons in the cylinders.
The electrons that excite it are fed in from the four symmetry portions of the structure that lie above and below it. The magnetic “piece of bread” accelerates electrons and creates opposite spin populations which cancel one another, thus producing the Cooper Pair electrons that are the “raw material” of superconducting currents. Once the Cooper electrons are onto the superconducting sheets, the diamagnetic atoms superconduct them instantly throughout the entire structure from which the metols are fabricated (such as a spacecraft).
There are 4-5-4 magnetic metols and 4-5-4 diamagnetic metols. In the four symmetry metols, magnetism and diamagnetism occur separately, but in the five symmetry quasicrystals, magnetism and diamagnetism occur together. In these crystals, diamagnetic and magnetic atoms occur together as the cation or positively charged ion groups of the quasicrystalline crystalline structure. These groups consist of anywhere between two and five atoms. They occur at the vertex points of the quasicrystalline structure as substitutes for a single anion (negative ion).
The cation groups create the superluminal field of the metal quasicrystal by trapping electrons in the fields that develop between them when they are excited with electromagnetic energy. The photons from these field effects are then broken down into force fields as they are radiating their way out of the quasicrystals.
The interface of the four with the five symmetry layers is critical to the production of the force field. It occurs in biological membranes when various ionic salts move through them to create the phenomenon of biological superconductivity.
6. CRYSTAL TYPES, GEOMETRIES, AND DOPANT RATIOS
a. Quasicrystal: The macro crystal with a negative hyperbolic surface of infinite size. A positive electric field profile based upon multi-valence and the “asymmetric positive” figure eight. Strong electric dipoles but no magnetic fields, as the valence bonding pattern of individual molecules prevails. The anions of the quasicrystals retain their pentagon symmetry when the unit spiral cells are grown out from their planar surfaces. When the USCs grow, they form containers (egg shells) around them.
The USCs are severe nonlinear optical rotation (SNOR) crystals. They implode light and convert its energy into a force that acts through a distance or through time. The USC has a transitional-rotational form with pentagon framework: anions enclosing magnetic and diamagnetic atoms that are arranged on the surfaces of spiral planes that are described by the helicoid transcendental equations (p. 302). The magnetic fields that are used to pull the USC out from the plane surface of the quasicrystal spin the individual ions??? [sic]. The spin forces act to align the magnetic atoms into the spiral planes of the helicoid, and the diamagnetic atoms are repulsed by the magnetic forces into the center of each plane in the helicoid.
b. Geodesic Crystal: The micro crystal with a positive spherical surface with a minimum size that is determined by the size of the framework atoms. Quadrivalent bonding instead of valence bonding. An asymmetric figure-eight bonding between atoms, but “asymmetric negative” limaçon curvature with all electrons on surface of geodesic. Strong magnetic (or diamagnetic) fields, but a total electric charge of zero as individual electric dipole fields are concentrated at same point. Supermagnetic or superconducting crystals, and superluminal with dopant color centers. Dynamic crystals with exploding light fields. Four symmetric lattice with precise tetrahedral coordination between dopant atoms (magnetic or diamagnetic) and framework atoms.
The geodesic evolves (is grown) into a “living crystal” with a buckled conformation to its surface. This is the basic feature of all living proteins. This conformation is produced when the dopant atoms, which are either magnetic or diamagnetic, are added to the initial geodesic lattice. This lattice is a body-centered cubic.
The superconductor uses strong diamagnetic atoms, such as copper, gold, or silver, while the magnetic core material of the induction coils uses the ferromagnetic elements, iron, nickel, and cobalt. When these atoms bond to the surface of a geodesic, the bonds that occur between the individual pentagons in the geodesic are broken and re-attached to the dopant atoms in tetrahedral coordination. Three connecting legs must be used to construct one tetrahedron. These legs normally connect the pentagons and hexagons in the Fuller Geodesic. One pentagon has five connecting legs. Four of these are used to construct two sides in two tetrahedrons, and the remaining one is used to construct one side in one tetrahedron.
There are five connecting legs per pentagon, one for each side. There are always 12 pentagons in one geodesic, no matter how many hexagons there might be. This is the number that is required to curve the hexagons into a spherical surface. The number of connecting legs is 60 for all geodesics. If three legs [sic] are required to construct one tetrahedron, then there are a maximum of 20 of them per geodesic. This is the number of hexagons in the 60-member Fullerene Geodesic.
The pentagons in the new geodesic structure are all connected to one another by tetrahedrons. When these grow into the cubic lattice of the superconductor, the pressure from the other geodesics in the lattice distorts the doped geodesics into their living conformational structure. The surface is no longer regular, as each tetrahedron assumes a slightly different angular orientation.
The new geodesics could be called “phonodesics” (short for phonon geodesics) because their new structures are very susceptible to phonon vibrations. The tetrahedron bonds between the pentagons are much looser than the hexagon bonds of the original structure, and this makes the entire structure very pliable. Each pentagon is able to move independent from its neighboring pentagons. In combination with the electron cloud that surrounds the surface of the new geodesic structure, the phonodesic is an ideal converter of infrared photon energies into phonon energies.
This is an initial statement on the nature of form and charge as it occurs in these new crystalline structures.
The two basic forms of the pentagon occur in surfaces with either a positive or a negative curvature. These surfaces in turn have opposite electric field charge distribution curves.
A quasicrystal has a negative curvature because it grows as a large single crystal of potentially infinite size. The quasicrystal can be taken as a plane surface of infinite size. When spacecraft are constructed, they are grown as a single large quasicrystal. Each plane surface of the quasicrystal can be thought of and analyzed as the negative curvature of the hyperbola.
The geodesic crystal has a positive curvature that can be described by the sphere, which has the same equation as the hyperbola, except that all of its terms are positive, while the hyperbola has one negative term. The single negative term of the hyperbola is related to the single negative ion (anion) of the quasicrystal.
The electron cloud profiles of these two basic structures also can be described in terms of positive and negative curves. The quasicrystal has the electron cloud configuration of a normal molecule. This is described mathematically as a lemniscate by the plane surface bifolium curve. This curve is an asymmetric figure eight, where the two halves of the figure eight are not in directly opposite positions. Instead, they occur at angles to one another. These angles define the positions of the electron clouds in many molecules, water being one example.
Water is a triatomic substance, one that is composed of three atoms. The bifolium defines the electron cloud that orbits between the two hydrogen atoms and the single oxygen atom. In a quadratomic molecule, such as ammonia, a trifolium must be used to describe the electron clouds of the three hydrogen atoms; in a molecule that has five atoms, such as methane, a quadrafolium must be used to describe the electron clouds of the four hydrogen atoms.
Electrons in the bifolium fields are occupying their traditional valence positions of molecules. They tend to ionize easily, as the electron cloud can be broken at its periphery. The curve of these clouds is in the lemniscate family. This is an example of a negative surface curvature having a positive electric field curvature.
The geodesic has a positive curvature to its surface and a negative curvature to its electron field. Some of the outer electrons in the geodesic’s framework atoms have been squeezed out of their normal orbitals. These orbit the entire geodesic as if it were a single atom with a larger than normal diameter. The electron cloud of the geodesic can be described by two different plane surface curves. One is the lemniscate, which is the figure eight, and the other is the limaçon, which is a reversed-asymmetric figure eight.
The lemniscate defines the mathematical quantum state of the electrons that are shared in the multivalent bonds between the quadrivalent framework atoms of the geodesic. This is not the normal molecular bond which was described by the bifolium curvature. This bond is the same as the one that occurs in the carbon-carbon bonds of hydrocarbon molecules. Electrons are shared between adjacent framework atoms in the phonodesic pentagons, but they do not belong to one or the other atom as they would if they occurred in a normal molecular bond.
Figure eight bonds occur in tetrahedral coordination between all of the framework atoms that make up a geodesic structure, whether it is a doped or undoped structure. Each framework atom is surrounded by and bonded to three other framework atoms in tetrahedral coordination. Each of these is defined in quantum curve mathematics by a lemniscate function in the two dimensions of a plane surface.
As the geodesic crystal is grown, the critical factor is the degree of force that is impacted onto its lattice structure. This force determines the ground state of the electrons that are holding the structure together by sharing orbitals between the adjacent framework atoms. If the ground state is a high energy one, then all of the geodesic atom’s outer electrons will be free to form into a single electron cloud which will orbit the entire crystal en masse.
This is a special bonding state which is necessary for the geodesics that are used in the superconducting metol crystals. It is defined by the limaçon plane surface curve. This curve defines the path of the electrons that form into the geodesic electron cloud. It is a “negative asymmetric” figure eight that has one of its halves folded back over the first half. This “backfolding” defines its negative curvature. The smaller half of the curvature of the limaçon defines the quantum orbits of the elevated ground state electrons in a single framework atom, and the larger half defines the same electrons in the common orbitals of the entire geodesic. If there are 60 framework atoms in a geodesic, and each atom has one free electron to contribute to the common cloud, then there are 60 limaçon curves that describe their quantum states.
In the molecular electron cloud, the electric field becomes unbalanced and a dipole field with a charge bias develops. This is the negative curved plane crystal surface of the quasicrystal and the superconducting square planes of superconductors. Here valence bonds dominate.
In the geodesic electric field, the unbalancing folds back on itself, and the electric dipole field for individual atoms on the surface disappears, and instead concentrates at the center of the atom. The positive electric field occurs at every atom, but the negative electron cloud occurs uniformly over the entire surface, and its center of charge is the center of the atom. This is the same center as the center of charge for the positive charges, so the two charges cancel and the overall geodesic structure has no dipole field. It does, however, have a net charge, either positive or negative, depending upon its degree of ionization which, in turn, is related to the number and energy density of electrons that are traveling over its surface. The charge of the geodesic is related entirely to the effects of the superconducting current. Geodesics can have strong magnetic fields if magnetic atoms are used to construct them. The structure holds them in place, and if they are magnetized when they are grown, the field has a high coercive force and a high gauss level.
In the phonodesic, superconduction only occurs if the number of electrons in the limaçon??? [sic] cloud is more than twice the number of diamagnetic atoms that are loosely bonded onto the geodesic structure. The number of possible diamagnetic atoms is considered first.
There are always at least 20 diamagnetic atoms per geodesic, one for each of the hexagons in the normal 60-member Fullerene Geodesic. Additional diamagnetic atoms occur in the edge, face, and diagonal positions of the cubic lattice structure. These positions are between individual geodesics. The maximum possible number is either seven or eight, so the total number of diamagnetic atoms per geodesic is either 27 or 28.
If the multivalent bonds between framework atoms in a geodesic are “+3” and “-3” for an adjacent pair of atoms, then both atoms have one electron orbital left over that they can contribute to the common electron cloud. This means that there would be 60 common cloud electrons in a 60-member geodesic. The ratio between the number of common cloud electrons and the number of diamagnetic atoms is: 60/27 = 2.222…, or: 60/28 = 2.143.
The ratios are the same as those that occur between the diamagnetic copper atoms in a Perovskite superconductor and the electron contributing oxygen atoms. There are several different types of Perovskites, each having a slightly different ratio of oxygen to copper atoms. These ratios tend to follow the sequence: 2 1/3, 2 1/4, 2 1/5….
These values are close to those that have been calculated for the geodesic superconductors, and so it can be assumed that the valence laws for all superconducting materials are identical, and that the ratio of the electron supplier atoms (such as oxygen) to the diamagnetic atoms must always be greater than “2.”
The atoms that are used to make a geodesic crystal have a common electron cloud that averages about one electron per framework atom. These electrons form into the common cloud, which has different quantum properties than the electrons that occur as the anions in most materials. The electrons that are in the common cloud can have the quantum energy distributions of molecules, even though they are still attached to atomic orbitals.
The vibrational bands of molecules are wide, while the quantum absorption bands of atoms are narrow. When the geodesic is grown under enough pressure so that a common cloud is formed, the quantum levels in the cloud have the same wide band energies as those that are found in molecules. Usually, this occurs over a wide band in the infrared portion of the spectrum of the framework atoms. Because the electrons are simultaneously occupying molecular and atomic orbitals, their energies are able to convert mutually between photon energies in the atomic orbitals and photons in the geodesic-molecular orbitals. This mutual conversion means that energy can be transposed without loss between a phonon at the velocity of sound and a photon at the velocity of light. This has profound implications for all of modern physics.
7. METOL GROWTH
The metol is grown in stages. First the quadrivalent geodesics are grown from a growth mix that has only framework atoms. This is the most drastic growth stage, the one where the greatest changes are grown into the material, so it must be as pure as possible for the results to be uniform.
When the initial growth stage has been completed, the 60-member geodesics have been formed into a rigid cubic lattice structure. The individual geodesics are in a super-compressed form, where their ground state energies are in a lower orbital than would normally occur in a Fullerene Geodesic. This high energy ground state frees approximately one outer electron per atom in the structure to form into a common electron cloud. This is not an ionized electron, as it remains in a quantum atomic orbital. However, it also combines with all of the other 59 electrons from the other 59 framework atoms to orbit the entire structure as an electron cloud.
Electron clouds usually only occur in molecules between the anions and cations. When they occur in a geodesic structure, they have the dual characteristics of molecular electrons and atomic electrons. The electrons have very precise frequencies and energies when they are in their atomic state, but when they are in their molecular vibrational state, their energies can be very wide band.
The wide band energies of the common cloud electrons of a geodesic are composites of the narrow band energies of the 60 possible quantum states of the 60 atoms that make up each geodesic. They can occur over any energy range that is compatible with those of the outer electron shells’ energies of the framework atoms. These are usually infrared frequencies.
The dual molecular-atomic nature of the vibrations of a geodesic’s electrons gives these structures some very unique characteristics. One of these is the ability to convert photon energies with no loss of energy into phonon energies. This conversion happens in many types of crystalline lattice structures, but with less efficiency, as many of the phonon energies in these structures cannot be converted into photon energies because their energy levels are not the same. With the wide band energies of the geodesics, an efficient conversion is possible through wide portions of the infrared spectrum.
Once the compressed geodesic has been grown, it is quickly assembled into its natural cubic lattice structure. This happens in the same growth process. This lattice structure has large spaces between the individual geodesics, so its density is less than that of the atoms that compose it. In the first stage of the initial growth process, the atoms are compressed into a greater density in the individual geodesics, but in this second stage of the initial growth process, the geodesics are grown into an expanded lattice structure which lowers their overall density to a value that is less than the original density of their amorphous atomic masses. This is the end of the initial growth process.
In the second growth process, the expanded lattice geodesic is doped with diamagnetic or magnetic atoms. Which one is used depends whether a magnetic or diamagnetic field is desired in the final crystalline material.
In the diagram [sic], the diamagnetic atoms are shown as small dark circles that occur in two locations in the lattice, the centers of the hexagons, and in the spaces of the expanded lattice structure. (see above for ratios.)
A superconductor must have a layer of cations in its lattice if it is to superconduct. These ions form bonds with the centers of the electric fields of the electron clouds. These are the superluminal fields that are so important to the operation of the metol. These are molecular valence oscillations between the cations and the electron clouds of the geodesics. Electrons are moved into and out of the orbitals of the cations at a rapid rate, and this produces a level of luminescence that is unknown in any materials that have been discovered or synthesized to date.
The cations modulate other infrared frequencies onto the wide band energies of the common cloud, making it into any even wider band of energies. Because of their valence, the cations bond strongly into the lattice structure of the crystal. The diamagnetic atoms, however, do not.
Without the cations in the crystalline structure, the photon-phonon energy bands would not be wide enough to remove all of the heat that is produced during superconduction of the outer or infrared electron bands, and the lattice structure would disintegrate from the heat.
The ratio of framework atoms to diamagnetic atoms to cations in the crystalline lattice is approximately: 60:27:1. The last value for the cations is somewhat in question, and is likely to be a lower fractional value.