A bstract We explore baryon-number-violating (|∆ B | = 2) processes beyond the well-known neutron-antineutron ( $$ n-\overline{n} $$ <mml:math xmlns:mml="http://www.
A bstract We explore baryon-number-violating (|∆ B | = 2) processes beyond the well-known neutron-antineutron ( n-n̄ n − n ¯ ) oscillations, focusing on the Λ -Λ̄ Λ − Λ ¯ system. The presence of a strange quark in the Λ baryon introduces a new set of six-quark operators roughly of the form ( uds ) 2 , which are different from the ( udd ) 2 operators responsible for n-n̄ n − n ¯ oscillations. Using the Standard Model Effective Field Theory (SMEFT), we classify all dimension-9 operators that cause |∆ B | = 2 transitions and study their UV completions mediated by exotic scalar fields with trilinear interactions. We demonstrate that in these models, Λ -Λ̄ Λ − Λ ¯ oscillations can occur at tree level, with n-n̄ n − n ¯ mixing potentially appearing at higher loop levels. We employ a chiral effective theory to constrain the effective mass mixing δm Λ , deriving bounds from current experimental limits on n-n̄ n − n ¯ oscillations and dinucleon decays such as pp → K + K + . These bounds indicate that Λ -Λ̄ Λ − Λ ¯ oscillations probe a complementary parameter space, sensitive to baryon-number violation at scales up to 10 2 − 10 3 TeV. We show that the existing indirect bounds make it challenging to provide a competitive bound on δm Λ at BESIII.
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Beneito et al. (2026) studied this question.
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