2021
DOI: 10.1103/physrevd.103.055012
|View full text |Cite
|
Sign up to set email alerts
|

Colored scalar mediated nucleon decays to an invisible fermion

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
21
0

Year Published

2021
2021
2024
2024

Publication Types

Select...
6
2

Relationship

0
8

Authors

Journals

citations
Cited by 22 publications
(22 citation statements)
references
References 60 publications
0
21
0
Order By: Relevance
“…Since in Model 2 the interaction of Φ with second generation quarks is independent of y ud and y χd , no concrete predictions for hyperon decays can be made, but a sizable hyperon decay rate is possible. The situation is different for Model 1, for which the allowed branching ratio for n → χγ is smaller than ∼ 10 −6 [273]. This is due to the antisymmetric nature of the Yukawa coupling which forbids interactions of Ψ with only first generation quarks, and the stringent flavor constraints from kaon mixing:…”
Section: Discussion: Relevance For the Neutron Decay Anomaly And B-me...mentioning
confidence: 97%
See 1 more Smart Citation
“…Since in Model 2 the interaction of Φ with second generation quarks is independent of y ud and y χd , no concrete predictions for hyperon decays can be made, but a sizable hyperon decay rate is possible. The situation is different for Model 1, for which the allowed branching ratio for n → χγ is smaller than ∼ 10 −6 [273]. This is due to the antisymmetric nature of the Yukawa coupling which forbids interactions of Ψ with only first generation quarks, and the stringent flavor constraints from kaon mixing:…”
Section: Discussion: Relevance For the Neutron Decay Anomaly And B-me...mentioning
confidence: 97%
“…The studies [268][269][270] (see also [271][272][273][274]) have highlighted that hadrons could have rather large branching fractions into final states containing light dark baryons, which would appear as missing energy in a detector. It is quite remarkable that, in the light of current data, branching fractions as large as 1% for the neutron and 0.5% for the B meson are allowed if the decays occur into states in the dark sector which carry baryon number.…”
Section: Modelmentioning
confidence: 99%
“…Thinking broadly, we emphasize that dark decay models [21,159,160,163,168], even if they ultimately make a negligible contribution to the neutron lifetime anomaly, nevertheless allow for much larger apparent BNV effects than that permitted from direct searches for explicit BNV. For example, the minimal dark sector model with Φ in the (3, 1) 2/3 representation can mediate n → χγ up to the ∼ 10 −6 level, with a Φ at the TeV scale, opening the possibility for its discovery at the LHC [163]. Moreover, this model permits Λ → χγ, for which there are no direct constraints, and it is possible to trade the size of n → χγ for Λ → χγ, or vice versa, given the existing constraint from D 0 − D0 oscillations [163].…”
Section: Implications Of Apparent Bnvmentioning
confidence: 92%
“…Alternatively, e.g., a Φ with (3, 1) 2/3 would also work [21], though it cannot couple to two first-generation d-like quarks; n → χγ can, however, appear via the strange quark content of the neutron [21] or through a one-loop weak process [163]. In contrast, the realization of the invisible decay n → χφ, with the particle content thus far noted, requires the introduction of another Dirac fermion χ as well [21].…”
Section: Implications Of Apparent Bnvmentioning
confidence: 99%
“…In UV complete theories they can be induced via a see-saw like mechanism involving new heavy particles, colored scalars and neutral fermions, with masses ∼ M [33,35]. Hence, for M at few TeV, the underlying theories can be testable at the LHC and future accelerators [35,36]. Operators (3) induce n − n mass mixing (2) with…”
Section: Introductionmentioning
confidence: 99%