Abstract

We show how exotic stringy instantons can generate an effective interaction between color diquark sextets in a Pati-Salam model, inducing a Majorana mass term for the neutron. In particular, we discuss a simple quiver theory for a Pati-Salam like model, as an example in which the calculations of exotic instanton effects are simple and controllable. We discuss some different possibilities in order to generate $$ n-\overline{n} $$ oscillations testable in the next generation of experiments, Majorana mass matrices for neutrini and a Post-Sphaleron Baryogenesis scenario. Connections with Dark Matter issues and the Higgs mass Hierarchy problem are discussed, in view of implications for LHC and rare processes physics. The model may be viewed as a completion of a Left-Right symmetric extension of the Standard Model, alternative to a GUT-inspired scenario. Combined measures in Neutron-Antineutron physics, FCNC, LHC, Dark Matter could rule out the proposed model or uncover aspects of physics at the Planck scale!

Highlights

  • InstantonsIn 4-dimensional gauge theory, instantons are point-like configurations, that extremize the Euclidean action for a given topological charge

  • We show how exotic stringy instantons can generate an effective interaction between color diquark sextets in a Pati-Salam model, inducing a Majorana mass term for the neutron

  • We discuss some different possibilities in order to generate n − noscillations testable in the generation of experiments, Majorana mass matrices for neutrini and a Post-Sphaleron Baryogenesis scenario

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Summary

Instantons

In 4-dimensional gauge theory, instantons are point-like configurations, that extremize the Euclidean action for a given topological charge. Instantons admit a simple geometric interpretation: they are special Euclidean branes wrapping some (internal) cycle. In theories with (unoriented) open strings, these are Euclidean D-branes (E-branes) that can intersect the ‘physical’ D-branes.. In (un-)oriented type IIA, gauge instantons can be classified as Euclidean D2 (E2) branes wrapping the same 3-cycle as a stack of “physical” D6-branes. In (un-)oriented IIB, instantons are E(-1) or E3 wrapping the same holomorphic divisor as a stack of “physical” D7-branes. In type I, instantons are E5 branes in the internal space, with the same magnetization as the D9, wrapping the entire CY3

Quivers
An unoriented quiver for a Pati-Salam model
M1 φαβ
No-proton decays
Neutron-Antineutron oscillation through color diquark sextets
Conclusions and remarks
Full Text
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