The unified theory at eleven parameters and the experiments: instrument by instrument, what is tested and what would refute
Abstract
The theory at eleven parameters predicts by identities and exact zeros, with a few numbers beside them, and its twenty-five papers state those predictions where the algebra that produces them is, sector by sector. An experimentalist reads the other way, instrument by instrument. This paper reorganises the series for that reader. It takes each class of instrument in turn: the colliders, the neutrino experiments, the precision measurements at low energy, the strong-field lasers, the gravitational tests from the solar system to the black-hole ringdowns, the astrophysical objects, the dark-matter searches and the cosmological surveys. For each it states what the theory says the instrument will find, whether the statement is an identity, a conditional or a located number, and what result would refute it. The statements are the series'. The Higgs self-coupling is at its Standard-Model value up to the loops of a permitted second doublet, there is no new gauge boson and no proton decay within reach, and the constants are constant. There is no fifth force and no composition dependence of free fall, Einstein's exterior for every black hole and no echo, and tensor polarisations only. The Schwinger field is the electron's acceleration bound with the Furrypicture rates on both sides of it, and the electric dipole moments and magnetic anomalies are the Standard Model's. There are three right-handed neutrinos with a benchmark at 88.5 GeV, a second Higgs doublet permitted at or above a TeV, three dark-matter candidates permitted and none predicted, and the Palatini plateau's spectral index of 0.960 at most. The paper adds the state of each measurement in 2026 and the instrument and date that decide it, and ranks what fires first. First the spectral index, the dark-energy equation of state and the cosmic birefringence, three hints already leaning against one bound and two zeros. Then the searches for the doublet at Belle II and the LHC and for the inert doublet at LZ and IceCube; then the neutrino ordering and the neutrinoless decay; then the tensor ratio, the echoes at the third-generation detectors and the top mass at a future collider. The neutrino experiments are one section; the theory of the neutrino sector, which has more to say than the instruments can yet hear, is left to a paper of its own.
Related
- Feynman diagrams of the unified theory at eleven parameters
- Renormalisation of the unified theory at eleven parameters
- The new particle allowed by the unified theory at eleven parameters: the second doublet of the empty slot and where to look for it
- The unified theory at eleven parameters: general relativity and the Standard Model on one algebra
- The inverse of the algebraic element of the unified theory at eleven parameters, M 4 (C) ⊕ M 4 (H) ⊕ M 12 (C)
BibTeX
@misc{reynaud2026unified,
title = {{The unified theory at eleven parameters and the experiments: instrument by instrument, what is tested and what would refute}},
author = {Patrick B. Reynaud},
howpublished = {HAL},
year = {2026},
month = sep,
url = {https://hal.science/hal-05765511v2},
note = {CC BY 4.0},
}
RIS
TY - UNPB
TI - The unified theory at eleven parameters and the experiments: instrument by instrument, what is tested and what would refute
AU - Patrick B. Reynaud
PY - 2026
DA - 2026/09/26
PB - HAL
UR - https://hal.science/hal-05765511v2
AB - The theory at eleven parameters predicts by identities and exact zeros, with a few numbers beside them, and its twenty-five papers state those predictions where the algebra that produces them is, sector by sector. An experimentalist reads the other way, instrument by instrument. This paper reorganises the series for that reader. It takes each class of instrument in turn: the colliders, the neutrino experiments, the precision measurements at low energy, the strong-field lasers, the gravitational tests from the solar system to the black-hole ringdowns, the astrophysical objects, the dark-matter searches and the cosmological surveys. For each it states what the theory says the instrument will find, whether the statement is an identity, a conditional or a located number, and what result would refute it. The statements are the series'. The Higgs self-coupling is at its Standard-Model value up to the loops of a permitted second doublet, there is no new gauge boson and no proton decay within reach, and the constants are constant. There is no fifth force and no composition dependence of free fall, Einstein's exterior for every black hole and no echo, and tensor polarisations only. The Schwinger field is the electron's acceleration bound with the Furrypicture rates on both sides of it, and the electric dipole moments and magnetic anomalies are the Standard Model's. There are three right-handed neutrinos with a benchmark at 88.5 GeV, a second Higgs doublet permitted at or above a TeV, three dark-matter candidates permitted and none predicted, and the Palatini plateau's spectral index of 0.960 at most. The paper adds the state of each measurement in 2026 and the instrument and date that decide it, and ranks what fires first. First the spectral index, the dark-energy equation of state and the cosmic birefringence, three hints already leaning against one bound and two zeros. Then the searches for the doublet at Belle II and the LHC and for the inert doublet at LZ and IceCube; then the neutrino ordering and the neutrinoless decay; then the tensor ratio, the echoes at the third-generation detectors and the top mass at a future collider. The neutrino experiments are one section; the theory of the neutrino sector, which has more to say than the instruments can yet hear, is left to a paper of its own.
ER -