RECORD
A natural MSSM from a novel $\mathsf{SO(10)}$, Yukawa unification, light sparticles, and SUSY implications at LHC
High Energy Physics - Phenomenology · Submitted 25 Mar 2025
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Thus a natural deduction of MSSM arises from the $\mathsf{SO(10)}$ model with no fine tuning needed.
The compiled record
The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
Open the compiled record
The abstract, sentence by sentence
The $\mathsf{SO(10)}$ model with a heavy Higgs spectrum consisting of $\mathsf{560+\overline{560}}$ and a light Higgs spectrum consisting of $2\mathsf{\times 10+320}$ plet representations of $\mathsf{SO(10)}$ is unique among $\mathsf{SO(10)}$ models.,It has the remarkable property that VEVs of $\mathsf{560}$ and $\mathsf{\overline{560}}$ can simultaneously reduce the rank of the gauge group and further reduce the remaining symmetry down to the standard model gauge group. Additionally, on mixing with the light fields all the Higgs fields become heavy except for one pair of light Higgs doublets just as in MSSM. This model has not been fully explored thus far because of the technical difficulty of computing the couplings of the heavy and the light Higgs sectors, specifically the interaction $(\mathsf{560\times 560)\cdot 320}$ involving the coupling of tensor-spinors with a third rank ~mixed tensor $\mathsf{320}$. An explicit analysis of such couplings is given in this paper. Spontaneous symmetry breaking of the $\mathsf{SO(10)}$ symmetry is carried out reducing the gauge group to $\mathsf{SU(3)}_c\times \mathsf{SU(2)}_L\times \mathsf{U(1)}_Y$ with just one just pair of light Higgs. Thus a natural deduction of MSSM arises from the $\mathsf{SO(10)}$ model with no fine tuning needed. Further, it is shown that the light Higgs doublet of the model is a linear combination of the Higgs doublet fields of the $2\mathsf{\times 10}$ and the $\mathsf{320}$ Higgs fields. It is shown that in this class of $\mathsf{SO(10)}$ models $b-t-\tau$ unification can be achieved with $\tan\beta$ as low as 5-10. An analysis of the sparticle spectrum within ${\tilde g}$SUGRA renormalization group evolution is given which leads to a bi-modal sparticle spectrum consisting of a compressed low mass spectrum for sleptons and weakinos and a high mass spectrum of gluino, squarks, and heavy Higgs.LHC.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The $\mathsf{SO(10)}$ model with a heavy Higgs spectrum consisting of $\mathsf{560+\overline{560}}$ and a light Higgs spectrum consisting of $2\mathsf{\times 10+320}$ plet representations of $\mathsf{SO(10)}$ is unique among $\mathsf{SO(10)}$ models.,It has the remarkable property that VEVs of $\mathsf{560}$ and $\mathsf{\overline{560}}$ can simultaneously reduce the rank of the gauge group and further reduce the remaining symmetry down to the standard model gauge group. | background 0.63 | 0.22 | 0.12 | asserted 1.00 |
| s1 | Additionally, on mixing with the light fields all the Higgs fields become heavy except for one pair of light Higgs doublets just as in MSSM. | result 0.88 | 0.51 | 0.09 | asserted 1.00 |
| s2 | This model has not been fully explored thus far because of the technical difficulty of computing the couplings of the heavy and the light Higgs sectors, specifically the interaction $(\mathsf{560\times 560)\cdot 320}$ involving the coupling of tensor-spinors with a third rank ~mixed tensor $\mathsf{320}$. | gap 0.99 | 0.09 | 0.03 | asserted 1.00 |
| s3 | An explicit analysis of such couplings is given in this paper. | contribution 1.00 | 0.88 | 0.04 | asserted 0.99 |
| s4 | Spontaneous symmetry breaking of the $\mathsf{SO(10)}$ symmetry is carried out reducing the gauge group to $\mathsf{SU(3)}_c\times \mathsf{SU(2)}_L\times \mathsf{U(1)}_Y$ with just one just pair of light Higgs. | result 0.49 | 0.82 | 0.13 | asserted 1.00 |
| s5 | Thus a natural deduction of MSSM arises from the $\mathsf{SO(10)}$ model with no fine tuning needed. | interpretation 0.86 | 0.74 | 0.51 | asserted 1.00 |
| s6 | Further, it is shown that the light Higgs doublet of the model is a linear combination of the Higgs doublet fields of the $2\mathsf{\times 10}$ and the $\mathsf{320}$ Higgs fields. | result 0.98 | 0.90 | 0.07 | asserted 1.00 |
| s7 | It is shown that in this class of $\mathsf{SO(10)}$ models $b-t-\tau$ unification can be achieved with $\tan\beta$ as low as 5-10. | result 0.99 | 0.88 | 0.12 | asserted 0.98 |
| s8 | An analysis of the sparticle spectrum within ${\tilde g}$SUGRA renormalization group evolution is given which leads to a bi-modal sparticle spectrum consisting of a compressed low mass spectrum for sleptons and weakinos and a high mass spectrum of gluino, squarks, and heavy Higgs.LHC. | result 0.87 | 0.92 | 0.18 | asserted 1.00 |
What was examined, and what was not
- arXiv listing abstract v1
- full text
- figures and tables
- references and citing sentences
- relations to other papers
- P abstract
- S sections
- T body sentences
- C citations
- R cross-paper relations
The paper
Original abstract
The $\mathsf{SO(10)}$ model with a heavy Higgs spectrum consisting of $\mathsf{560+\overline{560}}$ and a light Higgs spectrum consisting of $2\mathsf{\times 10+320}$ plet representations of $\mathsf{SO(10)}$ is unique among $\mathsf{SO(10)}$ models.,It has the remarkable property that VEVs of $\mathsf{560}$ and $\mathsf{\overline{560}}$ can simultaneously reduce the rank of the gauge group and further reduce the remaining symmetry down to the standard model gauge group. Additionally, on mixing with the light fields all the Higgs fields become heavy except for one pair of light Higgs doublets just as in MSSM. This model has not been fully explored thus far because of the technical difficulty of computing the couplings of the heavy and the light Higgs sectors, specifically the interaction $(\mathsf{560\times 560)\cdot 320}$ involving the coupling of tensor-spinors with a third rank ~mixed tensor $\mathsf{320}$. An explicit analysis of such couplings is given in this paper. Spontaneous symmetry breaking of the $\mathsf{SO(10)}$ symmetry is carried out reducing the gauge group to $\mathsf{SU(3)}_c\times \mathsf{SU(2)}_L\times \mathsf{U(1)}_Y$ with just one just pair of light Higgs. Thus a natural deduction of MSSM arises from the $\mathsf{SO(10)}$ model with no fine tuning needed. Further, it is shown that the light Higgs doublet of the model is a linear combination of the Higgs doublet fields of the $2\mathsf{\times 10}$ and the $\mathsf{320}$ Higgs fields. It is shown that in this class of $\mathsf{SO(10)}$ models $b-t-\tau$ unification can be achieved with $\tan\beta$ as low as 5-10. An analysis of the sparticle spectrum within ${\tilde g}$SUGRA renormalization group evolution is given which leads to a bi-modal sparticle spectrum consisting of a compressed low mass spectrum for sleptons and weakinos and a high mass spectrum of gluino, squarks, and heavy Higgs.LHC.
Human review
How the literature uses it
2 arXiv papers cite this in 2 sentences
Discussion
Know something about this paper? Leave a comment, or highlight any passage above to comment on it.