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The Relativistic and the Hidden Momentum of Minkowski and Abraham in Relativistic Energy Wave

An analysis of the consistency of the Abraham and Minkowski momenta in the determination of the photon trajectory was carried out considering a new principle of conservation of the photon's mechanical energy, in which the photon conserves translational energy in orbital angular momentum when transiting between two media, introducing the relativistic energy wave (REW). The confrontation between REW and the recent theory of space-time waves (ST) was considered, pondering your differences. Throughout this study it was possible to verify that the Abraham momentum appears a relativistic photon ignition device in the transition between two media, acting as the hidden momentum of the Minkowski’s relativistic momentum. The wavy behavior in the matter is relativistic, and the relativistic trajectory appears with delays and advances, with points of synchronization between source-observer. The classical or relativistic trajectories are determined as a function of the angle of incidence and the relative refractive index, by one of two distinct non-additive torques, the classic by Abraham or the relativistic by Minkowski. It was found that the same analysis conducted under the principle of conservation of the mechanical energy of the photon can be treated by an new Doppler, Relativistic Apparent, that can be confused with other Dopplers in the treatment of redshift from distant sources. It was found that the conservation of energy in Orbital Angular Momentum (OAM), in the interaction with matter, explains that the synchronization instants are found in the inversion of the OAM, where the advances and delays of REW occur under negligible variations of the OAM, however, opposites.


INTRODUCTION
Countless phenomena that characterize the properties of light are known and well established in the literature, whether in corpuscular or wavy treatment. However, the photon's behavior is the center of a series of discussions that has been going on for decades, such as the orbital photogalvanic effect to the induced current, due to its distinction, whereas it originates from the OAM of light.
Schmiegelow et al. [42], considering that in the photon-matter interaction an OAM carrying a photon can transfer OAM to a free electron, conducted a study analyzing the transference of OAM to a bound electron, demonstrating the transference of OAM and spin angular momentum, SAM, from the field to the ion.
According to Forbes et al. [22], the total angular momentum is composed of the OAM momenta [1] and SAM, where the SAM is present, regardless of the presence of a material media, conserving the helicity which, in its turn, is not transferable to the matter. The OAM by photon along the propagation axis characterizes the movement of a particle around the propagation axis is transferable to matter. The OAM features a cross-beam structure, where the experience [23] demonstrates that the transverse structure causes a delay in the average speed of photons in a beam, when compared to a beam without structure, even in air.
In a theoretical analysis of the corpuscular behavior of light, Cardoso [13] introduces a principle for the conservation of the photon's mechanical energy, where the photon transiting between two media conserves translational energy in OAM, shifting its wavelength. Later [10], this wave displacement is verified in the prediction of interference fringes comparing to experimental data from a Michelson interferometer, verifying that the model according to the principle of conservation of the photon mechanical energy presents estimative with smaller percentage of uncertainties (< 0.5%) and smaller percentage of deviations (< 2.0%) when compared to the literature model estimative in the data representation.
Recently, Cardoso [12] demonstrates the nature of the redshift according to the principle of conservation of the mechanical energy of the photon, presenting the gravitational redshifts (z CEF-G ) and refractive (z CEF-G ) which individually are able to describe the gravitational and cosmological redshifts keeping constant the Hubble constant. However, the author considered the composition of all the effects capable of promoting a displacement of the light's wavelength, possibles in the trajectory, presenting a balance through the redshift Z CEF , considering the Doppler effect, demonstrating that in the absence of the principle of conservation of mechanical energy, the Hubble constant must vary by small variations in the relative velocity between source-observer.
In this analysis verified the consistency between Abraham and Minkowski momenta in the determination of the photon trajectory, and its implications regarding the incidence angle and relative refractive index, considering the conservation of the photon's mechanical energy in rotational energy.
A comparative analysis was conducted between the relativistic behavior of the photon and the recent space-time (ST) waves, in the perspective of delays between the source and observer perceptions. It was verified the existence of refraction possible anomalies in the perspective of a single photon, in an analogue weighing the differences with those recently associated with group speeds [6], [33], [46]. The relationship between the variation of the OAM and the delays between the source-observer perceptions was verified, in the perspective of the conservation of the mechanical energy of the photon.

METHODOLOGY
The analysis considers the transmission of a single photon in the transition between pairs of media previously known in the literature, with regard to refractive properties. The refraction data established in the literature and the Laws of Refraction are compared to verify the variability of the data estimated by the proposed models.
In the corpuscular treatment of the photon-matter interaction, the conservations of energy, linear momentum, and angular momentum, were considered. In the characterization as an energy package, the quantization of energy and the uncertainty principle were considered. The analysis of the state of movement considered a relativistic description consistent with the behavior of the data.

DEVELOPMENT AND DISCUSSION
We will assume that the photon far from a vacuum behaves like a material wave of energy, where its state of movement is characterized by the De Broglie momentum [18]: although clearly it's about the quantized quantity, we can satisfy that there is a classic part that can be described by the Snell-Descates Law [36] (λn 21 = λ 0 ): so we can write: where the wavelength shift in the transition between two media: In the interaction with matter, the unabsorbed or scattered photons interact with electrons at short distances and without contact, characterizing an elastic collision. In the model of Compton, the electron was at rest before the interaction, but in agreement with Cardoso [13] the electron has linear and angular momenta before the interaction, where the conservation of linear momentum: In accordance with the literature [20], when an electron is found in a region delimited by r, the moment uncertainty: where each component of linear momentum carries i can a uncertainty, so that we can approximate: satisfying that we can represent increases or decreases in the mechanical energy of the electron, in terms of the variation of the linear momentum of the photon, considering relations (5) and (7): so that the displacement of the photon's wavelength in part characterizes the De Broglie wavelength shift [18] in the description of matter waves, such that replacing (8) in (4): The variation of the photon's linear momentum has an associated energy that should make up the balance of the conservation of the photon's mechanical energy: where the increase in energy: considering again the Snell-Descates Law and in terms of the quantized energy of the photon: In the interaction with matter, the unabsorbed or scattered photons interact with electrons at short distances and without contact, characterizing an elastic collision where the intensities agree: such that the displacement of the wavelength characterizes the new principle of conservation of mechanical energy for the photon acoording Cardoso [13], [10], [12]: 3.1

PHOTON RELATIVISTIC IGNITION
The expression (14) demonstrates that the wavelength shift is relativistic 1 : according to Saldanha [38] there is a material part, where the De Broglie wavelength can now represent this amount: simplifying the expression (15): where it is noted that the De Broglie wavelength dilation (γλ) is a consequence of the variation of the photon's energy, associated with the angular momentum acquired by the photon in the interaction: satisfying that the photon before the interaction had only linear momentum.
Considering the angular momenta of Abraham and Minkowisk for the photon [39], we can write: where "l" is the Laguerre-Gauss mode.
The energy given by equation (12) can be associated with angular momentum due to the torque associated with Abraham and Minkowski momenta: where the eq. (20), considering eq. (19) reveals a structure 2 of the photon movement where analogue l = 2 is consistent with other studies [26], although we will verify in section 3.4 that a more peculiar modulation appears in the photon-matter interaction. Naturally satisfying that the photon conserves its energy in a form of movement, for if the increment in energy is transferred for media, it will soon be dissipated. The refraction process, for example, is a process in which the photon transits between two media with constant frequency and naturally conserves energy in forms of movement.
1 The equation (15) will only have a relativistic character if the speed of the photon in the refringent media (in the second term of the radical) is the relative speed between two reference frames. Here we follow the analysis previously treating it as relativistic, although this criterion is discussed later in section 3.2. 2 In section 3.4 the modulations are presented as a function of the relative refractive index and the incidence angle.
The increment in energy conserved in OAM implies in a decrease in linear momentum, which is now characterized by Abraham's 3 momentum (hn 12 /λ), acting as a relativistic ignition device that drives the photon into a relativistic movement: explaining a greater moment in the refringent environment, center of the Abraham-Minkowski conflict, resultant from a dilation of the moment. We can treat the Mikonwski momentum as a relativistic momentum in the material refringent: Characterized, the relativistic moment in accordance with the principle of energy conservation of photon's mechanics [13], [10], [12], with representation of the Mikonwski momentum, we can verify the relationship directly from the Mikonwski momentum itself [3], it is: considering the relation (7), we can write: similarly, considering again the Snell-Descates Law: where in the subtraction between eq.(s) (23) and (22) eq. (4), of which following the same analysis of eq. (s) (8, 9, 12 and 13) results in eq. (14).
The eq. (15) shows that the displacement of a relativistic wave for photon results from the decrease in energy associated with the translational movement. Abraham's linear momentum (hn12/λ) characterizes a hidden momentum, according to Saldanha [38], being now the hidden momentum of Mikowski's relativistic momentum.
The material part of the eq. (15) shows agreement with Goray et al. [24], while saying that light as a particle when incident on the separating surface between two media will present a wavy behavior. Here we demonstrate the composition of a material energy wave characterized by the De Broglie momentum, where the photon in the material media has a wavelength and relativistic moment equivalent to that of an electron with energy hν. Tan [44], in a study of the photon's imaginary rest mass, found a relationship similar to eq. (15), where is discussed that the excitation of matter implies a material wave of a particle similar to the electron neutrino, with energy hν.
In this context, we present that the photon, when interacting with the matter, starts to behave in the form of a relativistic energy wave whose linear trajectory can be found through the relativistic deformation of the linear momentum of the wave: although a classical trajectory is also allowed, which agrees with the Snell'-Descates Law for small angles, and it happens by a decrease for the Abraham momentum: It can be noticed that eq. (25) has a classic character while (24) is relativistic, and it is noticeable that in the latter, the variation of the linear momentum characterizes its projection in the direction perpendicular to the actual path of the photon Figura 1, while the variation of the linear momentum of Abraham represents the deformation of small angles, properly. Although relativistic effects occur in the transition between the two media, the real trajectory to be followed by the photon can be defined by two non-additive torques, as they are in different scenarios, a classic (τ Abraham ) and the relativistic (τ Minkowski ), where we will verify that Minkowski's agrees with the relativistic trajectory that arises with delays, advances, and synchronizations as we will discuss in this analysis. Relativistic delays are found in different scenarios [43], [6], [30].
In the Figura 1 there are two regions defined by the angle of incidence. In the classical region, the incidence up to approximately 41º, the trajectory imposed on the photon in refraction is that determined by the Abraham torque, while in the relativistic region the relativistic trajectory comes up with a certain delay as discussed in section 3.2, determined by the Minkowski torque, for angles of incidence greater than 41º. In this way, the angular deformation for an incidence of up to 41º: For angles greater than 41º, the angular deformation is represented by the deformation of the Minkowski linear momentum according to eq.(24), with characteristics similar to frequency independent rotational Doppler as reported by Martin et al. [32], discussed in the section 3.2, as: where the transition from the deformation regime is around 41°: The eq.(s) (26) and (27), treated below as strains, are checked against the refracted angle estimates according to the Snell-Descates Law and the behavior of the data.
Tabela 1 compares the refracted angle estimates between the Snell-Descates Law of sines and the strains given by eq.(s) (26) and (27), noting that the mean deviation of the strain estimates in relation to the data, is eight times smaller than those of Snell-Descates. This comparison was chosen due to the historical fact that the Snell-Descates Law stood out against different models that sought to describe the refraction process, with propositions from Ptolemy and Kepler [9], between others. Notoriously, the deformations are well-fitted, representing the behavior of the data. The Figure 2 present the estimates of the deformations of eq.(s) (26) and (27) and the data the refracted angles, where the trajectories followed by the photon are verified as a function of the angle of incidence. The classical trajectory determined by the torque of Abraham represents the refraction data of water, as shown in Table 1, for incidences up to approximately 41°, while for larger angles the photon follows the relativistic trajectory determined by the Minkowski torque.

RELATIVISTIC APPARENT DOPPLER
The deformations presented in eq.(s) (26) and (27)  It is a Doppler effect for light, with constant frequency, in which the photon when transiting between two media presents a decrease in its momentum, the effect of which is analogous to the appearance of movement source-observer relative, which we now observe in the example configuration in Figure 3. From the observer's perspective, the wavelengths in both media: where N 1 and N 2 , the numbers of wavefronts associated with the refringent media n 1 and n 2 , respectively. The wavelength shift recorded by the observer: where it was considered a process in which the frequency is constant, such as: In a translational Doppler analog, the decrease in the speed of the photon in relation to the observer characterizes an effect of relative movement between source-observer, such that in terms of proper time: where in accordance with the relations (29), we can: characterizing the displacement presented in eq. (15), the proper wavelength in the material media can be characterized by that of De Broglie.
An important aspect to characterize the apparent relativistic moviment is that in fact the speed of the photon in n 2 be the perception of apparent relative velocity between source-observer, although there is no real movement between them. We know that both will have perceptions of apparent positions in relation to the other. In the source referential, the perception of the apparent position of the image the observer allows us to say that the image has moved in a very small amount of time (∆t 1 + ∆t 2 ) with a very high speed v image = (c 2 -v 2 ) 1/2 , projected on the opposite cateto of the triangle featured in Figure 1, where in this case the photon velocity (v) in n 2 is the apparent relative speed of approximation between source and observer, characterizing an apparent relativistic movement between source and observer. The use of photon speed after transmission as relative speed can be found in other studies [14], [35], [40].
In the Figure 2, we noticed that the relativistic apparent Doppler is predominant for angles greater than 41º. The greater the angle of incidence, the greater the displacement of the image, which implies that the displacement time will be greater since the apparent relative velocity is independent of the angular position, but of the refringence, for both references. In this sense the time is relativistically dilated, with greater effect for large angles, where considering equations (24) and (25), we can write: where, in the perspective of the source's referential, the position of the image moves in an interval: Eq. (35) demonstrates that as the angle of incidence increases, time dilation becomes purely relativistic in the perception of the source referential. It can be seen that for angles of incidence up to 41º, the time is contracted in the perception of the source referential, expanding if for larger angles until the next synchronization as will be discussed in Figure 4, which implies a delay in the relativistic trajectory: Although the last relativistic analyzes took place in the perception of the source referential, the fact that both can describe apparent positions, we could obtain the same results adopting the other observer, in the perspective of the apparent position of the source.
The Doppler characterized in eq. (33) for distant media, it can be confused with other Dopplers if the only criterion is the wavelength shift or redshift. In astronomy, an Apparent Doppler can lead to inaccurate distances and velocities of systems or stars. The solution is to differentiate the effects that are in the frequency domain from those that are in the wavelength domain. In the analyzes conducted [12] over the gravitational and cosmological redshifts a Z CEF balance was suggested which weighs the different effects capable and liable on the trajectory of perform shifting the wavelength of light.

RELATIVISTIC ENERGY WAVE (REW)
The analysis conducted by Bhaduri et. al [6], which deals with space-time refraction (ST) reveal that in the transition between two media there will be a wave package that crosses the In the representation of refraction by ST waves [6], the angular treatment is in relation to spectral plane tilt, however, when we are dealing here with a single photon, in the absence of a spectral plane, the inclination of the spectrum coincides with the angle of incidence of the photon, where we can conduct an analogous analysis weighing all the differences between the two descriptions. Figure 4 presents the behavior of REW where the estimate of the angles of refraction is verified, according to eq. (24), in a spectrum of angles of incidence. It was not found for a single photon, anomalies presented by Bhaduri et al.
[6] where θ 2 > θ 1 in n 2 > n 1 , of which the authors associated the anomalies with group velocities and not with trajectories.
According to Kondaksi et al. [29], the ST waves feature acceleration of wave packets in air.
The results presented here demonstrate that there are delays, synchronization, and advances between the clocks in the source and observer references. The REW wave characterizes the variability of time dilations, momentum and wavelength displacement, which can be seen in the results presented in the Figures 2 and 4, that the relativistic momentum of Minkowski shown here, by itself, is not able to compensate for delays as the compensation depends on the angle of incidence.
Checking the distance independency of source-observer synchronizations, as shown in Figure 4, it appears that the wave packets characterized by REW are able to connect source-receiver synchronously, precisely when the classical and relativistic trajectories overlap. The Snell-Descartes Law is not able to represent the behavior of data for large angles, as well as do not lay down a connection where delays are null between source-receiver, as predicted [6].
In the Figure 4, it is verified that the classical model given by eq. (25) which agrees with the Snell-Descates Law for small angles has a greater representation of the data behavior up to approximately 41º of incidence, while the REW is delayed. The synchronization points demarcate the delay-advance inversion of the clock in the source referential, where the REW agrees with the classic model of eq. (25), but with the increase in the incidence angle, the photon starts to describe a relativistic trajectory with an advance of the clock in the reference of the source. For angles of incidence greater than 100º, the relativistic deformation is close to the classic deformation, where the clock in the reference of the source is slower and after synchronization the REW is delayed again, for large angles of incidence.
Although comparative analysis between ST and REW waves, we must consider that they deal with different refractions, in part. REW deals with refraction considering the actual trajectories of the wave packet, not finding any anomalies like those found in ST waves. The refraction anomalies found through ST waves are anomalies associated with group velocities within the scope of geometry adopted for the wave packet according to the authors [6], found in relation to the inclination of the spectral plane characteristic of the authors' approach.
In the Figure 5 the REW lag and lead zones are presented, as well as the refraction synchronizations for different pairs of media. For both pairs, in the incidence sloped in relation to normal, the delay is explained by the perception of time in the referential of the source and with the increase of the incidence slope, the source-observer synchronization/desynchronization occurs. In air the REW has no delay, except for slopes slightly close to normal. One might ponder that the relation of which we deal with the delay, eq. (36) is different from that treated in the studies discussed here [6], [33] and [46], as the authors divide the observation between before and after the separating surface, considering that the pulses will travel equal distances. In this study the delays presented by eq. (36) are independent of the source/observer distances in relation to the surface and consider the total sufficient time for the observer/source to perceive the source/observer.

CONSERVATION OF ENERGY IN ANGULAR ORBITAL MOMENTUM (OAM)
A photon or a very large number of photons passing through different media in a process where there is a shift in wavelength, keeping the frequency constant, will conserve energy in some form of movement. We show in eq.(s) (19) and (20) that the decrease of energy in the transition between two media is conserved in OAM, one characterized by Abraham's and the other by Minkowski, where we started to verify the variation of these momenta as a function of the angle of incidence.
Considering that the Abraham and Minkowski torques elapse during the delay interval, we can express the variation of the OAM from the perspective of the source's referential given by: In the Figure 6, it can be seen from eq.  The OAM variation signature shown in the Figure 6 is characteristic of its variability as treated by other authors [37], [25]. The intensities found in this study are small, whereas in this theoretical perspective the pulse is not previously modulated.
The variation of the OAM as a function of the angle of incidence characterized in the Figure   6 features new modulations. OAM modes are widely applied in quantum computing and information [11].
The conservation of photon mechanical energy in orbital angular movement discussed in this study, in agreement with Cardoso [13], [12], [10], describes a natural OAM of the photonmatter interaction, far from the perspective of artificial modulators. Recently, studies showed preliminary results of the OAM of photons emitted by natural sources [45] and theoretical and experimental results characterize the natural OAM(s) of ejection and photon-matter interaction, either by scattering [28].

CONCLUSIONS
It can be concluded in this study that the photon, when transiting between two media is subject to two non-additive torques, a classic associated with the Abraham momentum and a relativistic one characterized by the Minkowski momentum. The determination of the photon trajectory as classical or relativistic is a function of the incidence angle and the pair of refractive media, where the relativistic trajectory appears with delays.
The photon's energetic decrease, in the transition between two media, conditions the photon to Abraham's momentum, but also to a relativistic dynamic. Although it does not enjoy its common velocity in a vacuum, it moves at a velocity close to c, becoming a relativistic particle where its momentum and wavelength shift are dilated and the photon finds itself in a new state of movement, described by momentum of Minkowski, characterizing the momentum of Abraham as the hidden momentum of the relativistic momentum of Minkowski, while it appears as a relativistic photon ignition device.
An Apparent Doppler was found for a system where the source and observer are fixed, where the photon velocity in the refringent media characterizes the apparent relative velocity between source and observer, characterizing a Doppler effect for a constant frequency system, with wavelength shift.
The REW appears with a certain delay depending on the angle of incidence and the pair of media involved in the refraction scenario. In an analogue with ST waves, it was able to predict synchronization points between source and observer. The synchronization instants demarcate the alternations between REW delays and advances and also the agreement between classical and relativistic description.
The conservation of the photon's mechanical energy in Orbital Angular Momentum indicates negligible variations while the REW presents delays and advances, inversion of the direction of the OAM in synchronization, indicating that the variations in the determination while classical or relativistic trajectories, is preceded by an inversion of the OAM. These OAM variations depend on the pair of media involved and the angle of incidence and may characterize new modulations for computation and quantum information.

INDICATION OF POSSIBILITIES FOR FUTURE STUDIES
Considering that the astigmatic behavior of light in refraction processes are acquaintances [4], [41], dealing with OAM-structured waves, where the pulse incident on a flat surface of a second refractive medium will present two contributions, one wave traveling the real path of the refracted beam and another local wave which has a path very close to the real path, although the slope relative to normal is slightly higher.
As well as, considering that in agreement with Gui et al. [26], an OAM -ST carrier pulse, second harmonic (l = 2) is distorted when being generated and propagated in crystals, associated with an ST astigmatism, consistent with the conservation of transverse OAM.
A study is suggested to verify the models dealt with in the present study, from the perspective of a pulse with AOM, where the astigmatic effect can be characterized by classical and relativistic trajectories determined by eq.(s) (24) and (25).