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Tera-Leptons Shadows over Sinister Universe
High Energy Physics - Phenomenology · Submitted 7 Jul 2005
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The e(4HeE)+ behave chemically like an anomalous hydrogen isotope.Also tera-positronium (eE+) relics are over-abundant and they behave like an anomalous hydrogen atom: these gases do not fit by many orders of magnitude known severe bounds on hydrogen anomalous isotope, making grave shadows over a Sinister Universe.
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The abstract, sentence by sentence
The role of Sinister Heavy Fermions in recent Glashow's SU(3)*SU(2)*SU(2)'*U(1) model is to offer in a unique frame relic Helium-like products (an ingenious candidate to the dark matter puzzle), a solution to the See-Saw mechanism for light neutrino masses as well as to strong CP violation problem in QCD. The Sinister model requires a three additional families of leptons and quarks, but only the lightest of them Heavy U-quark and E-"electron" are stable. Final neutral Helium-like UUUEE state is an ideal evanescent dark-matter candidate. However it is reached by multi-body interactions along a tail of more manifest secondary frozen blocks. They should be now here polluting the surrounding matter. Moreover, in opposition to effective pair quark annihilations, there is no such an early or late tera-lepton pairs suppressions, because:a) electromagnetic interactions are "weaker" than nuclear ones and b) helium ion 4He++ is able to attract and capture, E-, fixing it into a hybrid tera helium "ion" trap. This leads to a pile up of relic (4HeE)+ traces, a lethal compound for any Sinister Universe. This capture leaves no Tera-Lepton frozen in Ep relic (otherwise an ideal catalyzer to achieve effective late E+E- annihilations possibly saving the model). The (4HeE)+ Coulomb screening is also avoiding the synthesis of the desired UUUEE hidden dark matter gas. The e(4HeE)+ behave chemically like an anomalous hydrogen isotope.Also tera-positronium (eE+) relics are over-abundant and they behave like an anomalous hydrogen atom: these gases do not fit by many orders of magnitude known severe bounds on hydrogen anomalous isotope, making grave shadows over a Sinister Universe. However a surprising and resolver role for Tera-Pions in UHECR astrophysics has been revealed.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The role of Sinister Heavy Fermions in recent Glashow's SU(3)*SU(2)*SU(2)'*U(1) model is to offer in a unique frame relic Helium-like products (an ingenious candidate to the dark matter puzzle), a solution to the See-Saw mechanism for light neutrino masses as well as to strong CP violation problem in QCD. | background 0.93 | 0.11 | 0.09 | asserted 0.97 |
| s1 | The Sinister model requires a three additional families of leptons and quarks, but only the lightest of them Heavy U-quark and E-"electron" are stable. | background 0.93 | 0.12 | 0.04 | asserted 1.00 |
| s2 | Final neutral Helium-like UUUEE state is an ideal evanescent dark-matter candidate. | background 0.37 | 0.23 | 0.10 | asserted 0.98 |
| s3 | However it is reached by multi-body interactions along a tail of more manifest secondary frozen blocks. | result 0.47 | 0.27 | 0.04 | asserted 0.98 |
| s4 | They should be now here polluting the surrounding matter. | interpretation 0.77 | 0.11 | 0.07 | asserted 0.65 |
| s5 | Moreover, in opposition to effective pair quark annihilations, there is no such an early or late tera-lepton pairs suppressions, because:a) electromagnetic interactions are "weaker" than nuclear ones and b) helium ion 4He++ is able to attract and capture, E-, fixing it into a hybrid tera helium "ion" trap. | interpretation 0.61 | 0.30 | 0.07 | asserted 1.00 |
| s6 | This leads to a pile up of relic (4HeE)+ traces, a lethal compound for any Sinister Universe. | interpretation 0.76 | 0.38 | 0.27 | asserted 1.00 |
| s7 | This capture leaves no Tera-Lepton frozen in Ep relic (otherwise an ideal catalyzer to achieve effective late E+E- annihilations possibly saving the model). | interpretation 0.63 | 0.36 | 0.12 | asserted 0.95 |
| s8 | The (4HeE)+ Coulomb screening is also avoiding the synthesis of the desired UUUEE hidden dark matter gas. | interpretation 0.53 | 0.38 | 0.13 | asserted 1.00 |
| s9 | The e(4HeE)+ behave chemically like an anomalous hydrogen isotope.Also tera-positronium (eE+) relics are over-abundant and they behave like an anomalous hydrogen atom: these gases do not fit by many orders of magnitude known severe bounds on hydrogen anomalous isotope, making grave shadows over a Sinister Universe. | result 0.50 | 0.36 | 0.46 | asserted 1.00 |
| s10 | However a surprising and resolver role for Tera-Pions in UHECR astrophysics has been revealed. | result 0.68 | 0.55 | 0.22 | asserted 1.00 |
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The paper
Original abstract
The role of Sinister Heavy Fermions in recent Glashow's SU(3)*SU(2)*SU(2)'*U(1) model is to offer in a unique frame relic Helium-like products (an ingenious candidate to the dark matter puzzle), a solution to the See-Saw mechanism for light neutrino masses as well as to strong CP violation problem in QCD. The Sinister model requires a three additional families of leptons and quarks, but only the lightest of them Heavy U-quark and E-"electron" are stable. Final neutral Helium-like UUUEE state is an ideal evanescent dark-matter candidate. However it is reached by multi-body interactions along a tail of more manifest secondary frozen blocks. They should be now here polluting the surrounding matter. Moreover, in opposition to effective pair quark annihilations, there is no such an early or late tera-lepton pairs suppressions, because:a) electromagnetic interactions are "weaker" than nuclear ones and b) helium ion 4He++ is able to attract and capture, E-, fixing it into a hybrid tera helium "ion" trap. This leads to a pile up of relic (4HeE)+ traces, a lethal compound for any Sinister Universe. This capture leaves no Tera-Lepton frozen in Ep relic (otherwise an ideal catalyzer to achieve effective late E+E- annihilations possibly saving the model). The (4HeE)+ Coulomb screening is also avoiding the synthesis of the desired UUUEE hidden dark matter gas. The e(4HeE)+ behave chemically like an anomalous hydrogen isotope.Also tera-positronium (eE+) relics are over-abundant and they behave like an anomalous hydrogen atom: these gases do not fit by many orders of magnitude known severe bounds on hydrogen anomalous isotope, making grave shadows over a Sinister Universe. However a surprising and resolver role for Tera-Pions in UHECR astrophysics has been revealed.
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References
How the literature uses it
31 arXiv papers cite this in 66 sentences
Papers citing it · 51 sentences without a confident label
Contests it 2 papers
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The original approach of the sinister model [ref] could not overcome the trouble of overproduction of anomalous hydrogen and helium [ref] .
10 years of dark atoms of composite dark matter · Conclusion · contest 0.89
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In particular, the idea of stable charged particles bound in neutral dark atoms put forward by Sheldon Glashow in his sinister model [ref] found the unrecoverable problem of anomalous istotope overproduction, revealed in [ref] .
Nonstandard cosmologies from physics beyond the Standard model · Composite dark matter and OHe cosmology · contest 0.86
Compares with it 1 paper
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Similar to the case of the AC-leptons [ref] , it differs significantly from the situation revealed in [ref] for the tera-positrons in Glashow's sinister model [ref] .
Strong Interactive Massive Particles from a Strong Coupled Theory · $ζ̅$ annihilation in $ζ$-positronium states · 1.00
Cites it as support 5 papers
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Stability of double and triple $U$ bound states $(UUu)$, $(UUU)$ and $UUu$, $UUU$ is provided by the large chromo-Coulomb binding energy ($∝α_QCD^2 ·m_Q$) [ref] .
Stable quarks of the 4th family? · Introduction · 0.97
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Owing to large chromo-Coulomb binding energy ($∝α_c^2 ·m_U$, where $α_c$ is the QCD constant) stable double and triple $U$ bound states $(UUq)$, $(UUU)$ and their antiparticles $(U̅ U̅ u̅)$, $(U̅ U̅ U̅)$ can exist [ref] .
Dark matter from stable charged particles? · Stable pieces of 4th generation matter · 0.96
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The unrecoverable problem of this scenario, revealed in [ref] , was inevitable overproduction of +1 and +2 charged remnants of incomplete binding, like (Uud), (UUu) hadrons or (UUU)E ions, which bind with ordinary electrons in atomic states that look like anomalous isotopes of hydrogen and helium.
10 years of dark atoms of composite dark matter · Introduction · 0.96
Cites it as background 7 papers
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Recently several elementary particle frames for heavy stable charged particles were considered: (a) A heavy quark quark and heavy neutral lepton lepton (neutrino neutrino with mass above half the Z-Boson mass) of fourth generation [ref] ; which can avoid experimental constraints [ref] and form composite dark matter species [ref] ; (b) A Glashow's “Sinister” heavy tera-quark tera-quark $U$ and tera-electron tera-electron $E$, which can form a tower of tera-hadronic and tera-atomic bound states with “tera-helium atoms” $(UUUEE)$ considered as dominant dark matter [ref] .
Primordial heavy elements in composite dark matter models · Introduction · 0.89
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Recently several elementary particle frames for heavy stable charged particles were proposed: (a) A heavy quark of fourth generation [ref] accompanied by heavy neutrino [ref] ; which can avoid experimental constraints [ref] and form composite dark matter species; (b) A Glashow's “sinister” heavy tera-quark $U$ and tera-electron $E$, forming a tower of tera-hadronic and tera-atomic bound states with “tera-helium atoms” $(UUUEE)$ considered as dominant dark matter [ref] .
Composite dark matter from stable charged constituents · Introduction · 0.81
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In the latter case, WTC offers a new exciting realization of a composite dark matter scenario, which was earlier considered in different aspects in the model of teraparticles [ref] , in the AC model [ref] , based on the approach of an almost commutative geometry [ref] , and in the model of 4th generation [ref] , assuming existence of stable heavy $U$ quark [ref] .
Composite dark matter from a model with composite Higgs boson · Introduction · 0.87
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