Electromagnetic Gauges and Maxwell Lagrangians Applied to the Determination of Curvature in the Space-Time and Their Applications

If we consider the finite actions of electromagnetic fields in Hamiltonian regime and use vector bundles of geodesic in movement of the charges with a shape operator (connection) that measures the curvature of a geometrical space on these geodesic (using the light caused from these points (charges) acting with the infinite null of gravitational field (background)) we can establish a model of the curvature through gauges inside the electromagnetic context. In particular this point of view is useful when it is about to go on in a quantized version from the curvature where the space is distorted by the interactions between particles. This demonstrates that curvature and torsion effect in the space-time are caused in the quantum dimension as back-reaction effects in photon propagation. Also this permits the observational verification and encodes of the gravity through of light fields deformations. The much theoretical information obtained using the observable effects like distortions is used to establish inside this Lagrangian context a classification of useful spaces of electro-dynamic configuration for the description of different interactions of field in the Universe related with gravity. We propose and design one detector of curvature using a cosmic censor of the space-time developed through distortional 3-dimensional sphere. Some technological applications of the used methods are exhibited.


Introduction
The curvature perception in the space is associated increasingly with their interpretation as a distortion of the micro-local structure of the space-time due to the interaction of particles of the matter and energy with diverse field manifestations [1,2]. The matter is shaped by hypothetical particles that take as basic the background radiation of the space, which in the last studies due to QFT, SUSY-theory and brane theory, the strings are organized and tacked to form spaces of major dimensions [3,4] represented by diverse particles of the matter as they are gravitons, barions, fermions of three generations, etc., shaping the gravity at quantum level, obtaining representations of the same one for classes of cohomology of the QFT, like for example the FRW-cohomology, which considers diverse symmetries of cylindrical and spherical type for the gravity modeling like a wave of gravitational energy "quasi-locally" [5][6][7][8]. Their integrals of action define a energy density (Hamiltonian) given for the gravitational case like [9][10][11][12][13]: where L α is the Lagrangian, T αβ , is the corresponding tensor of matter and energy, Γ, is a Hamiltonian density and X β , is the corresponding field of displacement of the particles in the space moving for action of L α influenced by the tensor one of matter and energy T αβ . it is necessary to indicate that L α has component that is invariant yet under movements influenced by the tensor T αβ , which is their electromagnetic component L MAX , (Maxwell Lagrangian (see Table 1 in Section 4, and Table 2 in Section 6).
In case of the energy and through the neo-relativistic models of strings it was possible to have established that this is only a manifestation of the matter in their deep level, being a product of the interaction with particles as [17]. Then 4-dimensional strings (curved part of the background) can be interwoven to form strings that give birth to the quantum gravity that can be measured by the energy due to the backreaction of the photons with the background through a deviation (distortion) in their Lagrangian, reflected the above mentioned deviation in the action dilaton-gravity that would take in the space-time as an electro-gravitational wave with gravitational norm obtained by quantized electromagnetic fields interacting with the gravity. In this interaction dilatón-gravity, the field action is given theoretically Table 1. Connections by Maxwell tensors [5].
where R, is the curvature, d D g x  , is the quantized metric of the metric tensor and , is the dilaton potential. 

Gauges of Maxwell and Variation Principle
Geometrically, a gauge as a physical concept is a vector bundle with a connection or shape operator between points of the space where the shape operator is an invariant under movements and rotations realized in the space [3].
This determines a quality invariant [2,3] of any of the actions in a field that acts on points among the space, which is useful for the effects measurement or observables of the field such as curvature and torsion [2,3], through an operator so that it could decide by means in other fields using a variation principle [1,5]. In particular we are interested in using finite actions (measurable) of electromagnetic fields with an shape operator determined through Lagrangians of Maxwell to measure observables or effects in other fields, for example, the observable ones of curvature and torsion due to the gravitational fields, or the distortion effects in spaces of energy (quantum curvature [5]) given by strong interactions or quantum fields. Interactions between two photons classes, one created by the matter (fermions), and the photon of the integer spin. Before entering in the quantum context, we consider to behavior particles in the macroscopic case.
Maxwell equations can be obtained like equations of a variation principle: Hamilton principle of a stationary action [2].
In effect, be M, a space of points or particles under movement of the action in a conservative electromagnetic field whose group of actions is SU (2), (group that defines the finite actions through unitary anti-Hermitians matrix of range). Be L MAX , the Maxwell operator on this group of points that establishes the law of conservation of movement in M, and that is produced by the fields of Maxwell F (dF = 0, dF* = 0).
If we consider that Maxwell equations can be obtained also like solution for a variational problem, then due to the actions of the fields F, that they produce the movement of all the particles in the space M, and using the corresponding vector bundle of these electromagnetic fields to define it geometrically we can define the above mentioned action as [4,5]: If we consider the global evaluation of the operator who acts on the points space x(s), this is given by The integral Equation (6) represents the action (), in which Hamilton's principle establishes that the particle will cover that trajectory that minimizes the action. Likewise, the movement equation is predetermined by the minimum of this action (), and pre-established for the variation condition [2]: Particularly, if we want the evaluation of this Maxwell's action along a trajectory chosen inside the field of minimal trajectories, as the principle of the minimal action we have the execution of the action of Maxwell's fields [1,5], where s  , is the corresponding measure of the trajectory  , in M.

Shape Operators and Curvature in the Lagrangian Context
In particular, the action , of a field that curls the space M, is given by with R, a scalar curvature and  a metric form of volume in a system of invariant generalized coordinates under translations and rotations of coordinates in the space M. Let's define to j i R , the 2-form of curvature of the shape operator or corresponding connection D.
Then for a region of the space affected by the action , the product   R , can be expressed through surface sections , where establishes the minimal condition of the trajectories followed by particles (mentioned in the Section 2) under the action of the field of displacement [2] (remember that the displacement field does not have character of a tensor but it implies the existence of a tensor which is that curvature [2]) in M, that we will estab-lish by means of the Lagrangian, to know But this new expression of the form of curvature is useful to determine the distortion of the space through the value of the integrals along the minimal trajectories considered in surfaces that shape the form of the space, and whose deviations in conserving regime will determine the curvature of a universe.
The variation respect to the shape operator is established by the "free torsion" to us and therefore the equation of the shape operator 0, that in the context of the finite actions produced by the fields of distortion in Hamiltonian regime, otherwise the Equation (11) is equivalent to the equation which has solutions in all the geometric models of constant curvature in a space M, and their geodesic curvatures are determined by the shape operator evaluated along the geodesic  in the corresponding section of the bundle defined by Equation (3). The Lagrangian writing through a scalar density of energy h, that produces energy as the determined one by Equation (5) in a pure context of the mechanics, we have that the action   , takes the form where h ij , is determined by , The identity from Equation (14), suggests the possibility of using an anti-symmetrical structure similar to the given by the fields of displacement [6], like for example, a structure given by the fields of Maxwell F, in a space of finite actions like the given by the super-canonical algebra [3][4][5]: (15) In fact in general the elements in the Equation (15) , which proceed of considering to as a bilateral ideal as a bilateral ideal [5,7].
The importance of this one formal structure in electromagnetism is its representation and realization for operators of the quantum mechanics [5,8]. It can be demonstrated under certain restrictions in a co-algebra to the curvature connection in case of a Hamiltonian density of curvature [9]. Other algebra of this co-algebra is the relative one to the curvature of space-time [5], that is what we are interested in.
To reinforce the idea of using an shape operator so that used energy of another field origin (like the of electromagnetic field) and to prepare the use of Lagrangian of Maxwell, for the curvature determination under Hamiltonian regime, let's consider where the form of volume in M, remains given for ijkl  , which is a Lagrange multiplier for the Equation (11) [5]. Then studying the variations happened in the integral of Equation (16) with respect to ijkl  , we obtain a variation condition for the curvature tensor through its shape operator with the new introduced elements, to be known This implies that all the terms of the symmetrical tensor of curvature [5] in R ij , are annulled, the Equation (12) being satisfied on the whole  [10].

Electromagnetic Model of Quantum Curvature
We use the generalization of the Maxwell theory given in the Section 2, and let's express the Maxwell-Lagrange operators according to the shape operator or connection and its curvature. Let S G (M) 0 , be a bundle of vector fields on M, with structural topological group G. Let D, be the shape operator in S G (M) 0 , defined by the correspondence to a field X  , and let  D , be the action defined by the form of curvature corresponding to the shape operator D, defined in (18). The shape operator this way definite induces a transformation in the bundle vector fields S G (M) 0 , [5]. This bears to that we could realise gauge transformations on the space M, through generalizing vector fields [5], since it there are the electromagnetic fields of [5], in the structural context given by the topological group of finite actions, with the Hamiltonian formulation given in the Section 2.
The Hamiltonian formulation mentioned can be obtained like solution to a variation problem directly of the Maxwell equations [5], namely: Let ijkl , be a form on volume in M, and let * be the Hodge operator defined by the metric of M. Then This way, Maxwell equations are precisely the Euler-Lagrange equations of the corresponding variation problem. Their action is given by Equation (6). But we want curvature under the action of these Maxwell fields using the minimal trajectories  , possible movement of the particles in a microscopic space-time M [5]. Then the finite action originated from the curvature must be the that comes from a finite action of Maxwell fields in Hamiltonian regime as it is defined from Equation (3) to Equation (6), more the action defined by the form of curvature corresponding to the shape operator D, defined in Equation (18) and that is related to Maxwell fields for the form of curvature described in terms of the Maxwell tensor F: The tensor defined in the Equation (20) is the quantized version of the curvature tensor [5], way that is necessary to be applied to define the curvature according to bundles of light [3,5] (to see Table 1). In fact it is possible to surmise that the reinterpretation of the curvature by electromagnetic fields is established from a quantum or microscopic level using their spinor fields of light [5].
From the Lagrangians described and their gauges (electromagnetic fields), given the following classification of curvature:

An Inferior Bound to Localizing Curvature Measured through Energy of Matter
Be considered to be a connection for this phenomenon of quantum curvature the shape operator, where F D , is the linear connection used in the Equation (20), (that is the linear connection of the gauge transformation (quantized electromagnetic fields) and D  , the connection of movement (translation) of the affine connection describing a small distortion of the space respect to a reference inertial frame, due to this electromagneticgravitational interaction.
Then ,   is a nonholonomic frame. Then the connection D  , must be considered to be like the connection of the censoring that contains quantum curvature.
All R 4 , must be obtained through a micro-local structure of the space-time, whose connection is a generalizetion in a certain sense of the given connection.
Escolium 5.1. The curvature action , on R 4 , measured by the electromagnetic field through the Lagrangian L MAX , comes given for where is the action of Maxwell tensor ones as it is defined in the Equation (6) and  D , is the action defined by the form of curvature corresponding to the shape operator defined in the Equation (18). ,  Proof: We consider inequality: and we consider the energy due to the action ,   [2], to know: (24) from which the curvature Langragian is given by Coupling the energy of Maxwell tensor [5] of the structure of the U(1)-bundle [3], to the equality in the Equation (23) and considering that their compositions , are conformably invariants, we have that under the principle of curved translation [11], the endomorphism ,  is the curvature of which according to the unified conformably invariant field theory [12], is a good approach to the Bach tensor B ij and their correspondent spinor, the Eastwood-Dighton tensor E ijk [4]. This way we have that the action of curvature through the Lagrangian on is precisely the contribution of the Bach and Eastwood-Dighton tensors, [12] to know: where is the compact Riemannian manifold, oriented and of dimension n, of the Riemannian manifold M and g, is the Riemannian metric of M.
Then the curvature on the geodesic one  calibrated through the electromagnetism of the Equation (26) using the concept of gravitational norm used in the Equation (21) is given by The Equation (28) is the geodesic curvature of light. The bilinear form 2 ,

Propagation of Photons and Gravity
We consider the photons propagation in a cut of a cone of light with the infinity null of the space-time (that is to say, only the regions of the space-time where photons interaction exists with hypothetical gravity particles) [13] (hypothesis of Kozameh), then we can obtain a curvature expression according to the quantized electromagnetic fields. But the questions arise: how to obtain a formula that includes the effects of distortion of the light for the gravity presence (curvature), using the condition happened in the Equation (16) and that is simultaneously, an electromagnetic representation of curvature? Will it be possible to design an instrument to detect photons radiated by gravity?
Theoretically, the region that can be capable to these electromagnetic measurements must be the shaped one with strings of such theoretical particles like the graviton and the dilaton that magnetic distortions of the photon detect [14].
We want quantum curvature though fields of light that interact with the gravity, but also we want to measure like quantized electromagnetic energy, which comes from the above mentioned distortion.
Then it is necessary to use the Kozameh hypothesis [13], more curvature hypotheses in theory of the geometrical invariants of the space-time that allows us to measure the distortion of the lines of movement in any particle that falls down under the influence of the gravity field at quantum level, using the back-reaction in the background of the space, with certain hypotheses (to see    Conjecture. The quantum curvature can be measureable or detectable across the effects of reaction of the radiation of the electromagnetic fields with the gravitational field that produces the whose curvature, but these can only measure themselves for its Hamiltonians in the kinematics of the curved space in R 4 , with respect to its micro-local structure. The previous conjecture establishes that the electromagnetic measurement can be realised, but only in indirect form and with fields without mass of electromagnetic origin (photons) which is not detectable for measuring devices (measuring devices do not exist for these ends).

Model of Magnetic Distortion:Magnetic Deformationof Cuadri-Dimensional Part of the Strinf of Background Radiation
We consider , like the 4-dimensional part of the string of background 10-dimensional in which we replace the flat part of , (that is to say, we are considering the part of , where there is distortion We consider the corresponding algebra of electromagnetic fields at level k, given by the gauge group to this scale SU(2) k [15], and   as a real dilaton [14], both appearing in the exact string of background realised by the theory of 2-dimensional superconformal fields. The distortion of such 4-dimensional curved part of the background will be designed in the heteroric superstring theory [12], in the language of the Lagrangian given by 1 2 ( , , , ) d d , The idea is to use the fields i  , to establish a map of the basic space (that is a 2-dimensional manifold fitted like string in the space-time) to the real space-time in question, the latter modeling for a Riemanniana manifold [10]. The distortions will correspond the introduction of a constant magnetic field and its gravitational back-reaction on the 4-dimensional part curled of the background.
In theory not deformed and using the notation of Dirac the action of the Lagrangian described for our string in where     bedding inside) as string in the space-time, g, determines the metrics of the target and Q, is the dilaton charge with x L , is the coordinate of   . On the other hand, the action of a bosonic Lagrangian is given like ( Table 2): Comparing this action with the Equation (6) we obtain the fields of background radiation (since we want to obtain actions dilaton-gravity): 2 Def. 2.1. A dilaton is a hypothetical particle that appears for to do compact strings or quantum dimensions as the theory of Kaluza-Klein. Also is a particle of a scalar field  , that always accompanies to the gravity.
After introducing the complex fermions combination and the corresponding change of the affine bosonic currents J ± = J 1 ± iJ 2 , the supersym-metric affine currents read:  The new space with the action  + , is conformally invariant. The background radiation corresponding to the perturbation of the Equation (10) is determined by fields of background radiation, that is to say, by gravitons G αβ , through gauge fields F   , (electromagnetism), a antisymmetrical field given for H  , and a dilaton Φ, which ones are the solutions of the equations of movement [14,15]: These are obtained of the changes of the following action 4-dimensional effective gauge (effective Lagrangian): where C, is a constant of the Equation (11). Realizing some gauge considerations of the vector potentials A   , and the normalization to g, and H  , we have that the background radiation, expiring with the distortions considered in the action of Equation (10) where H is the magnetic field as in (34). Similarly, when gravitational marginal deformations as in the vertex V gr = R(J 3 + ψ 1 ψ 2 )J 3 , are included, where R is the curvature parameter of the deformation, one can derive corresponding exact background of string theory via Lagrangian calculations, [17][18][19]. Again, the fields in this background which solve the effective field theory Equation (10), are [17]: The dependence on ξ, shows the existence of gravitational backreaction which was absent in the purely magnetic deformed background (40) (to see Figure 2).
In the following Table 2 we do an inventory of the actions of the used Lagrangians.

Electromagnetic Detectors of Curvature: Design of s Cosmic Sensor of Curvature with Penrose Censor
Due there are no instruments for detection and direct measurement of the electromagnetic back-reaction, we can propose the design of an indirect detector based on the concept of cosmic censoring to detect curvature in regions near to a singularity of the space-time. Nevertheless we can use certain studies of the models of the space of de Sitter, to determine through Hilbert inequality and based on certain bound of cosmic censoring constructed by Penrose [20], the possible integral expression of the total Hamiltonian of electromagnetic energy, establishing a condition of domineering energy [11], where there is curvature (that is to say, if the energy is given by this cosmic censor, there is curvature measured like energy that makes the censoring appear).
The latter condition is in a certain sense similar in the mathematical context to the property of obstruction to the integrability of the field equations but in a practical form (similar physicist) who can serve to us to design a detec-tor and curvature meter at quantum level, using theoretical hypotheses [13].
To realise curvature detection it is necessary to be sure, that the above mentioned property or observable it comes from an intrinsic property of the gravitational field in the space-time, which create the geometric stage of the space.
But the space is influenced by this field on every particle that composes it, that is to say, an intersection between the cone of light of every particle and the infinity null exists of the gravitational field that creates the distortion of the space [21].
In these intersections exist the detectable and measureable part that can be measured through microscopic electromagnetic fields and on the other hand that has the gravitational nature that provokes the curvature, generating enough energy to be bounded by the cosmic censor of Penrose [22].
Relative studies to curvature from quantum distortions (like established in the previous section), confirm the hypotheses of consider the Lagrangian to be able to measure curvature from a quantum level, the above mentioned with the geometric hypotheses on a cinematic model of the predefined space for the geometry for the case of curvature.
We consider the kinematic models given by the spaces that are asymptotically de Sitter and anti-de Sitter [23,24]. Proposition 8.1. Considerating the Cosmic Censorship hypothesis given by Penrose [20], we have that the area A , of a singularity (black hole visualized as a spherically symmetric space) is proportionally minor that the quasilocal mass around of singularity given for 16πM 2 [11]. Then in the events of the space like one asymptotically de Sitter space its have: which represents the curvature measured like energy doing to appear the censure given in the second member of the inequality and that it goes out to re-shine for the Lagrangian action of gravitational field moving away or approaching the singularity (asymptotically de Sitter and anti-de Sitter spaces).
Proof. [22,25]. The minimum energy (second member of the In-Equation (42)) must be obtained directly in a geometrical condition given by an invariant of curvature. From the exponential of empty expect value , of the effect action given by the Equation (39), we obtain the coupling constant g, and as by the generalized Gauss-Bonnet theorem we have [7,26]. For the case of M, see it like a space 4-dimensional, it is necessary to consider the spherical map M  S 3 , in this case the electromagnetic fields can be used like gauges remembering that SU(2)  S 3 .
Then the cohomological classes of the Cartan forms  1 , and  2 are annulled (H 1 (SU(2), R) = 0, that is the case of the integrals like discussed in the page foot 1, since the electromagnetic energy with respect to the energy of background radiation can fulfill that Then from (44), (46) y (47), the condition is had which is (42) for a singularity detected of spherical type [25,28] (see Figures 4 and 5). A table given for manifestations of mass-energy "detected" by this indirect method showing curvature existence [29] is the Table 3.

Applications and Technological Development
The equivalence class of the potentials A i , can be re-interpreted precisely as a connection (operator of form) on a trivial bundle of lines and admitting bundles of not trivial lines with form operator provided with arbitrary fields F (like the curvature of this connection). The Aharonov-Bohm effect [5], it provides of a physical justification of this formulation. Precisely the resultant physical theory and their generalizations are known like the gauge theory [30].
The following Table 4, establishes the correspondence of operators of form provided with arbitrary fields of Maxwell under the action of the corresponding Lagrangian and their corresponding curvature tensor [31]: Certain simulations have been realized considering certain restrictive conditions to models of the space-time (to see Figure 6). In particular there have been considered to be models with Lorentzian metrics of negative curvature: Has been innovated into the design and making of several electromagnetic devices of measurement and detection of curvature (to see Figures 7 and 8), which use signals of light to measure the curvature with the information of the angles of deviation of the incidental signals of light in the surface of the object or body. In case of curvature detection is designed a sensor of curvature based on an integral operator on Gaussian curvature. The patent of these devices is in administrative step.
There are many technological applications that cans be realised by the concept of gravity quantum through their observable that is quantum curvature. For example in nanostructures, we can create through geometrical potentials and light waves the Curvature-induced geometric potential in strain-driven nanostructures [32], and evaluate their curvature in this level [32].
The use of electromagnetic fields to measure observ-able of other fields like the curvature that is an observable geometric one of the gravitational field in the spacetime they suggest the possibility of a unified theory in a curved similar sense of their vector bundle. The equation 0, D F   (given in the Equation (20)) is not quite different of the Equation (12), simply is a particular case of this last equation to the case of the actions of a electromagnetic field determined to the 2-forms F, defined in a SU(n)-vector bundle.
This way there are obtained fundamental 2-forms of curvature F D , that are integrable in the same sense as the integrals of line given by the Hermitian forms for the Maxwell tensor of the Lagrangian, namely:     on embeddings of in M. Using the Stokes theorem it is possible to demonstrate that the contours established by the minimal trajectories in Hamiltonian regime on the sphere given for S 2 , and under the action of Maxwell field to displace particles of M, along the minimal circles, there is obtained a tensor of curvature similar to the tensor of Riemann in the electromagnetic context and their symmetrical part, that is to say, a useful version of the Ricci tensor to calculate Gaussian curvature (to see Figures 7 and 8). The action of Maxwell fields displacing particles of M, along deformable circles is similar to the action continued by the field of displacement defined in mechanics to determine curvature using the deformable contours of field [5].

, S
A possible progress of this approach of proposed curvature, through bundle of light it is the securing of a field of displacement of the curled (curved) similar one of the similar operator D, according to Maxwell tensor ones considering the similar structure of the space-time. This is precisely what allows to glimpse the Eastwood-Dighton tensor E ijk , in the securing of a model of conformal curvature for Einstein equations in a spinor bundle [12].
Defining the concept of conformal gravity, there is an approach of the tensor of Riemann obtained through the calculation of the Ricci tensor using a conformal factor determined by the anti-symmetrical component of R ij ( [4], which is comparable to the use of a bundle of lines for any quadric of a Lorentzian manifold. This opens the possibilities mentioned previously of a shape operator defines through rays of light that give shape to the curved image of the space-time, similar to a celestial vault. 0, ijk E 

Applications to the Coherency, Background and Expansion of the Space-Time
The temperature of the Cosmic Microwave Background (CMB) is nearly isotropic. That is, when you look at different patches of the CMB, their temperatures are the same to within 1 part in 10,000. This implies that when the universe became transparent (about 300,000 years after the Big Bang), it was nearly homogeneous [33]. The homogeneity, or smoothness, of the universe is referred to by cosmologists as the horizon problem (Figures 9  and 10).

Electrodynamical Configuration
Using the cohomological classes of the integrals in elec-trodynamics calculated by Lagrangianos module the groups calibrates, U(1), U(2), SO (2), SU (2), SU(2, 2), etc we can establish the following spaces of electrodynamic configuration and their constituent elements (see Table  5). For other side the the Table 5, it serves to us to understand the decomposition of an electrodynamic space in their orbits considering their manifold structure (to see Figure 11). Likewise, considering the backreaction in the space-time, the orbital spaces become more clear (Figure 11).

Factible Electro-Gravitational Ultra-Sensor
The Theoretical devices to measure gravity it haves designed from the first serious affirmations on gravitation given by Galileo and Newton. Nevertheless, with the step of the time and due to born of new theories of the universe based in studies inside the field theory from the theory of the relativity, up to the theory M, they have marked the need to design using gauge theories, instruments that could measure at least in indirect form or by means of sophisticated methods of metrology based on dimensional relations gauge field that are constructed by Gaussians units or of another type observables of field as the curvature [34].
An example of such devices there are the electrogravitational devices that try to use electromagnetic waves and electromagnetic field interactions to measure gravity using the concept of background radiation [35] and the traces of particles obtained in the laboratories of the atomic accelerators as the given in the CERN (Organisation européenne pour la recherche nucléaire), measuring the distortion of these waves based on the traces of the particles left in the fog cameras of the accelerators. Other better attempts have been realized by the CMB (Cosmic Microwave Back-ground), radiation spectrums being obtained in the direct measurements by the satellites in the space, for example SMAP.
One important idea inside the study of the microscopic space-time is the group representations of SU (2), where one of which considering the super-symmetry is S 3 (sphere of dimension 3) [5,15]. In her the topological invariant of their 2-form ω 3 , given in the Equation (45) and whose cohomology in not null (see Section 8) it shows clearly that the gravity presence can be warned at least on the surface of this sphere, which can be considered to be a mini-twistor in the presence of gravity considering a ambitwistor space of couples ( Z  ,W  ), to the microscopic space-time, where Z  , are the fields of gauge nature (in this case electromagnetic fields) and the fields of particles of the gravity (gravitons), (that in this case is the background).
Based on it, and considering the value of curvature to be the contour deformation on a surface (initial idea created by relativity to understand curvature in a space-time surface [2]), at the same time that a field distortion created like an undulation in the space time for back-reaction for photon propagation in the presence of gravity (see Figures 2 and 3 (using string theory)), we can extrapolate this idea to the design of a type of accelerometer that can be connected to the devices of navigation of a traveling satellite by the space, where said accelerometer involves in their interior a sensor of ultra-sensitive gravity based on a solid sphere S 3 , of material similar to a colloid, captured the changes of the weight of a liquid also of colloid type (perhaps of major density that of the ball S 3 ) due to the universal factor G.

Conclusions
The methods through Lagrangian actions are useful to obtain expressions of measurable electro-gravitational gauges in a gravitational dynamic system that can be adapted for the detection of observable of the energymatter tensor expressed from the microscopic level in the equations like the given by the system (35,36,37,38) (which one is a gravitational-dilaton version of the Dirac equation) up to the macroscopic dimension of Einstein's space-time, for tensor saying T  .
Then the existence of the observable gravity effects initiate from a field of quantum gravity generating quantum curvature and torsion observables of the space, which can be detected in Einstein's dimension like cosmic censoring for gravitational waves shaped by electromagnetic waves according to the cosmic censor calculated for Penrose [11,12,20,22]. This cosmic censoring can be detected by a model of ultra-sensor that we design on the ball S 3 , of certain distortion of the space-time created for back-reaction (Figure 12).
But these methods are based on much in the gauge theory and of the information of the gravity through models of gravitational waves by means of electromagnetic waves where the detection will be realized by means of spiraling created for the back-reaction that will take place through traces of a electro-gravitationally observable type, whose geometry is a 6-dimensional superstring. The method that we propose in the Section 9.3, might adapt itself at quantum level capturing these small interactions and recording in information of quantum gravity codified by field elements already classified under the different types of sub-particles that define at quantum level material forces.