TY - JOUR
T1 - Using sorted invariant mass variables to evade combinatorial ambiguities in cascade decays
AU - Kim, Doojin
AU - Matchev, Konstantin T.
AU - Park, Myeonghun
N1 - Publisher Copyright:
© 2016, The Author(s).
PY - 2016/2/1
Y1 - 2016/2/1
N2 - Abstract: The classic method for mass determination in a SUSY-like cascade decay chain relies on measurements of the kinematic endpoints in the invariant mass distributions of suitable collections of visible decay products. However, the procedure is complicated by combinatorial ambiguities: e.g., the visible final state particles may be indistinguishable (as in the case of QCD jets), or one may not know the exact order in which they are emitted along the decay chain. In order to avoid such combinatorial ambiguities, we propose to treat the final state particles fully democratically and consider the sorted set of the invariant masses of all possible partitions of the visible particles in the decay chain. In particular, for a decay to N visible particles, one considers the sorted sets of all possible n-body invariant mass combinations (2 ≤ n ≤ N) and determines the kinematic endpoint m(n,r) max of the distribution of the r-th largest n-body invariant mass m(n,r) for each possible value of n and r. For the classic example of a squark decay in supersymmetry, we provide analytical formulas for the interpretation of these endpoints in terms of the underlying physical masses. We point out that these measurements can be used to determine the structure of the decay topology, e.g., the number and position of intermediate on-shell resonances.
AB - Abstract: The classic method for mass determination in a SUSY-like cascade decay chain relies on measurements of the kinematic endpoints in the invariant mass distributions of suitable collections of visible decay products. However, the procedure is complicated by combinatorial ambiguities: e.g., the visible final state particles may be indistinguishable (as in the case of QCD jets), or one may not know the exact order in which they are emitted along the decay chain. In order to avoid such combinatorial ambiguities, we propose to treat the final state particles fully democratically and consider the sorted set of the invariant masses of all possible partitions of the visible particles in the decay chain. In particular, for a decay to N visible particles, one considers the sorted sets of all possible n-body invariant mass combinations (2 ≤ n ≤ N) and determines the kinematic endpoint m(n,r) max of the distribution of the r-th largest n-body invariant mass m(n,r) for each possible value of n and r. For the classic example of a squark decay in supersymmetry, we provide analytical formulas for the interpretation of these endpoints in terms of the underlying physical masses. We point out that these measurements can be used to determine the structure of the decay topology, e.g., the number and position of intermediate on-shell resonances.
KW - Deep Inelastic Scattering (Phenomenology)
UR - https://www.scopus.com/pages/publications/84963812906
U2 - 10.1007/JHEP02(2016)129
DO - 10.1007/JHEP02(2016)129
M3 - Article
AN - SCOPUS:84963812906
SN - 1126-6708
VL - 2016
SP - 1
EP - 41
JO - Journal of High Energy Physics
JF - Journal of High Energy Physics
IS - 2
M1 - 129
ER -