Methods and apparatus for quantum wireless energy transmission

Abstract

There is provided a system for quantum wireless energy transmission, comprising: a transmitter, comprising: a transmitting element, the transmitting element comprising a first electrically conductive mirror matching layer and a first electrically conductive mirror synchronisation layer, the first electrically conductive mirror matching layer and the first electrically conductive mirror synchronisation layer separated by a dielectric layer; means for sending an energy information packet, the energy information packet comprising information about an energy quantized by the transmitting element; a receiver, comprising: receiving element, the receiving element comprising a second electrically conductive mirror matching layer and a second electrically conductive mirror synchronisation layer; means for receiving the energy information packet, wherein, in response to receiving the energy information packet, the receiver is operable to control the receiving element to decompress the energy quantized by the transmitting element.

Description

METHODS AND APPARATUS FOR QUANTUM WIRELESS ENERGY TRANSMISSIONFIELD OF THE INVENTION

[0001] The present disclosure relates to energy transfer using a quantum vacuum as an energy transfer medium. In particular, the disclosure relates to methods and apparatus for wireless energy transmission based on energy quantization and creation of persistent energy structures in space.BACKGROUND

[0002] A range of methods of wireless power transmission are known. In near-field wireless power transmission, also known as electromagnetic coupling wireless power transmission, power is transmitted over a short distance using magnetic fields (i.e. inductive coupling between wire coils) or using electric fields (i.e. capacitive coupling between metal electrodes). In far-field wireless power transmission, also known as radiative wireless power transmission, power is transmitted by electromagnetic beams, such as microwave or optical (e.g. laser) radiation.SUMMARY OF THE INVENTION

[0003] Embodiments of the invention provide a system for quantum wireless energy transmission, comprising: a transmitter, comprising: a transmitting element, the transmitting element comprising a first electrically conductive mirror matching layer and a first electrically conductive mirror synchronisation layer, the first electrically conductive mirror matching layer and the first electrically conductive mirror synchronisation layer separated by a dielectric layer; means for sending an energy information packet, the energy information packet comprising information about an energy quantized by the transmitting element; a receiver, comprising: receiving element, the receiving element comprising a second electrically conductive mirror matching layer and a second electrically conductive mirror synchronisation layer; means for receiving the energy information packet, wherein, in response to receiving the energy information packet, the receiver is operable to control the receiving element to decompress the energy quantized by the transmitting element.

[0004] Further embodiments of the invention provide a method of transferring energy, comprising: receiving, at a transmitter element, an electrical input signal; quantizing an energy comprised in the electrical input signal to generate a quantized energy; transmitting, from the transmitter element, an energy information packet comprising information about the quantized energy; receiving, at a receiver element, the energy information packet; based on the energy information packet, decompressing the quantized electrical input signal to generate an electrical output signal.

[0005] Still further embodiments of the invention provide a transceiver element for a quantum wireless energy transmission system, comprising: a matching layer, comprising a first electrically conductive mirror layer; a synchronisation layer, comprising a second electrically conductive mirror layer; a dielectric layer, thedielectric layer arranged between the matching layer and the synchronisation layer; a plurality of signal contacts, the plurality of signal contacts arranged on a surface of the matching layer.BRIEF DESCRIPTION OF THE DRAWINGS

[0006] Further details, aspects and embodiments of the invention will be described, by way of example only, with reference to the drawings. In the drawings, like reference numbers are used to identify like or functionally similar elements. Elements in the figures are illustrated for simplicity and clarity and have not necessarily been drawn to scale.

[0007] Figures 1Ato 1C show a theoretical model of the behaviour of a free electron in a copper conductor without an applied electromotive force.

[0008] Figures 2A to 2C show a theoretical model of the behaviour of a free electron in a copper conductor under the influence of an applied electromotive force.

[0009] Figures 3A to 3C show a theoretical model of the behaviour of a free electron in a copper conductor, and the process of absorbing local energy.

[0010] Figure 4 shows the decrease of energy transmission efficiency as distance increases, as displayed in classical energy transmission methods of the near-field type.

[0011] Figure 5 shows an energy distribution model specific to quantum wireless transmission.

[0012] Figure 6 shows a graph of the compression of local energy and the decompression of said energy at a certain distance.

[0013] Figure ? shows a unified modelfor quantum wireless transmission.

[0014] Figure 8 shows a diagram of the interaction of two configured layers of electrically conductive mirrors with the formed images IMG1 and IMG2, and the interaction components that form as a result of setting up these two layers.

[0015] Figures 9Aand 9B show a diagram of how design features affect the appearance of forcesand basic properties of a transmitting or receiving element.

[0016] Figure 10 shows a diagram of the interaction between transmitting and receiving quantum wireless transmission elements and their respective interaction components, which occur after the matching of two or more layers of electrically conductive mirrors.

[0017] Figure 11 shows the properties of the wireless element, which depend on the intersection area, IONA.

[0018] Figures 12Ato 12D show the process of quantizing (compressing) local energy by the transmitting element of a quantum wireless power transfer system, for a simple double layer transfer element.

[0019] Figures 13A and 13B show a sector of a wireless multisector element, according to some aspects of the present disclosure.

[0020] Figure 14A shows a physical area that will be formed by the intersection of two electrically conductive mirrors.

[0021] Figure 14B shows an IONA area and the generation of a unique code for a wireless element, with the current direction indicated by arrows.

[0022] Figure 15 shows an example of an IONA area for a multi-sector wireless receiving element for collecting / harvestingfree energy from space.

[0023] Figure 16 shows an example of a transmission element of a quantum wireless transmission system, according to aspects of the present disclosure.

[0024] Figure 17A shows a front view of a transmitting element of a quantum wireless transmission system, according to aspects of the present disclosure.

[0025] Figure 17B shows a back view of a transmitting element of a quantum wireless transmission system, according to aspects of the present disclosure.

[0026] Figures 18A (front) and 18B (back) show an example of a transmitting element for a quantum wireless transmission system, the element having multiple sectors, according to aspects of the present disclosure.

[0027] Figure 19A and Figure 19B show an example of a multilayer element for a quantum wireless transfer system, according to aspects of the present disclosure.

[0028] Figure 20 shows a diagram describing possible combinations and variants of quantum wireless transfer elements.

[0029] Figure 21 shows a block diagram of a quantum wireless power transfer system and the energy flow from a source to a load.

[0030] Figure 22 shows a graph depicting the modes of transmission element operation.

[0031] Figure 23 shows a block diagram of a transmitter unit.

[0032] Figure 24 shows a block diagram of a control unit.

[0033] Figure 25A shows a topology of a class-E inverter circuit suitable for generating a signal for supply to a transmitting element, and Figure 25B shows a graph of the output voltage and current of the class-E inverter of Figure 25A.

[0034] Figures 26A to 26C show rectifier circuits suitable for rectifying a signal received by a receiving element for output to a load.

[0035] Figure 27 shows an efficiency diagram of a quantum wireless power transfer system and its components.DETAILED DESCRIPTION

[0036] In the following description, for purposes of explanation, numerous specific details of certain examples are set forth. Reference in the specification to “an example” or similar language means that a particular feature, structure, or characteristic described in connection with the example is included in at least that example, but not necessarily in other examples.

[0037] According to quantum theory, a vacuum is not truly empty. Instead, the quantum vacuum state contains pairs of particles that continuously appear and disappear, which leave their signature behind by affecting the energy levels of atoms. A zero point energy is an energy that exists in molecules and atoms even at temperatures close to absolute zero (0 Kelvin) in vacuum. At this low temperature, atoms experience atomic or subatomic fluctuations in accordance with the Heisenberg uncertainty principle, with said fluctuations or vibrations being caused by the zero point energy.

[0038] Techniques described herein make use of methods of energy compression through formation of persistent quantum energy structures in space, transfer of said energy and energy information over a distance, decompression of said energy from the energy information, and restoration of the state of the energy to the original energy state following decompression.

[0039] Local energy undergoes compression by passing between layers of tuned electrically conductive mirrors of a transmission element. An electrically conductive mirror may comprise a copper layer that has been polished to a mirror state, in order that the copper layer achieves improved contact with a dielectric material. Compression, in the sense used herein, refers to a significant compression of the energy, i.e. a decrease in the amount. However, this decrease of energy does not mean the decay of said energy or the transition of said energy from one classical state to another (such as electrical energy to thermal energy). Rather, the decrease of energy occurs due to the transfer (or ‘shredding’) of local energy to a quantum vacuum. The result of this transfer of local energy to the quantum vacuum is the compensation of the positive component by the negative, in order to maintain energy equilibrium for a particular point in space. Accordingly, the consequence of the compression is the formation of information in the form of a weak electromagnetic signal. The power of the electromagnetic signal is unequal with respect to the energy that is being transmitted. Local energy is compressible when the tuned mirrors of a transmitting element pass between the layers by completely or partially decaying the local energy as a result of compensation for the negative component created as a result of suppressing the quantum vacuum. When local energy in the form of an electrical or magnetic field passes from one electrically conductive mirror to another through the dielectric, it is compressed (or quantized), meaning that there is compression of a negative component that is present between the layers of electrically conductive mirrors as a result of suppressing the quantum vacuum. This effect is similar in operation to the Casimir effect. The thickness of the dielectric adjusts the distance betweenthe electrically conductive mirrors, which has the effect of increasing or decreasing the suppression force of the quantum vacuum.

[0040] Decompression, in the sense used herein, refers to the complete or partial restoration of energy between layers of tuned electrically conductive mirrors of a receiving element using the received energy information signal, said signal created as a result of the energy compression at the transmitting element.

[0041] The information signal functions to transmit information about an amount of energy that has been quantized. The information signal on energy quantization is transmitted by the transmitting element to the receiving element. In turn, the receiving element processes the received information about the compressed energy and releases / decompresses the energy from the internal structure of the receiving element. The received energy can then be converted into electricity of a suitable voltage and current for a desired load or application.

[0042] Transmitting and receiving elements may have at least two layers, or be multi-layered. The layers can be classified into two groups according to their functionality and properties: a synchronisation layer and a matching layer. The layers may be pressed together and isolated by a dielectric lining such that there is no contact between the main layers, but instead a formation of an interlayer force, k(mir). The force of interlayer interaction increases the level of persistent anomalies in the behaviour of free electrons.

[0043] According to some examples, the transmitting and receiving elements may comprise one or more simple or combined sectors. Simple sectors include sectors separated from each other with their own respective addresses. For example, a transmitting element having two simple unequal sectors can compress local energy using its own addresses, meaning that the transmitter may have multiple active independent transmission sectors, such that local energy from two independent RF (radio frequency) sources can be supplied to the transmitter. Combined sectors include sectors that are connected by physi cal contacts with each other. Due to addresses that have sectors, accurate point delivery of wireless power to an assigned destination can be achieved.

[0044] Figures 1 A to 3C are provided for the aid in understanding the principles and teachings disclosed herein.

[0045] Figures 1Ato 1 C show a theoretical model of the behaviour of a free electron in a copper conductor without an applied electromotive force. This free electron corresponds to the energy level Eo, i.e. the starting initial state, or ‘zero state’. Each electron in the cloud of free electrons moves in random directions and with different velocities.

[0046] Figure 1A shows a diagram of the probability of free electron detection for an electron e10 with starting position 100 and final position 102. The diagram of Figure 1A is concerned with the displacement of the electron along the x-axis, in order to determine a final probability. Therefore, positions 100 and 102 can be considered equivalent. To provide a simplified classical model of electron behaviour, the position of electron e10 is unchanged because the energy level corresponds to zero. In Figure 1A, the constancy of thisposition can be seen. The starting position 100 is the same as the final position 102, and so the electron path travelled is zero. This means that there is no electrical current, i.e. l=0. The complete uncertainty path of electron e10 from starting position 100 to final position 102 is formed from sequential probabilities. P10 is the first sequential probability of the position of the electron e10. P20 is the second sequential probability of the position of electron e10. P30 shows the third sequential probability of the position of electron e10. P40 shows the fourth sequential probability of the position of electron e10. Figure 1 A therefore shows the path sequence of the zero energy electron e10. In this case, according to the classical model, the full energy level in the copper conductor corresponds to zero. The dashed line between point 100 and 102 in Figure 1A indicates that the copper conductor is in a state without an applied electromotive force (i.e. energy = 0). Along the x-axis the electron does not undergo displacement at the end point of the sequential probabilities, which indicates an absence of electron flow in this direction. The y-offset here is considered negligible for the purpose of visual representation. Any displacement from the dotted line (i.e. displacement in the x-axis) of the final probability of the electron e10 at point 102 would give rise to electron flux (i.e. a current). The diagram of Figure 1A represents a simplified model with the behaviour of the electron represented in two axes for ease of understanding. In reality, the spatial behaviour may include various variations of probable positions and behaviours in the x-, y- and z-axes (not shown).

[0047] Figure 1 B shows a graph of the non-zero behaviourof a free electron at the zero level of total energy, relative to the classical model of electron behaviour over a certain theoretical period of time. The graph illustrates the fluctuation 105 of the free electron over time At. An upward oscillation of the positive component 103 represents an emission of electromagnetic energy by the quantum vacuum. An upward oscillation of the negative component 104 represents a suppression of electromagnetic energy by the quantum vacuum. The total energy level 106, according to the classical model, shows that the positive component compensates for the negative component, thus ensuring the equilibrium of the system. Total energy level 106, Eo, is therefore:E0= + 2 - 2 + 1 - 1 + 4 - 3 - 1As such, the classical model is not violated. The longer an emission of electromagnetic energy from the quantum vacuum is absent, the higher the negative component of the oscillation grows. Quantum vacuum suppression can occur on its own or can be recreated artificially (for example, through the use of Casimir mirrors). The nature of suppression has a short-term character and in most circumstances will be compensated by a positive component, which is generally present in free space since a quantum vacuum emits electromagnetic energy in most situations.

[0048] Figure 1 C shows a graph of the total energy level of the free electron, over a certain theoretical period of time, according to the classical model. The output of the system is therefore a zero total energy level. The total energy level 106 is shown by the dashed line, which indicates zero total energy level - i.e. no growth or fall.

[0049] Figures 2A to 2C show a theoretical model of the behaviour of a free electron in a copper conductor under the influence of an applied electromotive force, said electromotive force corresponding to the energy level Ei, where Ei * 0.

[0050] Figure 2A shows a diagram of the probability of the position of a free electron e10 with starting position 200. Without the applied electromotive force, the free electron e10 will have a final position 202. Electrons e10 and e11 represent the same theoretical electron, where e10 represents said electron in a calm state, whereas e11 represents an alternative behaviour of aid electron in the presence of an applied electromotive force. Thus the probabilistic paths can be compared for the electron in a calm state versus a state with an electromotive force applied. The dotted line indicates the probable path to a probable final position 208 of the free electron e11 - i.e. the behaviour of the electron e11 with the electromotive force applied to it. Without electromotive force, the starting position 200 and final position 202 of electron e10 are equal, and therefore the total energy position is Eo= 0. If however a certain electromotive force is applied to the copper conductor, then the end position 208 of electron e11 will be completed with a slight deviation from end position 202 of electron e10. This indicates a directional movement in the opposite direction with respect to the applied electromotive force. The position shift will not be significant, and corresponds to the classical model, because the magnitude of the electromotive force affects only the flow of electrons and not the speed of the movement of said electrons, meaning that displacement along the x-axis will remain within the classical model. The probability path will be identical, as it stores the basic picture of successive probabilities, however each of these probabilities will be extended, because an electromotive force will act all the way over a certain period of time. The basic picture is one of many alternative probabilities of the electron motion path for an imaginary type of electron behaviour. This probability expansion will not affect the finite electron path, despite the fact that the probability is slightly elongated. The reason for this is that probabilistic processes occur at a high rate, and ultimately the electron ends up at the endpoint of said probabilistic path. The sequential probability 207 (i.e. the path Pn, P2i, P31, P41) is elongated because of the action of the electromagnetic force on the probabilities, but the direction of the sequential probability is maintained, i.e. - P30 = - P31 . In this context, an elongated probabilistic path means that the probability of finding the electron e11 at position 208 is greater than the probability of finding the electron e10 at position 202. The probability has a direction vector, which will be directed to the endpoint 208 for electron e11 and to endpoint 202 for electron e10. Whilst the presence of an electromotive force can influence the probability, the vector of said probability will not change. The final position 208 of electron e11 is caused due to the action of the applied electromotive force. The parameter vdrepresents the drift velocity, which is the average velocity of particles, for example electrons, that occurs as a result of the influence of an electric field. This influence of the electric field on the conductor causes a small drift of randomly moving electrons in a certain direction. In this case, there is a non-zero electron flux (i.e. I * 0), meaning that there is the emergence of movement. Figure 2A therefore demonstrates compliance with the classical model, whereby everything happens within the expected ‘normal’, without any anomalies. Along the x-axis the electron does not undergo displacement at the end point of the sequential probabilities, which indicates an absence of electron flow in this direction.The y-offset here is considered negligible for the purpose of visual representation. Any displacement from the dotted line (i.e. displacement in the x-axis) of the final probability of the electron e10 at point 202 would give rise to electron flux (i.e. a current). The diagram of Figure 2A represents a simplified model with the behaviour of the electron represented in two axes for ease of understanding. In reality, the spatial behaviour may include various variations of probable positions and behaviours in the x-, y- and z-axes.

[0051] By way of further explanation, the behaviour of an electron can be divided into two components: real and imaginary. The real component of the behaviour is responsible for the illustrated component x, and is responsible for the behaviour if the electron under the classical model, which can be predicted through the application of a electromotive force to the conductor, whereupon it is expected that the electron will demonstrate movement in the opposite direction to the applied electromotive force. The imaginary component of the behaviour is that which defines all probabilistic processes that occur within the electron. This is to say, one can assume either the probability of finding said electron, or the trajectory of motion. Changes in this imaginary behaviour of the electron will not affect the classical (i.e. real) behaviour, because the effects on the imaginary model are caused bythe classical model. Under certain conditions, the imaginary part can be influenced in such a way as to change the classical model, which is considered bythe methods of Figure 3. This is to say, the present application makes use of the creation of conditions under which the influence on the imaginary component of electron behaviour can result in anomalies in the classical behaviour of said electron.

[0052] Figure 2B shows a graph of the behaviour of a free electron when the local energy is increased to E1 , where Ei > 0. The graph shows an increase of the local energy over a certain theoretical period of time, At. The fluctuation of the free electron does not take into account that an increase in the local energy has taken place. Accordingly, oscillation in the direction of increase and decrease of positive and negative occurs in a constant manner, even with the increase of local energy. The classical model of behaviour of a free electron is therefore not violated. The line 210 shows increase in the local energy of the conductor. The varying line 211a represents fluctuations with increasing local energy on the conductor. Note that fluctuations of the free electron do not change. Dashed line 211 indicates an output, initial level of total energy Eo, where Eo= 0. This means that no current flows through the conductor. Such a conductor, through which no current runs, can be understood as the initial state. When current is passed through the conductor, the level of local energy is increased. A comparison can therefore be made in how the state of the conductor has changed, comparing a conductor through which current runs and said conductor in the absence of a current.

[0053] Figure 2C shows a graph of the total energy over a certain theoretical period of time, according to the classical model. In this context, total energy means the total energy of the conductor of this example, including energy released from the conductor in the form of magnetic fields, electric fields, or heat. The graph shows the increasing of energy levels from Eoto +E, and then returning to Eo, where Eois the minimum possible energy level according to the classical model. +E represents the energy that can be found in space in the form of electrical fields, magnetic fields, and heat, which can be measured (in the classical model) using fieldmeters. The increasing of the local energy causes the movement of the free electron, which passes the path di, where di * 0, over a certain theoretical period of time. The path dl represents the distance that the electron will travel over a certain period of time through the conductor. The dashed line indicates the initial level of total energy Eo, where Eo= 0. In the graph of Figure 2C, the increase of the total energy level does not occur immediately, but instead after a short period of time, and with a short pulse. When the energy state changes from the initial zero state Eoto a positive +E, where +E > 0, the sequential probability is elongated, but the direction of said sequential probability is not changed. Therefore, the electron will pass a certain distance, which will result in the emergence of a certain magnetic field. The directional movement of the free electrons will lead to the magnetic moments of said electrons aligning in a row, which will in turn lead to an increase in the magnetic field of the entire conductor. This property is applied in most conventional wireless energy transfer methods. Thus, it is possible to track all of the energy that is transmitted into free space, which is denoted as +E, which includes all total energy including in the form of heat.

[0054] Figures 3A to 3C show a theoretical model of the behaviour of a free electron in a copper conductor, and the process of absorbing local energy, i.e. compression of said local energy. This involves the occurrence of anomalies in the behaviour of the free electron.

[0055] Figure 3A shows a diagram of the probability of the position of a free electron e10 with starting position 300. Without the applied electromotive force, the free electron e10 will have a final position 300. The dashed line indicates the probable path (i.e. sequential trajectory) to a probable final position 317 of the free electron e12, when an anomaly occurs in the behaviour of said free electron e12. The complete path 314 shows the sequential probabilities of electron e12 from starting position 300 to final position 317. P12 is the first consecutive probability of the electron e12. P22 is the second consecutive probability of the electron e12. P32 is the third consecutive probability of the electron e12. P42 is the fourth consecutive probability of the electron e12. The direction of the sequential probabilities is maintained, i.e. - P10 = -tP12, however the path of the sequential probabilities is reduced. This is to say, the path of sequential probabilities is decreased under the influence of an anomaly. A characteristic sign of the effect of an anomaly on the sequential probability of an electron is in the braking of the electron (according to the imaginary component of the electron behaviour). A characteristic feature of electron braking when quantizing energy is a slight cooling of the conductor. The position 313 of the electron e12 and its sequential probability P32 under the action of the anomaly lags behind the position 312 of the electron e10 and its sequential probability P30, respectively. The final position 316 of the sequential probability P40 for electron e10 and thefinal position 317 of the sequential probability P42 for electron e12 will be on the same conditional line 315, i.e. will not change. This means that with the quantization of energy, the final sequential probability P42 will end on approximately the same line as for free electron e10, such that the final consecutive probabilities e10 and e12 will end at the same point (i.e. point 316 = point 317). With an increase in local energy, E2, such as a certain electromotive force applied over a certain period of time, the position of electron e12 will not change - i.e. the electron will not move in the opposite direction to the applied electromotive force. Accordingly, the behaviour of a free electron, as ischaracteristic under the classical model, will not take place. The induced anomalies that affect the behaviour of the electron e12 will create an initial state identical to the electron e10 (in the conductor) without the electromotive force applied to it - specifically the state e10 = e12.

[0056] Figure 3B shows a graph of the behaviour of a free electron when the local energy is increased to E2, where E2> 0. The graph shows an increase of the local energy over a certain theoretical period of time, At. The line 319 shows the fluctuation of the quantum vacuum with anomalies present. In the graph of Figure 3B, there is a suppression of the quantum vacuum, and accordingly an increasing of the negative component 322. However, because any system strives for equilibrium, the increasing of the negative component can be considered a deviation - i.e. an anomaly. In turn, a positive component is not able to balance a negative component over a certain period of time. Accordingly, a local energy, which is supplied or present at the point of occurrence of the anomaly, will be partially or completely absorbed in order to balance the system. This is to say, compensation of the negative component due to local energy will take place.

[0057] The line 318 shows an increase of the local energy to the level E2. The line 321 shows a compensation of the negative component, due to the local energy E2and the conditional residue of the local energy, E2a. The line 322 shows an increasing level of the negative component, - E. The line 320 shows the initial level of the total energy Eorelative to the fluctuation of the positive level E2. The conditional residue of the local energy means that if an anomaly occurs and the negative component grows on the conductor, to which some energy is supplied, then the conductor will simply absorb a part of this energy.

[0058] The anomaly is the process of absorbing energy by a quantum vacuum in a guide. For example, if 1 Watt of energy is supplied to a conductor (e.g. a wire) unaffected by anomalies from one end, then on the other end of the conductor 1 Watt of energy can be measured. However, if the conductor is exposed to anomalies, then by supplying the conductor with 1 Watt of energy, we may be able to measure only 0.1 Watt of energy at the other end of the conductor. This loss of energy is not related to heating or resistance of the conductor; rather, the higher the anomaly level the colder the conductor becomes no matter how much energy we apply to it.

[0059] Figure 3C shows a graph of the total energy of the system over a certain theoretical period of time. According to the classical model, the influence of local energy on the total energy level, + E, should be observed. However, due to the occurrence of anomalies in the behaviour of the free electron, a level of total energy + Ea is instead observed, where + Ea < + E. The energy +Ea is a residue of the total energy +E that the anomaly has absorbed. This difference in total energy level confirms the presence of the anomaly. Under this condition, the path travelled by the electron over a certain theoretical period of time corresponds to d2= 0. This is to say, there is no characteristic movement of the electron. According to the classical model, di for the electron will always be greater than d2. But if di > d2characteristic features should be observed - i.e. the directional movement of electrons, the coincidence of magnetic moments in one direction, and as a result the appearance of a magnetic field. Here d is the distance that the electron will travel under the influence of an applied electromotive force acting on the conductor (see Fig. 4). Under E2there is an electromotive forceapplied to a conductor that experiences anomalies in the behaviour of free electrons. Accordingly, in such a conductor, free electrons will travel a smaller distance than under normal conditions.

[0060] The line 323 shows an increase of the total energy level to + E. Line 318 shows the addition of local energy, E2. The line 320 shows the initial level of the total energy Eo= 0.324 is a theoretical energy level which can be measured.

[0061] The increase in the total energy level, + Ea, is not significant and does not correspond to the level of + E, which should be the total energy level when adding the amount of energy E2, as shown in Figure 3B. In the graph of Figure 3C, the increase of the total energy level does not occur immediately, but instead after a short period of time, and with a short pulse. Under conditions of anomaly, when the state of energy changes Eo E2E2a, the sequential probability of an electron is inhibited (in contrast to the classical model, where the electron is in a calm state), which should not happen -thus indicating the occurrence of the anomaly.

[0062] Figures 2A to 2C indicate that, according to the classical model, the sequential probability of electron motion is always greater than the sequential probability of movement of an electron under conditions of anomaly, as shown in Figures 2A to 2C. This indicates that the energy quantization model is opposite in process to the classical model. Evidence that the classical model works is the mandatory presence of magnetic and electric fields. However, these features are absent in the energy quantization model.

[0063] The classical model of local energy from one state to another depends on the source of transmission. For example, magnetic and electric fields are accompanied by the formation in free space of features characteristic to each of the fields. Accordingly, wireless power transmission methods can be classified according to the electrical characteristics of the transmission source into two types:(a) an electric field transmission source with a constant voltage source (CV), where CV refers to a value of an RMS amplitude in accordance with a sinusoidal alternating voltage; and(b) a magnetic field transmission source with a constant current source (CC) where CC refers to a value of an RMS amplitude in accordance with a sinusoidal alternating current.

[0064] For an electric field transmission source, an alternating electric field is generated in space through the source CV at the source of transmission of the electric field, and only the energy of the electric field is accumulated near the source of the transmission. As a result, the spatial impedance becomes high (ignoring the effect of the bias current). A portion of the energy is accumulated as magnetic energy at a distance from the source, while the remaining energy is reduced as electric field energy. This is to say, an alternating electric field occurs in space because of a CV source in the electric field source transmission, and only electrical field energy accumulates in the region proximate the transmission source, such that the spatial impedance becomes high. Accordingly, come of the energy accumulates as magnetic field energy in a location a distance from the source, whereas the remainder of the energy decreases as electric field energy. On the other hand, the energy of the magnetic field is gradually growing over time. Accordingly, the impedance of space decreases.

[0065] For a magnetic field transmission source, an alternating magnetic field occurs in space due to a direct current source (CC) in the magnetic field transmission source, and only the magnetic field energy is stored near the transmission source. As a result, the spatial impedance decreases. Part of the energy is accumulated as electric field energy at a distance from the source according to Faraday’s law, while the rest of the energy is reduced as a magnetic field. Conversely, the energy of the electric field is gradually growing. Therefore, the impedance of space increases (constrained by the bias current, which causes the growth to approach a constant value).

[0066] The units of measurement of spatial density of the electrical or magnetic energy (i.e. storage energy) are joules per cubic centimetre. In both cases, for the electric field source and the magnetic field source, electromagnetic energy is accumulated in space, and the amount of stored energy changes overtime.

[0067] Many phenomena of nature, such as light, obey the law of inverse squares. This means that as you move away from the source, the intensity decreases in proportion to the square of the distance. This law of inverse squares applies to light, gravity, and electrostatic charge.

[0068] Figure 4 shows the decrease of energy transmission efficiency as distance increases, as displayed in classical energy transmission methods of the near-field type. As the transmitted energy moves away from the source, there will be attenuation of the radiated field as the distance increases from d0to dn. Accordingly, we can observe a decreasing of energy transmission efficiency as the distance increases. This is a characteristic feature of classical energy transmission methods of the near-field type. The efficiency at a particular transmission distance is shown by the dashed line. Area 401 of the figure is a near-field area, which is subject to near area efficiency with the use of a coil receiver. The design of the electromagnetic wave antenna will not yield a useful result, because antennas cannot operate effectively in the near zone since the electromagnetic wave will not yet be fully formed, and with distance the amount of electromagnetic energy decreases. Area 402 of the figure is a far zone area, with low coil efficiency. In this case, all emitted energy can be calculated and measured using measuring tools, as the energy is subject to classical spatial energy distribution. In the example of Figure 4, the transmission efficiency and the distribution of electromagnetic energy in space are matched.

[0069] Considering the use of quantum wireless energy transmission methods using electrically conductive mirrors, the formation of persistent anomalies is observed. This means that the process of quantizing energy occurs, and accordingly the distribution of energy in space has a different form. When local energy passes through the electrically conductive mirror of the transmitting element, the instantaneous attenuation (disappearance) of energy in space can be observed, which is not a characteristic of the classical model of energy distribution.

[0070] Figure 5 shows an energy distribution model specific to quantum wireless transmission. The dashed line represents the wireless power transmission efficiency. The dotted line represents the distribution of electromagnetic energy in space. Point 501 shows the peak of maximum efficiency of energy transmission.502 shows the spatial distribution of energy, which indicates that the distribution of electromagnetic energy (represented by the dotted line) is completely absent at the peak of maximum efficiency (represented by the dashed line). The graph of Figure 5 shows an ultra-low level of stored energy in space, which tends to nearly zero at point 502. At this point, the maximum peak in energy transfer 501 occurs. This means that persistent anomalies are formed that distinguish quantum wireless transmission from classical energy transmission methods. The efficiency of quantum wireless transmission depends mainly on the synchronisation of wireless elements (transmitter and receiver). The distance, in this case, has no significant effect on the efficiency. This means that the configuration of the receiving and transmitting elements should be calculated taking into account the distance over which energy will be transmitted, in order to achieve maximum efficiency. It can be seen that the efficiency of the wireless transmission does not match with the distribution of wireless energy in space.

[0071] Moving the receiving element closer to the transmitting element will cause the opposite effect, namely the occurrence of out-of-sync behaviour and loss of efficiency. The power transfer efficiency depends on the sync area. The sync area is the area in which energy decompression occurs. Maximum decompression occurs at peak 208. The receiving element does not make direct contact with the energy that is transmitted, as would happen in the classical model of energy transmission. Instead, energy is released from the inner structure of the receiving element.

[0072] Point 503 represents a far area for the quantum wireless transmission, since the energy transfer is addressable. Measuring instruments do not record energy emissions, since there is no characteristic radiation, as in the classical model.

[0073] Figure 6 shows a graph of the compression of local energy and the decompression of said energy at a certain distance. The graph also shows the tracking of residual energy and the generation of information on the compressed energy. A first arrangement of configured electrically conductive mirrors is positioned at point A, configured to operate as a transmitting element. A second arrangement of configured electrically conductive mirrors is arranged at point B, configured to act as a receiving element. The solid line 601 at point A represents an amount of energy applied to the transmission element. The solid line 605 at point B represents an amount of energy extracted at the receiving element. The dashed line 603 represents a classical distribution of energy in space according to the classical model, whereas the dotted line represents the distribution of energy in space when quantizing energy (in this case, through the occurrence of anomalies in the behaviour of free electrons such that energy is absorbed by the quantum vacuum). The dotted line indicates a weak level of electromagnetic energy distribution in space compared to that of classical energy transfer (indicated by the dashed line). A supply of local energy 601 is provided by a short-term pulse over a certain period of time, causing an increase in the level of energy from Eoto E2. At point A, a transition of local energy 600, E2(A) through an arrangement of electrically conductive mirrors occurs, where E2(A) represents the local energy supplied to the transmitting element at point A. The moment of energy attenuation 602 occurs after passing through the configured electrically conductive mirrors at point A. This attenuation isassociated with the occurrence of anomalies in the electrically conductive mirror structure, which results in the quantization of energy and its absorption, causing the total energy to decrease from +E to +Ea. Here, +E is the total energy measured on the conductor and in the space near the conductor, and E2represents the energy supplied to the conductor (e.g. a pulse of a certain power for a certain period of time). After compression, the energy is moved to point B, the location of the receiving element. The classical distribution of energy in space is significantly different from that of the quantum wireless transmission method. The quantum wireless energy transmission efficiency is independent of the distance and amount of stored energy in space at a certain point of time.

[0074] For quantum wireless energy transmission, the energy compression / decompression coefficient shows how much energy can be compressed and decompressed. Forthe transmitter, this is governed by the equation:E2a(jnf)—(+E2(A) * ko) / d(Sync) where +E2(A) is the local energy supplied to the transmitting element at point A. The parameter k0is the coefficient of compression of the energy in the transmitting element, formed by matching layers of electrically conductive mirrors. The parameter d(SynC) is the synchronising distance, where d(SynC) for the transmitting element depends on the configuration of the physical parameters of both the transmitting element and the receiving element, and is influenced by factors including the types of the mirrors, the shape of the elements, the thickness, and the synchronisation frequencies.

[0075] The parameter E2a(inf) represents an information packet that includes the amount of energy, synchronising distance, address, and coefficient of compression of the transmitting element. The role of the information packet is to transfer the energy to a specific place for decompression of energy. The size of the information is smaller than the energy that it carries due to the coefficient of compression.

[0076] The transmitted energy can be decompressed only by a receiving element formed for interaction with, and the target of, the transmitted energy. A coefficient of decompression for the receiving element, ki, is calculated when the receiving element is created. For decompression, two cases exist:In the case where k0= ki, the energy is decompressed by 100%, under the condition that one transmitter-receiver pair exists;In the case where k0> ki , the energy is decompressed according to the value of ki , and thus 100% decompression is not carried out. This may be used where energy is to be distributed among a plurality of receiving elements.For example, having an information packet containing information about energy of 10W, the energy can be divided between two receiving elements by changing the coefficient ki such that k0> ki, and so each receiving element will receive 5W of energy.

[0077] The energy that is released at the receiving element at point B can be denoted as E2(B), and can be calculated as:E2(B) (E23(jnf) d(sync)) / kl where the information on long-range energy 604 is denoted by the parameter E2b(inf). E2a(inf) is information about the energy that has been sent by the transmitting element. Prior to receiving this information by the receiving element, this energy information may be damaged or distorted. Such damaged or distorted information can be denoted by E2b(inf). For example, metal objects or other obstructions between the transmitter and receiver may damage or distort the energy information. Thus, due to damage of the energy information (including due to attenuation of the electromagnetic signal), the receiving element will not be able to receive all of the energy sent by the transmitting element.

[0078] Decompression and release of compressed energy is performed between tuned electrically conductive mirrors. The level of the recovered energy 605 from the information stream corresponds to the level of local energy compressed at point A, such that E2(A) = E2(B).

[0079] A directional energy information package 606, denoted as E(inf), enables the transfer of energy over long distance. In some examples, the information package is generated by supplying local energy to the transmitter with a frequency greater than 100 MHz. Under such conditions, and information package is formed that can be moved over a long distance. In various examples, local energy can be supplied to the transmitter at frequencies ranging from several tens of MHz to several thousand MHz. As frequency increases, the packet of information will be subject to less distortion in free space, thus allowing energy information to be transmitted over longer distances. When the receiving element receives such an information package, the energy decompression process is the same if the receiver lies in the synchronisation region. The decompression is carried out in the opposite manner to the compression process. In the process of energy decompression, the quantum vacuum between the mirrors of the receiving element is suppressed. This processes is started when the energy information from the transmitting element reaches the receiving element. This signal contains information about the anomaly behaviour of free electrons at the transmitting element. Accordingly, the free electrons on the receiving element undergo the same anomaly as on the transmitting element. In such a situation, the process of taking energy comes from a quantum vacuum.

[0080] Advantageously, transfer of energy using quantum wireless transmission does not affect metal objects and does not cause heating (i.e. energy loss due to heat). Additionally, quantum wireless energy transmission does not present any negative impact, such as electromagnetic interference or similar, on any electronic devices in the area of operation, even if such devices are also built to make use of quantum wireless energy transmission. This enables an accurate and addressable means to transmit energy safely. The transmitted energy can be decompressed only by such a receiving elementthat is formed for interaction and is the target of such energy.

[0081] If a classical power source were to generate an electromagnetic signal of the same frequency at which the receiving element operates the receiving element would not receive this energy, because the electromagnetic signal of the classical source does not carry the appropriate information about the anomaly to which the free electrons are subjected, and thus the decompression process does not occur.

[0082] Figure 7 shows a unified model 700 for quantum wireless transmission. The method of Figure 7 enablesthe transfer of energy from a power supply 702 via a transmitting element 71 O to a receiving element 720 and to a load 704, using wireless energy transmission 740 based on energy quantization and the creation of stable energy structures in space.

[0083] An electrically conductive mirror IMG1 712 at the transmitting element 710 is a collection of components to form a corresponding layer that interacts with matching components of an electrically conductive mirror IMG2716 at the transmitting element 710. IMG1 712 and IMG2716 are combined layers that are involved in the internal processes of the transmitting elements. An electrically conductive mirror IMG1 722 at the receiving element 720 is a collection of components to form a corresponding layer that interacts with matching components of an electrically conductive mirror IMG2726 at the receiving element 720. IMG1 722 and IMG2726 are combined layers that are involved in the internal processes of the receiving elements. The transmitting element 710 and the receiving element 720 may each have a different number of such layers (e.g. matching layers and synchronisation layers).

[0084] Each layer has two levels of interaction, an upper layer denoted with the suffix (h) and a lower layer denoted with the suffix (I).

[0085] The upper layer of electrically conductive mirror IMG1 712 at the transmitting element 710 is denoted IMG1 (h) Tx. IMG1 (h) Tx provides interaction with external electronic components designed to interact with the transmitting element 710, such as a power supply 702, a signal source, or similar. Matching layer ML1 714 at the transmitting element 710 is a matching component that defines parameters for the external electronic components, such as the power supply 702, a signal source, or similar.

[0086] The lower layer of electrically conductive mirror IMG1 712 of the transmitting element 710 is denoted IMG1 (I) Tx. The lower layer of electrically conductive mirror IMG1 722 of the receiving element 720 is denoted IMG1 (I) Rx. IMG1 (L) Tx and IMG1 (L) Rx form the interlayer coupling coefficient k(mir) which indicates the strength of the coupling between the electrically conductive mirrors IMG1 Tx and IMG1 Rx. Each of the layers has two levels of interaction, indicated by the suffixes (I) and (h). The suffix (I) represents the low level of interaction, which is responsible for generating internal components of the wireless element, such as k(mir). This is to say k(mir) for the transmitting element is generated by IMG1 (I) Tx and I M G2 (L) Tx, and k(mir) for the receiving element is generated by IMG1 (I) Rx and I M G2(L) Rx. The suffix (h) denotes the high level of interaction with external components, including power generation, load, matching components, and transmitting and receiving elements (which can be considered external components for each other), k(mir) determines the level of communication between the layers of the IMG1 Tx and IMG2 Tx wireless element,where IMG1 Tx and IMG2 Tx are layers of the same wireless element. These layers however may have internal and external destinations, with the internal destinations denoted by (I) and the external destinations denoted by (h). The internal destination is responsible for making a functional wireless element, and the external destination is responsible for operating with external devices to which the wireless receiver element Rx also refers, k(mir) is the same for each of IMG1 and IMG2 because k(mir)will not arise until the mirrors are pressed together with an insulator between.

[0087] The upper layer of electrically conductive mirror IMG1 722 of the receiving element 720 is denoted IMG1 (h) Rx. IMG1 (h) Rx provides interaction with external electronic components designed to interact with the receiving element 720, such as load 704, an AC / DC converter, or similar. Matching layer ML1 724 at the receiving element 720 is a matching component that defines parameters for external electronic components that can be connected to the receiving element, such as AC / DC converters, external matching components, RF loads, or similar.

[0088] The upper layer of electrically conductive mirror IMG2 716 of the transmitting element 710 is denoted IMG2(h) Tx. The upper layer of electrically conductive mirror IMG2726 of the receiving element 720 is denoted IMG2(h) Rx. IMG2(h) Tx and IMG2(h) Rx act as the synchronisation layer, and function to synchronise the transmitting and receiving elements with each other. Synchronisation is achieved when the synchronisation distance d(sync) and the interaction addresses ADR(Fx) of IMG2 Tx and IMG2 Rx coincide.

[0089] IMG2 is a collection of all of the components used to form a corresponding layer. IMG2 interacts with the matching components of the IMG1 mirror. In order to connect an external device to an IMG1 layer, the IMG1 layer shall be able to perceive this external device. Accordingly, IMG1 may comprise components to facilitate the connection of external devices. In addition, the layer IMG1, once connected to an external device, should also be able to interact with layer IMG2. Therefore, internal components are used to match the IMG2 layer. For a transmitting / receiving element layer IMG2 to be formed, it may consist of components that enable the interaction with the corresponding transmitting / receiving element layer IMG1 . The IMG2 layer should also consist of components for facilitating interaction with external devices. An IMG2 layer is therefore a collection of all internal and external components which allow for matching both internal and external components of an IMG1 layer. For the IMG2 Tx layer, the IMG2 Rx layer can be considered to be an external device, and vice versa.

[0090] The lower layer of electrically conductive mirror IMG2 716 of the transmitting element 710 is denoted IMG2(l) Tx. The lower layer of electrically conductive mirror IMG2726 of the receiving element 710 is denoted IMG2(l) Rx. IMG2(l) Tx and IMG2(l) Rx form the interlayer coupling coefficient k(mir) which indicates the strength of the coupling between the electrically conductive mirrors, k(mir) is formed by layers IMG1 Tx and IMG2 Tx between each other for the transmitter, and by layers IMG1 Rx and IMG2 Rx between each other for the receiver. In other words, k(mir) connects two independent layers on a flat piece of dielectric, and will not occur where there is only a single mirror layer (i.e. only IMG1 or IMG2).

[0091] Energy packet E(inf) 730 is an information package comprising information about directed energy.

[0092] Synchronisation layer SL2718 at the transmitting element 710 is the basis for the formation of the energy information packet +E(inf). Synchronisation layer SL2 728 at the receiving element functions to process the received energy information packet +E(inf). The IMG1 and IMG2 layers are figures in which various geometric shapes can be depicted, and do not in themselves have unique properties until the layers intersect. Upon intersection, the two independent layers begin to demonstrate additional properties. For example, where IMG2 and IMG1 are placed on opposing sides of a dielectric layer, the IMG2 layer will exhibit an additional property that enables the synchronisation of two wireless elements at a distance. This property allows for a new secondary name to be given to the IMG2 layer as SL2. The synchronisation of the two wireless element is the same when the synchronisation distance is correctly configured ad the interaction addresses are the same. A wireless transmitting element should therefore be considered as a whole series of complex interactions between properties and components, resulting from the combination of the IMG1 and IMG2 layers.

[0093] Figure 8 shows a diagram of the interaction of two configured layers of electrically conductive mirrors with the formed images IMG1 and IMG2, and the interaction components that form as a result of setting up these two layers.

[0094] A first layer has a first formed electrically conductive mirror pattern IMG1 801. A second layer has a second formed electrically conductive mirror pattern IMG2 802. Electrically conductive mirror IMG1 and electrically conductive mirror IMG2 have a synchronisation distance, d(Sync), 806.

[0095] The interlayer coefficient of coupling, k(mir), 807 indicates the interaction strength of mirrors with patterns IMG1 801 and IMG2 802, where the coefficient of coupling k(mir) is defined as: k(mir)=IONA / X(mir) where IONA represents the intersection area, which is the level of interaction formed by the represented patterns of the electrically conductive mirrors.

[0096] The intersection are IONA is defined as:IONA = IMG1 nlMG2 where x(mir) is a variable parameter which describes a unique quantity of interaction between two configured mirrors that is characteristic of a specially designed element. From this, the interlayer coefficient of coupling, k(mir), can be calculated. The IONA generation is the intersection of IMG1 and IMG2, i.e. the intersection of the electrically conductive parts of the pattern, with the dielectric separating these parts. The x(mir) depends on the material of the dielectric, the thickness of metal coating of the layers, and the type of metal (including but not limited to silver, gold, copper, or similar). How strongly said images intersect with conductive elements of the image forms the coupling coefficient k(mir). Such intersections create mirrors that operate ina similar manner to Casimir mirrors, which are able to suppress the quantum vacuum and affect the amount of the negative component in the conductive mirror materials.

[0097] ADR(Fi) 808 is the matching layer address of IMG1 . ADR(F2) 809 is the synchronisation matching layer address of IMG2. The address is the frequency of the start. This means that one layer of IMG1 is activated from one frequency and another layer of IMG2 is activated from another frequency. The synchronisation matching layer of the transmitting element functions to maintain syntonisation with one or more receiving elements and control the power distribution between them. The function of ADR(Fi) 808 and ADR(F2) 809 is to adjust and match the electrically conductive mirrors of the element. The formation of the address depends on the components of which layers IMG1 and IMG2 consist. Addresses can be adjusted or corrected by changing the component or image (i.e. pattern) on the IMG1 or IMG2 layers, in order to adjust the intersection. Matching layers are considered only when another ADR address, at frequency F3, occurs. This address should interact with both the IMG1 layer and the IMG2 layer. ADR(F3) occurs after combining two layers of a wireless element. If ADR(F3) does not interact with at least one of the layers IMG1 or IMG2 of the wireless element, then the element is not consistent, meaning that the element is incorrectly configured and will not be functional.

[0098] The address of the entire element, ADR(F3), 810, is generated using ADR(Fi) 808 and ADR(F2) 809. The function of ADR(F3) is the interaction between transmitting and receiving elements. If the transmitting and receiving elements have different addresses then they will be unable to communicate.

[0099] Figures 9A and 9B show a diagram 900 of how design features affect the appearance of forces and basic properties of a transmitting or receiving element.

[0100] According to the examples of Figures 9A and 9B, the dimension of active layer IMG1 is less than the dimension of active layer IMG2. Layer IMG1 is filled with electrically conductive material PLT1 at an amount of 35%. Layer IMG2 is filled with an electrically conductive material PLT2 at an amount 72%.

[0101] In Figure 9A, a matching layer 910 and synchronisation layer 920 are separated. When these layers 910, 920 are separated from each other they are not functional, because a first native layer address is not generated by ADR(Fi) = 0, and the synchronisation distance of layer IMG1 , denoted by d(sync)1 , has a value that is greater than or equal to zero, such that d(sync)1 > 0. This means that the layer IMG1 is not matching with another layer. Because the layers are separated, the interaction area, IONA, is also equal to zero, i.e. IONA = 0. Accordingly, the interlayer interaction coefficient k(mir) is also zero, i.e. k(mir) = 0, meaning that the force of interlayer interaction does not happen. In this case, energy compression does not take place. A wireless address of the wireless element, ADR(F3), will also not be generated, i.e. ADR(F3) = 0.

[0102] In Figure 9B, layers IMG1 and IMG2 intersect with an intersection area, IONA, of 12% from the maximum matching / harmonisation. The layers IMG1 and IMG2 are not combined by a physical conductive contact, but are instead separated by an interlayer isolator of dielectric material with thickness d, and additional protective coatings for the matching layer and synchronisation layer. The strength of the interlayerinteraction depends on the type of interlayer isolator, the thickness of the interlayer isolator, and the relative positioning of the two patterns. Areas 904 and 905 represent the interaction area of the IMG1 and IMG2 layers. The mirrors are formed as Casimir mirrors. In this case, of interest is the intersection area of the metal elements. The intersection area may be expressed as a percentage representing the intersecting area compared to the original area of the layer / mirror plate.

[0103] The formation of properties and forces in the element depends on factors including: the type of material of the electrically conductive mirror, the mirror pattern (drawing), the area covered by the pattern, the length of the pattern, the intersection of the mirrors, the coating of protective materials on the surface of the mirrors, the intrinsic resistance of the layers, the material and thickness of the interlayer isolator, and the medium in which the element is used. The type of material of the electrically conductive mirror, such as silver, gold, platinum, or copper, will affect the formation of k(mir) and d(sync). The image or pattern on the IMG1 and IMG2 mirrors will affect the IONA, k(mir) and ADR(Fx). The area covered by said image or pattern will affect the parameters PLT1 , PLT2, and IONA. The pattern length will influence the ADR(Fx) and d(sync). The intersection of the mirrors will affect IONA. The coating of protective materials on the surface of the mirrors will affect the k(mir) and ADR(F3). The intrinsic resistance of the layers will affect ADR(Fx) and d(sync). The material and thickness of the interlayer isolator (or interlayer insulator) will affect k(mir) ADR(F1 ) and ADR(F2). The environment in which the element is used will affect k(mir).

[0104] After the layers of wireless mirrors are matched and pressed, the formation of properties and forces will take place, specifically the address of the layer, ADR(Fi) = x1 ; ADR (F2) = x2; the layer synchronisation distance: d(sync)1 -> <»; d(sync)2 -> <»; and intersection of the patterns will cause an IONA interlayer interaction level and formation of the interlayer interaction coefficient, Ak(mir) 906.

[0105] Figure 10 shows a diagram of the interaction between transmitting and receiving quantum wireless transmission elements and their respective interaction components, which occur after the matching of two or more layers of electrically conductive mirrors. The generation of a common component of interaction between the transmitting and receiving elements facilitates energy transfer.

[0106] Energy information packet, E(inf), 1010 includes synchronising distance, d(sync), 1012 and the transmitter-receiver interaction address, ADR(FX), 1014. The energy information packet will get a new unique address, ADR(FX), 1014, for the interaction of transmitter and receiver. The generation of ADR(FX) 1014 also depends on the environment in which the wireless power is transmitted.

[0107] Compression coefficient k01022 and decompression coefficient ki 1024 are responsible for the level of compression and decompression of energy. Coefficient k01022 and ki 1024 are independent of each other. This enables a wide variation in the setting of these parameters, making it possible to distribute energy among multiple receivers using a single transmission source. This means that the coefficients can be configured such that a receiver will not receive more energy than it needs.

[0108] Formation of the information packet occurs after full activation of layers of electrically conductive mirrors. Depending on the manner in which the mirrors are activated, the type of energy information packet formed can be defined. Methods of activating the electrically conductive mirrors are:(a) Generating an information packet with a certain synchronisation distance.(b) Generating an information packetwithout a certain synchronisation distance.(c) Generating a virtual information packet without a synchronisation distance.

[0109] For method (a), generating an information packet with a certain synchronisation distance, the mirrors are fully activated due to the presence of the receiving element at the synchronisation distance. This means that the receiving element itself, due to its presence, stimulates the energy transfer through the tuned electrically conductive mirrors of the transmitting element.

[0110] For method (b), generating an information packetwithout a certain synchronisation distance, the configuration of the matching layer, ML1 , of the transmitter enables a method whereby configuring a negotiation component causes the mirrors (transmitting mirrors) to be artificially activated. In this mode, the energy information packet includes the addresses of the transmitting and receiving elements, and the decompression coefficient, but does not include the synchronisation distance. The output parameters of a RF power generator for the transmitting element are set directly for a ML1 negotiation layer, without consideration for possible synchronisation distance. When the system is tunes with the synchronisation distance, the RF power generator is tuned with the layer ML1 taking into account the presence of the receiving element. This is to say, the properties of the ML1 layer change when the receiving element(s) are near the transmitter, such that the layer ML1 has information about synchronisation distance. Through measurements of ML1, it is possible to obtain data on the synchronisation distance and on the addresses of the receiving elements. The negotiation component provides setting of the output parameters of the RF power generator according to the configuration of the transmitting element, and will have static parameters, including an operating frequency, power, resistance, and signal shape (e.g. sinusoidal). Parameters for configuration of the RF power generator according to distance of the synchronisation involve the dynamic setting of parameters. This means that the distance of synchronisation influences the frequency, output resistance, switching of power. Inclusion or shutdown of power can change these parameters, and therefore configuration can be done using a synchronisation analyser. The synchronisation analyser determines the connection quality, efficiency, amount of power required, resistance change, and similar. Thus, this setting determines whether the transmitting element is locked or not. Artificial activation means that information is ignored that mirrors receive from space, and whether there are receiving elements nearby or not, and instead the presence of receiving element is simulated even if no such receiving element is near. When receiving elements are present near the transmitting element, information on the timing distance appears on the mirrors of the transmitting element. Artificial activation of the mirrors of the transmitting element allows for ignoring this synchronization distance. If the distance of synchronization is ignored, local energy passesthrough the first mirror IMG1 of the transmitting element, and then through the second mirror IMG2 and is ejected into space. Under such conditions, a larger amount of emitted energy is recorded into the space in the form of an electromagnetic wave. This transmitter tuning method is suitable for high frequency and long distance applications.

[0111] For method (c), generating a virtual energy information packet without a synchronisation distance, such a process occurs when local energy from a source passes through the first mirror of the transmitting element and is reflected from the second mirror of the transmitting element. In this method, the quantum wireless transmission system receives more energy than it generates, with the additional energy coming from the quantum vacuum through the extraction of zero-point energy from said vacuum. For example, consider that the transmitting element is supplied with 20 W power, it passes through the first mirror (IMG1 ) of the transmitting element and is reflected from the second mirror (IMG2), That is, the power returns back to the system, where it can be re-processed. However, at the receiving element, 20 W power is generated / received, which has been transmitted by the transmitter. That is, information about the transmitted energy was received by the receiving element and accordingly it extracted the energy from the quantum vacuum. This effect is possible by creating a stable growth of the negative component on the transmitter side. Reflection from the second mirror (IMG2) of the transmitting element makes it possible not to compensate the negative component due to local energy, but the negative component is compensated due to electromagnetic radiation of the quantum vacuum. A total of 40W of energy is obtained: 20W on the transmitting side and 20W on the receiving side. This example is ideal, a total efficiency of 200%. In reality, the total efficiency can reach 125-145% or more.

[0112] Figure 11 shows the properties of the wireless element, which depend on the intersection area, IONA.

[0113] The address, ADR(Fi), of the layer IMG1 is defined as:ADR(Fr) = / (JMGl * kimir)) and the address, ADR(F2), of the layer IMG2 is defined as:ADR(F2) = (IMG2 * k(miry)

[0114] The synchronisation component, syncl for layer IMG1 is defined as: syncl = ADR(F ) * IMG2 and the synchronisation component, for layer IMG2 is defined as:sync2 = ADR(F2) * IMG1

[0115] The equation checks whether the IMG1 layer is matched through the IONA intersection:

[0116] From which we can determine a wireless element address, ADR(F3), by the equation:ADR(F3) = lMG * (( / c(mir) * x(F3) )) and a layer synchronisation component sync(x) (not to be confused with the wireless element synchronisation distance):

[0117] The formed intersection area, IONA, together with the IMG2 layer, creates the layer address and the layer synchronisation component. The synchronisation distance, d(sync), of an element depends on the synchronisation level of IMG1 with the IONA intersection area. For this reason, ADR(F1 ) is used to check the synchronisation component. The constant, x(F3), is the ratio of one pattern to another, creating the IONA area - i.e. the ratio of IMG2 to IMG1 and IONA.

[0118] x(F3) therefore determines how the layers are aligned with each other and the IONA for a correctly formed element. A correctly formed element is one that has an ADR(F3) according to the above equations. A deviation in x(F3) affects the quality of the energy quantization. For each individual size of wireless element, material, and environment in which it will be used, the value of x(F3) will be a unique parameter.

[0119] Figures 12Ato 12D show the process of quantizing (compressing) local energy by the transmitting element of a quantum wireless power transfer system, for a simple double layer transfer element. As shown in Figure 12A, the double layer transfer element 1200 has two layers of conductive mirrors IMG1 , IMG2, and an embedded dielectric isolator arranged therebetween. The side of the conductive mirror IMG1 may comprise two input contacts 1201 , 1202 for power input, which may comprise local energy converted by an inverter.

[0120] Figure 12B shows a side view 1204 of a transmitting element. Through the process of rubbing / grinding, the absorption of low-level energy occurs between the layers of electrically conductive mirrors, and the transition of energy to a high level. Some or all of the power supplied to the element and which flows between the conductive contacts of the mirror IMG1 is absorbed by a quantum vacuum. The absorption of power that is supplied to the transmitting element occurs due to the activation of the unique IONA area and its program code. Rubbing / grinding describes the process of splitting energy into small portions. When local energy passes through the electrically conductive material of the wireless element, the intersections form the IONA region. At the intersection points of the metal elements (IMG1 and IMG2) thereis a deficit of the positive component due to the effect of suppressing the quantum vacuum (like in the Casimir effect) such that energy is absorbed. The quality of the created wireless element may determine whether all or part of the energy is absorbed. If the wireless element is not ideal, the it may be able to absorb only part of the supplied power. In some examples, creation of an ideal wireless element may be limited due to manufacturing constraints and material qualities, or similar. The address activates the IONA area. The IONA intersection area consists of many small mirrors arranged in a row, column, or line. This arrangement of mirrors is considered the program code. In order to activate these small mirrors, local energy is supplied at a certain frequency according to the ADR(F3) address.

[0121] Figure 12C shows a skeleton of a wireless element, as well as compression vectors for a portion of energy. Each element and fragment of the pattern of the wireless element has an influence on such vectors.

[0122] Figure 12D shows that the wireless transmitting element of the quantum wireless power transfer system does not emit power 1206 in the form of magnetic or electric fields into free space, but instead some or all of the power is quantized. The efficiency of operation of the wireless element and the synchronisation level thereof can be determined from the remaining input power 1207. Area 1205 represents the intersection area of the metal elements (IMG1 and IMG2).

[0123] Figures 13A and 13B show a sector of a wireless multisector element, accordingto some aspects of the present disclosure. The sector of the wireless multisector element of Figures 13A and 13B is a doublelayer element comprising layers 1310 and 1320. Layer 1310, on a top side of the element, has an electrically conductive mirror pattern IMG1 . Layer 1320, on a bottom side of the element, has an electrically conductive mirror pattern IMG2. These layers, after further pressing, create a unique intersection area, IONA. The IONA occurs after two layers (IMG1 and IMG2) are combined with a dielectric pad between them. The IONA is the physical area in which local energy is compressed - i.e. it is the place where the local low-level energy is ‘rubbed’ into a quantum vacuum and saturates it. Layer 1310, filled with electrically conductive mirror pattern IMG1 , creates a PLT1 (plate 1 ) 1312 by 34% (i.e. 34% of the surface is occupied by the conductive pattern). Layer 1320, filled with electrically conductive mirror pattern IMG2, creates a PLT2 (plate 2) 1322 by 25%. The IONA created by the two electrically conductive mirror patterns IMG1 and IMG2, and layers 1310, 1320, respectively, is 15%. Layer 1320 comprises contacts A, B, B1 for supplying local energy to the element or releasing local energy from the element. A1 is the sector number of the illustrated sector of the multisector element.

[0124] Figure 14A shows a physical area that will be formed by the intersection of two electrically conductive mirrors, such as patterns IMG1 and IMG2 of Figures 13A and 13B. The area of intersection 1400 creates an area in which conditions are created for persistent anomalies in the behaviour of a free electron. This area is responsible for the quality of local energy compression. For each wireless element, such an area is unique, and can be compared to a software code. Each of the cells of the pattern can be considered a sequential fragment of such a code. For example, cell 1401 corresponds to +3, and the free area after strip 1402 corresponds to -3, the cell 1403 corresponds to +5, and the cell 1404 corresponds to +1. In thisexample, the cell 1401 may occupy 3mm of metal, with the + symbol representing the presence of metal. The free area after 1402 may comprise 3mm without metal, with the - symbol representing the absence of metal. When the electron passes through this area, there is a slowing down, thus causing an anomaly in the behaviour of the electron.

[0125] In order to read the IONA code for the intersection pattern, one needs to start at point 1405 and move counterclockwise in the direction of successive lines of the matching layer. The first sign that indicates the direction of the elementary particle is the vector:(+12) -> (±4)x7 - (+15+7) + ±4 + +5 + ±4 + +5 + (±4)x3 + +30e <- where the code is read from right to left, and the above represents just a fragment of the code. Here, the notation (±4)x3 means the repetition of a +4 and a -4 region three times. The arrow indicates the direction of energy input - i.e. the theoretical direction of motion of the electron. The notation (+15+7) indicates that there are two parallel elements between which there is an emptiness, thus giving the length of a line of 15mm parallel with a line of 7mm, such that these both meet in the direction of the electron, and the electron experiences an anomaly from the two parallel lines +15 and +7.

[0126] A further feature of the interlayer interaction is the formation of the element’s own address. The own address of the element not only enables communication between transmitting and receiving elements of the quantum wireless transmission technology, but also runs the program code causing energy quantization. The address is therefore the frequency that activates the program code, with said program code constantly changing direction over a certain period of time. This means that is RF power is applied to a transmitting element at an inappropriate frequency, the wireless element will not function correctly. At an inappropriate frequency, energy compression will not occur, and instead relevant features of classical energy transmission will occur, such as fixation of magnetic and electric fields, and the wireless element will begin to heat up.

[0127] In the classical case, energy is supplied to the conductor with some frequency, for example 1 MHz. Accordingly, the oscillation of the electromagnetic fields will occur at the same frequency. If the same frequency of 1 MHz is applied to the conductor of the wireless element, and the frequency does not correspond to the operating frequency of the element, then the same oscillations of the electromagnetic field as in the classical case are exhibited. When creating an element, an important component is ADR(F3) as previously described. If ADR(F3) tuned to a specific frequency, for example 10 MHz, then the supplied frequency of 1 MHz, will not be able to start the process of activating the mirrors of the element. Accordingly, the transmission of energy information as well as the transmission of energy will not be possible. However, if the frequency is given correctly, in this case - 10 MHz (i.e. ADR(F3)), energy absorption (that is, the process of anomaly in the behaviour of the electron) will occur.

[0128] Figure 14B shows an IONA area and the generation of a unique code for a wireless element. The input of local energy or the release thereof by the element is carried out through contacts A, B and B1 .

[0129] Code generation is caused by local energy input at the transmitting element at point 1405. Current direction is indicated in Figure 14B by arrows, with the current applied as a pulse for a certain period of time At. The code is generated from right to left. Components 1406a and 1406b of the code are referred to as totalisers, specifically (+15+7) - (+12(+6x2))+, and represent areas in which cells are parallel, and will always have the same directional vector. In some examples, these cells may comprise parallel patterns of lines with a curved shape. Totaliser components are designated in code by a single vector. Component 1407 is a repeater component, and isformed from identical cells in the direction of the vector. The repeater component is also designated in code by a single vector. All components of the adder can have the same vector. Each code modification, or transition from one component type to another, is separated by an arrow, such that the changes that the electron will undergo can be seen from the code.

[0130] Should the filling of PLT1 or PLT2 of at least one of patterns IMG1 or IMG2, respectively, then the IONA is changed, which leads to a change in the code and the address of the element that activates said code. The sum of the IONA code may comprise a sum of the IONA area in pm2, and may be unique to each wireless element. For example: initial parameters: filling ofPLTI by 34% and PLT2 by 25%; causes an IONA of 15% the sum of the IONA code is 361085306,9673585 changed parameters: filing of PLT1 by 59.5% and PLT2 by 40%; IONA will change by 35.8% the sum of the IONA code is 800288615,524115

[0131] A change in the parameters of at least one layer, namely in the pattern or the amount of filling with an electrically conductive mirror, will lead to a change in the IONA area, the program code, and the address of the wireless element that runs said program code. Accordingly, a change to an element can render it nonfunctional due to IONA code damage, and thus there can only be one IONA code for each well-designed element.

[0132] Figure 15 shows an example of an IONA area for a multi-sector wireless receiving element 1500 for collecting / harvesting free energy from space. Figure 15 shoes how much an IONA code for each sector of a wireless element can differ with a slight change in one of the parameters, specifically the pattern of electrically conductive mirror IMG1 , the synchronisation layer. The IMG2 matching layer remains unchanged.

[0133] A first sector of the element, 1501 , has a code fragment:(+6+5)+(-1 +2)x11 ->-2+2->(-1 +2)x4++6+(-1 +2)x5+-2+2+(-1 +2)x11 +(+6+5)+(-1 +2)x11 ->-2+2->(-1 +2)x5+ and a second sector of the element, 1502, has a code fragment:(+5+4)+(-2+1 )x11 ->-3+1 +(-2+1 )x4++5+(-2+1 )x5+-3+1 +(-2+1 )x11 +(+5+4)+(-2+1 )x11 ->-3+1 +(-2+1 )x5+

[0134] Here, sectors 1501 and 1502 have the same direction vectors, but their values have changed. This indicates that one of the electrically conductive mirrors (the IMG2 matching layer) in sectors 1501 and 1502has remained the same, but the other of the electrically conductive mirrors (the IMG1 synchronisation layer) is different. The two sectors 1501 and 1502 are therefore programmed to collect energy from different points of the spectrum. In Figure 15, the wireless element has four sectors, 1501 , 1502, 1503, 1504, each of which has their own codes and IONA code sums.

[0135] When creating two wireless elements, the sum of the IONA codes may be the same but the codes may be different. In this case, the two elements will have different ADR, which will result in the two elements not functioning together. This is to say, theoretically the sum of the IONA code can match, but the program code ( + (-2 + 1 ) x11 ->-3+1 ■+ (-2 + 1 ) x5+ ) of starting wireless elements may differ.

[0136] Where the addresses of the wireless elements ADR(F3) match, this does not necessarily mean that the IONA area code will be the same. This means that for each specific size, shape, thickness and material there will be an IONA code. In practice, the IONA code is a result of the design of the wireless element, and is difficult to influence, and therefore it is highly unlikely that multiple elements will comprise the same IONA code, although such an occurrence is theoretically possible.

[0137] Wireless element addresses have their own frequency characteristics. Only one frequency can be used to enable an IONA code, which corresponds to the element code itself. The frequency is used to activate the wireless element address, whereby only if the ‘correct’ frequency matches the ‘correct’ code of the element itself will the energy quantization process occur. In all other cases, where an ‘incorrect’ frequency is used, classical processes will be observed and fixed, including the occurrence of electrical and magnetic fields, and heating of the element. The IONA address and code are generated simultaneously during design of an element, such that the two parameters are not separable from one another.

[0138] Figure 16 shows an example of a transmission element of a quantum wireless transmission system, according to aspects of the present disclosure. This example shows a simple structure of a wireless transmission element, consisting of two simple mirrors 1600 and 1601. According to other examples, transmitting elements may comprise two or more mirrors. Some examples comprise 5, 8 or 11 mirrors. Each mirror has a pattern 1603, which can comprise one or more sectors. A front face pattern IMG2, 1603, is shown in Figure 16. A dielectric stratum 1602 may be arranged between layers of electrically conductive mirrors. The stratum may be formed from various materials with dielectric properties, including but not limited to plastic, glass, epoxy, carboxylic fibre, and similar.

[0139] Transmitting and receiving elements may have at least two layers, or be multi-layered. The layers can be classified into two groups according to their functionality and properties: a synchronisation layer and a matching layer. The layers may be pressed together and isolated by a dielectric lining such that there is no contact between the main layers, but instead a formation of an interlayer force, k(mir). The force of interlayer interaction increases the level of persistent anomalies in the behaviour of free electrons.

[0140] According to some examples, the transmitting and receiving elements may comprise one or more simple or combined sectors. Simple sectors include sectors separated from each other with their ownrespective addresses. For example, a transmitting element having two simple unequal sectors can compress local energy using its own addresses, meaning that the transmitter may have multiple active independent transmission sectors, such that local energy from two independent RF sources can be supplied to the transmitter. Combined sectors include sectors that are connected by physical contacts with each other. Due to addresses that have sectors, accurate point delivery of wireless power to an assigned destination can be achieved.

[0141] Figure 17A shows a front view of a transmitting element 1700 of a quantum wireless transmission system, according to aspects of the present disclosure. An electrically conductive mirror, IMG2, 1704, forms the synchronisation layer of the transmitting element 1700. The material of the electrically conductive mirror of the synchronisation layer may comprise a conductive material, including but not limited to copper, gold, silver, aluminium, or similar. Persistent anomalies form at points 1705 at which interaction of the mirror layers is strongest - i.e. the points of maximum intersection between the two mirror layers. A simple single-sector pattern 1706 is formed on the electrically conductive mirror 1704. Transmitting element 1700, with an electrically conductive mirror 1704 in pattern 1706 has one sector, and accordingly one address, ADR(F3). In some examples, a wireless element may have a plurality of sectors, which enables an element to have several own addresses at the same time. Transmitting element 1700 has a non-symmetrical pattern 1706. In some examples, a wireless element may have symmetrical or non-symmetrical patterns. Additional components 1707 of the matching layer are on thefront side of the transmitting element 1700, although these do not belong to the IMG2 mirror. The additional components 1707 are associated with component ML1 , and serve to configure a transmitter element with external power supply components.

[0142] Figure 17B shows a back view of a transmitting element 1700 of a quantum wireless transmission system, according to aspects of the present disclosure. An electrically conductive mirror, IMG1 , 1711 , forms the matching layer of the transmitting element 1700. The material of the electrically conductive mirror of the synchronisation layer may comprise a conductive material, including but not limited to copper, gold, silver, aluminium, or similar. Persistent anomalies form at points 1705 at which interaction of the mirror layers is strongest - i.e. the points of maximum intersection between the two mirror layers. The pattern of IMG1 , 1711 , is also non-symmetrical. Accordingly, the transmitting element 1700 of Figures 17A and 17B is completely asymmetrical. In some examples, front-side elements 1708 of mirror IMG2 may not be connected to other parts of the electrically conductive mirror pattern. The back view of the transmitting element 1700 mayfurther comprise contacts 1709 for the connection of additional structural elements, a power supply, a signal generator, an amplifier, or similar. Part ML1, 1710, is located on the rear side of the transmitting element 1700, and directly interacts with external components of the quantum wireless transmission system.

[0143] Figures 18A and 18B show an example of a transmitting element for a quantum wireless transmission system, the element having multiple sectors, according to aspects of the present disclosure. Figure 18A shows a front view of a transmitting element having an electrically conductive mirror, IMG2, 1800, forming a synchronisation layer of the transmitting element. The material of the electrically conductive mirrorof the synchronisation layer may comprise a conductive material, including but not limited to copper, gold, silver, aluminium, or similar. The pattern sectors 1801 of the multisector transmitting element are not combined, and are operable independently of each other. The example multisector transmitting element can therefore have multiple addresses at the same time, ADR(Fn). In this example, n = 24. Transmitting elements that are of the multisector type may use one or more power supplies. The pattern displayed in Figure 18A is a multisector pattern of a symmetrical type, wherein the sectors are formed with simple symmetric figures. In some examples, non-symmetric patters may include one or more multisector patterns that have at least one non-symmetric sector. A non-symmetric sector is a sectorthat is constructed from a single continuous line that forms a non-symmetric shape or pattern, such as that of Figure 17A.

[0144] Figure 18B shows a rearview of the transmitting element having an electrically conductive mirror, IMG1 , 1804, forming a matching layer of the transmitting element. The image of this rear side, IMG1 , 1804, is a multisector non-symmetrical pattern. This means that the pattern consists of non-symmetric matching sectors 1805. The formation of the interlayer interaction force, k(mir) is made complicated, since the complex structure of IONA intersections for each sector arises separately. Segment numbers 1806 may be provided above contacts for a segment in order to assist in connecting of a matching component. In examples, the matching component is external, and therefore not applied to the pattern IMG1. Components 1807a and 1807b are applied to non-symmetrical segments to increase the interaction force, k(mir). Each segment 1805 of this matching layer is different from each other, enabling the obtaining of different segment addresses. This means that for each of the segments A1 to A24, there will be a different ADR address; ADR(Fi) to ADR(F24).

[0145] If the synchronisation layer and matching layer are not properly formed and matched, the formation of the interaction force k(mir) will be disrupted. Accordingly, the transmitting and receiving elements would be unable to transmit energy according to quantum wireless transfer methods. Accordingly, properly formed and matched synchronisation and matching layers will enable the creation of persistent anomalies in the behaviour of free electrons, thus enabling the quantization of local energy.

[0146] Figure 19A and Figure 19B show an example of a multilayer element for a quantum wireless transfer system, according to aspects of the present disclosure. A simple multi-layer element 1900a of a quantum wireless transfer system is shown. Electrically conductive layers are not combined by electrically conductive contacts, but instead operate independently of each other. The layers are instead joined by interlayer interaction force k(mir). Electrically conductive layers 1901 a and 1901 b are synchronization mirror layers pressed together. Layer 1901 b is considered a inner layer. A dielectric insulator layer 1903 is formed between these electrically conductive layers. The dielectric insulator layer 1903 may comprise one or more of glass, plastic, epoxy, carboxylic fibre, or similar. A internal electrically conductive matching layer 1902 may perform synchronisation or negotiation. The difference between the matching and synchronization layer in the example figures is typically that the matching layer consists of simple figures, has a smaller amount of metal coating, and consists of thick lines. Conversely, the synchronization layer may have many objects on it, and the lines are much thinner than the matching layer. The matching and synchronization layer has differentpurposes. The multilayer elements may have multiple layers of either matching or synchronization, which are compressed in the multilayer structure of the wireless element. In some examples, if there is insufficient area of a wireless elementto place a matching layer on it, an internal layer can be added on which it is possible to place part of the matching layer that has not fit on one side. The formation of the multilayer element comprises a synchronisation layer 1901 a on one side and a matching layer 1904 on the other side. The wireless element may be further covered in a protective layer of varnish 1905, paint, or other dielectric material disposed above the outer synchronisation layer 1901 a or matching layer 1904. In this case, free access to the synchronisation and matching layers is closed. This further stabilises the parameters of the wireless elements, increasing the suitability of use in aggressive operating environments. Figure 19A shows an electrically conductive synchronisation layer 1906 having pattern IMG1 , and an electrically conductive matching layer 1909 having pattern IMG2, with an interlayer dielectric insulator 1907 disposed between the synchronisation layer 1906 and the matching layer 1909. One or more electrically conductive contacts 1908 may be used to combine one or more layers with each other. The use of conductive contacts 1908 between layers indicates that the element is of the combined type. The main synchronisation layer 1906 and the main matching layer 1909 are separated by the dielectric insulator 1907 and are therefore not connected together by physical conductive contacts. Main layers 1906 and 1909 may be combined by physical conductive contacts only with inner layers, but not with each other. A combination of the main layers with each other would destroy the interlayer interaction force, k(mir), which would lead to non-functionality of the resulting element.

[0147] Figure 20 shows a diagram describing possible combinations and variants of quantum wireless transfer elements. Wireless elements may be two-layer or multi-layer. Multi-layer elements may be divided into a simple type and a combined type. Simple multi-layer wireless elements have layers combined only by the interlayer force, k(mir). Combined multi-layer wireless elements are combined not only by the interlayer force, k(mir), but also by conductive contacts (also referred to as transition holes) between one or more of the layers. With respect to the patterns of the elements, wireless elements can be divided into one sector and multi-sector patterns, and both symmetric and non-symmetric (asymmetric) types. Symmetrical patterns can be formed in the form of simple geometric figures, including but not limited to squares, circles, hexagons, octagons, and similar, provided that the symmetry of the pattern is preserved. Symmetrical patterns are formed using one continuous line. A pattern is an asymmetric pattern if at least one sector of the pattern of an element is asymmetric, thus causing the symmetry of the entire pattern to be violated. Multisector patterns can be divided into combined and simple. Sectors are considered combined when they are interconnected by electrically conductive contacts. Simple sectors are not combined by electrically conductive contacts. In the case of simple sectors, each sector is independent and has its own unique address.

[0148] The type of quantum wireless transfer element used will depend on the tasks and the environment within which energy is to be transferred, as well as the load at the receiver-side. For a first example, for awireless element for the purpose of transmitting energy to a single addressee, the complexity would be a simple element. The resulting element would be a transmitting element having two layers, and a one sector, asymmetric pattern type. For a second example, for a wireless elementfor the purpose of collecting energy from free space, the complexity would be a complex, mixed element. The resulting element would be a receiving element having two layers, and a muti-sector, asymmetric pattern type with simple multi-sector patterns.

[0149] Figure 21 shows a block diagram 2100 of a quantum wireless power transfer system and the energy flow from a source 2110 to a load 2190. According to examples, a power supply 2110 for the system can be the electrical power network and an AC / DC converter or power supply connected to it, or a renewable energy source such as solar cells, wind turbines, thermal elements, or similar. A control system 2120 performs functions including analysing received data of wireless elements, determining a quality of energy compression by a transmitting wireless element 2150, calculating an efficiency, and distributing energy among the system components.

[0150] The synchronisation analyser 2140 collects synchronisation status information between wireless elements and sends it to the control unit 2120, which calculated and adjusts the wireless system for maximum efficiency based on the received information. Synchronisation analysers can be of two types: passive and active. A passive synchronisation analyser monitors the synchronisation state during the transmission of RF power from the DC / AC inverter 2130 to the transmitting element 2150, and sends the information to a control unit 2120 that directs and operates the system during the wireless power transmission process. An active synchronisation analyser independently generates and sends a weak radio frequency signal to the transmitting element 2150, receives a response from the transmitting element 2150 about the synchronisation state, and sends information to the control unit 2120, which sets the system to high efficiency before RF power is supplied to the transmitting element 2150.

[0151] A DC to AC inverter 2130 uses switching devices which are switched on and off according to a control signal. The main frequency component of the switch voltage may then be emitted through an LCR resonant filter, in order to obtain an AC output. Since the switching time is determined by the control signal, there may be cases where the voltage of the switch is not zero at the time of switching on, which can lead to switching losses. Therefore, an inverter that satisfies soft switching condition achieves a high power conversion efficiency. It is therefore possible to select several classes of consecutive resonant inverters taking into account soft switching conditions.

[0152] The DC-AC inverter 2130 supplies power to the transmitting element 2150. The transmitting element 2150 in turn compresses the wireless energy by quantizing the energy in the structure of the transmitting element 2150. Between the layers of tuned electrically conductive mirrors, the energy is ‘rubbed’ into a quantum vacuum, and is therefore compressed.

[0153] During quantisation of energy, wireless elementsof a quantum wireless power transfer system may be low noise, i.e. they do not emit electromagnetic interference and there are no conductive emissions. The absorption of local energy into the structure of the transmitting element and the occurrence of persistent anomalies leads to the absence of heating of the transmitting element (deceleration of the free electron sequential probability, i.e. decrease in movement of free electrons in the mirror structure), which enables obtaining ultra-high efficiency wireless energy transmission.

[0154] After the receiving element 2160 receives an information signal about compressed (quantized) energy, an internal mechanism for counting inverse anomalies is started. This means that the information signal triggers the elongation of a sequential probability of a free electron, and the movement of free electrons begins. The source of the energy release is the quantum vacuum, which is filled with quantized energy in real time at the synchronisation distance by the transmitting element 2150. In this case, low-level energy is generated from the collected high-level energy.

[0155] The receiving element 2160 decompresses energy through the releasing of energy from the internal structure of said receiving element 2160. Energy is generated, released, and formed between two tuned conductive mirrors IMG1 and IMG2. The decompression process takes place in the reverse to the compression process, meaning that the compressed energy atthe transmitting element 2150 is completely or partially released on the receiving element 2160 in the same form in which it was supplied to the conductive mirror IMG1 (Tx) of the transmitting element2150 . The decompression process completes through the appearance of alternating current at the outputs of the electrically conductive mirror IMG1 (Rx) of the receiving element 2160. Decompression is the complete or partial reproduction of energy between layers of tuned mirrors of the receiving element 2160 from the received energy information signal created as a result of the decay of energy on the transmitting element 2150.

[0156] A receiving element 2160 and RF-DC rectifier 2180 are responsible for the efficient conversion of AC power to DC. Additionally, in some examples, a level matching module 2170 may be arranged between the receiving element 2160 and the RF-DC rectifier 2180, in order to stabilise the output power for the RF-DC converter 2180. The DC power may be adjusted by a DC-DC converter 2185 before being provided to a load 2190.

[0157] Figure 22 shows a graph depicting the modes of transmission element operation. The operation of the wireless element can be divided into two main models: the classical model and the energy quantization model. If the wireless elements of the quantum wireless power transfer system operate according to the classical model the entire system does not function correctly, and exhibits behaviour such as the heating of the wireless element, appearance of electric and magnetic fields, and the occurrence of electromagnetic interference. This occurs when the AC frequency, amplitudes, or ratio (current / voltage) do not correspond to the input parameters of the transmitting element, such that f(x) * ADR(Fi). Therefore, the input parameters of the wireless element should be taken into account, which are contained in the address of the wireless element, ADR(Fi).

[0158] Where wireless elements operate on the energy quantization model, all internal components of the wireless element are balanced, and so energy compression (quantization) occurs. When the process of quantization occurs, characteristic signs appear, including lack of heating, non-fixed or very weak electric and magnetic fields. This is to say, the density of such a field does not correspond to the energy that is carried. This model of operation occurs when the input parameters of the transmitting element coincide with the output parameters of the DC / AC inverter.

[0159] Figure 23 shows a block diagram of a transmitter unit 2300. Transmitting element 2350 compresses the power supplied from an AC / DC inverter. The power that passes through the electrically conductive mirror IMG1 is absorbed and compressed between two tuned layers of conductive mirrors, IMG1 and IMG2. The Casimir force, the force between parallel conductive plates, exists during operation, in this case between the two tuned electrically conductive mirrors. These electrically conductive mirrors are capable of rubbing low-level energy and saturating a quantum vacuum with high-level energy. The occurrence of anomalies (deceleration of electron sequential probability) is the behaviour of an electron during the operation of the wireless elements indicates that the absorption (quantization) of such energy is taking place. A powerfrom a DC / AC inverter is supplied to the transmitting element 2350 at the matching layer, electrically conductive mirror IMG1. The synchronisation analyser 2340 receives a response from the transmitting element 2350 about the power, part of which has been absorbed and compressed by the transmitting element 2350. The synchronisation analyser 2340 transmits power data to a control unit 2320.

[0160] The control unit 2320 makes a decision, based on a program or set of instructions, about increasing or decreasing the output power. Thus, the control unit 2320 may constantly receive information from the synchronisation analyser 2340 about the level of synchronisation at which the transmitting element 2350 is operating. If the transmitting element 2350 at its synchronisation level is able to process all ot the incoming power, then the control unit 2320 can increase the power level to check whether the synchronisation and energy compression is at an effective or maximum level. If the control unit 2320 receives data from the synchronisation analyser 2340 that not all energy has been compressed (i.e. excess energy is recorded), then the control unit 2320 can reduce output power until optimal synchronisation conditions arise. In some examples, the control unit 2320 may shut down the system in the case of complete absence of synchronisation, which may indicate damage to the transmitting or receiving element.

[0161] In the example of Figure 23, the power submitted to the transmitting element 2350 is not radiated into free space in the form of magnetic or electric fields, but is instead absorbed in the structure of the transmitting element 2350.

[0162] Figure 24 shows a block diagram of a control unit 2400. The control unit 2400 may control all components of a wireless power transfer system. The control unit 2400 may comprise a power source 2410, which may be operable to provide multiple power levels 2416, 2417, 2418. The power management stage of the control unit 2400 may further include an input protection module 2415, which may protect the control unit or other parts of the system from overheating, erroneous signals, exceeding of the permitted power level,short circuits, or similar. The power management stage of the control unit 2400 may further include a power switching module 2430 to amplify the voltage of the input power. Communication may be performed by the control unit 2400 by one or more of a remote control module 2422, a system status analyser 2424, or a data synchronisation analyser 2440. The remote control module 2422 may function to adjust the system to the conditions in which the wireless power transfer system will be used. Analysis of the data, by the system status analyser may comprise receiving data from the data synchronisation analyser, system temperature indicators, power indicators, or similar. A signal generator module 2435 may adjust the type and frequency of the generated signal on the basis of received and analysed data from the synchronisation analyser 2440. A frequency change may occur if the environment in which the wireless system is to operate is changed. A preamplifier 2436may be arranged at an output of the signal generator module 2435. The control unit 2400 may further include an output protection module 2431, which may protect the system from overheating, erroneous signals, exceeding of the permitted power level, short circuits, or similar. The control unit 2400 may comprise a signal output 2450 and a power output 2451 .

[0163] Figure 25A shows a topology of a class-E inverter circuit 2500 suitable for generating a signal for supply to a transmitting element. The class-E inverter circuit 2500 comprises a voltage source 2510. The circuit 2500 further comprises a switching transistor 2562 controlled by a signal generation source 2535. The circuit 2500 further comprises an arrangement of an inductor LC, 2560, a capacitor Cs, 2564, an inductor L, 2566, and a capacitor C, 2568. The output from the inverter circuit 2500 may be provided to a load 2550, such as a transmitting element for a quantum wireless transfer system.

[0164] Figure 25B shows a graph of the output voltage and current of the class-E inverter of Figure 25A. Notably, the voltage and the current on the transistor do not overlap, resulting in a reduced power loss.

[0165] In some examples, a class-D inverter may be used. In the operation of the class-D inverter, the voltage and current never occur simultaneously due to an ideal switch. Therefore, the power loss in the switching device is considered zero.

[0166] In some examples, a class-E inverter may be used. A class-E inverter may also be known as a high frequency and high efficiency inverter. By satisfying conditions of the class-E zero voltage switching and zero differential switching, at the moment of switching on, the switching loss is reduced to zero.

[0167] In some examples, a class-E / F inverter may be used. In a class-E / F inverterthere is a decrease in the peak value of the switching voltage compared to a class-E inverter, which can be achieved through removing the harmonic component from the current that flows through the shunt capacitance.

[0168] In some examples, a class-F inverter may be used. A class-F inverter is designed to achieve high efficiency and low distortion. In the amplifier, the resonance contour monitors harmonic components at each stage to reduce distortion and increase efficiency.

[0169] High voltage operating amplifiers with a low quiescent current can be used to autofocus wireless elements. In this context, autofocus refers to the dynamic change in the output resistance of the amplifier. Insome examples, the output resistance of the amplifier can be varied between 10 and 1000 Ohms. High efficiency is achieved by automatically starting the wireless element at the moment of synchronisation and tracking a smooth transition (i.e. power increase / decrease) during operation.

[0170] Figure 26A shows a class-D rectifier circuit 2600a suitable for rectifying a signal received by a receiving element 2610a for output to a load 2630a. Optionally, a level matching module may 2620a may be used to stabilise the output power for the rectifier.

[0171] Figure 26B shows a class-E rectifier circuit 2600b suitable for rectifying a signal received by a receiving element 2610b for output to a load 2630b. Optionally, a level matching module may 2620b may be used to stabilise the output power for the rectifier.

[0172] Figure 26C shows a class-E / F rectifier circuit 2600c suitable for rectifying a signal received by a receiving element 2610c for output to a load 2630c. Optionally, a level matching module may 2620c may be used to stabilise the output power for the rectifier.

[0173] Figure 27 shows an efficiency diagram of a quantum wireless power transfer system 2700 and its components. The efficiency of the entire system depends on the transmitting element, the receiving element, and components of the system. By increasing the efficiency of each component, the overall system efficiency is improved.

[0174] At the transmitting side, the system 2700 comprises a power supply 2710 which may further include AC to DC conversion. The power supply 2710 is electrically coupled to an radio frequency (RF) supply 2720 which generates a RF signal for the transmitter. The RF supply 2720 is electrically coupled to a level matching module 2745, which is operable to convert the RF signal to a level suitable for providing to a transmitter element 2750. The transmitter element 2750 is operable to quantize energy into a quantum vacuum and transmit an information packet.

[0175] At the receiving side, the system 2700 comprises a receiving element 2760 operable to receive the information packet from the transmitting element 2750 and decompress energy from a quantum vacuum and output an RF signal. The receiving element 2760 is electrically coupled to a level matching module 2770, which is operable to convert the received RF signal from the receiving element 2760 and convert a level of said RF signal to one suitable for processing by one or more converters. A RF to DC rectifier 2780 is electrically coupled to the level matching module 2770. The RF to DC rectifier 2780 is operable to convert the received RF signal to a DC signal. DC to DC converter 2785 is operable to adjust a voltage of the DC signal, and output said adjusted DC signal to a load 2790.

[0176] Improvement in the efficiency of one or more of the power supply 2710, the RF supply 2720, the level matching module 2745, the level matching module 2770, the RD-DC rectifier 2780, the DC-DC converter 2785, or the load 2790, by improvement to the classical way in which said components operate will contribute to an improvement in the efficiency of the system 2700 without affecting the operation of thequantum wireless power transfer methods occurring at the transmitter element 2750 and the receiving element 2760.

[0177] Wireless energy transmission based on energy quantisation has a very high efficiency due to the use of targeted energy transmission. This is to say, wireless elements according to the disclosed technologies do not experience heating during energy transfer, because all local energy is compressed and ‘rubbed’ into a quantum vacuum. Energy compressed in this manner has no significant effect on the motion of free electrons - i.e. there is no increased movement of free electrons as in classical energy transmission methods. For example, in classical energy transmission, using a copper conductor through which free electrons flow, heating of the copper conductor occurs, as well as radiation of magnetic and electric fields. For transmission of energy using the disclosed quantum wireless transmission teachings, free electrons remain in a relatively stable (clam) state, and therefore no heating or formation of magnetic or electric fields occurs.

[0178] Wireless transmission of energy using a quantum vacuum as the environment for energy transfer, due to the absence of magnetic and electric fields, do not harm or interfere with electronic devices which require power and / or charging. Conversely, for wireless energy transmission by classical methods (such as magnetic induction), a loss of efficiency can occur in the case of poor contact between transmitter and receiver. Poor contact of wireless coils for traditional wireless systems, which use a magnetic field as the medium for transmitting energy, leads to uncontrolled release of energy into free space. This uncontrolled energy in the form of magnetic fields is induced on magnetic materials, leading to eddy currents.

[0179] Even with poor contact, the wireless elements according to the disclosed quantum wireless transfer methods provide high efficiency of energy transmission. The use of a quantum vacuum as the medium of energy transfer prevents such energy from being directed to metallic materials that may be located between the transmitting and receiving elements. Addressable delivery of energy assures that wireless elements cannot receive wireless energy that is assigned to another destination or recipient.

[0180] Aspects of the present disclosure may include wireless elements formed according to the principles described herein. Aspects may further include variants of unique IONA codes and unique native codes for elements and / or sectors and / or layers thereof. Elements may vary according to type form and purpose, with such purposes including transmission of energy, reception of energy, collection of energy from space, and information transfer.

[0181] Further aspects of the preset disclosure may relate to methods of creating wireless elements, and integration of said elements into electronic devices that make use of wireless power and / or charging. Further aspects relate to methods of converting energy, transmitting said energy, and obtaining free energy from space by wireless receiving elements of quantum wireless transmission systems.

[0182] In accordance with aspects and embodiments disclosed herein, a first step of a method of creating a wireless element may comprise selection of materials. This may include selection of a dielectric layer and two electrically conductive layers. A material for the dielectric layer may be selected from one or more ofglass, ceramic, carbon, acrylic, Polytetrafluoroethythene (PTFE), or similar. In some examples a material for the dielectric layer may be selected from one or more of plastic, glass, epoxy, ceramic, porcelain, wood, rubber, silicone or carboxylic fibre. A material for a conductive material of the electrically conductive mirror layers may be selected from one or more of copper, aluminium, gold, silver, platinum, nickel, or similar. The wireless element may comprise a plate (dielectric layer) coated on both sides with conductive materials (mirror layers). In some examples the thickness of the dielectric layer may be from 0.1 mm to 10 mm. In some examples the thickness of the dielectric layer may be greater than 10mm. In some examples the thickness of conductive coating of the mirror layer may be greater than or equal to 18 pm. The electrically conductive mirror layers are not combined by the use of electrically conductive contacts, but instead operate independently of each other.

[0183] In accordance with aspects and embodiments described herein, a second step of a method of creating a wireless element may comprise calculation of transmitter and receiver elements and the associated internal matching parameters. In some examples, calculating the transmitter and receiver elements may comprise determining a working address (ADR(F3)) of the wireless element. ADR(F3) may represent a final measure of operating parameters of the element, which is determined by the designated frequency. ADR(F3) may perform the role of activating a correctly calculated and configured electrically conductive mirror. Determination of ADR(F3) may comprise calculation of one or more internal matching parameters, including one or more of ADR(F1 ), ADR(F2), d(sync), k(mir), syncl , sync2, or x(F3).

[0184] In some examples, calculating ADR(F1 ) may comprise calculation of IMG1. IMG1 may comprise a continuous line formed in one of the conductive layers (e.g. the lower layer), where a conductive material is removed from the layer such that only the pattern of IMG1 remains. The line IMG1 may be defined by parameters including one or more of line thickness and line length. Calculating ADR(F2) may comprise calculation of IMG2. IMG2 may comprise a continuous line formed in one of the conductive layers (e.g. the upper layer), where a conductive material is removed from the layer such that only the pattern of IMG2 remains. The line IMG2 may be defined by parameters including one or more of line thickness and line length. The same calculation process may be applied for determining addresses at both the transmitting and receiving elements.

[0185] In some examples, x(mir) may depend on one or more of the type of material, the dielectric, the thickness of the conductive coating, the type of conductive material (e.g. silver, gold, copper, or similar). The force of interlayer interaction, k(mir), may therefore be determined as:IONA / c(mir) = x(mir)

[0186] Using the force of interlayer interaction, k(mir), addresses ADR(F1 ) and ADR(F2) can be obtained:ADR F = / (IMGl * k(mir))ADR(F2) = (IMG2 * k(mir )

[0187] From this, syncl and sync2 can be calculated: syncl = ADR F) * IMG2 sync2 = ADR(F ) * 1MG1

[0188] In some examples, the address ADR(F3) of the wireless element can be calculated. The parameter x(F3) determines how the layers are aligned with each other and the IONA for a correctly formed element. A deviation in x(F3) affects the quality of the energy quantization. For each individual size of wireless element, material, and environment in which it will be used, the value of x(F3) will be a unique parameter. The address ADR(F3) can therefore be determined as:ADR(F3) = lMGl * (( / c(mir) * x(F3) ))

[0189] In some examples calculation of the wireless element synchronisation distance, d(sync), can be determined as:

[0190] In accordance with aspects and embodiments described herein, a third step of a method of creating a wireless element may comprise forming a structure of the wireless element. The antenna structure elements may be formed using conventional modern materials processing techniques. Creation of IMG1 and IMG2 may comprise one or more of cutting, engraving, milling, or similar. In some examples, after laser engraving of a selected material, removal of excess material on the plate can be accomplished through chemical treatment.

[0191] In accordance with aspects and embodiments described herein, a fourth step of a method of creating a wireless element may comprise applying a protective coating to at least one surface of the wireless element. The protective coating may comprise a lacquer or paint that possesses appropriate properties for protection against one or more of moisture, dust, or corrosion.

[0192] In accordance with aspects and embodiments described herein, a fifth step of a method of creating a wireless element may comprise determining an efficiency of the wireless element. In examples a transmitter and receiver with matching ADR(F3) can be taken and measurement performed at a plurality of distances between the transmitter and receiver. The synchronisation distance is a calculated theoretical maximum effective transmission distance forthe transmitter and receiver pair. Tests may be performed at a plurality of transmission output powers.

[0193] In various embodiments and examples, one or more of the above-described steps of a method of creating a wireless element may be omitted or performed in a different order.

[0194] Various aspects and embodiments as disclosed herein have applicability in a range of applications. Some embodiments are suitable for medical applications. For example, methods and apparatus disclosed herein may be used for the creation of next-generation active implants, thus making it possible to reduce thenumber of permanent operations to replace implants in the human body for replacement and / or charging of an internal battery of the active implant. The absence of radiation when charging an active implant using the disclosed teachings ensures reliable and uninterrupted operation of internal components of the implant, with the method of charging being safe for humans. Similarly, the disclosed teachings can be used to charge other medical devices that currently use permanent energy consumptions, wires, or batteries, as well as medical equipment and bionic components such as limbs, hands, legs, or similar.

[0195] Some embodiments are suitable for use in electronic devices such as laptops, smartphone devices, tablet devices, portable game consoles, and other similar devices that require constant energy consumption. The disclosed methods and apparatus for wireless power transmission can enable a reduction in unnecessary wires and increase the safety of consumer electronics.

[0196] Some embodiments are suitable for providing wireless power transmission for transportation applications. For example, the disclosed teachings can enable fully autonomous solutions for electric cars, drones, electric scooters, electric bikes, robots, and similar.

[0197] Some embodiments are suitable for the extraction or harvesting of free energy from space. The disclosed teachings provide a unique solution for collecting energy from free space. There is a significant surplus of parasitic energy that is generated, for example, by power transmission lines, household devices, radio transmission devices, and similar. Due to the features of the disclosed methods and apparatus, it is possible to convert this parasitic energy into useful energy for use in other applications. Such elements capable of collecting energy from free space may include elements of the multisector type of wireless transceiver element. Sectors may be divided into synchronous and asynchronous sectors, and have addressed formed according to the spectrum of desired frequencies.

[0198] Wireless transceiver elements that are constructed on the basis of synchronous sectors are considered narrow-action elements, and are therefore able to absorb energy of one specific frequency. Narrow-action elements are suitable for places of a large accumulation of parasitic energy, such as proximate power transmission lines. Wireless transceiver elements that are constructed on the basis of asynchronous sectors are considered broadband elements, and are therefore able to absorb the energy of a mixed frequency spectrum. Broadband elements are suitable for places of accumulation of radio transmission devices, such as Wi-Fi, cellular networks, and similar.

[0199] The disclosed teachings for the collection or harvesting of energy from free space can be used for the creation of solar receivers with ultra-high reception efficiency. The high efficiency of such solar receivers is achieved by capturing the entire electromagnetic spectrum of solar radiation.

[0200] Various examples and embodiments described herein provide a system for quantum wireless energy transmission, comprising: a transmitter, comprising: a transmitting element, the transmitting element comprising a first electrically conductive mirror matching layer and a first electrically conductive mirror synchronisation layer, the first electrically conductive mirror matching layer and the first electricallyconductive mirror synchronisation layer separated by a dielectric layer; means for sending an energy information packet, the energy information packet comprising information about an energy quantized by the transmitting element; a receiver, comprising: receiving element, the receiving element comprising a second electrically conductive mirror matching layer and a second electrically conductive mirror synchronisation layer; means for receiving the energy information packet, wherein, in response to receiving the energy information packet, the receiver is operable to control the receiving element to decompress the energy quantized by the transmitting element.

[0201] In some examples and embodiments described herein, the energy information packet comprises one or more of a synchronising distance, or a transmitter-receiver interaction address.

[0202] In some examples and embodiments described herein, the transmitter further comprises one or more of an energy supply, a signal generator, or a power switching arrangement.

[0203] In some examples and embodiments described herein, the transmitter further comprises an synchronisation analyser.

[0204] In some examples and embodiments described herein, the transmitter further comprises a control unit, the control unit operable to receive a data signal from the synchronisation analyser.

[0205] In some examples and embodiments described herein, the receiver further comprises a level matching module.

[0206] In some examples and embodiments described herein, the receiver further comprises a rectifier, the rectifier operable to convert an alternating current signal into a direct current signal.

[0207] In some examples and embodiments described herein, the receiver further comprises a direct current to direct current converter.

[0208] Various examples and embodiments described herein provide a method of transferring energy, comprising: receiving, at a transmitter element, an electrical input signal; quantizing an energy comprised in the electrical input signal to generate a quantized energy; transmitting, from the transmitter element, an energy information packet comprising information about the quantized energy; receiving, at a receiver element, the energy information packet; based on the energy information packet, decompressing the quantized electrical input signal to generate an electrical output signal.

[0209] In some examples and embodiments described herein, the method further comprises generating, at an inverter, the electrical input signal from a local energy supply input.

[0210] In some examples and embodiments described herein, the method further comprises converting the electrical output signal into a direct current output signal.

[0211] In some examples and embodiments described herein, the information about the quantized electrical input signal comprises one or more of a synchronising distance, or a transmitter-receiver interaction address.

[0212] Various examples and embodiments described herein provide a transceiver element for a quantum wireless energy transmission system, comprising: a matching layer, comprising a first electrically conductive mirror layer; a synchronisation layer, comprising a second electrically conductive mirror layer; a dielectric layer, the dielectric layer arranged between the matching layer and the synchronisation layer; a plurality of signal contacts, the plurality of signal contacts arranged on a surface of the matching layer.

[0213] In some examples and embodiments described herein, one or more of the first electrically conductive mirror layer or the second electrically conductive mirror layer comprises an asymmetric conductive pattern.

[0214] In some examples and embodiments described herein, the second electrically conductive mirror layer comprises a symmetric conductive pattern.

[0215] In some examples and embodiments described herein, the second conductive pattern comprises a single continuous conductive line.

[0216] In some examples and embodiments described herein, one or more of the first electrically conductive mirror layer or the second electrically conductive mirror layer comprises a plurality of conductive pattern sectors.

[0217] In some examples and embodiments described herein, the first electrically conductive mirror layer comprises a plurality of conductive pattern sectors, wherein each of the conductive pattern sectors are not electrically connected to one or more other conductive pattern sectors.

[0218] In some examples and embodiments described herein, the dielectric comprises one or more of plastic, glass, epoxy, ceramic, porcelain, wood, rubber, silicone or carboxylic fibre.

[0219] Some examples and embodiments described herein further comprise one or more further synchronisation layers.

[0220] Some examples and embodiments described herein further comprise one or more further matching layers.

[0221] All of thefeatures disclosed in this specification (including any accompanying claims, abstract, and drawings) may be combined in any combination, except combinations where some features are mutually exclusive. Each feature disclosed in this specification, including any accompanying claims, abstract, and drawings, may be replaced by alternative features serving the same, equivalent, or similar purpose, unless expressly stated otherwise. Thus, unless expressly stated otherwise, each feature disclosed in one example of a generic series of equivalent or similar features.

[0222] The present teachings are not restricted to the details of any of the foregoing examples. Any novel combination of the features disclosed in this specification (including any accompanying claims, abstract, and drawings) may be envisaged. The claims should not be construed to cover merely the foregoing examples, but also any variants which fall within the scope of the claims.

Claims

AMENDED CLAIMS received by the International Bureau on 20 November 2025 (20.11.2025)CLAIMS1. A system for quantum wireless energy transmission, comprising: a transmitter, comprising: a transmitting element, the transmitting element comprising a first electrically conductive mirror matching layer and a first electrically conductive mirror synchronisation layer, the first electrically conductive mirror matching layer and the first electrically conductive mirror synchronisation layer separated by a dielectric layer; means for sending an energy information packet, the energy information packet comprising information about an energy quantized by the transmitting element; a receiver, comprising: receiving element, the receiving element comprising a second electrically conductive mirror matching layer and a second electrically conductive mirror synchronisation layer; means for receiving the energy information packet, wherein, in response to receiving the energy information packet, the receiver is operable to control the receiving element to decompress the energy quantized bythe transmitting element.

2. The system of claim 1 , wherein the energy information packet comprises one or more of a synchronising distance, or a transmitter-receiver interaction address.

3. The system of claim 1 or 2, wherein the transmitter further comprises one or more of an energy supply, a signal generator, or a power switching arrangement.

4. The system of any of claims 1 to 3, wherein the transmitter further comprises an synchronisation analyser.

5. The system of any of claims 1 to 4, wherein the transmitter further comprises a control unit, the control unit operable to receive a data signal from the synchronisation analyser.

6. The system of any of claims 1 to 5, wherein the receiver further comprises a level matching module.The system of any of claims 1 to 6, wherein the receiver further comprises a rectifier, the rectifier operable to convert an alternating current signal into a direct current signal.

8. The system of any of claims 1 to 7, wherein the receiver further comprises a direct current to direct current converter.

9. A method of transferring energy, comprising: providing, at a transmitter element, a first electrically conductive mirror matching layer and a first electrically conductive mirror synchronisation layer, the first electrically conductive mirror matching layer and the first electrically conductive synchronisation layer separated by a dielectric layer; receiving, at the transmitter element, an electrical input signal; quantizing an energy comprised in the electrical input signal to generate a quantized energy; transmitting, from the transmitter element, an energy information packet comprising information about the quantized energy; receiving, at a receiver element, the energy information packet, the receiver element comprising a second electrically conductive mirror matching layer and a second electrically conductive mirror synchronisation layer; and the energy information packet, controlling the receiving element to decompress the energy quantized by the transmitting element to generate an electrical output signal.

10. The method of claim 9, wherein the method further comprises generating, at an inverter, the electrical input signal from a local energy supply input.

11. The method of claim 9 or 10, wherein the method further comprises converting the electrical output signal into a direct current output signal.

12. The method of any of claims 9 to 11 , wherein the information about the quantized electrical input signal comprises one or more of a synchronising distance, or a transmitter-receiver interaction address.

13. A transceiver element for a quantum wireless energy transmission system, comprising: a matching layer, comprising a first electrically conductive mirror layer; a synchronisation layer, comprising a second electrically conductive mirror layer; a dielectric layer, the dielectric layer arranged between the matching layer and the synchronisation layer; a plurality of signal contacts, the plurality of signal contacts arranged on a surface of the matching layer.

14. The transceiver element of claim 13, wherein one or more of the first electrically conductive mirror layer orthe second electrically conductive mirror layer comprises an asymmetric conductive pattern.

15. The transceiver element of claim 13 or 14, wherein the second electrically conductive mirror layer comprises a symmetric conductive pattern.

16. The transceiver element of any of claims 13 to 15, wherein the second conductive pattern comprises a single continuous conductive line.

17. The transceiver element of any of claims 13 to 16, wherein one or more of the first electrically conductive mirror layer or the second electrically conductive mirror layer comprises a plurality of conductive pattern sectors.

18. The transceiver element of any of claims 13 to 17, wherein the first electrically conductive mirror layer comprises a plurality of conductive pattern sectors, wherein each of the conductive pattern sectors are not electrically connected to one or more other conductive pattern sectors.

19. The transceiver element of any of claims 13 to 18, wherein the dielectric comprises one or more of plastic, glass, epoxy, ceramic, porcelain, wood, rubber, silicone or carboxylic fibre.

20. The transceiver element of any of claims 13 to 19, further comprising one or more further synchronisation layers.

21. The transceiver element of any of claims 13 to 20, further comprising one or more further matching layers.

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