1. Introduction

In the usual communication processes, the transmission of electromagnetic waves is realised with limitations given due to the scattering in continuum media, interference for appearing of other waves and signals, and also pollution by free electrons, molecular absorption of the air, or a defecting routing of the TEM and TMM, as well as their secondary modes, the latter in the case of the optical fibre. Even nonthinking is the effective transmission through impermeable media and nonpermissible or invasive media such as the communication through ambient with continuum media, saturated continuum media in communications or in the presence of multi-radiative objects of big density, etc.

Likewise, the continuum transmission media produces a limiting whose dependence of the macroscopic characteristics of the space-time do that the electromagnetic fields suffer refraction and reflection due to the substance of the proper media. For eliminate this direct action of media in the signal transmission, it is necessary that our signal communication concept does not depend on the media characteristics, even that are not 'accessible or available' in the dimension of the usual space-time where we have placed the continuum media phenomena. For example, the gravitation in the macroscopic sense has interference in the ordinary communication where field observables of an Einstein space (as could be the curvature and torsion of the space-time, seen as gravitational observable effects or of electromagnetic scattering) act as distortion waves to produce a field radiation due the background in the universe. Then the signal transmission must have the invariance of the electromagnetic fields but with quantization of these fields, in a space that topologically is viable to their transmission [1].

Considering the quantum field theory [2] (QFT) with their second duality principle, that is to say, the duality wave/field applied to certain fermions and bosons, we can give a good fundament on the possible behaviour of these particles and their action with the communication intention [3]. However, it is necessary to consider the invariance of the Maxwell equations in quantum electrodynamics (QED) [1, 4], which we can design a form of quantum communication that establishes new paradigms of information transmission through quantum waves. However, in this new communication process, the intertwining concept of the particles is required [5] that will transmit the information via a chain of photons using gauge bosons as supports (selectors or linkers) of the electrodynamic space to their quantum level.

The material part of the transmission is generated in the transceptors through their solid state. Therefore, using electrons as solid-state source to generate a source of photons through a process derived from certain spintronic devices as dots, magnetons, etc., the bosons can be conformed to the information of the communication in waveform and the plasmons as a quantum media of transmission of these information waves. The gauge bosons also will be necessary as transmission nodes. If we want to obtain voice communication, this will be obtained introducing phonons [5] in the photonic wave. We establish some fundamental precisions using quantum mechanics to explain those particles intertwining. We must consider that to that this intertwining happens, are necessary more dimensions that Minkowski space-time dimension.

then Eq. (1) can be written as (to m-border points and n-inner points)

Introductory Chapter: Advanced Communication and Nano-Processing of Quantum Signals

ð

¼

Iqdφ1m1…dφnmn…

� �…dφnm<sup>1</sup> � �… (3)

ððð <sup>I</sup>dφ1mn

This defines an infiltration in the space-time due to the action I that happens in the space Ω � C, to each component of the space Ω Γð Þ, with energy conservative principle expressed for the Lagrangian ω, of Eq. (2). Likewise, in Eq. (3), the integration of the space is realised with the infiltration of the time, integrating only

Let , be the space-time constituted by the particles x1ð Þt , x2ð Þt , x3ð Þt , …, whose states φ1, φ2, φ3, … are such that satisfies Eq. (3); then the information is transmitted like the quantum wave ϕ, of the state φ, replaced with the state

> 1 � �ϕφ<sup>2</sup> <sup>t</sup>φ<sup>0</sup>

where the transmission of the quantum wave is realised on the spinor space (see spinor technology [6]) of t<sup>σ</sup> and where t<sup>σ</sup> is the intertwining technology that is

The states of distinguishable particles that are bosons or fermions realise the arrangement that eliminates an infinity of the states that by their sum of spins are annulled, remaining only those that realise an effective action. These are annulled between the perturbed states and those that are affected by scattering. We consider again the space of configuration Cn, <sup>m</sup>, equivalent to the complex given for C Mð Þ, which can be thought as composed for n�hypercubes U, defined by 000…0 boxes. Then we can define a net of paths that will be able to establish routes of organised transformations on diagrams of Feynman type (with path integrals with actions given by Oc and path integrals as Eq. (1)). Likewise the ideal route of the intention

Then these arrangements can happen in the nets designed on a field of particles that can be arranged in 0000…0 boxes [7], where the action can be calculated in a point (node of the crystalline net of a field [7]) corresponding to the n� states of

<sup>1</sup> ð Þ<sup>ϕ</sup> <sup>X</sup><sup>α</sup>2W<sup>α</sup><sup>0</sup>

2 � �ϕφ<sup>3</sup> <sup>t</sup>φ<sup>0</sup>

3 � �ϕφ<sup>4</sup> <sup>t</sup>φ<sup>0</sup>

<sup>2</sup> ð Þ⋯<sup>ϕ</sup> <sup>X</sup><sup>α</sup>nW<sup>α</sup><sup>0</sup>

4

� �⋯ (4)

<sup>n</sup> ð Þ (5)

i, ið Þ ¼ 1, 2, 3, … , in the infinite homomorphism (which is of the type

ð

DOI: http://dx.doi.org/10.5772/intechopen.89069

2. Quantum communication link waves

spinor elements of the field.

ϕð Þ¼ n ∗ m ϕð Þ n ϕð Þ m ):

ϕ tφ<sup>0</sup>

created in the class σ:

þ

5

½ � x <sup>U</sup> ¼

<sup>1</sup> ∗ tφ<sup>0</sup>

<sup>2</sup> ∗ tφ<sup>0</sup>

<sup>3</sup> ∗ tφ<sup>0</sup> <sup>4</sup><sup>⋯</sup> � � <sup>¼</sup> ϕφ<sup>1</sup> <sup>t</sup>φ<sup>0</sup>

is established, considering the action in every node of the net.

ð

000⋯0�boxes

energy φið Þ i ¼ 1, 2, 3, …, n , having the superposition n the node given for

ϕ X<sup>α</sup>1W<sup>α</sup><sup>0</sup>

In the quantum zone, the quantum particles field is permanent and interminable, since matter and energy are equivalent and the electrons are interminable and thus the photon production also. What gets worn is that there are the linkages between atoms which can weaken or get lost for the absence of a transmission of the states of suitable energy (routes given by path integrals). Infiltrating the intention on every path γ and under the condition of permanent field given by the operators Oc, the transmission of the states will be revitalised by every node, transmitting the

dz<sup>n</sup>

φ0

Ið Þ φð Þ x dφð Þ x ¼

We consider a particle system <sup>p</sup>1, p2, … in a space-time <sup>M</sup> ffi <sup>R</sup>4. Let x tð Þ<sup>∈</sup> Ω Γð Þ⊂R<sup>3</sup> It, a trajectory, which predetermines a position x∈R<sup>3</sup> , for all time t∈It: Also we consider the field X, which infiltrates their action to whole space of points x1ð Þt , x2ð Þt , x3ð Þt , … ∈ Ω Γð Þ, predetermining the points φið Þ xið Þt , that are field particles of the field X and evaluated in the position of every particle. In each point, a defined force exists given by the action I, of X, along the geodesic γt, and determines direction by their tangent bundle given for TX<sup>1</sup> ð Þ Ω Γð Þ ; that is to say, the field gives direction to every field particle φi, having their tangent bundle has a spinor bundle <sup>S</sup>, where the field <sup>X</sup> comes given as <sup>X</sup> <sup>¼</sup> <sup>P</sup> i φ<sup>i</sup> <sup>∂</sup> ∂φ<sup>i</sup> � � � xi , <sup>φ</sup><sup>i</sup> ð Þ, <sup>∀</sup>φ1, <sup>φ</sup>2,

φ3, … ∈ X<sup>1</sup> , on every particle pi ¼ xið Þt , ið Þ ¼ 1, 2, 3, … : Then a direct intention is the map or connection <sup>∇</sup><sup>I</sup> : <sup>T</sup>Ω Γð Þ! <sup>T</sup><sup>1</sup> ð Þ Ω Γð Þ ,ð Þ ≃T ∗ M , with the rule of correspondence xi, ∂txi � �↦ φ<sup>i</sup> , ∂μφ<sup>i</sup> � �, which produces one ith-spinor field φ<sup>i</sup> , where the action I, of the field X, infiltrates and transmits from particle to particle in whole space Ω Γð Þ, using a configuration given by their Lagrangian L (conscience operator), along all the trajectories of Ω Γð Þ: Then of a sum of trajectories, <sup>Ð</sup> DFð Þ x tð Þ , one has the sumÐ dð Þ φð Þ x , on all the possible field configurations Cn, <sup>m</sup>:

We can to extend these to whole space Ω Γð Þ⊂ M, on all the elections of possible paths whose statistical weight corresponds to the determined one by the intention of the field, and realising the integration in paths for an infinity of particles-fields in TΩ Γð Þ, is had that

$$I(\boldsymbol{\varrho}^i(\mathbf{x})) = \bigcap\_{T\mathfrak{Q}(\boldsymbol{I})} \boldsymbol{\varrho}(\boldsymbol{\varrho}(\mathbf{x})) = \limsup\_{\delta \to -\infty} \frac{1}{B} \int\_{-\infty}^{+\infty} \frac{d\boldsymbol{\varrho}\_1}{B} \dots \int\_{-\infty}^{+\infty} \frac{d\boldsymbol{\varrho}\_n}{B} \dots$$

$$= \prod\_{i=1}^{+\infty} \int\_{-\infty}^{\infty} e^{i\Im[\boldsymbol{\varrho}^i, \boldsymbol{\vartheta}\_\ell \boldsymbol{\varrho}^i]} d\boldsymbol{\varrho}^i(\mathbf{x}(s)) \tag{1}$$

where <sup>B</sup> <sup>¼</sup> <sup>m</sup> 2π iδs � �<sup>1</sup>=<sup>2</sup> is the amplitude of their propagator. Then we have the corresponding Feynman integral of the volume form ω φð Þ ð Þ x , obtaining the real path of the particle (where we have chosen quantized trajectories, that is to say, Ð dð Þ φð Þ x : But this superposition of paths is realised under an action whose corresponding energy Lagrangian is ω φð Þ¼ ð Þ x I<sup>ξ</sup>ð Þ <sup>x</sup> dð Þ φð Þ x :

Then to a configuration on the space-time M, given for C Mð Þ, in a space-time region where there have been interfered paths in the experiment given by multiple split, given for <sup>Ω</sup>ð Þ <sup>M</sup> , we have the pairing <sup>Ð</sup> : C Mð Þ� Ω ∗ ð Þ! M R, where Ω ∗ ð Þ M is some dual complex ('forms on configuration spaces'), and then the 'Stokes theorem' holds

$$\int\_{\Omega \times \mathbb{C}} a = <\Im \zeta \, da > \tag{2}$$

Introductory Chapter: Advanced Communication and Nano-Processing of Quantum Signals DOI: http://dx.doi.org/10.5772/intechopen.89069

then Eq. (1) can be written as (to m-border points and n-inner points)

$$\begin{split} \int \Im(\varrho(\varkappa))d\varrho(\varkappa) &= \int \Im\_q d\rho\_{1^{m\_1}}...d\rho\_{n^{m\_n}}... \\ &= \int \Big( \Big( \int \Im d\rho\_{1^{m\_n}} \Big)...d\rho\_{n^{m\_1}} \Big)... \end{split} \tag{3}$$

This defines an infiltration in the space-time due to the action I that happens in the space Ω � C, to each component of the space Ω Γð Þ, with energy conservative principle expressed for the Lagrangian ω, of Eq. (2). Likewise, in Eq. (3), the integration of the space is realised with the infiltration of the time, integrating only spinor elements of the field.
