ChildrenKinematics

A set of studies relating to the decay children of truth-tops. These studies aim to investigate the kinematics of the decay products from resonance tops and compare these to background spectator tops. For these studies, the invariant mass of the injected resonance is varied from 400 - 1000 GeV.

Figures Relating to the Study

Figure 3.a) A collection of normalized transverse momentum distributions for truth children originating either resonance and spectator tops at various injected resonance mass points.

Figure 3.b) A collection of stacked normalized transverse momentum distributions using the truth children matched to a resonant top-quark. The overall distribution is partitioned into whether the PDGID of the truth child is a lepton, neutrino, light quark, b-quark or rarely a photon.

Figure 3.c) A collection of stacked normalized transverse momentum distributions using the truth children matched to a spectator top-quark. The overall distribution is partitioned into whether the PDGID of the truth child is a lepton, neutrino, light quark, b-quark or rarely a photon.

Figure 3.d) A collection of normalized pseudorapidity distributions for truth children originating either resonance and spectator tops at various injected resonance mass points.

Figure 3.e) A collection of stacked normalized pseudorapidity distributions using the truth children matched to a resonant top-quark. The overall distribution is partitioned into whether the PDGID of the truth child is a lepton, neutrino, light quark, b-quark or rarely a photon.

Figure 3.f) A collection of stacked normalized pseudorapidity distributions using the truth children matched to a spectator top-quark. The overall distribution is partitioned into whether the PDGID of the truth child is a lepton, neutrino, light quark, b-quark or rarely a photon.

Figure 3.g) A collection of normalized azimuthal distributions for truth children originating either resonance and spectator tops at various injected resonance mass points.

Figure 3.h) A collection of stacked normalized azimuthal distributions using the truth children matched to a resonant top-quark. The overall distribution is partitioned into whether the PDGID of the truth child is a lepton, neutrino, light quark, b-quark or rarely a photon.

Figure 3.i) A collection of stacked normalized azimuthal distributions using the truth children matched to a spectator top-quark. The overall distribution is partitioned into whether the PDGID of the truth child is a lepton, neutrino, light quark, b-quark or rarely a photon.

Figure 3.j) A collection of normalized energy distributions for truth children originating either from resonance and spectator tops at various injected resonance mass points.

Figure 3.k) A collection of stacked normalized energy distributions using the truth children matched to a resonant top-quark. The overall distribution is partitioned into whether the PDGID of the truth child is a lepton, neutrino, light quark or b-quark or rarely a photon.

Figure 3.l) A collection of stacked normalized energy distributions using the truth children matched to a spectator top-quark. The overall distribution is partitioned into whether the PDGID of the truth child is a lepton, neutrino, light quark or b-quark or rarely a photon.

Figure 3.m) A collection of transverse momentum distributions of truth children originating from resonance and spectator and decaying either leptonically or hadronically.

Figure 3.n) A collection of normalized pseudorapidity distributions of truth children originating from resonance and spectator and decaying either leptonically or hadronically.

Figure 3.o) A collection of normalized azimuthal distributions of truth children originating from resonance and spectator and decaying either leptonically or hadronically.

Figure 3.p) A collection of energy distributions of truth children originating from resonance and spectator and decaying either leptonically or hadronically.

Figure 3.q) R between truth children originating from (non)-mutual tops involving resonance and spectator tops.

Figure 3.r) A collection of figures illustrating the fractional transverse momentum dispersed to truth children from resonance tops. The distribution is segmented into whether the PDGID of the truth child is a lepton, neutrino, light quark or b-quark or rarely a photon.

Figure 3.s) A collection of figures illustrating the fractional transverse momentum dispersed to truth children from spectator tops. The distribution is segmented into whether the PDGID of the truth child is a lepton, neutrino, light quark or b-quark or rarely a photon.

Figure 3.t) A collection of figures illustrating the fractional energy dispersed to truth children from resonance tops. The distribution is segmented into whether the PDGID of the truth child is a lepton, neutrino, light quark or b-quark or rarely a photon.

Figure 3.u) A collection of figures illustrating the fractional energy dispersed to truth children from spectator tops. The distribution is segmented into whether the PDGID of the truth child is a lepton, neutrino, light quark or b-quark or rarely a photon.