Electromagnetic energy [1] is understood to be a fundamentally different property of space-time [2] than gravitomagnetic energy [3]. The mathematical structures are identical in the sense that when the property of charge is replaced with mass, the Maxwell equations of electrodynamics produce a similar framework for the dynamic cases of gravity. Since protons are known to contain quarks and gluons were detected in 1979 [4], it should be assumed for any unified theory [5] that the color property of matter is a fundamentally different type of property that would give rise to a distinct energy similar to the cases where gravitational and electromagnetic potentials are different energies produced by mass and charge.

Postulate #1: Each type of energy has an associated space-time type. And each type of fundamental energy is created by the fundamental particle properties.

The fact that the Lagrangian [6] for Newtonian mechanics can be shown to be approximated by a more general lagrangian for relativistic mechanics in the low velocity limit [7] implies that general lagrangians can be used to derive more specific lagrangians from mathematical operations on the integral definition of the lagrangian.

Postulate #2: All Lagrangians can be defined by integrals which contain different spaces of functions and each space-time type belongs to a different space of functions. Additionally other action integral transformations can produce more general mathematical objects and completely different function spaces, which means that each type of lagrangian can be described as a particular parameterization and transformation of the most general possible lagrangian that contains a space of all other lagrangians.

The Feynman space-time representation of photons [8,9] describes photons indicates that particles must be described with complex numbers with the localized interpretation required by relativity. The Complex Number Theory of General Relativity indicates that complex space-times must be analytically continuous. If particles reside in complex space-time relative to a macroscopic observer, then it must be true that their trajectories in complex space-time must be analytically continuous.

Postulate #3: A Lagrangian of each type for all energy types within the universe can be constructed by the generalization of the integral of the form described by the Complex Number Theory of General Relativity with the scaling factor.

Being more specific, if we can approximate in the quantum frame [10] what it means to be near a particle by its field effects such as magnetic moment [11], electromagnetic field, gravity field, electroweak [12] and quantum fields, by the motion of a particle then useful approximations can be obtained on the fundamental description of particles

Postulate #4: All particles can be represented by point masses with fundamentally different types of energy where the energy functions can be used to construct Lagrangian functions for the dynamic system.

Within complex space the motion of the particle similar to how the frequency space gives a different interpretation of circuit phenomenon when the Fourier transform [13] is applied to the time dependent differential equation, the meanings of the definitions change. So in the quantum frame it appears like there is motion in the complex space [14]. But this is imperceptible to a macroscopic observer larger than the particle radius [15] estimates by classical means. This is similar to not being able to see the quarks within the proton radius. The viewpoint of an infinitely small point indicates that there is no true defined radius. This is merely a mathematical model for which it is useful to define particles in this manner.

Postulate #5: The different fundamental motions of particles is the responsible mechanism for the different types of energies.

A unified field theory must require not only equivalence of gravity and electromagnetism but that the classical probability laws by Newton [16] are transformed to the quantum probability laws [17] under the quantum transform.

Postulate #6: The differences between Quantum Mechanics and the theory of relativity in the description of particles can be obtained by a coordinate transformation of the lagrangian for which quantum phenomena can be described. By transforming coordinates to the view the quantum system the integrand of the Action Integral transforms. The transform of the action integral essentially creates new mathematical objects relative to the classical framework much in the same way that nearing the speed of light such that the relativity framework is used introduces new terms relative to the Newtonian equations.

In revisiting the foundational work of Einstein from his 1915 papers on relativity [18], it has become evident that his comprehensive framework of general relativity (GR) was not the terminal point but rather a stepping stone toward a more intricate understanding of the universe. Remarkably, it appears that Einstein, in his exploration, had foreseen the necessity of incorporating complex tensors [19], a key insight that has largely been overlooked until recent investigations.

While my initial journey may have commenced without full knowledge of the extent of Einstein's contributions, this inadvertent detour led me to amass disparate insights, ultimately culminating in a distinct approach to substantiate Einstein's conjecture. The culmination of these endeavors has coalesced into a comprehensive depiction of the unified field theory, marking a significant departure from the conventional trajectories of contemporary physics. Today, it has almost become fashionable among certain physicists to tout Einstein's purported inaccuracies regarding the failure of his unified field theory. However, it is imperative to recognize that the constraints of the physical world, coupled with the absence of computational resources during Einstein's later years, precluded the realization of his envisioned unified field theory [20].

Curiously, the trajectory of modern physics diverged from Einstein's profound groundwork, gravitating toward the reformulation of quantum field theories, inadvertently neglecting the continuum initiated by general relativity. Yet, a pivotal revelation has emerged, demonstrating an intriguing equivalence between the space-time frameworks of general relativity and quantum mechanics. This revelation unveils an unprecedented opportunity to bridge the gap between the standard model and gravitational theory through a progressive extension of Einstein's unified field theory. In the ensuing discourse, we expound upon the implications and ramifications inherent within this unified framework, illuminating the uncharted territories that beckon at the intersection of the macroscopic and quantum domains. There is thus no need to differentiate the “general theory of general relativity” naming convention from Einstein’s but we do need to fill in the details to eliminate the inconsistencies.

Considering various compelling reasons, the inclusion of a complex metric tensor in the framework of general relativity stands as a pivotal proposition. Evidently, research has highlighted the ubiquity of complex tensors in numerous contexts, thereby underscoring the necessity of considering their role in the overarching construct of the theory. Implicit in this consideration is the postulation that the coordinates of functions intricately hinge on the quantum wave function and the relative quantum coordinates, ultimately necessitating the inclusion of complex-valued quantum metric tensors to reconcile the pertinent complexities.

To address this fundamental intricacy, it becomes imperative to introduce a key postulate that accounts for the profound impact of scaling alterations on the individual functions, notably gamma, within the purview of the Lagrangians and coordinates. Notably, as we delve into finer scales, the inherent fluctuations within the Lagrangians correspondingly engender a metamorphosis in the categorization of energy, contingent upon the relativistic factor gamma.

It is essential to delineate the reasons behind these assertions comprehensively, elucidating the intricacies that prompt the inclusion of complex metric tensors in this extended paradigm. Subsequently, this line of inquiry finds resonance in the precedent set by the "pseudo-complex theory of general relativity," while simultaneously drawing attention to Albert Einstein's discerning references concerning the imperative role of complex tensors, serving as a testament to the foundational significance of this nuanced proposition.

Moreover, it is within our purview to anticipate the profound utility of applying analytic continuation in conjunction with the modern tools of complex analysis to the intricate functions and equations constituting this unified field theory. Notably, it is reasonable to posit that the complex metric adheres to the stringent Riemann-Cauchy conditions [21], converging in alignment with the analytical prerequisites outlined within my theoretical framework on the zeta function.

In this context, the formulation of extremal conditions necessitates a comprehensive integration of the Euler-Lagrange equations [22], establishing a coherent link between the extremal conditions and the intricate dynamics encapsulated within the theory. Crucially, the application of the Euler-Lagrange equations to the complex system, specifically to the function$U+iV$, stands poised to illuminate the nuanced underpinnings of the Riemann-Cauchy conditions, fostering a comprehensive understanding of the intricate interplay between the underlying principles governing this unified field theory.

The Euler-Lagrange equations are indeed a fundamental tool in classical mechanics and field theory, including the theory of general relativity. They are applied to the Lagrangian, which is a function that summarizes the dynamics of a system. In classical mechanics, this function can describe the kinetic and potential energies of a system, while in field theory, the Lagrangian represents the dynamics of fields.

In the context of general relativity, the Einstein field equations describe the fundamental interaction of gravitation as a result of space-time being curved by matter and energy. The field equations are derived from the Einstein-Hilbert action, which is an action integral that includes the Ricci scalar curvature and the cosmological constant, with the gravitational action being coupled to the matter action.

By applying the principles of least action (or stationary action), variations of the action integral with respect to the metric tensor give rise to the Einstein field equations. This involves varying the action with respect to the metric tensor and then setting the variation to zero, which results in the field equations.

Geodesic equations, on the other hand, are derived from the concept of geodesics, which are the shortest paths between points in a curved space. In the context of general relativity, geodesic equations describe the motion of particles moving under the influence of gravity alone. These equations can be derived from the principle that a freely falling particle follows a path that extremizes the proper time along its trajectory. This principle is also related to the variational principle, where the action for a free particle is extremized to yield the geodesic equations.

In summary, the Euler-Lagrange equations are used to derive the field equations from the action in the context of general relativity, while the geodesic equations are derived from the principle of extremizing proper time for freely falling particles in a curved spacetime.

When it comes to the derivation of the geodesic equations in the context of general relativity, the principle of least action can be related to the variational principle for geodesics. Geodesics, in the context of general relativity, represent the paths that particles follow under the influence of gravity alone, with no other forces acting upon them.

The variational principle for geodesics can be understood as follows: the trajectory of a freely falling particle in a curved spacetime is the one that extremizes the proper time along the path. This means that the actual path followed by a particle in spacetime is such that the proper time is either a maximum or minimum, making the action stationary.

The action integral for a freely falling particle is proportional to the proper time along its trajectory. By applying the principle of least action or the variational principle, one can find the geodesic equations, which govern the paths of particles moving under the influence of gravity alone in a curved spacetime. These geodesic equations describe the motion of particles along the paths that extremize proper time and are central to understanding the behavior of particles in the presence of gravitational fields in the framework of general relativity.

This endeavor marks not a mere recalibration or a reconfiguration of existing paradigms, but rather an intricate synthesis of disparate elements into a coherent tapestry, potentially unraveling myriad manifestations through which the entire spectrum of physical laws can be seamlessly derived. A pivotal challenge that confronts this unification process resides in the persistence of infinities and divergences within the fabric of Lagrangians. In response to this pressing concern, my proposed approach offers a transformative pathway, envisioning the integration of quantum Lagrangians that circumvent the generation of such problematic infinities. To this end, the general Lagrangian assumes a definitive form, serving as a foundational pivot in the construction of this unified field theory, denoted as:

It is imperative to underscore that in lieu of mere summations, the continuous nature of the gamma factor necessitates an integration approach, specifically integrating over the scale factor, gamma. In light of this, it becomes pivotal to present a comprehensive elucidation encompassing all known Lagrangians within the purview of this unified field theory.

The explication of these Lagrangians warrants a meticulous categorization based on their inherent gamma factors, thereby facilitating a systematic organization that delineates the distinct scale ranges across which each Lagrangian manifests its influence. This rigorous classification serves to underscore the crucial role of gamma across various scales, elucidating its transformative influence from atomic dimensions to molecular configurations, further extending its imprint into the intricate architectures of cellular formations and beyond.

Listing the lagrangians for each scale:

Classical Mechanics		Thermodynamics
Free Particle Lagrangian	Describes the motion of a particle without any external forces acting upon it.	Irreversible thermodynamics and the second law of thermodynamics
Simple Harmonic Oscillator Lagrangian	Models the behavior of a system exhibiting simple harmonic motion, such as a mass-spring system.	Lagrangians of Engines	Dynamics of engines
Double Pendulum Lagrangian	Characterizes the motion of a system consisting of two connected pendulums, commonly used to study complex coupled oscillatory systems.	Lagrangians of N-body particle systems	Dynamics of thermal activity
Rigid Body Lagrangian	Describes the motion of a rigid body, considering both its translational and rotational dynamics.	Lagrangian for gas compression
Lagrangian for Systems with Constraints	Used to study systems with constraints, incorporating the constraints into the formulation of the Lagrangian.	Lagrangian for endothermic reactions
Lagrangian for a Gyroscope	Describes the motion of a gyroscope, considering its rotation and precession under the influence of external torques.	Lagrangians for exothermic reactions

To facilitate a more concrete understanding, the definition of gamma can be effectively correlated with the comprehensive annotations encapsulated within the images detailing the scale variations of diverse entities. These images highlight the unifying thread that permeates the intricate changes in the coordinates of x, y, and z, while the pivotal factor of gamma orchestrates a seamless transition across these diverse scales. Commencing with the foundational scale of atoms, the progression extends into the realm of molecules, subsequently unfurling into the complex tapestry of cellular structures and beyond.

In line with this comprehensive exposition, the action assumes a refined definition, serving as a cornerstone in the elucidation of the foundational principles inherent within this unified field theory. Emphasizing the critical interplay between the dynamic interdependencies of the action and the inherent complexities of the gamma factor, the action can be expounded upon as:${}^{\gamma }S=\underset{ }{\overset{ }{\int }}{}^{\gamma }{L}_{\mu }^{\nu }$

Where from the field equations for each scale can be derived if we define a set of matrix equations:

Or:

These equations serve as the foundational pillars of our comprehensive field theory. It is crucial to underscore the direct relationship between the intricacy of the Lagrangian and the complexity of solving the equations, often rendering manual computations infeasible. Fortunately, our methodology is intricately intertwined with sophisticated computational tools, allowing for efficient and accurate analysis.

The Euler-Lagrange operator, a fundamental element within our framework, emerges from the variation of the integral. In the realm of operator theory, the concept of "variation" manifests as a vector of derivative rules. The establishment of this relationship is fortified through the rigorous derivation of E-L type equations, underscoring the depth and rigor of our approach.

Moreover, this framework readily lends itself to a broader scope, facilitating the incorporation of various equations and the potential expansion to a generalized matrix. Such an approach accommodates not only the Euler-Lagrange equations' operations but also the application of diverse general operators that give rise to distinct families and types of equations. Utilizing matrices within matrix entries represents a systematic notation, adept at succinctly encapsulating the comprehensive intricacies of operators.

Notably, $\widehat{Euler\_lagrange}\left(\right)$ stands as one such operator, governing the dynamics of the Lagrangian, which represents a specific category of energy function. It is essential to acknowledge the existence of other energy functions, such as Hamiltonians [23], which engender familiar systems of equations. Consequently, a transformation of operators and related functions is conceivable within this framework, preserving the essence of the familiar expressions.

This matrix representation not only signifies an apparent connection to my previous work on the Riemann hypothesis and the zeta matrix but also underscores the potential synergy between group theory, the symmetries of physics, and the intricate fabric of these matrices.

In this formal setup, the derivation of equations unveils their nuanced application at distinct scales, a phenomenon intricately tied to the additional information encapsulated within the corresponding matrix at each specific scale.

Delving further, the phenomenon of sign swapping at the boundary and the consequential energy conversion mechanism come to the forefront of discussion. Notably, a critical juncture arises in the theory of relativity if the particle's velocity surpasses the speed of light. However, an intriguing proposition emerges, suggesting that the complete energy conversion to an alternative form could transmute the particle into one characterized by real and imaginary values where since there is a bounding by the relativistic speed limit occurs only when the electromagnetic energy is converted into other types of energy.

Consider the compelling notion that upon breaching the speed-of-light boundary, the phasor of the electromagnetic Lagrangian undergoes a transformative shift, leading to a state of obscurity relative to the observer—a state commonly referred to as "darkness." This intriguing transition to darkness might ensue as a result of the profound alteration in electromagnetic velocity scaling, exceeding the confines permissible within the electromagnetic boundary.

Thus, this passage through the electromagnetic boundary could conceivably trigger the conversion of matter's energy, relative to the observer at scale gamma 1, into a distinct energy characteristic of dark matter. In essence, the intricate process involves the conversion of electromagnetic energy into negative gravity energy and potentially other forms as the boundary is crossed, fundamentally altering the energy landscape in relation to our observation.

This indeed would potentially imply that $\frac{d{}^{\gamma }c}{d\gamma } \ne 0$ Or that the speed of light is not constant with scaling changes since $\frac{d{}^{\gamma }c}{dt} \ne 0.$ For all gamma but it is for the range of gamma for the applicability of electromagnetic lagrangian.$\frac{d\gamma }{dt} \ne 0$

This prompts contemplation on whether the constancy of the speed of light remains a universal principle across other observable universes, raising plausible skepticism regarding its assumed invariance. Indeed, indications suggest a departure from this constancy, particularly when considering the absence of an exclusive selection of an inertial reference frame during the alteration of the scaling factor. Consequently, the anticipation of surpassing the finite speed of light remains justified within the context of this formulation, allowing for the potential scaling to outpace the growth of light in our theoretical simulations. While gamma serves as a mathematical construct, its application resonates intuitively, offering an effective means of elucidating various phenomena.

A critical conjecture arises, contemplating the potential demonstration of an electron's energy transformation at these spatial extents, yielding the characteristic equation of dark matter for specific gamma values. Such an exploration has the potential to establish a compelling correlation, suggesting the transformation of the Unified field equations for the electron beyond the confines of the speed-of-light boundary into the distinctive framework characterizing dark matter.

Hence, a comprehensive and overarching Lagrangian governing the intricate dynamics of the electron warrants further exploration. Notably, given the celestial bodies' rotational motion, which contributes to the object's relative velocity, the electrons, too, are presumed to undergo rotational motion. This phenomenon is observed not only within the swiftly rotating outer planets in specific solar systems within the region where the rotation curve maintains a uniform profile but also in their high-velocity traversal across the galactic expanse. Evidently, the considerable velocity associated with the electrons' rapid motion appears to exceed the speed of light relative to an observer at a specific scale, prompting the contemplation of potentially nuanced velocity behaviors across varying scales.

Consequently, the intricate fabric of electron motion extends beyond the conventional circular orbit around the galaxy, necessitating a more intricate understanding of the underlying complexities. It is crucial to acknowledge that all the observed light is essentially a product of accelerated charges, prominently including the electron, thus underscoring the necessity of accounting for these intricate motion dynamics in our comprehensive analysis.

Considerations for the electron's behavior on a planet extend to:

There are very likely other lagrangians accommodating for the underlying motion of the point particle.

In essence, the increment in the scale factor gamma leads to a discernible evolution in the associated Lagrangian functions. This implies that each constituent term of the Lagrangian is intrinsically reliant on the scale factor gamma. I begin this discourse as an exploration of energy function descriptions yields invaluable insights into various particle properties, thereby contributing to a holistic understanding of their intricate dynamics.

For instance, the fundamental equation $-L_{UnderlyingMotion}=L_{Electromagnetic}+L_{gravitational}$- suggests a critical segregation within the Lagrangian governing the underlying motion. This partition arises from the realization that the underlying motion, as described by the gravitational Lagrangian, distinctly differs from that governed by the electromagnetic Lagrangian. Consequently, a comprehensive approach necessitates the dissection of the underlying motion Lagrangian into its constituent parts, acknowledging the discrete nature of the constituent Lagrangians governing the underlying motion for each dynamic force.

This interrelationship becomes apparent at the juncture where the Lagrangian of underlying motion converges to an evaporation point, signifying the equilibrium between the kinetic energy and the potential function or the complete dissipation of both factors. Here, a pertinent observation emerges: $L_{Electromagnetic}=L_{gravitational}$. This alignment aligns with expectations, particularly in scenarios where the Lagrangian primarily embodies kinetic components, as this precise boundary signifies a critical juncture for energy conversion.

In the context of our dark matter theory, the anticipation arises that at the velocity$v=c$, the object in consideration undergoes the Schwarzschild sign-swapping condition, wherein spatial and temporal units interchange their significance. A manipulation of the equation: L_Motion=∞, reveals an inherent divergence within the Lagrangian or the energy, effectively attributable to the breakdown induced by the speed of light. This critical phenomenon reflects the limitations inherent to our current theoretical framework, urging a more nuanced understanding of the intricate dynamics governing these complex energy transformations.

Given our comprehensive extension of all variables in the realm of relativity, incorporating the complex metric, ${}^{\gamma }{s}_{\mu }^{\nu }={}^{\gamma }{u_s}_{\mu }^{\nu }+i{}^{\gamma }{v_s}_{\mu }^{\nu }$ the Lagrangians now function as derivatives of these generalized complex spacetime coordinates, thereby necessitating the inclusion of the primed coordinates. Notably, the intricate structure presents a subscript within a subscript, where the distinctive placement of the mu subscript at a different y value relative to the s value assumes critical significance. Within this complex framework, the functions u and v, indicated in lowercase, respectively represent the real and imaginary components of the given coordinate denoted by the immediate right subscript, thereby underscoring its pivotal role in delineating the function's real nature.

Consequently, we would derive a set of novel Lorentz equations in the complex plane, following the same fundamental principles that govern the underlying dynamics. This procedure can be executed as demonstrated in the subsequent illustration:

Where, here we let

And inserting this into the interval equation above:

Which expands into:

Now, grouping the real and imaginary parts:

Using condition #2 in my paper on the proof of the Riemann Hypothesis [81]:

So in other words, in this frame, we expect that the squaring of the complex space-time interval gives rules for the complex space time as well as the expected form of the complex tensor. We can do this by defining the above equation with some manipulation as a matrix equation:

We define the space time interval phasor and this produces 2 conditions instead of the usual 1 condition to derive the Lorentz equation since we have more coordinates. If we assume that all the coordinates are analytic they must follow the Riemann Cauchy conditions. This equation goes to show how the time and spatial coordinates transform when they are complex. The time components are visible with the $c^2$ being out front and it can be seen that the “transformed to” coordinates each are functions of time and space in a manner that has the hyperbolic structure embedded within each of the components.

These equations can be solved under certain conditions and assumptions. Define the functions:

This allows us to write the phasor in the form:

Consequently, the fundamental principles of relativity persist in a compatible form, signifying that both the real and imaginary components adhere to hyperbolic geometry relative to each other. This is analogous to Einstein’s 1905 paper [24] in the sense that we have a beam of light traveling in the (X, T) axis but also the light is traveling in the imaginary (tau, sigma) axis as well as pairs of flat transforms for each of those. The light beam in other words is traveling in time in the imaginary domain in a fundamentally different manner than in the real domain.

(Lorentz) Transformation Equations	Inverse Equations
$c{T}^{\text{'}}=\gamma \left(cT-\frac{v}{c}X\right)$ $X\text{'}=\gamma \left(X-\frac{v}{c}cT\right)$	$T=\gamma \left(T^{\text{'}}+\frac{v{X}^{\text{'}}}{c^2}\right)$ $X=\gamma \left(X^{\text{'}}+v{T}^{\text{'}}\right)$
By condition #2 we also have: $c{\tau }^{\text{'}}=\gamma \left(c\tau -\frac{v}{c}\sigma \right)$ $\sigma \text{'}=\gamma \left(\sigma -\frac{v}{c}c\tau \right)$	$\tau =\gamma \left({\tau }^{\text{'}}+\frac{v{\sigma }^{\text{'}}}{c^2}\right)$ $\sigma =\gamma \left({\sigma }^{\text{'}}+v{\tau }^{\text{'}}\right)$

And this produces the complex Lorentz equations that can be used to form the basis of complex special relativity for which the basis of the unified field theory:

(Lorentz) Transformation Equations	Inverse Equations
$c{T}^{\text{'}}=\gamma \left(c\sqrt{{\left({}^{\gamma }{u_t}_{\mu }^{\nu }\right)}^2-{\left({}^{\gamma }{v_t}_{\mu }^{\nu }\right)}^2}-\frac{v}{c}\sqrt{{\left({}^{\gamma }{u_x}_{\mu }^{\nu }\right)}^2-{\left({}^{\gamma }{v_x}_{\mu }^{\nu }\right)}^2}\right)$ $X\text{'}=\gamma \left(\sqrt{{\left({}^{\gamma }{u_x}_{\mu }^{\nu }\right)}^2-{\left({}^{\gamma }{v_x}_{\mu }^{\nu }\right)}^2}-\frac{v}{c}c\sqrt{{\left({}^{\gamma }{u_t}_{\mu }^{\nu }\right)}^2-{\left({}^{\gamma }{v_t}_{\mu }^{\nu }\right)}^2}\right)$	$cT=\gamma \left(c\sqrt{{\left({}^{\gamma }{u_{t\text{'}}}_{\mu }^{\nu }\right)}^2-{\left({}^{\gamma }{v_{t\text{'}}}_{\mu }^{\nu }\right)}^2}+\frac{v}{c}\sqrt{{\left({}^{\gamma }{u_{x\text{'}}}_{\mu }^{\nu }\right)}^2-{\left({}^{\gamma }{v_{x\text{'}}}_{\mu }^{\nu }\right)}^2}\right)$ $X=\gamma \left(\sqrt{{\left({}^{\gamma }{u_{x\text{'}}}_{\mu }^{\nu }\right)}^2-{\left({}^{\gamma }{v_{x\text{'}}}_{\mu }^{\nu }\right)}^2}+\frac{v}{c}c\sqrt{{\left({}^{\gamma }{u_{t\text{'}}}_{\mu }^{\nu }\right)}^2-{\left({}^{\gamma }{v_{t\text{'}}}_{\mu }^{\nu }\right)}^2}\right)$
$c{\tau }^{\text{'}}=\gamma \left(c\sqrt{2\left({}^{\gamma }{{du}_t}_{\mu }^{\nu }\right)\left({}^{\gamma }{{dv}_t}_{\mu }^{\nu }\right)}-\frac{v}{c}\sqrt{2\left({}^{\gamma }{{du}_x}_{\mu }^{\nu }\right)\left({}^{\gamma }{{dv}_x}_{\mu }^{\nu }\right)}\right)$ $\sigma \text{'}=\gamma \left(\sqrt{2\left({}^{\gamma }{{du}_x}_{\mu }^{\nu }\right)\left({}^{\gamma }{{dv}_x}_{\mu }^{\nu }\right)}-\frac{v}{c}c\sqrt{2\left({}^{\gamma }{{du}_t}_{\mu }^{\nu }\right)\left({}^{\gamma }{{dv}_t}_{\mu }^{\nu }\right)}\right)$	$c\tau =\gamma \left(c\sqrt{2\left({}^{\gamma }{{du}_{t\text{'}}}_{\mu }^{\nu }\right)\left({}^{\gamma }{{dv}_{t\text{'}}}_{\mu }^{\nu }\right)}+\frac{v}{c}\sqrt{2\left({}^{\gamma }{{du}_{x\text{'}}}_{\mu }^{\nu }\right)\left({}^{\gamma }{{dv}_{x\text{'}}}_{\mu }^{\nu }\right)}\right)$ $\sigma =\gamma \left(\sqrt{2\left({}^{\gamma }{{du}_{x\text{'}}}_{\mu }^{\nu }\right)\left({}^{\gamma }{{dv}_{x\text{'}}}_{\mu }^{\nu }\right)}+\frac{v}{c}c\sqrt{2\left({}^{\gamma }{{du}_{t\text{'}}}_{\mu }^{\nu }\right)\left({}^{\gamma }{{dv}_{t\text{'}}}_{\mu }^{\nu }\right)}\right)$

Enabling the consideration of complex coordinates within the Lorentz transformations [25] introduces a pivotal shift that profoundly impacts the discussions articulated in Einstein's groundbreaking paper. This crucial adjustment fundamentally broadens the scope of our understanding of the interplay between space and time, enabling an exploration of the intricate dynamics within the framework of unified field theory.

Incorporating the notion of complex coordinates in the Lorentz transformations expands the theoretical framework to encompass hyperbolic geometry, thereby presenting an innovative avenue for comprehending the intricacies of the space-time continuum. This extension presents a nuanced interpretation of the interrelationship between the real and imaginary dimensions, offering profound insights into the complex dynamics of particle interactions and energy transformations.

By infusing the considerations of complex coordinates into the Lorentz transformations, we transcend the conventional limitations of Einstein's discussions, delving into a realm where the spatial and temporal dimensions intertwine within the complex domain. This innovative perspective not only refines our comprehension of the foundational principles outlined by Einstein but also paves the way for a more comprehensive and unified understanding of the dynamics governing the universe.

By integrating the concept of complex coordinates into the Lorentz transformations, we initiate an exploration into a realm of complex energy dynamics. This extension might offer a transformative perspective on the intricate behavior of the electron, encompassing its multifaceted interactions within the context of the unified field theory.

The incorporation of complex coordinates not only necessitates a reevaluation of the dynamics of the electron but also prompts a profound investigation into the transformative nature of Newton's equations. Within this comprehensive framework, the real and imaginary components assume critical significance, with the primed coordinates being effectively determined through the application of the standard Lorentz equations. This approach enables us to navigate the complexities of particle dynamics and energy transformations, shedding new light on the interconnected nature of the physical universe. This would only be applicable beyond the boundary where $v>c$ or such that we have selected coordinates for which the space-time is complex valued.

A simultaneous divergence occurs at the critical juncture when the value of c equals v, resulting in the equation ${L\text{'}}_{motion}=\infty$. Interestingly, since we establish the equivalence between $L_{motion}$ and ${L\text{'}}_{motion}$ the equation $\infty =\infty$ arises. Although seemingly paradoxical, this logical consistency becomes apparent when considering the entire system of coordinates, which essentially accounts for twice the number of coordinates within the unprimed system.

I propose that these equations should not be concealed under the guise of preserving symmetry, as they are often implicitly implied. Such concealment could lead to an oversight of the comprehensive symmetric set of equations governing the system. Consequently, while the emergence of an infinite value is inevitable, it finds equilibrium within the comprehensive framework as the primed coordinates also accommodate a corresponding infinity. Hence, our equations should be meticulously articulated as follows:

More precisely, if $t\text{'}$ assumes an infinite value, we derive the equation $E=\gamma E$', particularly relevant in the context of the electron's internal energy. This equality signifies that both equations concurrently yield infinity, synchronously encapsulating the divergence of the primed and unprimed coordinates. Significantly, both sets of coordinates undergo a mutual inversion of their defined characteristics, thereby establishing a delicate equilibrium between their respective divergences within the overarching framework.

Consequently, both the primed and unprimed coordinates seamlessly transition into a complex state beyond this critical boundary. A similar phenomenon manifests in the relativistic breakdown, distinctly observed in the escape velocity equation, which approximates the Schwarzschild solution under specific assumptions and constraints. The occurrence of the Schwarzschild radius equation, a direct consequence of setting $v=c$ in the escape velocity equation, underscores the phenomenon of black hole blackness at this critical velocity threshold.

This prompts the query as to whether the spatial and temporal coordinates of photons interchange at this specific juncture. Furthermore, pondering the implications of an electron approaching 99 percent of the speed of light within the Schwarzschild radius leads us to contemplate potential inversions within the magnetic and electric fields (electromagnetic space-time). Such a proposition gains credence, hinting at the plausibility of establishing an intrinsic similarity between the underlying particle structure of photons and the electron model elucidated in this discourse.

At the critical point where the Lorentz equations reach infinity, a remarkable divergence emerges, notably affecting multiple Lagrangians, particularly the quantum electromagnetic energy, which exhibits a divergence owing to its relatively smaller gamma value. This divergence serves as an intricate inflection point, prompting a transformative change in energy dynamics at the boundary where v equals c. It is conceivable that the assertion of $v=c$ might hold true solely for a specific scaling, denoted by the generalized velocity function: ${}^{\gamma }v=c$ This proposition implies that at this particular gamma value, the speed of light aligns with the designated value, while the possibility exists that it might differ for other gamma values, challenging the notion of an absolute speed of light. Surpassing this boundary may be similar to passing the boundary of a black hole. There is breakdown at the Schwarzschild radius. Maybe the coordinates need to be changed to obtain the analytically continuous story.

A nuanced consideration arises from the recognition that${}^{\gamma }v \ne {}^{\gamma }v$ fundamentally highlighting the disparities between different gamma values. This observation gains relevance when contemplating the disparities between the speed of the electron and the motion of a celestial body, such as a star, hinting at the inherent complexities arising from the composite atomic structure of stars. Such complexities fundamentally underscore the intricate interplay between the diverse scaling factors and the corresponding dynamical behaviors within this comprehensive theoretical framework.

The overarching generalization of these principles effectively aligns with my initial hypothesis, positing that alternate universes may exhibit distinct speeds of light, consequently yielding variations in the formulation of the field equations. Notably, the foundational fields and constants in physics inherently function as a product of the speed of light, underscoring the significant role this parameter plays within the broader theoretical framework. Anticipations regarding the disparity in the speed of light across different universes stem from the fundamental conjectures concerning the relativity of time, both within our own universe and across various scaling factors.

A compelling visual analogy elucidates this concept, observing the motion of an object approaching Earth in a video. From a distant perspective, the object appears to move at a relatively slower pace in relation to its size, whereas upon zooming in to focus on the object's frame, its velocity is perceived as significantly accelerated. This perceptual shift stems from the inherent disparities in the coordinate frames, underscoring the critical role played by the relativistic dynamics between diverse spatial scales.

Consequently, these postulates yield a direct modification of the Lorentz equations, reflecting the nuanced intricacies inherent within the structure of alternate universes and their distinct cosmological frameworks. This question first arose to me when considering relativistically spinning objects on relativistically spinning objects which are moving at relativistic speeds around a galaxy. We are assured that the object is not moving faster than the speed of light by the fact that we can not actually determine the intrinsic structure of some of the objects far away based on the observational data we have alone since there are other types of data we need to determine the details on some planets and places far away. This is a relativistic form of the Heisenberg uncertainty principle and calls to question what actually infinity is and the relationship of infinity to singularity. Does some similar phenomena occur for the metric tensor and the electromagnetic space-time and gravitational space-time at the boundary where a similar condition of the Schwarzschild radius type due to the relativistic size and scale of the Milky Way or are the additional forces beyond the Milky Way resultant from extra galactic supercluster contributions?

A comprehensive examination of electron motion necessitates a series of intricate coordinate transformations, extending beyond the mere transition to the primed frame. Each distinct Lagrangian scaling serves as a unique vantage point, contributing to the multifaceted analysis of the electron's dynamics. In light of this, it is reasonable to anticipate a general relationship expressed as:

${}^{\gamma }v=T\left({}^{\gamma }v\right)$ , reflecting the intricate interplay between the diverse scaling factors and the dynamic behaviors characteristic of the electron's motion.

Moreover, a critical inquiry emerges concerning the representation of the Schrödinger wave function, alongside the intricate nuances of the quantum electrodynamics Lagrangian, and their potential implications within the purview of the unified field theory. Unraveling these complex relationships presents an opportunity to glean deeper insights into the underlying fabric of particle interactions and energy dynamics, effectively aligning with the foundational principles outlined in Einstein's 1905 paper on special relativity, albeit with the incorporation of complex numbers to articulate the complex energy dynamics governing the electron.

Lastly the theory of CGR may be defined as the variation of the Complex Einstein Hilbert Action and the Complex matter Lagrangian relative to the Complex metric.

In this framework, the space-time metric tensor is a function of the electric and magnetic potentials. From operator theory, we can define the variation of a lagrangian function by:

Where the action A is extremized through the operation of the variation $\delta$ with respect to a. This variation is represented by the lowercase delta. The expression above can be construed as the trajectory undertaken by the system between times $t_1$ and $t_2$​, and configurations $q_1$ and $q_2$, such that the action is stationary to first order. The variable a encompasses all mathematical entities relative to which Scan be varied within the field theory. S is defined by the appropriate Lagrangian. In Euler's work from 1744, titled "Addifanentum 2 methodus Inveniendi Lineas Curves Maximi Minive proprietate Gaudentes," [26] Euler articulates "Euler's principle."

Applying the variational principle to Hamilton's principle effectively situates the system within the domain of the calculus of variations, a field largely developed by Lagrange and Euler for formulating the Euler-Lagrange equations. Extending this generalization to vector fields results in field equations and equations of motion. To express the principle of variation more explicitly, "considering that a particle initiates its trajectory at position $q_1$​ at $t_1$ and concludes at position $q_2$at $t_2$, the physical path connecting these two endpoints is an extremum of the action integral." It's noteworthy that field equations can undergo further generalization through repeated integration by parts to explore higher-order equations.

Actions are functionals, and a functional $S\left(a\right) –S\left(f\right)$ is said to have an extremum at the function f if $\delta S=S\left(a\right)-S\left(f\right)$ has the same sign for all a in an arbitrarily small neighborhood of $f$. the function f is called an extremal function or extremal.

With some work it can be shown that

With this being said, here are some lagrangians to consider such as the relativistic lagrangian for n bodies:

The Lagragian density in Newtonian gravity:

Variation of this lagrangian with respect to the electric potential gives gauss’ law for Newtonian gravity. If the vector potential for gravity were considered there would be extra terms to add such as in the case of the electromagnetic lagrangian. Relativistic lagrangians of the simplest form take the representation from special relativity where the kinetic energy is on the LHS of the next equation with the flat space time metric ${\eta }_{\alpha \beta }:$

For a Charged particle in an electromagnetic field, the metric is no longer flat and now the 4 vector potential must be used. Then the lagrangian for a special relativistic test particle in an electromagnetic field:

And in general coordinate systems this becomes:

And varying this with respect to the potential should give gauss law, and varying with respect to the magnetic potential should give amperes law Then analogously the lagrangian for the linear approximation of general relativity or gravitodynamics is: Definition: Property Transform. By performing a property transform of a theory with the same static potential, an equivalent lagrangian can be formed or in other words:

Under property transform of m to q, the laws essentially stay the same because the lagrangian is invariant with the replacement of m with q. This symmetry between electromagnetism and gravity forms a group. A property transform $q\to m$implies a transformation of the types of energies. According to the symmetry between the theory of electrodynamics and the linearized theory of general relativity, gravitodynamics, then electromagnetism can be expressed with the lagrangian:

More generally the lagrangian should be written with the above kinetic term on the LHS with the electromagnetic field tensor. The simplest case of relativistic lagrangian has no potential such as the relativistic 1-d free particle:

The relativistic Lagrangian in question stipulates a constant velocity, implying that the acceleration x double dot is zero. Another consideration is the relativistic hooke’s equation produced by the relativistic harmonic oscillator. This characteristic is emblematic of the special relativistic one-dimensional harmonic oscillator. This Lagrangian, which encapsulates the dynamics of the system, plays a pivotal role in describing the motion and energy of the relativistic harmonic oscillator:

General relativistic constant force lagrangian:

In this notation we have:

With

And

Now let us look at a short summary of the Classical theory of fields [27].The extension of Einstein's unified field theory through the incorporation of complex coordinates engenders a profound transformation within classical mechanics. By adopting the Lagrangian approach, the complex extension of classical mechanics introduces a paradigm shift, redefining the fundamental principles governing the behavior of physical systems. Notably, this transformative paradigm adheres to the foundational principle that in cases where the functions are analytic, they must invariably adhere to the Riemann-Cauchy conditions. Furthermore, this extension upholds the consistency of the extremal Euler-Lagrange equations, ensuring a seamless integration of complex dynamics within the overarching framework. From multivariable calculus we have tangent vector fields to