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Finding the Strong CP problem at the LHC
High Energy Physics - Phenomenology · Submitted 1 Jul 2015
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We show that a class of parity based solutions to the strong CP problem predicts new colored particles with mass at the TeV scale, due to constraints from Planck suppressed operators.
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The abstract, sentence by sentence
We show that a class of parity based solutions to the strong CP problem predicts new colored particles with mass at the TeV scale, due to constraints from Planck suppressed operators. The new particles are copies of the Standard Model quarks and leptons. The new quarks can be produced at the LHC and are either collider stable or decay into Standard Model quarks through a Higgs, a W or a Z boson. We discuss some simple but generic predictions of the models for the LHC and find signatures not related to the traditional solutions of the hierarchy problem. We thus provide alternative motivation for new physics searches at the weak scale. We also briefly discuss the cosmological history of these models and how to obtain successful baryogenesis.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We show that a class of parity based solutions to the strong CP problem predicts new colored particles with mass at the TeV scale, due to constraints from Planck suppressed operators. | result 0.74 | 0.90 | 0.75 | asserted 1.00 |
| s1 | The new particles are copies of the Standard Model quarks and leptons. | result 0.74 | 0.47 | 0.07 | asserted 1.00 |
| s2 | The new quarks can be produced at the LHC and are either collider stable or decay into Standard Model quarks through a Higgs, a W or a Z boson. | result 0.81 | 0.57 | 0.16 | asserted 0.83 |
| s3 | We discuss some simple but generic predictions of the models for the LHC and find signatures not related to the traditional solutions of the hierarchy problem. | contribution 0.71 | 0.95 | 0.20 | asserted 1.00 |
| s4 | We thus provide alternative motivation for new physics searches at the weak scale. | interpretation 0.99 | 0.77 | 0.34 | asserted 0.99 |
| s5 | We also briefly discuss the cosmological history of these models and how to obtain successful baryogenesis. | contribution 0.98 | 0.75 | 0.04 | asserted 0.62 |
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The paper
Original abstract
We show that a class of parity based solutions to the strong CP problem predicts new colored particles with mass at the TeV scale, due to constraints from Planck suppressed operators. The new particles are copies of the Standard Model quarks and leptons. The new quarks can be produced at the LHC and are either collider stable or decay into Standard Model quarks through a Higgs, a W or a Z boson. We discuss some simple but generic predictions of the models for the LHC and find signatures not related to the traditional solutions of the hierarchy problem. We thus provide alternative motivation for new physics searches at the weak scale. We also briefly discuss the cosmological history of these models and how to obtain successful baryogenesis.
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References
How the literature uses it
17 arXiv papers cite this in 22 sentences
Papers citing it · 14 sentences without a confident label
Cites it as background 8 papers
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The phenomenology of parity solutions to strong CP in this regime was discussed recently in [ref] .
P not PQ · Fermion masses and a low parity-breaking scale · 0.91
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The simplest implementation expands the SM gauge group to $SU(3)×SU(2)_L×SU(2)_R×U(1)_Y$, and parity exchanges $SU(2)_L↔SU(2)_R$ [ref] (see also the recent study [ref] ).
Diphotons, New Vacuum Angles, and Strong CP · Solutions to Strong CP: UV vs. IR · 0.85
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Thus our starting point is a $ℤ_2$ or parity symmetric theory, where the symmetry operation exchanges SM fields for their “mirror” partners.[Similar $_2$-symmetric constructions have been used, for example, to explain dark matter and the baryon asymmetry of the universe, naturalness of the weak scale and to solve the strong CP problem – see Refs. [ref] and references therein.] The discrete symmetry guarantees that the renormalization group running of couplings in the mirror sector is identical to the SM at high scales.
Solving the Wrong Hierarchy Problem · Introduction · 0.85
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