TY - JOUR
T1 - Sharpening mT2 cusps
T2 - The mass determination of semi-invisibly decaying particles from a resonance
AU - Harland-Lang, Lucian A.
AU - Kom, Chun Hay
AU - Sakurai, Kazuki
AU - Tonini, Marco
PY - 2014/6/30
Y1 - 2014/6/30
N2 - We revisit mass determination techniques for the minimum symmetric event topology, namely X pair production followed by X → ℓN, where X and N are unknown particles with the masses to be measured, and N is an invisible particle, concentrating on the case where X is pair produced from a resonance. We consider separate scenarios, with different initial constraints on the invisible particle momenta, and present a systematic method to identify the kinematically allowed mass regions in the (mN, mX ) plane. These allowed regions exhibit a cusp structure at the true mass point, which is equivalent to the one observed in the mT2 endpoints in certain cases. By considering the boundary of the allowed mass region we systematically define kinematical variables which can be used in measuring the unknown masses, and find a new expression for the mT2 variable as well as its inverse. We explicitly apply our method to the case that X is pair produced from a resonance, and as a case study, we consider the process pp → A → χ̃+1 χ̃1-, followed by χ̃1±→ℓ ± ν̃ℓ, in the Minimal Supersymmetric Standard Model and show that our method provides a precise measurement of the chargino and sneutrino masses, mX and mN, at 14 TeV LHC with 300 fb-1 luminosity.
AB - We revisit mass determination techniques for the minimum symmetric event topology, namely X pair production followed by X → ℓN, where X and N are unknown particles with the masses to be measured, and N is an invisible particle, concentrating on the case where X is pair produced from a resonance. We consider separate scenarios, with different initial constraints on the invisible particle momenta, and present a systematic method to identify the kinematically allowed mass regions in the (mN, mX ) plane. These allowed regions exhibit a cusp structure at the true mass point, which is equivalent to the one observed in the mT2 endpoints in certain cases. By considering the boundary of the allowed mass region we systematically define kinematical variables which can be used in measuring the unknown masses, and find a new expression for the mT2 variable as well as its inverse. We explicitly apply our method to the case that X is pair produced from a resonance, and as a case study, we consider the process pp → A → χ̃+1 χ̃1-, followed by χ̃1±→ℓ ± ν̃ℓ, in the Minimal Supersymmetric Standard Model and show that our method provides a precise measurement of the chargino and sneutrino masses, mX and mN, at 14 TeV LHC with 300 fb-1 luminosity.
KW - Supersymmetry Phenomenology
UR - http://www.scopus.com/inward/record.url?scp=84904363107&partnerID=8YFLogxK
U2 - 10.1007/JHEP06(2014)175
DO - 10.1007/JHEP06(2014)175
M3 - Article
AN - SCOPUS:84904363107
SN - 1126-6708
VL - 2014
JO - Journal of High Energy Physics
JF - Journal of High Energy Physics
IS - 6
M1 - 175
ER -