no code implementations • 21 May 2021 • Doojin Kim, Kyoungchul Kong, Konstantin T. Matchev, Myeonghun Park, Prasanth Shyamsundar
The choice of optimal event variables is crucial for achieving the maximal sensitivity of experimental analyses.
no code implementations • 21 Jan 2021 • P. S. Bhupal Dev, Doojin Kim, Kuver Sinha, Yongchao Zhang
There are broadly three channels to probe axion-like particles (ALPs) produced in the laboratory: through their subsequent decay to Standard Model (SM) particles, their scattering with SM particles, or their subsequent conversion to photons.
High Energy Physics - Phenomenology High Energy Physics - Experiment
1 code implementation • 20 Dec 2016 • Doojin Kim, Jong-Chul Park, Seodong Shin
We propose a novel dark matter (DM) detection strategy for the models with non-minimal dark sector.
High Energy Physics - Phenomenology High Energy Physics - Experiment
1 code implementation • 3 Aug 2015 • Won Sang Cho, James S. Gainer, Doojin Kim, Sung Hak Lim, Konstantin T. Matchev, Filip Moortgat, Luc Pape, Myeonghun Park
Reconstructed mass variables, such as $M_2$, $M_{2C}$, $M_T^\star$, and $M_{T2}^W$, play an essential role in searches for new physics at hadron colliders.
High Energy Physics - Phenomenology High Energy Physics - Experiment
1 code implementation • 7 Jan 2014 • Won Sang Cho, James S. Gainer, Doojin Kim, Konstantin T. Matchev, Filip Moortgat, Luc Pape, Myeonghun Park
The tests are able to determine: 1) whether the decays in the event are two-body or three-body, 2) if the decay is two-body, whether the intermediate resonances in the two decay chains are the same, and 3) the exact sequence in which the visible particles are emitted from each decay chain.
High Energy Physics - Phenomenology High Energy Physics - Experiment
