The Periodic Table of Elementary Particles for Baryonic Matter and Dark Matter: Upward-Going ANITA Events

This paper posits that the upward-going ANITA events are derived from the cosmic ray of the baryonic-dark matter (BDM) Higgs boson. In the extended standard model (ESM) for baryonic matter and dark matter, the spontaneous symmetry breaking through the Higgs mechanism for the symmetrical massless baryonic matter left-handed neutrinos and massless dark matter right-handed neutrinos produced massless baryonic matter left-handed neutrinos, sterile massive dark matter neutrinos, and the BDM Higgs boson. The BDM Higgs boson is the composite of the high-mass tau neutrino and the high-mass dark matter neutrino. During the passage through the high-density part of the Earth, the BDM Higgs boson is transformed into the oscillating BDM Higgs boson between the composite of the high-mass tau neutrino and the high-mass dark matter neutrino and the composite of the high-mass tau neutrino and the low-mass dark matter neutrino. The oscillating BDM Higgs boson decays into the high-mass tau neutrino with the extra energy and the low-mass dark matter neutrino (27 eV) in the low-density water-ice layer of the Earth. The high-mass tau neutrino is converted into ultra-high-energy tau neutrino which decays into tau lepton through the charged-current interactions, and tau lepton emerges from the surface of ice. Based on the periodic table of elementary particles, the calculated value for the high-mass tau neutrino with the extra energy is 0.47 EeV in good agreement with the observed 0.56 and 0.6 EeV. The periodic table of elementary particles for baryonic matter, dark matter, and gravity is based on the seven principal mass dimensional orbitals for stable baryonic matter leptons (electron and left-handed neutrinos), gauge bosons, gravity, and dark matter and the seven auxiliary mass dimensional orbitals for unstable leptons (muon and tau) and quarks, and calculates accurately the masses of all elementary particles and the cosmic rays by using only five known constants.


Introduction
The Antarctic Impulsive Transient Antenna (ANITA) experiment [1] is established to the detection of the cosmogenic ultra-high-energy (UHE) neutrinos at the scale of EeV. The three balloon flights of the ANITA experiment have produced two unusual steeply upward-going cosmic ray events with energies of ≈0.6 EeV [2] and ≈0.56 EeV [3]. These shower events have the characteristics of the decay of a tau lepton, which emerges from the surface of the ice, and the tau lepton is explained as the product of a UHE parent tau neutrino by the charged-current interactions with the Earth matter. However, such UHE tau neutrino cannot survive the passage through the Earth. The explanations for such anomalous events include the sterile neutrino origin [4] [5], the decay of the quasi-stable dark matter in the Earth's core [6] [7], and supersymmetric stau slepton [8].
This paper posits that the upward-going ANITA events are derived from the cosmic ray of the baryonic-dark matter (BDM) Higgs boson that travels through the Earth. In the standard model (SM) for baryonic matter, the SM spontaneous symmetry breaking through the Higgs mechanism for the symmetrical massless electromagnetism and massless weak interaction produced massless photon, massive weak bosons, and the standard model Higgs boson. (The standard model classifies all known elementary particles for baryonic matter, describes the electromagnetic, weak, and strong interactions, and does not include dark matter and the gravitational force.) Equally, in the extended standard model (ESM) for baryonic matter, dark matter, and gravity, the BDM spontaneous symmetry breaking through the Higgs mechanism for the symmetrical massless baryonic matter left-handed neutrinos and massless dark matter right-handed neutrinos produced massless baryonic matter left-handed neutrinos, sterile massive dark matter neutrinos, and the BDM Higgs boson. Dark matter particles are the sterile massive neutrinos. This paper proposes the BDM Higgs boson is the composite of the high-mass tau neutrino and the high-mass dark matter neutrino.
Other than gravity, sterile dark matter does not undergo any interaction with baryonic matter. Meanwhile, dark matter is incompatible to dense baryonic matter [9], because the incompatibility explains the failure to detect dark matter by the contact (interaction) between dark matter and baryonic matter on the Earth. The BDM Higgs boson is both baryonic matter and dark matter. The inactive dark matter in the BDM Higgs boson allows the BDM Higgs boson to be stable (inactive) in space, air, water, and ice. However, during the passage through the high-density part of the Earth, because of the inactivity and the incompati-

The BDM Spontaneous Symmetry Breaking for Symmetrical Baryonic Matter and Dark Matter
The first step in the formation of the periodic stable of elementary particles is the BDM spontaneous symmetry breaking for baryonic matter and dark matter. As described in the previous paper [14], there are one type of baryonic matter and five types of dark matter, resulting in the mass ratio of dark matter to baryonic matter as 5 to 1 in the good agreement with the observation [15]. Initially, the symmetry U(1) L × U(1) R between baryonic matter and dark matter in each mass dimensional orbital provided the symmetrical distribution between baryonic matter as the five massless left-handed neutrinos (ν L5 , ν L6 , ν L7 , ν L8 , and ν L9 ) and dark matter as the five massless right-handed neutrinos (ν R5 , ν R6 , ν R7 , ν R8 , and ν R9 ) on the principal mass dimensional orbitals from d (mass dimensional orbital number) = 5 to d = 9 as in Figure 1.
The seven mass dimensional orbitals are arranged as F 5 B 5 F 6 B 6 F 7 B 7 F 8 B 8 F 9 B 9 F 10 B 10 F 11 B 11 , where F d and B d are mass dimensional fermion and mass dimensional boson, respectively. As described in the previous papers [10] [11], the masses of massive dark matter neutrinos are related to each other with three simple formulae as the follows. D.-Y. Chung where d is the mass dimensional orbital number, F is fermion, and B is boson.
Each dimension has its own α d , and all α d 's except α 7 (α w ) of the seventh dimension (weak interaction) are equal to α, the fine structure constant of electromagnetism. The given observed masses are the mass of electron for F 6 and the mass of Z boson for B 7 . From Equations (1) and (3), α w = α 7 = α of week interaction = (M B6/ M B7 ) 1/2 = (M F6 /α/M B7 ) 1/2 = (M e /α/M Z ) 1/2 = 0.02771. Therefore, the masses of dark matter neutrinos are as in Table 1.

The Addition of U(1), the Standard Model Spontaneous Symmetry Breaking, and the Upward-Going ANITA Events
In the second step in the formation of the periodic table of elementary particles, electromagnetism as massless U(1) EM was added to ν L6 to become election which formed massless SU(2) L × U(1) Y with baryonic matter neutrino, and then the standard model spontaneous symmetry breaking involved SU(2) L × U(1) Y → U(1) EM through the Higgs mechanism to produce massive electron-massless photon, massless neutrino-massive weak bosons, and the standard model Higgs boson as in Figure 2 and Table 2.      Table 2.
The BDM Higgs boson as the composite of high-mass neutrinos is a decay product of the UHE pion and neutron from the UHE interaction with the cosmic microwave background [16] [17] which is p + γ CMB → p (or n) + n π, p + γ CMB → Δ + (1232) → p + π 0 (or n + π + ) where n is the total number of the produced π's. Other than gravity, sterile dark matter does not undergo any interaction with baryonic matter. Meanwhile, dark matter is incompatible to dense baryonic matter [9], because the incompatibility explains the failure to detect dark matter by the contact (interaction) between dark matter and baryonic matter on

The Periodic Table of Elementary Particles for Baryonic Matter and Dark Matter and the Cosmic Rays
In the ESM to include baryonic matter, dark matter, and gravity, the periodic table of elementary particles for baryonic matter, dark matter, and gravity is based on the seven principal mass dimensional orbitals for stable baryonic matter leptons (electron and left-handed neutrinos), gauge bosons, gravity, and dark matter and the seven auxiliary mass dimensional orbitals for unstable leptons (muon and tau) and quarks [10] [11] as in Figure 3 and in Table 3.  ν DM7 , ν DM8 , and ν DM9 ), six gauge bosons, and gravity. The standard model Higgs boson is the composite of the extra-muon μ' and anti-extra muon µ′ in Table   3 [12] [19].  knees-ankles-toe as described in the previous paper [13]. The energy spectrum from 10 9 eV to 10 20 eV appears to follow a single power law except few breaks at the knees-ankles-toe [20]. The power index increases at the first knee and the second knee, and decreases at the ankle. Above 4 × 10 19 eV, the power index increases as the "toe" as the last power index increase below the GZK limit (5 × 10 19 eV) as the upper limit of the cosmic rays [16] [17]. The fine structure of the cosmic ray spectrum [21] shows that an ankle with decrease in power index is in between the first knee and the second knee, resulting in two knees, two ankles, The calculations of the the knees-ankles-toe are in the first knee, the first ankle, the second knee, the second ankle, and the toe, respectively as in Table 4. The observed second knee is for the formation of F 9 which is the high-mass tau neutrino τ ν ′ corresponding to the observed high-mass tau neutrino without the extra energy in the upward-going ANITA events.

Summary
This  EeV. The decay products of tau lepton were detected by the ANITA.
In the periodic table of

Conflicts of Interest
The author declares no conflicts of interest regarding the publication of this paper.