Litcius/Paper detail

Collider signature of <i>U</i> <sub>1</sub> Leptoquark and constraints from <i>b</i>  →  <i>c</i> observables

Aritra Biswas, Dilip Kumar Ghosh, Nivedita Ghosh, Avirup Shaw, Abhaya Kumar Swain

2020Journal of Physics G Nuclear and Particle Physics23 citationsDOIOpen Access PDF

Abstract

Abstract One of the most popular models that is known to be able to solve the lepton flavour universality violating charged ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi>b</mml:mi> <mml:mo>→</mml:mo> <mml:mi>c</mml:mi> </mml:math> ) and neutral current ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi>b</mml:mi> <mml:mo>→</mml:mo> <mml:mi>s</mml:mi> </mml:math> ) anomalies is the Leptoquark Model. In this work we examine the multijet + <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msub> <mml:mrow> <mml:menclose notation="updiagonalstrike"> <mml:mi>E</mml:mi> </mml:menclose> </mml:mrow> <mml:mrow> <mml:mi>T</mml:mi> </mml:mrow> </mml:msub> </mml:math> collider signature of a vector leptoquark ( U 1 ) which has the potential to mediate both the charged and neutral current processes at tree level. From our collider analysis we derive the exclusion limits on mass for the U 1 leptoquark at 95% C.L. at the current and future experiment of the Large Hadron Collider. We also calculate the effect of such a leptoquark in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi>b</mml:mi> <mml:mo>→</mml:mo> <mml:mi>c</mml:mi> </mml:math> observables.

Topics & Concepts

LeptoquarkPhysicsParticle physicsObservableLeptonColliderPhysics beyond the Standard ModelUniversality (dynamical systems)Neutral currentLarge Hadron ColliderNuclear physicsNeutrinoQuantum mechanicsElectronParticle physics theoretical and experimental studiesDark Matter and Cosmic PhenomenaComputational Physics and Python Applications