For updated version—see www.Aquater2050.com/2015/11/

Abstract

In a previous paper (ref 1, AP4.7), a self-consistent theory called Model 1 was developed to answer ten major connected questions in astrophysics. The most important of these questions are:

How can dark matter be explained and described?
How can dark energy be explained and described?
Where do the extremely high-energy cosmic rays that occur beyond the GZK cutoff come from?

Model 1 appears to successfully answer these questions. The unique features of this model are:

There are two spaces in the universe, particle space and quantum vacuum space. A potential barrier separates them. One space contains visible matter, and the other space contains dark matter.

There is a cycling of mass-energy between these spaces through the black holes that connect them. Particles pass from our space through black holes where they are converted into super particles that operate with unified force. They then pass into the high-energy vacuum space where they become dark matter operating behind the potential barrier.

Dark matter particles interact with each other and form a slowly building and moving bubble centered on a galaxy. The bubbles of dark matter are connected to each other by corridors of dark matter forming a cosmic web, which guides the development of new galaxies.

There, behind a potential barrier, the dark matter particles gain energy, build up in number and eventually exceed the ability of the barrier to contain them. They then explode back into particle space as a big bang. This process repeats to make an endless series of new universes.

After the big bang exhausts itself, super particles continue to tunnel through the barrier into particle space. The super particles are unstable and break down into particles (protons) with extreme kinetic energy. In doing so, they give up potential energy into particle space. The potential energy gradually builds up to become the dark energy that we observe as the cause of our accelerating, expanding universe. The extreme energy protons are observed as cosmic rays with energy between the energy of force unification and the Planck energy, which is beyond the GZK cutoff.

Model 1 has a very important argument in favor of its acceptance. It starts with two basic constants from quantum mechanics and the standard model of particle physics (force unification energy and the Planck energy), and then chooses two new constants (the spherical barrier radius and the barrier thickness), and then quantitatively explains five observed phenomena that have yet to find a single consistent explanation, namely:

The accelerating expansion of the universe (Dark energy).
The process of creation and rotation of the galaxies (Dark matter).
The UHECR (cosmic rays) that have been observed in the energy range beyond the GZK cutoff.
The huge disparity in the different estimates of the vacuum potential.
The large-scale cutoff and asymmetry in the Microwave Background Energy.

Two variables cannot satisfy five equations without apriori connections in at least three of those equations. Not since the discovery of Planck’s constant have so many phenomena been explained by so few constants.

In working out this model, some problems arose that are connected with it. A fundamental issue arose with respect to ultra high-energy cosmic rays (UHECR’s). It became important to ask if UHECR’s could be decomposed super particles-i.e. super particles whose symmetry has been spontaneously broken, and changed into protons. This problem will be addressed here.

The Problem

Blasi (Blasi, 1) describes the problem of a set of ultra high-energy cosmic rays (UHECRs), which are observed in an energy range where there should be no cosmic rays. The reason is as follows. A cosmic ray is usually a very high-energy proton. When it interacts with the earth’s upper atmosphere, it produces gammas that penetrate to earth and are detected there. It was found, using the standard model of particle physics, that a proton with energy above a certain energy (the GZK cutoff ~ 4×10¹⁹ eV or ~ 4×10¹⁰ GeV), interacts with the microwave background in particle space to form other particles (pions). Since microwave background is everywhere, protons with extremely high energy (i.e. from super nova etc.) should not last very long in particle space. This means that particle space should be dark above this energy unless the source is common within our galaxy and close to our solar system. Yet such sources (neutron stars, AGN’s, white dwarfs, radio lobes, etc) are not common enough in our galaxy and especially in our neighborhood to account for the UHECR’s we observe. Furthermore the observed UHECR’s are omni directional, and the particles from neutron stars, AGN’s, white dwarfs and radio lobes are not (Blasi, 2).

The Observed Data

The observations, as described in Blasi (Blasi, 2) are as follows. Cosmic rays have been observed from ~ 0.1 GeV up to 3 x 10¹¹ GeV. We note:

A total of 59 events have been observed above 4 x 10¹⁰ GeV. The spectrum of these events from ~5 GeV to ~10⁶ GeV has a power law increase with slope of ~ 2.7. From ~10⁶ GeV to ~10¹⁰ GeV, the slope increases to ~ 3.1. At energies larger than 10¹⁰GeV, the spectrum begins to flatten out.
The 59 events appear to be isotropic on the large scale..
On the small scale, 5 possible doublets and 1 possible triplet were found.
The primaries appear to be mostly protons. A recent study indicates less than 30% are possible photon primaries.

It should be noted that the GZK cutoff might actually be at higher energy (E > 10¹¹ GeV) due to non-linear relativity effects (Magueijo, 32).

The Solution

Model 1 predicts high-energy cosmic rays with the following characteristics.

Super particles will tunnel through the barrier between vacuum space and particle space with energies in a Gaussian distribution in the range ~10¹⁰to10¹⁹ GeV. The portion of the super particle Gaussian less than 10¹¹GeVis reduced because the vacuum space potential energy attenuates the super particles if they have kinetic energy less than this value (see Appendix 1). In particle space, they are unstable, so they break down (through spontaneous symmetry breaking) into extremely high-energy protons, giving up its extra potential energy to the particle space vacuum (becoming dark energy). The resulting protons in particle space will have energy in the range 10¹⁰ to 10¹⁹ GeV..
The super particles in vacuum space have a Gaussian distribution with a mean, which depends on the age of the universe. Thus:

– For a young universe, the mean will be low (energy range ~10¹⁰ to ~10¹¹ GeV), because the super particles coming in from the black hole (see ref 3, AP4.7C) meet a relatively large, empty vacuum space, so they expand into the volume and their temperature goes down.

– For an early mature universe, the mean will be modest (energy range ~10¹¹ to ~10¹² GeV), because the addition of more energetic super particles will have increased the particle temperature and density in vacuum space, and the cosmic net is beginning to build, so conditions are right for making galaxies.

– For a middle aged universe, the mean will be medium (energy range ~10¹² to 10¹⁸ GeV), because the super particle temperature and density will have increased enough to generate a mature cosmic net (see ref 4, AP4.7B), and the generation of galaxies along the net will be rapid.

– For an old universe, the mean will be high (energy range ~10¹⁸ to 10¹⁹ GeV), because the super particle temperature and density will have increased enough to be near to the Planck energy preparing for a new big bang.

The protons that result from super particles in particle space will be isotropic on the large scale, because they come from an isotropic distribution of super particles in thermodynamic equilibrium in vacuum space.
On the small scale, doublets and triplets can form from reactions in particle space.
Ultra high-energy protons will result from the super particles, but collisions with particles in particle space can also cause ultra high energy gammas.

The spectrum of the UHECR’s match the Model 1 spectrum for early in the “mature universe” stage. The (~10⁶ to 10¹² GeV) slope shows the spectrum of ordinary cosmic rays plus the rising contribution of the cosmic rays caused by the low energy tail of the super particle Gaussian. The rollover beyond ~10¹⁰ GeV is caused by the peak and then the drop-off of super particles as the Gaussian tails off. The isotropy, the doublets and triplets and the dominance of protons match the data satisfactorily.

Note that a shift (if any) of the GZV cutoff to a higher value has no impact on this match, because it only impacts what happens to the particles after entering particle space. Such a shift makes other sources for UHECR’s possible in terms of the cutoff. However, the generation sources and the spectrum of the protons produced do not appear to match those observed. Nonetheless getting cosmic ray data for events up to 10¹⁹ GeV will clarify this issue by showing any new cutoffs.

Summary and Conclusions

Ultra high energy cosmic rays (UHECR’s} have been studied to find their origin and characteristics. They are found to match the characteristics of Model 1 super particles (dark matter) that have tunneled through the barrier separating vacuum space from particle space in Model 1 described above. After tunneling, they broke down into a UHECR proton, which was observed as a cosmic ray. The observed spectrum of UHECR’s may match the expected spectrum of a “mature universe”, which means that the mean energy of the super particle Gaussian distribution of dark matter is at ~10¹² GeV. With time, the mean will increase until it reaches ~10¹⁹ GeV, and then it will start a new big bang.

Appendix 1

The Barrier Equations

Consider the following non-relativistic three-dimensional time independent Schrödinger equation (see ref 7, AP4.7).

[-(h²/8p²m)Ñ²+V(x, y, z)]Y(x, y, z) = EY(x, y, z)

Where:

V(x, y, z) = barrier potential

E = particle energy

If we convert to spherical coordinates, and let:

Y(r, q, f) = R(r) Y(q, f)

Where:

Y(l, m) = Spherical Harmonics = (4p) ^-1/2 , if l = 0 (spherical symmetry)

Now, let:

R(r) = U(r)/r, then:

Y(r, q, f) = (4pi) ^-1/2 U(r)/r

Now, consider:

[-(h²/2m d²/dr² + V(r)]U(r) = EU(r)

Where:

E = the energy of the particle.

V(r) = V_o[Q(r) – Q(r-w)] = the vacuum potential.

And:

Q(x) = the Heavyside step function of width a starting at x =0

w = the potential zone width.

Note that any solution to the equation is unchanged if the step function is moved along the r axis to r_ob. Then:

1. One can think of starting at 0 and moving to r_ov. Think of this as moving within the super particle itself, so the complex kinetic and potential energy distributions applicable within the particle exist here.

2. One then moves from r_ov to r_ob., so w = r_ob-r_ov.= v. This is vacuum space, so the vacuum potential is V(r) = V_ov[Q(r_ov) – Q( r_ov-v)] = the vacuum potential

3. One then moves from r_ob to r_ob + a, so w = a. this is the space within the barrier itself, i.e. between vacuum space and particle space, so the vacuum potential is V(r) = V_ob[Q(r_ov) – Q( r_ov-v)] = the vacuum potential.

Thus the equation governs passage from the super particle through vacuum space and then through the barrier and into particle space. For convenience, we will let r = 0for solving the equation. Note that what we are describing is two concentric spherical shells with thicknesses v and a wrapped around a super particle. The shell with thickness v is vacuum space. The shell with thickness a is the barrier between vacuum space and particle space.

Note that what we will calculate is the transmission probability density (T = t²= r) or probability of transmission. The solution to the equation is a combination of left and right moving wave functions that are continuous at the boundaries of the barrier (r = 0 and r = w) along with their derivatives.

The solution can be used to generate the transmission through the barrier T (see Ref 8), which is as follows:

If E>V

T = 1/(1+V₀²sin²(k₁w)/4E(E-V₀)

If E<V,

T = 1/(1+V_o² sinh²(k₁w)/4E(V₀-E),

Where k₁= (8p²m(V₀-E)/h²) ^1/2

Here we have set up the equations for either of two shells, a vacuum space shell and a barrier shell. The rate of passage of a particle through either spherical shell is:

R = T h/2p k₁

The best fit for the vacuum space sphere and the barrier shell of the very rough data available is:

r_ov= 10^-20 cm

r_ob= 10^-5 cm

a = 10^-7 cm

There are three important cases.

Case 1

E > 10¹⁷ GeV

V_ov= potential energy ~ 10¹⁷ GeV

V_ov/cc = potential energy density ~ 10³² GeV/cc

N = number of super particles in vacuum space = 10⁶⁰ super particles

This is the vacuum space case for particles with potential energy ~ 10¹⁷ GeV-i.e. super particles. We note that super particles with kinetic energy greater than 10¹⁷ GeV move freely in vacuum space. If the kinetic energy drops below 10¹⁷ GeV, however, the probability of operating in and passage through gradually attenuates.

Case 2

E ~ 10¹⁷ GeV

V_ob= 10¹⁹ GeV

V_ob/cc = potential energy density ~ 10³⁵ GeV/cc

N = number of super particles in vacuum space = 10⁶⁰ super particles

This is the case of leakage of super particles for the whole universe by tunneling through the barrier. In this case, T = 10^-50, and R = 10⁷⁴GeV/cm² sec. When these particles reach particle space, they break down to ordinary particles and give up their phase change energy (10¹⁷ GeV/particle) into the particle space vacuum energy, or dark energy, which over 10¹⁰ years has made a dark energy of ~ 10^-5 GeV/cc. This is the same dark energy that causes the accelerated expansion of space that requires a potential energy of ~ 10^-5 GeV/cc.

Case 3

E = 10¹⁹ GeV

V_ob= 10¹⁹ GeV

This is the case of big bang passage over the barrier. In this case, T = 1, and R = 10¹²⁴GeV/cm² sec. When these particles reach particle space, they break down into ordinary particles and give up their phase change energy into particle space vacuum energy, or expansion energy, which expands particle space. The amount needed is estimated to be ~10⁹⁴ GeV/cc (see ref 9), where the volume of space at the beginning of expansion is estimated to be (for one super particle barrier shell) 10^-14 cc. Thus the expansion potential energy required is ~ 10⁸⁰ GeV. The phase change energy (~10¹⁷ GeV/particle) from the ~10⁶⁰ particles in particle space including the dark matter is ~ 10⁷⁷ GeV. The discrepancy seen is not surprising considering the fact that the theories used to obtain the estimates cannot yet be matched for assumptions and conditions.

References

P. Blasi, “The Highest Energy Particles in the Universe: the Mystery and its Possible Solutions”, arxiv.org/pdf/astro-ph/0110401.pdf
J. Magueijo, New Varying Speed of Light Theories, arxiv.org/pdf/astro-ph/0305457.pdf
L. H. Wald, “AP4.7C DARK MATTER RATE EQUATIONS” www.Aquater2050.com/2015/09/
L. H. Wald, “AP4.7A SUPER PARTICLE CHARACTERISTICS” www.Aquater2050.com/2015/09/