Abstract

The interactions between nucleons contain a parity-violating component, which originates in the weak interaction between quarks and which is suppressed by a factor of approximately 10−7 compared to the dominant parity-conserving component. A theoretical framework based on effective field theory methods to analyze and interpret parity-violating interactions between nucleons is described and a number of applications are discussed.

Highlights

  • Interactions between nucleons are dominated by strong and electromagnetic effects, which conserve parity

  • There is a parity-violating (PV) component to nucleon-nucleon interactions, which is expected to be suppressed by a factor of roughly 10−7 to 10−6 compared to the parity-conserving (PC) component

  • The PV part of the nucleon interactions stems from an interplay of weak interactions between quarks and the strong interactions that confine the quarks into nucleons

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Summary

Introduction

Interactions between nucleons are dominated by strong and electromagnetic effects, which conserve parity. There is a parity-violating (PV) component to nucleon-nucleon interactions, which is expected to be suppressed by a factor of roughly 10−7 to 10−6 compared to the parity-conserving (PC) component. Parity-violating effects can be isolated in pseudoscalar observables, which would vanish if parity was conserved. Such observables include longitudinal and angular asymmetries, as well as induced polarizations in capture, break-up, and transmission experiments. While PV effects can be enhanced by several orders of magnitude in heavier systems I describe an approach to hadronic parity violation based on effective field theory (EFT) and present selected results from two- and three-nucleon systems

Hadronic parity violation in pionless EFT
Two-nucleon systems
Three-nucleon systems
Findings
Conclusions and outlook
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