The baryonic decay Lambda_b -> Lambda_c(-> Lambda pi) tau nu provides an independent probe of the R(D(*)) anomalies, with (C_VL, C_SR) as the most favored new physics solution and observables like K_1c, K_2ss showing high sensitivity.
Aokiet al., Review of lattice results concerning low-energy particle physics,Eur
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Extending the Glauber-Sitenko diffraction model for H(d,p)X by including longitudinal momentum Qz and transverse p_perp effects yields a decrease in cross section with rising transverse momentum and a modest shift plus growth in the cross-section peak.
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The Angular Observables of $\Lambda_b \to \Lambda_c(\to \Lambda^0 \pi^+) \, \tau^-(\to \pi^- \nu_\tau)\, \bar{\nu}_\tau$ within the Paradigm of FCCC Anomalies
The baryonic decay Lambda_b -> Lambda_c(-> Lambda pi) tau nu provides an independent probe of the R(D(*)) anomalies, with (C_VL, C_SR) as the most favored new physics solution and observables like K_1c, K_2ss showing high sensitivity.
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Inclusion of the Longitudinal Momentum-Transfer Component and Kinematic Factors in a diffraction approach for H(d,p)X Reactions
Extending the Glauber-Sitenko diffraction model for H(d,p)X by including longitudinal momentum Qz and transverse p_perp effects yields a decrease in cross section with rising transverse momentum and a modest shift plus growth in the cross-section peak.