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Research Article
Open Access Peer-reviewed

The Intrinsic Derivation of the Hubble Constant H in Cosmology

T. G. M. Gerlitz
International Journal of Physics. 2024, 12(4), 147-163. DOI: 10.12691/ijp-12-4-3
Received May 25, 2024; Revised June 26, 2024; Accepted July 02, 2024

Abstract

A special relativistic procedure forms the basis of a theory for the exact derivation and detailed representation of the Hubble constant. The results allow statements to be made about the three cosmological topologies for a universe and a clear comparison of these types to one another. The result obtained is based exclusively on natural constants and shows the meaningful value in supporting experimental observations and their conclusions. From the extensive mathematical presentation a good understanding of the matter emerges including the amounts of distances between small and respective large masses in cosmos together with the associated time intervals. An imagined model is supplemented by the possibility of a negative, anti-universe. The phenomena in the difference topic to passive gravitational or respective heavy mass and inertial mass is discussed.

1. Introduction

In general, the universe is assumed be homogeneous and isotropic. This means the "tiny little dots" called galaxies and stars are evenly distributed in space. However, the universe or respective cosmos is subject to a certain kinematics and dynamics resulting in a non-static state being the theme of the present investigation. Such an idea is reinforced in the observations showing as an example the galaxies have no orientation in space whereby no direction or angle is distinguished as favored in their orientation in space.

An age of about 14 billion years is predicted from the Hubble' law via the constant 1, 2, 3. In form of that meaning at the current rate of expansion it takes a billion years for an unbound structure to grow in 7% in good agreement with the best-estimate of 13.8. Admittedly, this law does not match the speeds of the observable farest galaxies. As always with all fundamental constants, such as Λ, G, and h, the question of temporal constancy arises. In a certain way, the law is always confronted with the belief in a big bang, BBT, and many scientists cling on an 𝓐 and Ω, which corresponds to human experience. A deviation in real factors could mind rather than a few percent. Then, time-dependent Hubble parameter

(1)

descibes the expansion rate and is the time-dependent derivative of the scale factor. The today's value of this H parameter is designated the Hubble's constant

(2)

with the world age. The measured value of the H provides the initial condition for solving the Friedmann equations 4 entailed from

(3)

Further, the expansion history depends on the density of the universe, Ω corresponding to the ratio of the matter density to the critical density for a matter dominated universe,

and this depends on the distance,

(4)

Then, an "acceleration" curve shows the trajectory of the scale factor for a universe with dark energy. The ratio of the H parameter to today's value is given as the expansion factor and can also be determined based on the respective total density.This connection are the Friedmann's equations in general form 4 as a set of equations in physical cosmology governing the expansion of space in homogeneous and isotropic models of the universe within the context of general relativity 5. They base on the Einstein's field equations of gravitation for the Friedmann–Lemaître–Robertson–Walker, FLRW metric 6, 7, 8, 9,

(5)

yielding a perfect fluid with a given mass density ρ, and pressure p. The equations for negative spatial curvature were given, too 10. The above expressions show a series of constants which can be obtained or estimated in a very uncertain way, and rather require a simple theory allowing eventually more insights.

A uniformly expanding universe causes the objects be arranged along a straight line through the origin 2 and report linear relationship between the distance of galaxies (extragalactic nebula) and their redshifts 2, 3. The image of the object must be resolved so well no light from other objects distorts the measurement result. This becomes increasingly difficult as the distance increases. Data used in the first Hubble diagram reached out to a distance of about 2 Mpc. Almost a century later measurements up to around 700 Mpc are possible 11. This makes it possible to provide a much more reliable indication of the H. The homogeneous process of expansion, the Hubble flow, and H are measured in systematically recording the distance and apparent speed of astronomical objects in relation to an observer. Since these must be distant astronomical objects, the measurements are complex and subject to large uncertainties compared to other natural constants, i., e, the results very fragile. A large distance means – anticipating the theoretical part of the current investigation – a predominance of the centrifugal force, compared to a short distance, where the attractive force, becomes essentially weak,. The “point”where changetakes place separating the two properties affecting an m-element does not really happen in a discrete manner or respective through a jump. Such behavior would only correspond to idealizatio: it is rather fluidly and continuously. So it is not a true clear point rather smooth transition and does not happen suddenly. Therefore, the distinct spiral property in the near movementis not immediately a complete given up, more maintained in an increasingly weakened form until with increasing distance D or respective R,the trace of the movement asymptotically approaches the shape of a straight line (Figure 1).

Admittedly, the measurement results vary considerably and the most recent detected show

Since galaxies not follow cosmic expansion, alone but rather also show their own movements of typically several hundred km/s, many galaxies have to be examined over a sufficiently large-range distance separating the two effectsseparated in a strict border mentioned above (Figure 2). The speed caused from cosmic expansion and the cosmological red shift have different origins rather than a proper (Eigen-) velocity and the red or blue shift associated with it through the Doppler effect.

From datae of the Spitzer-Space Telescope based on observations in the 3.6 μm (mid-infrared) range to recalibrate the Cepheid distance scale 12 the 'Carnegie−Hubble Program' scientists obtained new and highly accurate values for H. This means to now determining more precisely in factor 3 analogus an uncertainty of only three percent 11,

(6)

Depending on the universe's content of normal (baryonic) matter, say dark matter and dark energy, the expansion can be delayed or accelerated, and there exists a relationship between a world timeor respective world age and the Hubble time, e. g., 13. The reciprocal

(7)

is called the Hubble's time, precisely

(8)

with

(9)

it would be equal to the age of the world of around 14 billion years concerning uniform expansion in an empty universe, i. e., the time that has passed since the Big Bang, BB. This results in a Hubble timeof 14.561 billion years while the actual world age zero is approximately 13.844 billion years 2.

In accordance to the Hubble's law the distance D is to be distinguished from the relative expansion in moving distances being the rate of change in scale factorit is mostly talked about this scaled expansion. Consistent with the BBT as the expansion of the universe slowed after the initial inflation and during the first billion years of its existence. Since then, the relative rate of expansion has increased. The explanation of this observed accelerated expansion was subject of actual research and has led to the concept of dark energy. The absolute expansion speed, in turn, continues to be slowed down from gravity and, according to the concept of dark energy asymptotically approaches a constant final value. Since galaxies not only follow cosmic expansion, but also show their own movements of typically several hundred km/s, many galaxies have to be examined over a sufficiently large range distance separating the two effects in centrifugal and attractive forces separated at strict border . (Figure 2).

In the local universe, i. e. over small distancescompared to the radius of the observable universethe Hubble constant is the proportionality constant of the approximately linear relationship between the distances D of galaxies and the redshifts measured from their spectra. Important here is consequently the consideration and determination of the critical point. The productis often approximately interpreted as the recession velocity in terms of the Doppler effect,. The exact relationship between cosmological redshift and distance is nonlinear and truly requires integration over the time course of the scale factor. Though, exact relationship between cosmological redshift and distance is nonlinear and requires integration over the time course of the scale factor good approximation within the quasi-linear-velocity part is possible 14, 15. In this, arguments regarding the speed of faster than light, superluminarity 16, 17 should not be ignored 18, (Figure 1).

It is true limit galaxies not follow cosmic expansion, alone: they rather show their own movements of typically several hundred km / s, e., g., their (eigen-) proper rotation 19. This obligues many galaxies be examine over a sufficiently large range of distances to separate the two effects. The cosmological red or respective blue shift differ from proper velocity, and a critical point be bolden between linear and non-linear description.

In physical cosmology dark energy, DE as a hypothetical form of energy permeatesall of space to become the most accepted explanation. In this regard, there are of course a number of important parameters those predominate when describing the expansion of the universe and, e., g., energy density and curvature are contributions to the overall evaluation in density leading to expressions as fractions of the critical density.Moreover, investigations claim the positive cosmologic constant delta is equivalent to DE with respect to the cold matter model, CDM. Some theories on expansion, even deal with superluminality and negative mass to find application due to DE and dark matter, DM; creation of matter is discussed on the question to the remain of in this leaving mass, ∆M 20. One approach to identification of DE is found in modifying Robertson-Walker spacetime 6 It was suggested pressure causes the spatial expansion, a theory referring to the Schwarzschild's metric allowing mathematical prove on an inversely proportional relationship between H and cosmic density 21. Another possibility is found on the completeness given from comparison of shrinkage vice versa expansion 22. With the option part you can also make statements, at least approximately, about the parameters mentioned 21.

From unifying gravity and electromagnetism an investigation suggested a concept entailed from redshifts conected to the Planck's h changeble over time. It was shown the magnitude of h increases with increasing cosmic time as this quantum of enrgy gradually increases as well during cosmic evolution. From indepth formalism the dependence of H0 to h (t) becomes evident and related to a rotating universe 23, and compare the results could manifest agreement with experimental observations 24. In this paper the H constant could be shown emerged from the finestructure constant α. This is a very profound statement, as it could also lead to gravitoelectromagnetism, GEM.

As a consequence the experimental results are subject to great uncertainty, the desire arises for a plausible, clearly understandable, yet comprehensive theory and becomes the task of the current work.

2. Theory

1. General considerations and facts about geometry

In spacetime nothing is at rest, in accordance to the uncertainty in quantum mechanics, QM 25, 26 It should be mentioned according to the findings from the Lambda cold dark matter, ΛCDM theory the universe is assumed be globally flat (Ω ≳ 1), argably uncurved with infinite extension e., g., 27, 28 This does not result in any contradiction to the current work as not ignoring spherical distribution; justification will rather become obvious throughout the text in theory. The conditions are presented applying to a space using quasi introductory elements as this comes closer to understanding.

An initial idea of the assumed spherically symmetric distribution of mass, m respective M in the cosmos is well comparable to the spherical propagation of ions located around an electrically charged center in an electrochemical model 29: in particular, the ions near the center are subject to the attraction of the central ion, whereas the bodies seem to experience repulsion as the distance R from the center increases. An analogue to gravitational attraction and centrifugal forces can be seen here. A description of the location of the mass objects m, which do not change internally and are initially assumed be constant 30, obeys mathematically spherical coordinates (Figure 3, Figure 4).

In the work presented here space is handled 3-dimensionally in Cartesian coordinates. A later orientation of the universe within a 5-dimensional hyperspace 31 will just be discussed later. The direction of observation is the x- direction, driving forces basically go back to y and z. In spite of all a 3-dimensional overall space, first is assumed the calculation essentially take place in the x − y plane or, equivalently x − z (Figure 4). All the vector compounts in y and z render the fundamental in determining the variables radius r, active mass m, velocity υ , and angle velocity ω . It should also be noted the velocity or dealed speed υ appears in vector character clearly to obeye when and where its components occur. All of these variables are linked to one another.

As will be explained below, a negative space relates to a positive space exactly transposed-conjugated, not just mirrored. So the fraction in the first case contradicts the (usual) product in the second, as will become clear further below (Figure 5).

From both approximations termed week-field and slow-motion the Einstein's Field Equations, EFE reduce to the Newton's gravitation law to determine this G in the EFE, e., g., 32. In the present theory consequently, the conditions in this aspect are already simplified to fields occuring very low as are the velocities from the outset due to the initial condition.. If the conditions in real space exhibiting both very large distances and tremendous M had been assumed immediately, this simplified form would not be considered true. It is true the entire system seems unreal and too simple, but immediately provides insight into degree and amount of the variables to allow later transfer to the real cosmic system. It is noted parenthetically the present study can completely sufficient be based on Cartesian coordinates, which in a simple sense is already justified from the appearing small angles themselves.

2. Principles of the model

Figuratively speaking the central event is a disk rotating at angular velocity ω on which, at the beginning there is a mass, m element attached (Figure 6, Figure 7). As the object rotates, this object slides more and more outwards on the disk due to the centrifugal force acting on it. Finally, the influence of the attractive force on the disk decreases until it fades and is replaced from the centrifugal force increasing with rising distance r from the center (Figure 7). This is neither a complete disappearance of the first force nor the complete and exclusive predominance of the second (lat.: natura non facit saltus). Both forces remain, they are omnipresent in weaker or stronger. At the critical point of transition, there is no strict, abrupt end of one and the beginning of the other but rather continuous and flowing change, merely sometimes one wins over the other (Figure 8).

The opening of the mathematical process seems bit strange, but it will become clear, immediately. For describtion of a space like the universe five variables are necessary. These are the radius r, R connected to diameter d, D, mass m, M, velocity υ of any object in space, and the angular or circular velocity ω of the entire system. Further, the real cosmos certainly reveals flat curvature (Ω ≳ 1) 33 and a, then 2-dimensional representation of the real universe in Cartesian coordinates coming into question here is sufficient and does not need be justified. Albeit, the cosmos claims flat in its manifestation the entire treatment should always be universal. A spherical system with positive curvature (Ω < 1) as a general result poses difficulties with regard to the variables in this open system obliging the calculation begin with a closed (Ω > 1) anti- respective nega-verse 31 as exhaustively discussed elsewhere for a spatial distribution of negative curvature, e., g., 9, 10, 28, 33, 35.

A closed space can be compared to the size of subjets in atomic range exposing the feature be stabile in figure. Thisoffers the advantage determine its r contrasting the description of open and not necessarily stable spaces keeping free to expansion.

A stable and unchanging state is of course possible as well in open systems restrictedly appearing between the two mechanical forces attractive and centrifugal exactly at the point, alone. A transition occurs smoothly and continuously, not abruptly in a regular replacement of one force by the other. Here, both forces are omnipresent and must always be included at the same time, even if as the distance from the observer increases andpredominates to a large extent whilefades into the background, so to speak . This is obviously an important boundary between non-linear and quasi-linear behavior (Figure 1) in the (experimental) measurement of distances between two m or M from each other using redshifts. Thereupon, direct determination of the as required for the calculation of type open in its geometry, such as that of the universe, is difficult and limited to uncertain measurements or even estimates. For clarification be emphasized a nega-verse is directed inward with a vectorcorrectly located and ending at its "center" of this hyperbolic space (Figure 9), even if it sounds strange. The opposite is true for a posi-verse be mind in detail during treatment 26. A way across negative space is argued the only possibility for exact working, alone. Following these remarks, the attention will, first be turned to this mini-structure with r and the acquired expressions will then be transferred via reversal process into the “larger” space R, the universe. It is, then a reverse "inside-out". In the view of the above indices should be noted, as will become clear further down in the text, this index mentioned it is not exactly the outermost spherical shell in positive space being compared; it is rather the photon radius used for work on the technique (Figure 9).

3. Mass m in small space r

Given the entitlement of the present task an m is sought which can, if possible, be introduced without the help of existing quantities other than natural constants. Such a foundation is achieved from comparing the elementary electric charge e to a gravitational elementary m, .

A first approach is to generate a gravitational m via comparing to electrostatics. As a consequence of this finding and especially with regard to the gravitational interactions discussed here, an altercation of the two phenomenae mentioned is desirable as they depend mutually on each other. First step is an equating of the interaction forces in the Newton's law 36 disclosing

(10)
(11)

to finally show the gravito-electrostatic m value non-relativistic at rest of absolute amount

in arbitrary direction.

An almost infinitesimal small value of a subjet m can, of course, never compete or respective compared to an M within a theory dealing with interactions of entire galaxies demonstating their tremendous huge properties in a "usual" real cosmos (posi-verse). This ascertainment takes up that fact mentioned at the beginning and leads over to the ensuing section processing huge M located in a vaste space with almost infinite radii r and diameters d in the small (Figure 9, Figure 10). Clear, the r in the anti- or nega-verse is directed inwards, i., e. is negative, whereas the positive R in the real posi-verse points outwards labeling extremae and . As long as is truly kept about 1 to 2 percent below c it is essentially obvious the classical and non-relativistic m can be used (Figure 10, Figure 11). Throughout the theory applies CPT.

Clear, use in any calculation with subject electrodynmics care will be taken with respect to eventual shielding, but such anshould representatively denote the two m gravitationally interacting with each other. In the case the limit speeds are not reached their decisive effect as universal fades and the model is negated the reason, among other things separate consideration of υ is excluded finally or accentuated in other ways. The term incorporates the gravitational constant in 37, strictly speaking, actually belongs to any m itself. If there appears no counter-m in the space under consideration, i., e.,is unaccompanied it will show no weight,. If "rest" is canceled by an accelerated movement the m is identified inertia (see below). Light as electromagnetic wave, EMW exists through its movement, alone,

(12)

with variables and constants unveiling vector characters.

In view of a "turn over" via reverse small m into large M a problem arises. Due to the transition from extremely tiny dimensions to an actually enormously large space, simply making use of the principle in mathematical reciprocal of the above result, in a first view could never lead to a consistent result. Of course, such consideration is apposite in some aspects, but rather requires clear comparison. More, some kind of dimensionless transformation should expediently take place.

So, 5 variables are linked to each other, and a statement cannot be made independently be free. A first step is therefore taken to work out a reliable, real radius for a (mini-) nega-cosmos. Due to the later reverse process, the mini-universe into the real one, the m will of course also change significantly 38

4. Elements for the small radius r touching the angular frequency ω

or also angular speed. As mentioned above, all variables in the model are linked to one another. In contrast to the last statements these two subjetcs cannot be treated independently in separation of each other. In this section rotation of an entire small object comes to the fore introduced before as an anti- or nega-verse. In perception one m runs alternating between the two states Bradyon B and Tachyon T also an EMW as light can be descrived 39. Decisive are the two ought to match these limit speeds (Figure 10)

(13)

40, 41 confirmed experimentally, e. g., 37, 38, 39, 40 originated

(14)

fundamental for discussion of the kinetics in space (Figure 10) 16, 17, 40, 41. Then, the idea is directed to an object m descriptive a track around circumpherencing with a fictitious center, the required υ near close c. The latter formula is an unconditional requirement for the system to strictly be adhered, which is why a path

(15)

and at the same time a bring-forth distance d repective r should be precisely defined. This is in order to fulfill the conditions allowing to later make a correct statement about this effect and its influence on what is happening. Such an intended project is complicated in terms of the twoand of each other regarding the space circle (Figure 10). The distances to the fictitious center are certainly not clearly distinguishable, sincemoves faster thanto evoke

(16)

At this point be emphasized once again this model is the description of the movement of a single, albeit real and not "artificial as in EMW" 39, m breaking up into a pair of twins

(17)

due to the special effect used here 16, 17. Both m in this idea result 'per se' from one single

(18)

intrinsically, alone changing in state between sub- and superluminal and only exists when in motion respective directly bordering their critical speed limits − similar to a light wave. If these two twins, twin , be avoided here, were to meet, it would mean mutual annihilation to void − not even a death cry would be the result,

(19)

For safe description of the situation is emphasizedand to not describe a steady state from the outset, because the distances to their center are different for bradyon, B and tachyon, T from their unique orbit s they belong to (Figure 11). The original two m are of opposite sign demonstrate still and always the same absolute amount. Consequently, the absolute amounts m remain constant keeping the same amount while the two r separately refer to distances feeding in adjustment. Both options underwrite the same 31, 39, 46, 47. It has to be respected precisely as is the key for the orbiting m drawing a route s in its only path connected to r in question. Special about the twin couple is the two partners are always of the same absolute amount as a result of the basis statement: if one object changes in any way, the other will change to exactly the same extent, the mirroring appears 16, 17, valid in case of no tricky and awkward influences. Such a statement is limited, strictly speaking it applies exclusively to systems be undisturbed from the outside. This is generally true for external influences in the sense of other m-objects, i., e., in the view of the real universe strong impact from neighboring galaxies "left and right" of the observation line. Such a disturbance from outside this measurement direction can confidently ignore this because of the enormous effect on the current system considered to later become obvious. Since a realpemanentlly exists for any , their being is not the consequence due to the fundamentals of the relativistic derivation to the uniformly the same orbital speed: the reverse is proper, and the, themselves have not be relativistically adjusted as a consequence of their fast, say . This has already been indicated above via the factor α [40, 41] 40, 41 turning up

(20)

only to become important when considering distances exceeding the Hubble limit (Figure 1, Figure 2),

(21)

The theory is only correct if can be achieved, mean the respective maximum (limit) must be true and perpetuated. As fact, this section concerned with finding and defining a location where these conditions are fully met, and this can never be merely estimated because of the demands; it is the only requirement in the model together the extremely achievable proposed for this. Parenthetically, it is important to have clear indexing in order to draw attention to the facts and not to increase confusion in the text. A bradyon, for example, can move at 10 km / h or not at all, but this means it has reached a υ but still far from reaching a limit speed.

5. Indepth assessment of r

Crucial is the finding a concise place as the boundary of the (two) space models. It is conclusive this point be concluded for two reasons: the first is the predicted shrinking respective expansion, in which the universe, (Figure 10, Figure 11) under consideration ultimately expands at almost the speed of light, that is, from which the limit is to be determined; the other is, to a certain extent, the reversal of the first, namely this limit point of expansion is again reliably determined from the first-mentioned maximum speeds . Both arguments are for that linked to one another, certainly well founded for justification of this decision.

Including the balance as "weighting" the distance d between the two objects on their conjointly spherical orbit 31, 39, (Figure 12, Figure 13, Figure 14) is

(22)

From replacing the highlighted variables those separate the event per the above relations and yields with

(23)

still undetermined, since no m.

So far the principle for a perfectly spherical system, and now a suitable m must be chosen. Such a project once again requires a precise decision among the possible values for it, which is why the possible options are given. In order to achieve the actual numerical value a first attempt is using classical Newton's laws of gravity. It is, hence (Figure 12)

(24)
(25)

(Figure 12). These two expressions describe two forms of forces emphasizing m enters into the first equation only once, its "counterpart" is formed from rotation. Both formulae must be taken into account together within one representation alone, mind the equation of the attractive force, although receding at high speeds, is omnipresent. The word omnipresent points out with anthe contribution of the one force does not suddenly disappear but rather is completely always incorporated together with the influence of the other. A comparison in equate

(26)

permits non-vectorial notation. Since this υ is is related to the circumpherence s the factor (2 π) must be included. When calculated the result it opens up several possibilities for insight into the model, now keeping in mind the comments on the hyporbolic character (Figure 5),

(27)

with . It is, first

(28)

Due to the theory of the υ 16, 17, m remains unaffected in terms of magnitude, since this is already taken into account relativistically, whereas r must be adjusted to a relativistic basis in this sense (Figure 11),

(29)

manifying a perfect and flawless sphere or circle, why this demonstrates the only determining point for a perfect reflection of the angular speed or rotation ω of the space under consideration. This can be referred to as the influence "just outside the spinning disk" (Figure 6, Figure 7), say not adhering at least mat on it. The property as kinetic force is generally higher compared to the pure and static attractive one; it occurs precisely at this point the two twin m should fulfill exactly the conditions stated, more expressly required, and exclusively at this point. The force due to rotation, then applies further in and further out. The space under consideration is very clearly transferred from one ellipsoid to another ellipsoid, with the first appearing to be compressed and squeezed in the x direction from gravitational attraction, whereas initially both effects seem to cancel out at the critical distance. After that, now the cetrifugal force also creates an ellipsoid but appearing squeezed in y-z direction (Figure 13). In addition, in order to be complete, it should not go unmentioned a strong relativistic effect then, is very fragile when viewed.

After this interim result for the (mini-) nega-verse, which is reminiscent of atomic sizes, the ongoing investigation turns to the

6. Real dimensions in the universe

From a mathematical point of view the entire investigation is not complicated, but a precise and in-depth observation, even figuratively speaking, is somewhat demanding; in this sense, knowledge about black holes may be important 48, 49.

The mathematical derivation of an idealized Hubble's law for a uniformly expanding universe is fairly an elementary theorem of 3-dimensional Cartesian coordinate space considered a metric space. If assumed properties did not vary with location or respective direction it would be entirely homogeneous and isotropic. This not exactly hold true, albeit the results at very long distances correspond to good approximations. Before the implementation, which basically refers to philosophical aspects and is quasi-provoking in relation to large stretches, is discussed in more detail at this point, reference should be made to the discussion part; this is squarely indicated to say.

In mental imagination the innermost point, the centre as place of the observer in the real, i. e., posi-verse of, initially simplified, spherical shape (Ω > 1) touches the "outermost" place of the anti- or nega-verse of hyperbolic shape (Ω < 1) (Figure 5, Figure 9). In the reversed space a particle runs vectorially towards 1/ (− ∞) infinity, meaning inverse direction in shrinking space, whereas its pendent shows the reverse (+) /1. This idea is not new, and a series of works discuss this true possibility 9 33, 34, 35 38 50, 51, 52, 53, 54. Following this aspect is important ensure the dimensions are taken into account meticulously in such a reversal technics, so this task must be carried out in a substantially dimensionless manner. In addition, the theory is intended to show whether any corrections are necessary withstanding every doubt of its generality. Albeit, certain studies of this type already exist 31, 39 the task would be decide which of those results obtained from them could eventually drawn near to directly raise the phenomenon for the Hubble's theory.

The class and amounts be presented, named, and defined as essential parts of a clear mathematical construction of the model: maximal radius, photon radius, radius and distance in cosmic space R; just the same for a principle mathematical processing as for small spaces. A very important aspect is electrodynamics, especially electrostatics with long-range effect and shielding, whereas gravity is limited to short distances and contrasting no shielding occurs.

In this section the proper idea is tracked down. As R offers the junction invert, like

(30)

the labeling omitted. In indexing the respective object related photon radius, "ph" and the outer sphere "out" will be postulated principally

(31)

if units are ignored. This opens the onset

(32)

A commencement thorough investigation will show the validity. The comparison of the two radii, small and huge, is carried out by means of executing a suitable point for reciprocal "mirroring", i.e., conjugate-transponated. A rational basis settles on both two spaces, i., e., spheric, closed (Ω > 1) and hyperbolic as open (Ω < 1), reservatedly spoken touching each other at their photon radii. This means the sphere lying outside of the real positive space with , lying inside associated the tiny negative with inside directed space. Both types, the expanding space with the shrinking show reversal of their properties,

also here, which corresponds to spherical with hyperbolic behavior. This faces almost a singularity associated to the positive space. It is seen, however a ring-similar point inside (Figure 9) applies. In complying the relative spacingbetween both of the respective two sphere- / ring-printouts give

(33)

For clarification was stated here this is the maximum radius, which corresponds to a minimum extension in the mini-cosmos. To first provide some supportive insight the first step yields from replacing

(34)

for the further inside located sphere. sounds comprehensive (Figure 8) and more substantiating is

(35)

This is not to confuse with

but yields

Hence, the end formula appears

(37)

with a recognizable relativistic correction of the classic s-R ratio in α .

Before the actual cause of an expansion of the real universe is discussed, a result should be provided for the experimental astronomer. A distance measurement of galaxies is done based on the speed of light c , which is why it is sufficient to simply do the approach from

and the invert value can't hurt, either

(38)

Such values are usually depicted in cosmological units via

to display

(39)

commonly referred to as the Hubble's constant. Quod erat demonstrandum.

7. Examination of the angular velocity ω and M in real space

Such a constant would have been expected an exclusively positive sign. This property, originating from the root in the formula m can be assigned an oscillating behavior.

Due to the properties shown for the (negative) anti-space as well as for its positive counterpart, respective pendant 10 it is of course also righteous to open a visual comparison, when the facts (lat.:natura non facit saltus ?) downrightly invites to do so. As already briefly introduced above, there should be no obstacle to implementing the results into a torsion. Although, the vector image was largely avoided in the text the two spaces show exactly reciprocal behavior to each other, in analogy to the two maximum speeds. While the mini-, i.e. nega-verse impresses with an almost gigantic expansion (Figure 10) hardly be compensated for per relativistic influence, a real -structure is visible in the other with to a certain extent compressed structure; here their shapes interchange from negative (hyperbolic) curvature to positive (spheric), in mind the above expressions straightly involve the space between both the respective two (fragile photon-) circum-ferences. It is proper not just the size ratios being of considerable importance also their signs are as already been discussed in advance.

So now the driving forces would claim in principle

(41)

and the difference is immediately clear: in the first (spheric) space an expansion will prevail, whereas the second (hyperbolic) illuminates contraction or shrinkage (Figure 5),

First, the circumferences are established in

(42)
(43)

and of course, it must be referred to an "effective" circumference, which, according to what has been said, does not consist of ; especially in the positive space there seems to be an extraordinary "bloat" (Figure 11) based on the factual differences between its active routes. From here it is only a short walk to the driving testimony of the two spaces. First of all, the respective circulation time with becomes

(44)
(45)

making the apparent break in total symmetry noticeable. Sure, the mini-space rotates around almost infinite times while the real universe figures an eternity for a single turn,

The such low speeds that occur justify a quasi-classical treatment. It is, finally

(46)

neither showing anything unusual nor (directly) necessarily superluminal, apart from the basis. If the alternating sign, ± is ignored, indicating an oscillation, then, figuratively speaking, the negative or positive snail behaviors will be obvious. While the mini-cosmos "screws inwards" over time, the real one has a screw-like movement outwards (Figure 2, Figure 7, Figure 8) with circular times of the related space types.

In both cases there is a limit to this seemingly strict behavior, as has been drawn above as a certain transition to linearity (Figure 2, Figure 8). Although a hyperbolic system is not easy insightful, the limit can be found near a kind of center (no singularity), i., e., with very high negative exponents 31. In positive space the reverse is true and would correspond to a limit of the observable (!) universe. In this utterance there should be no burying to hide this difference if the Newton's laws were used again, even seeming simple. This still emerges strengthening the true picture to the impact mentioned figuratively, as the driving mechanism for rotation of the two different spaces, since the choice where to put the respective force is free, and the two equations are factual, even though the results reveal opposite behavior.

(47)

Finally and lastly two things still need to be discussed in order to round off the entire text. The first may sound ridiculous as is the question of an M in the real universe emerging from the analogy of both systems. The value is of course just a consequence of mathematics, because the results obtained cannot be achieved using the method presented here due to the enormous distances in a real posi-verse due to the associated interaction be based on c . Since r and m are linear to each other a relation m to M can be found via

(48)

For the G a comparison from uncovers 32

(49)

and the influence of the inert component is not negligible with regard to the other root results.

3. Results

The solution of the Einstein's field equations as a global chart is homeomorphic to the . In the theory developed here the entire universe rotates in an ellipsoidal shape and far away from the observer embedded in a hyperspace, since itself claims be described in the. The H constant reads including the recommended values of α and G 50, whereas including theoretically obtained values result in a slightly lower value of about 7 percent. Due to the low speeds compared to c and the slight m in the initial version, which allow and justify the treatment of a mini-space, the results are trustworthy and do not require any complaints due to a lack of general relativistic discourse.

The driving force for the rotation of the entire universe runs out

Albeit, only a very small segment of the area is covered, this comparatively tiny part is sufficient to constitue the required centrifugal force. Furthermore, the theoretical track s to be covered around the center claimed of the observer shows

Given the length of time a thought-objects will take, this distance will certainly not be able to be covered as this will take longer than the universe that exists today. An

analogous to the m in the anti- (mini-) universe could be determined via comparing the two radii r and R. According to the theory such an M is not to be viewed as a single m-packet, but rather this valueis figuratively speaking spread and filled in a ring shaped torso or tube (Figure 15) around the fictitious center of the universe, i., e. the observer's point of view.

Finally, a contribution related to G could help to verify a possible deviation from the experimental found Hubble's constant H, explained in the current investigation, arround 7 per cent,

If the (also maximum) expansion respective shrinking speed of anin the observable universe is assumed diferent the speed of light,

then the end of this space is not reached from the expansion at c but rather at the natural limits

All the latter points affect the distance D and the path or respective track s as the time t as well demonstrating small deviation from the figure of a perfect circle, say any circle-like movement of an m object in space is slightly bruised; it does not fullfil a perfect circle rather will describe an elipsoid-shaped trace (Figure 13, Figure 14) regardless of the truly dominant forces discussed

4. Discussion

As the equivalence principle, EP is the hypothesis the observed equivalence of gravitational and inertial mass be a consequence of nature. Notwithstanding highly precise experimental tests of the EP limit possible deviations from it be very small, eqs. (49). Nevertheless, it is necessary to take a closer look at those constants, e., g., G that experience has shown be meaningful and to include the weaker, and uncertainly determinable, if not difficult to estimate, components only as possible corrections

There is no widely accepted single theory that explains the sets of gravitational phenomenae separately attributed to dark energy, DE, dark matter, DM 56, 57, also with regard to weakly interacting massive particles, WIMP 58 and experimental investigations, e. g., 27. Though, these results enable further additional interpretation of the facts, they keep certainly fragile due to the complexity of the conditions in the cosmos, but are not doubtful as significant contribution. So, there occurs a dichotomy within gravitational science 34. The FLRW theory of an expanding universe without spatial curvature at very large scales, but through its determinations of spatial expansion 59, continues to be affirmed from observations. Based on the entire discussion to verify a true and plausible reason for expansion fails because of the variables determining the cosmos and still point back to estimates.

A work clearly taking into account the gravitational influence was presented through a basis on dimensionless unification of the fundamental interaction 60. In this interpretation, real expressions of Archimedes' constant are formed using the fraction of "e" as Euler's number and the exponential Gerford's constant allowing develpment into an arithmetic series. Then, these series to explain the strong-couplin constant were created in turn open the way to a geometric-graphitative treatment. Reference is made to the fine structure constant presented be correctly incorporated into the obtained final expressions via the 'golden angle' φ = 1.618 respective cosmic spiral for a gravitational structure. A reference to real sizes of proton and electron mass does not stand in the way of unification; rather, when considering the rotation of ideas means a reference to actual conditions. From unification between micro- and maxi-cosmos referenced to Planckian dimensions and based on the cosmological constat Λ the author obtained the actually exact value for H .

Although the actual paper bases the results found on a comparatively simple theory, these statements can still be assessed as very powerful, without belittle or even disparage investigations presented in other publications.

Sure, according the Hubble's law the escape velocity , confermed in the current study in, is sparse a magnitude despite applying quite well at a distance , in very good agreement to the results in the actual theory. The Andromeda Galaxy, in turn is only about 2.2 million light years respective 0.7 Mpc away mean the H-law not be applicable at small galactic scales. An verification based on this document, not explicitly shown, can confirm this on its own, as well. So it would be worthwhile to describe the missing 4 elements of the Einstein's tensor in order to supplement the 6 already existing for, e., g., black holes, BH 19, 48, 49 for unmitigated description. In view inside and about a BH 31, 46, 47, 50 this would favor an expansion in the distance though, this argument seems strange. For example, other results show a much more pronounced distance of the universe, as shown by a (once again) reversal of the conditions in a BH, Then, the observable universe is a roughly spherical region extending 46.5 billion light-years in all directions from any observer: in this case a theory similar to Hubble's actually behaves linear. If else it were a BH to actually mean singularity, compare 61. Sure, the research presented in this work could question the BBT granting an alternative to cosmic inflation 61 as well as the justification for expansion suggested from dark energy and further justifications.

It seems bit strange to base the theory presented on a certain anti- or negative universe, which is however supported from the density parameter Ω as a constant everywhere in space.

Generelly, scientists think the smallest BH are as small as just one atom 31. These are very tiny but have the mass of a large mountain. M respective m is the amount of matter, or “stuff,” in an object. Actually all those traces are embedded in the standard model 6, 7, 11 as mathematically self-consistent. Despite gravity as perhaps the most familiar fundamental interaction it is not described due to contradictions arising when general relativity, GR the modern theory of gravity, and quantum mechanics 62, QM is tried to combine: gravity is that weak at microscopic scales it is essentially unmeasurable. If assumed properties did not vary with location or respective direction it would be entirely homogeneous and isotropic e., g., 34, which according to this work is not exactly true, albeit at very long distances the results correspond to good approximations (Figure 1, Figure 2).

In view about the shape of the universe, the expanding property first, could be ignored; entailing separate the shape from time pretending it is not. When studying those investigations mentioned, the formulations in the present work may no longer sound absurd, although the execution is based on a single statement 16, 17. This, however, takes into account the possibility of superluminality, a circumstance strictly reduced to absurdity from a number of scientists as well as time recersal, which is expressly possible 16, 17, 18, 19 63, 34, 65. Such an idea reporting in modern physics the paradoxi troubled astronomers not laid to rest ancient times until nowadays. This perspective may contradict the special theory of relativity, SR but absolutely permissible as a recognized aspect in the general, GR 19

The idea of a negative universe 10 is no more new than the idea of a reversal of space respective space-time 9 33, 34, 35 51, 52, 53, 54 and is linked to views on BH. A kind of total reversal in the properties of a space using CPT-symmetry leads to a solid basis in the presented investigation and is no stranger to such considerations.

A final question is the linearity in measuring and evaluating the results

1, 14, 15. The key idea is less a question of a theory rather appropriately representing the facts and more of an interpretation of a cosmos as essentially void, but large distances show optical influences through the summation of the density units 58. In the case of cosmic distances this knowledge is taken into account; uncertainty in the aforementioned assumed "homogeneity and isotropy" of space remains the major challenge.

With regard to the objective the theory presented here is meaningful. Leaving aside the basis, neither high speeds nor large masses appear, and complex instruments of the GR can certainly be neglected. Certainly it seems strange to suggest a "rotation" of the entire universe as an explanation for its expansion, because of course the very long time span for a single complete rotation compared to the anticipated age sounds strange. It can be credibly admitted this work has more of a connection to philosophy. An embedding the 4-dimensional universe in a 5-dimensional hyperspace 57, 58 as meaningful can be confirmed.

5. Conclusion

The theory presented consists of the intrinsic derivation of the Hubble constant H. As basic requirement serves a rotation ω of the space under consideration, offering the advantage of a constancy of the overall space swept, in contrast to a specific speed υ that varies with the radius r respective R. Starting from the tiny counterpart of quasi atomic size to a real universe a first statement can be created to understand the conditions in a space that can initially be assigned to shrinking. A reference to the creation of these preparations is necessary, because here the mathematical requirements can be found in an initially spatial-limited system; this is the only possibilty, alone.

After determining the boundary conditions via the two light speeds, i. e., sub- and superluminal, the sizes together with the size ratios can be transferred sensibly and appropriately per folding in a complete reversal the small space into a large, real one. The knowledge gained in this way, then allows the exact determination of circumpherence, radius measured from the observer's location and the associated time period. From there, this time interval then leads to the exact statement and thus the exhibits evidence of the Hubble constant H. Further results can also be derived from this, like a torsus at the respective distance containing the mass density ϱ and the associated mass M in a space describing the universe. In addition to the H constant, the theory also allows conclusions to be drawn about possible deviations caused by the gravitational constant and properties of the states inherent in the masses.

An indication of validity for a galaxy and the outlook on what will happen when the limit of the universe is crossed opens up good prospects for new questions, and maybe there is a gravitational bye-bye of masses leaving the observable universe into another in the form of emitting gravitational waves many billion years of age ago, who knows?

ACKNOWLEDGEMENT

The thanks are due to Ms. Catherine Carmen Beatrice de la Rue to support aspects in terms of linguistically semantics on the text.

References

[1]  Hubble,E. P. Cepheids in spiral nebulae. The Observatory 48 (1925) 139 – 142.
In article      
 
[2]  Hubble, E. Relation between Distance and Radial Velocity among Extra-Galactic Nebulae. Proc. Nat. Acad. Sci. U. S. A. 15 (1929) 168 – 173.
In article      View Article  PubMed
 
[3]  Hubble, E. The observational approach to cosmology. The Clarendon Press, Oxford (1937).
In article      
 
[4]  Friedmann, A. (1922). "Ueber die Kruemmung des Raumes. Z. Phys. 10 (1922) 377 – 386.
In article      View Article
 
[5]  Einstein, A. On a Stationary System With Spherical Symmetry Consisting of Many Gravitating Masses. Ann. Math. Sec. Ser. 40 (1939) 922 – 936.
In article      View Article
 
[6]  Robertson, H. P. Kinematics and World-Structure. Astophys. J. 82 (1935) 284 – 301.
In article      View Article
 
[7]  Robertson, H. P. Kinematics and World-Structure 3. Astophys. J. 83 (1936) 257 – 271.
In article      View Article
 
[8]  Walker, A. G. On Milne's theory of world-structure. Proc. Lond. Math. Soc. 2, 42 (1937) 90 – 127.
In article      View Article
 
[9]  Ellis, G. F. R.; van Elst, H. Cosmological models (Cargèse lectures 1998). Marc Lachièze-Rey (ed.). Theoretical and Observational Cosmology. NATO Science Series C. 541 (1999) 1 – 116.
In article      View Article
 
[10]  Friedman, A. Ueber die Moeglichkeit einer Welt mit konstanter negativer Kruemmung des Raumes. Z. Phys. 21 (1924) 326 – 332.
In article      View Article
 
[11]  Freedman, W. L.; Madore, B. F.; Scowcroft, V.; Burns, C.; Monson, A.; Persson, S. E.; Seibert, M.; Rigby, J. Carnegie Hubble Program: A Mid-Infrared Calibration of the Hubble Constant. Astrophys. J. 758 (2012) 24 – 33.
In article      View Article
 
[12]  Leavitt, H. S. 1777 Variables in the Magellanic Clouds. Ann. Harvard. Coll. Obs. LX (1908) 87 – 111.
In article      
 
[13]  Friedman, A. Ueber die Kruemmung des Raumes. Z. Phys. 10 (1922) 377 – 386.
In article      View Article
 
[14]  Kirshner, R. P. Hubble's diagram and cosmic expansion. Proc. Nat. Acad. Sci. 101 (2003) 8 – 13.
In article      View Article  PubMed
 
[15]  Harrison, E. The redshift-distance and velocity-distance laws. Astrophys. J. 403 (1992) 28 – 31.
In article      View Article
 
[16]  Gerlitz, T. G. M. Superluminality and Finite Potential Light-Barrier Crossing. Int. J. Res. Pure and Appl. Phys. 5 (2015a). 19 – 24.
In article      
 
[17]  Gerlitz, T. G. M. Superluminality and Finite Potential Light-Barrier Crossing. Phys. J. 12 (2022a) 1 – 9.
In article      
 
[18]  Davis, T. M.; Lineweaver, C. H. Superluminal Recession Velocities. AIP Confer. Proc. 555 (2001) 348 – 351.
In article      View Article
 
[19]  Goedel, K. An Example of a New Type of Cosmological Solutions of Einstein's Field Equations of Gravitation. Rev. Mod. Phys. 21 (1949) 447 – 450.
In article      View Article
 
[20]  Farnes, J. S. A Unifying Theory of Dark Energy and Dark Matter: Negative Masses and Matter Creation within a Modified ΛCDM Framework. Astronomy Astrophys. 620 (2018) A92.
In article      View Article
 
[21]  Holland de Barcellos, J. C. Derivation of Hubble's Law and its relation to dark energy and dark matter. J. Math. Theor. Phys. 2 (2019) 29 – 32.
In article      
 
[22]  Wu, E. T. H. Hubble's Law Derived from Wu's Spacetime Shrinkage Theory. IOSR J. Appl. Phys. 11 (2019) 3 – 7.
In article      
 
[23]  Seshavatharam, U. V. S.; Lakshminarayana, S. An Outline Picture of a Growing and Rotating Planck Universe with Emerging Dark Foam. Asian J. Res. Rev. Phys. 2 (2019) 1 13.
In article      View Article
 
[24]  Seshavatharam, U. V. S.; Lakshminarayana, S. An Integrated Model of a Light Speed Roating Universe. Int. Astronomy Astrophys. Res. J. 2 (2021) 282 290.
In article      
 
[25]  Heisenberg, W. Ueber den anschaulichen Inhalt der quantentheoretischen Kiematik und Mechanik. Z. Phys. 43 (1927) 172 – 196.
In article      View Article
 
[26]  von Neumann, J. Wahrscheinlichkeitstheoretischer Aufbau der Quantenmechanik. Nach. Gesellsch. Wiss. Goettingen; Math.-Phys. Kl. 245 − 272 (1927).
In article      
 
[27]  Spergel, D. N.; Bean, R.; Doré, O.; Nolta, M. R.; Bennet, C. L.; Dunkley, J.; Hinshaw, G.; Jarosik, N.; Kornatsu, E.; Page, L;. Peiris, H. V.; Verde, L.; Halpern, M.; Hill, R. S.; Kogut, A.; Limon, M.; Mever, S. S.; Odegard, N.; Tucker, G. S.; Weiland, J. L.; Wollack, E.; Wright, E. L. Three-Year Wikinson Microwave Anisotrpy Probe (WMAP) Observations: Implication for Cosmology. Astrophys. J. Suppl. Ser. 170 (2007) 377 – 408.
In article      View Article
 
[28]  Cornish NJ, O'Beirne L.; Taylor SR.; Yunes N. Constraining Alternative Theories of Gravity Using Pulsar Timing Arrays. Phys. Rev. Lett.. 120 (2018) 181101.
In article      View Article  PubMed
 
[29]  Debye, P.; Hueckel, E. Zur Theorie der Elektrolyte. Phys. Z. 9 (1923) 185 – 206.
In article      
 
[30]  Lemaître, G. (1927). Un Univers homogène de masse constante et de rayon croissant rendant compte de la vitesse radiale des nébuleuses extra-galactiques". Ann. Soc. Scient. Brux. A47 (1927) 49 – 59.
In article      
 
[31]  Gerlitz, T. G. M.; Walden, W. An Idea to a World inside a Black Hole. Int. J. Phys. 5 (2017) 171 − 180.
In article      View Article
 
[32]  Clark, S. J.; Tabbotucker, R. W. Gauge symmetry and gravito-electromagnetism. Class. and Quant. Grav. 17 (2000) 4125 − 4157.
In article      View Article
 
[33]  Lachièze-Rey, M.; Luminet, J.-P. Cosmic topology. Phys. Rep. 254 (1996) 135 – 214.
In article      View Article
 
[34]  Liddle, A. An Introduction to Modern Cosmology. John Wiley and Sons, (eds.) 2nd ed., (2003).
In article      
 
[35]  Ojeda, P., Rosu, H. Supersymmetry of FRW barotropic cosmologies. Int. J. Theor. Phys. 45 (2006) 1191 – 1196.
In article      View Article
 
[36]  Newton, I. Philosophiae Naturalis Principia Mathematica (“Mathematical Principles of Natural Philosophy”). S. Pepys (ed.). London (1687).
In article      View Article
 
[37]  Walden, W.; Gerlitz, T. G. M. The Intrinsic Derivation of the Gravitation Constant G. Int. J. Phys. 10 (2022) 252 − 261.
In article      View Article
 
[38]  Landsberg, P. T. Mass Scales and the Cosmological Coincidentes. Ann. Phys. 496 (1984) 88 − 92.
In article      View Article
 
[39]  Gerlitz, T. G. M.; Walden, W. An Approach to an Element of Order Number Zero in the Periodic System. Int. J. Phys. 8 (2020) 134 − 146.
In article      View Article
 
[40]  Gerlitz T. G. M. The Mysterious Finestructure Constant α in Quantum Mechanics. Adv. Eng. and Appl. Sci.: An Int. J. 5 (2015b) 79 – 82.
In article      
 
[41]  Gerlitz, T. G. M. The Mysterious Constant Alpha (α) in Quantumphysics. Int. J. Phys.10 (2022b) 59 – 63.
In article      View Article
 
[42]  Agafonova, Yu, N.; et al. Measurement of the velocity of neutrinos from the CNGS beam with the Large Volume Detector. Phys. Rev. 76 (2007) 072005.
In article      
 
[43]  Agafonova, Yu, N.; et al. Measurements of the velocity of neutrinos from the CNGS beam with the Large Volume Detector. Phys; Rev. Lett. 109 (2012) 07001.
In article      View Article  PubMed
 
[44]  Adamson, P. Neutrino Velocity: Results and prospects of experiments at beamlines other than CNGS. Nucl. Phys. B: Proc. Suppl. 235 (2013) 296 – 300.
In article      View Article
 
[45]  Adam, T.; et al. Measurement of the neutrino velocity with the OPERA detector in the CNGS beam using 2012 dedicated data. J. High Energ. Phys. (2013) 153.
In article      
 
[46]  Gerlitz, T. G. M.; Walden, W. A Constant Rotating Kerr-Newman Black Hole with No Net Electrical Charge. Glob. J. Sci. Frontier Res. A 17 (2017) 5 – 14.
In article      
 
[47]  Gerlitz, T. G. M.; Walden, W. A Constant Rotating Kerr-Newman Black Hole with No Electrical Net Charge. Int. J. Phys. 6 (2018) 1 – 8.
In article      
 
[48]  Schwarzschild, K. Ueber das Gravitationsfeld eines Massepunktes nach der Einsteinschen Theorie. Sitz. Ber. Koen. Preuss. Akad. Wiss. 7 (1916a) 189 − 196
In article      
 
[49]  Schwarzschild, K. Ueber das Gravitationsfeld einer Kugel aus inkompressibler Fluessigkeit nach der Einsteinschen Theorie. Sitz. Ber. Koen. Preuss. Akad. Wiss. 18 (1916b) 424 − 434.
In article      
 
[50]  Pathria, R. K. The Universe as a Black Hole. Nature 240 (1972) 298 − 299 −− Good, I. J. Chinese universes. Physics Today 25 (1972) 15.
In article      View Article
 
[51]  Penrose, R. Singularities and Time-Asymmetry. General Relativity: An Einstein Centenary Survey. Cambridge University Press, Stephen Hawking, Werner Israel (eds.) (1979) 581 – 638.
In article      
 
[52]  Poplawski, N. J. Cosmology with torsio: An alternative to cosmic inflation. Phys. Lett. B 694 (2010) 181 – 185.
In article      View Article
 
[53]  Poplawski, N. J. Radial motion into an Einstein-Roden bridge. Phys. Lett. B 697 (2010) 110 – 113.
In article      View Article
 
[54]  Gambini, R.; Pullin, J. A First Course in Loop Quantum Gravity. Oxford University Press (2011).
In article      View Article
 
[55]  Tiesinga, E.; Mohr, P. J.; Newell, D. B.; Taylor, B. N. The 2018 CODATA, Committee on Data for Science and Technology, Recommended Values of the Fundamental Physical Constants. J. Baker, M. Douma, S. Kotochigova (Database dev.) National Institute of Standards and Technology, Gaithersburg, MD 20899, U. S. A. (2020).
In article      View Article  PubMed
 
[56]  Poincaré, H. The Milky Way and the Theory of Gases. Popular Astronomy 14 (1906) 475 – 488.
In article      
 
[57]  Carr, B. J.; Clesse, S.; García-Bellido, J.; Hawkins, M. R. S.; Kuehnel, F. Observational evidence for primordial black holes: A positivist perspective. Phys. Rep. 1054 (2024) 1 – 68.
In article      View Article
 
[58]  Timmer, J. No WIMPS! Heavy particles don't explain gravitational lensing oddities. Ars. Technica (2023) JHEP08 (2007)077.
In article      
 
[59]  Abbott, B. P.;. Abbott, T. D.; Abraham, S.; Acernese, F.; Ackley, K.; Adams, C.; Adhikari, R. X.; Adya, V. B.; Affeldt, C. A. Gravitational-wave Measurement of the Hubble Constant Following the Second Observing Run of Advanced LIGO and Virgo. Astrophys J. 909 (2021) 2018 pp.
In article      
 
[60]  Pellis, S. Unification Archimedes constant π, golden ratio φ, Euler's number e and imaginary number i. SSRN Electr. J. 10.2139/ssrn.3975869 (2021).
In article      View Article
 
[61]  Poplawski, N. J. Nonsingular, big-bounce cosmology from spinor-torsion coupling. Phys. Rev. D 85 (2012) 181 – 18.
In article      View Article
 
[62]  Jérôme, M. Everything you always wanted to know about the cosmoloical constant problem (but were afraid to ask). Compt. Rend. Phys. 13 (2012) 566 – 665.
In article      View Article
 
[63]  Bondi, H.; Gold, T. The Steady-State Theory of the Expanding Universe. Month. Not. Roy. Astron. Soc. 108 (1948) 252 – 270.
In article      View Article
 
[64]  Gold, T. The Arrow of Time. Am. J. Phys., AAPT 30 (1962) 403 – 410.
In article      View Article
 
[65]  Price, H. Time's arrow & Archimedes' point: new directions for the physics of time. Oxford University Press US (1997) pp. 81 – 82.
In article      
 

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T. G. M. Gerlitz. The Intrinsic Derivation of the Hubble Constant H in Cosmology. International Journal of Physics. Vol. 12, No. 4, 2024, pp 147-163. https://pubs.sciepub.com/ijp/12/4/3
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  • Figure 1. A variety of possible shapes from theories related to special and general relativity in linear presentation at low redshifts
  • Figure 2. A snail illustrates the locally possible stations in an object observed in space in connection with the associated velocities with the distance from the observer
  • Figure 5. Schematic illustration of the assignment and contrast in transference circumference s to radius r in hyperbolic and spheric spaces
  • Figure 8. Differences in the trajectory figured from the observed object depending on the varying speeds as function associated to Fattr and Fcentr
  • Figure 9. Schematic representation of the relationships between the photon radius (pH, dashed lines) and the “true” outer negative radius R-(left) respective inner positive radius R+ belonging to their distinct spaces
  • Figure 10. The specific influence of bradyon Vb and tachyon Vt velocities on their distinct track distances s to the "driving" difference speed VT,B toegether with their related angles φ and angular velocity ω
  • Figure 11. The influence of the different forces entailed from the assigned distances rB, rT clearly represented in the bloated result from the dimensionless factor α for a (negative, hyperbolic) mini-space
  • Figure 15. Supporting image for density distribution "smearing" M in filling a torso located in space around an observer in the center
[1]  Hubble,E. P. Cepheids in spiral nebulae. The Observatory 48 (1925) 139 – 142.
In article      
 
[2]  Hubble, E. Relation between Distance and Radial Velocity among Extra-Galactic Nebulae. Proc. Nat. Acad. Sci. U. S. A. 15 (1929) 168 – 173.
In article      View Article  PubMed
 
[3]  Hubble, E. The observational approach to cosmology. The Clarendon Press, Oxford (1937).
In article      
 
[4]  Friedmann, A. (1922). "Ueber die Kruemmung des Raumes. Z. Phys. 10 (1922) 377 – 386.
In article      View Article
 
[5]  Einstein, A. On a Stationary System With Spherical Symmetry Consisting of Many Gravitating Masses. Ann. Math. Sec. Ser. 40 (1939) 922 – 936.
In article      View Article
 
[6]  Robertson, H. P. Kinematics and World-Structure. Astophys. J. 82 (1935) 284 – 301.
In article      View Article
 
[7]  Robertson, H. P. Kinematics and World-Structure 3. Astophys. J. 83 (1936) 257 – 271.
In article      View Article
 
[8]  Walker, A. G. On Milne's theory of world-structure. Proc. Lond. Math. Soc. 2, 42 (1937) 90 – 127.
In article      View Article
 
[9]  Ellis, G. F. R.; van Elst, H. Cosmological models (Cargèse lectures 1998). Marc Lachièze-Rey (ed.). Theoretical and Observational Cosmology. NATO Science Series C. 541 (1999) 1 – 116.
In article      View Article
 
[10]  Friedman, A. Ueber die Moeglichkeit einer Welt mit konstanter negativer Kruemmung des Raumes. Z. Phys. 21 (1924) 326 – 332.
In article      View Article
 
[11]  Freedman, W. L.; Madore, B. F.; Scowcroft, V.; Burns, C.; Monson, A.; Persson, S. E.; Seibert, M.; Rigby, J. Carnegie Hubble Program: A Mid-Infrared Calibration of the Hubble Constant. Astrophys. J. 758 (2012) 24 – 33.
In article      View Article
 
[12]  Leavitt, H. S. 1777 Variables in the Magellanic Clouds. Ann. Harvard. Coll. Obs. LX (1908) 87 – 111.
In article      
 
[13]  Friedman, A. Ueber die Kruemmung des Raumes. Z. Phys. 10 (1922) 377 – 386.
In article      View Article
 
[14]  Kirshner, R. P. Hubble's diagram and cosmic expansion. Proc. Nat. Acad. Sci. 101 (2003) 8 – 13.
In article      View Article  PubMed
 
[15]  Harrison, E. The redshift-distance and velocity-distance laws. Astrophys. J. 403 (1992) 28 – 31.
In article      View Article
 
[16]  Gerlitz, T. G. M. Superluminality and Finite Potential Light-Barrier Crossing. Int. J. Res. Pure and Appl. Phys. 5 (2015a). 19 – 24.
In article      
 
[17]  Gerlitz, T. G. M. Superluminality and Finite Potential Light-Barrier Crossing. Phys. J. 12 (2022a) 1 – 9.
In article      
 
[18]  Davis, T. M.; Lineweaver, C. H. Superluminal Recession Velocities. AIP Confer. Proc. 555 (2001) 348 – 351.
In article      View Article
 
[19]  Goedel, K. An Example of a New Type of Cosmological Solutions of Einstein's Field Equations of Gravitation. Rev. Mod. Phys. 21 (1949) 447 – 450.
In article      View Article
 
[20]  Farnes, J. S. A Unifying Theory of Dark Energy and Dark Matter: Negative Masses and Matter Creation within a Modified ΛCDM Framework. Astronomy Astrophys. 620 (2018) A92.
In article      View Article
 
[21]  Holland de Barcellos, J. C. Derivation of Hubble's Law and its relation to dark energy and dark matter. J. Math. Theor. Phys. 2 (2019) 29 – 32.
In article      
 
[22]  Wu, E. T. H. Hubble's Law Derived from Wu's Spacetime Shrinkage Theory. IOSR J. Appl. Phys. 11 (2019) 3 – 7.
In article      
 
[23]  Seshavatharam, U. V. S.; Lakshminarayana, S. An Outline Picture of a Growing and Rotating Planck Universe with Emerging Dark Foam. Asian J. Res. Rev. Phys. 2 (2019) 1 13.
In article      View Article
 
[24]  Seshavatharam, U. V. S.; Lakshminarayana, S. An Integrated Model of a Light Speed Roating Universe. Int. Astronomy Astrophys. Res. J. 2 (2021) 282 290.
In article      
 
[25]  Heisenberg, W. Ueber den anschaulichen Inhalt der quantentheoretischen Kiematik und Mechanik. Z. Phys. 43 (1927) 172 – 196.
In article      View Article
 
[26]  von Neumann, J. Wahrscheinlichkeitstheoretischer Aufbau der Quantenmechanik. Nach. Gesellsch. Wiss. Goettingen; Math.-Phys. Kl. 245 − 272 (1927).
In article      
 
[27]  Spergel, D. N.; Bean, R.; Doré, O.; Nolta, M. R.; Bennet, C. L.; Dunkley, J.; Hinshaw, G.; Jarosik, N.; Kornatsu, E.; Page, L;. Peiris, H. V.; Verde, L.; Halpern, M.; Hill, R. S.; Kogut, A.; Limon, M.; Mever, S. S.; Odegard, N.; Tucker, G. S.; Weiland, J. L.; Wollack, E.; Wright, E. L. Three-Year Wikinson Microwave Anisotrpy Probe (WMAP) Observations: Implication for Cosmology. Astrophys. J. Suppl. Ser. 170 (2007) 377 – 408.
In article      View Article
 
[28]  Cornish NJ, O'Beirne L.; Taylor SR.; Yunes N. Constraining Alternative Theories of Gravity Using Pulsar Timing Arrays. Phys. Rev. Lett.. 120 (2018) 181101.
In article      View Article  PubMed
 
[29]  Debye, P.; Hueckel, E. Zur Theorie der Elektrolyte. Phys. Z. 9 (1923) 185 – 206.
In article      
 
[30]  Lemaître, G. (1927). Un Univers homogène de masse constante et de rayon croissant rendant compte de la vitesse radiale des nébuleuses extra-galactiques". Ann. Soc. Scient. Brux. A47 (1927) 49 – 59.
In article      
 
[31]  Gerlitz, T. G. M.; Walden, W. An Idea to a World inside a Black Hole. Int. J. Phys. 5 (2017) 171 − 180.
In article      View Article
 
[32]  Clark, S. J.; Tabbotucker, R. W. Gauge symmetry and gravito-electromagnetism. Class. and Quant. Grav. 17 (2000) 4125 − 4157.
In article      View Article
 
[33]  Lachièze-Rey, M.; Luminet, J.-P. Cosmic topology. Phys. Rep. 254 (1996) 135 – 214.
In article      View Article
 
[34]  Liddle, A. An Introduction to Modern Cosmology. John Wiley and Sons, (eds.) 2nd ed., (2003).
In article      
 
[35]  Ojeda, P., Rosu, H. Supersymmetry of FRW barotropic cosmologies. Int. J. Theor. Phys. 45 (2006) 1191 – 1196.
In article      View Article
 
[36]  Newton, I. Philosophiae Naturalis Principia Mathematica (“Mathematical Principles of Natural Philosophy”). S. Pepys (ed.). London (1687).
In article      View Article
 
[37]  Walden, W.; Gerlitz, T. G. M. The Intrinsic Derivation of the Gravitation Constant G. Int. J. Phys. 10 (2022) 252 − 261.
In article      View Article
 
[38]  Landsberg, P. T. Mass Scales and the Cosmological Coincidentes. Ann. Phys. 496 (1984) 88 − 92.
In article      View Article
 
[39]  Gerlitz, T. G. M.; Walden, W. An Approach to an Element of Order Number Zero in the Periodic System. Int. J. Phys. 8 (2020) 134 − 146.
In article      View Article
 
[40]  Gerlitz T. G. M. The Mysterious Finestructure Constant α in Quantum Mechanics. Adv. Eng. and Appl. Sci.: An Int. J. 5 (2015b) 79 – 82.
In article      
 
[41]  Gerlitz, T. G. M. The Mysterious Constant Alpha (α) in Quantumphysics. Int. J. Phys.10 (2022b) 59 – 63.
In article      View Article
 
[42]  Agafonova, Yu, N.; et al. Measurement of the velocity of neutrinos from the CNGS beam with the Large Volume Detector. Phys. Rev. 76 (2007) 072005.
In article      
 
[43]  Agafonova, Yu, N.; et al. Measurements of the velocity of neutrinos from the CNGS beam with the Large Volume Detector. Phys; Rev. Lett. 109 (2012) 07001.
In article      View Article  PubMed
 
[44]  Adamson, P. Neutrino Velocity: Results and prospects of experiments at beamlines other than CNGS. Nucl. Phys. B: Proc. Suppl. 235 (2013) 296 – 300.
In article      View Article
 
[45]  Adam, T.; et al. Measurement of the neutrino velocity with the OPERA detector in the CNGS beam using 2012 dedicated data. J. High Energ. Phys. (2013) 153.
In article      
 
[46]  Gerlitz, T. G. M.; Walden, W. A Constant Rotating Kerr-Newman Black Hole with No Net Electrical Charge. Glob. J. Sci. Frontier Res. A 17 (2017) 5 – 14.
In article      
 
[47]  Gerlitz, T. G. M.; Walden, W. A Constant Rotating Kerr-Newman Black Hole with No Electrical Net Charge. Int. J. Phys. 6 (2018) 1 – 8.
In article      
 
[48]  Schwarzschild, K. Ueber das Gravitationsfeld eines Massepunktes nach der Einsteinschen Theorie. Sitz. Ber. Koen. Preuss. Akad. Wiss. 7 (1916a) 189 − 196
In article      
 
[49]  Schwarzschild, K. Ueber das Gravitationsfeld einer Kugel aus inkompressibler Fluessigkeit nach der Einsteinschen Theorie. Sitz. Ber. Koen. Preuss. Akad. Wiss. 18 (1916b) 424 − 434.
In article      
 
[50]  Pathria, R. K. The Universe as a Black Hole. Nature 240 (1972) 298 − 299 −− Good, I. J. Chinese universes. Physics Today 25 (1972) 15.
In article      View Article
 
[51]  Penrose, R. Singularities and Time-Asymmetry. General Relativity: An Einstein Centenary Survey. Cambridge University Press, Stephen Hawking, Werner Israel (eds.) (1979) 581 – 638.
In article      
 
[52]  Poplawski, N. J. Cosmology with torsio: An alternative to cosmic inflation. Phys. Lett. B 694 (2010) 181 – 185.
In article      View Article
 
[53]  Poplawski, N. J. Radial motion into an Einstein-Roden bridge. Phys. Lett. B 697 (2010) 110 – 113.
In article      View Article
 
[54]  Gambini, R.; Pullin, J. A First Course in Loop Quantum Gravity. Oxford University Press (2011).
In article      View Article
 
[55]  Tiesinga, E.; Mohr, P. J.; Newell, D. B.; Taylor, B. N. The 2018 CODATA, Committee on Data for Science and Technology, Recommended Values of the Fundamental Physical Constants. J. Baker, M. Douma, S. Kotochigova (Database dev.) National Institute of Standards and Technology, Gaithersburg, MD 20899, U. S. A. (2020).
In article      View Article  PubMed
 
[56]  Poincaré, H. The Milky Way and the Theory of Gases. Popular Astronomy 14 (1906) 475 – 488.
In article      
 
[57]  Carr, B. J.; Clesse, S.; García-Bellido, J.; Hawkins, M. R. S.; Kuehnel, F. Observational evidence for primordial black holes: A positivist perspective. Phys. Rep. 1054 (2024) 1 – 68.
In article      View Article
 
[58]  Timmer, J. No WIMPS! Heavy particles don't explain gravitational lensing oddities. Ars. Technica (2023) JHEP08 (2007)077.
In article      
 
[59]  Abbott, B. P.;. Abbott, T. D.; Abraham, S.; Acernese, F.; Ackley, K.; Adams, C.; Adhikari, R. X.; Adya, V. B.; Affeldt, C. A. Gravitational-wave Measurement of the Hubble Constant Following the Second Observing Run of Advanced LIGO and Virgo. Astrophys J. 909 (2021) 2018 pp.
In article      
 
[60]  Pellis, S. Unification Archimedes constant π, golden ratio φ, Euler's number e and imaginary number i. SSRN Electr. J. 10.2139/ssrn.3975869 (2021).
In article      View Article
 
[61]  Poplawski, N. J. Nonsingular, big-bounce cosmology from spinor-torsion coupling. Phys. Rev. D 85 (2012) 181 – 18.
In article      View Article
 
[62]  Jérôme, M. Everything you always wanted to know about the cosmoloical constant problem (but were afraid to ask). Compt. Rend. Phys. 13 (2012) 566 – 665.
In article      View Article
 
[63]  Bondi, H.; Gold, T. The Steady-State Theory of the Expanding Universe. Month. Not. Roy. Astron. Soc. 108 (1948) 252 – 270.
In article      View Article
 
[64]  Gold, T. The Arrow of Time. Am. J. Phys., AAPT 30 (1962) 403 – 410.
In article      View Article
 
[65]  Price, H. Time's arrow & Archimedes' point: new directions for the physics of time. Oxford University Press US (1997) pp. 81 – 82.
In article