In the data sets provided are many variables. Their meanings are described here.
LHCb uses a right-handed coordinate system with the origin at the nominal interaction point. The 'z' axis is along the beam pipe, from the interaction point towards the muon stations. 'y' is vertically upwards and 'x' is towards the centre of the LHC.
- The final state particles are labelled by
K
,Pi
,mu_plus
,mu_minus
. TheK
andPi
combination is labelled byKstar
and the two muons are combined intoJ_psi
. Finally the the B candidate is labelled byB0
.
ProbNNx
- the probability that a given track is positively identified as a given hypotheses. For examplemu_plus_ProbNNmu
is the probability that themu_plus
is a real muon,(1 - mu_plus_ProbNNpi)
would be the probability that it is not a pion.PV
- primary vertex, the point of the proton-proton collisionENDVERTEX
- position of the reconstructed decay vertex of the particleENDVERTEX_CHI2
- of the vertex fit. Essentially how well do the tracks form a vertexIPCHI2
- The IP . The IP is the impact parameter - the perpendicular distance between a trajectory and the PV. The uncertainty is a combination of the vertex and the uncertainty on the particle trajectory. TheIPCHI2
is the square of the IP divided by the square of the uncertainty to from a type qauntity.P
- momentum of the particle in units of MeVPT
- momentum of the particle transverse to the beam line in units of MeVPX
,PY
,PZ
,PE
- components of the 4-momentum.M
, 'mass' - the invariant mass of a particle. If the particle is composite the mass is the product of a fit of the kinematics of the decay products.FD
- distance between a particles end vertex and origin vertex in units of mmFDCHI2
- FD , where the uncertainty is the combination of the of the two verticesETA
- the pseudorapidity of the particleDIRA
- the cosine of the angle between the particle's flight vector and momentum vectorOWNPV
- quantities labelled withOWNPV
mean they are calculated with respect to that particle's assigned primary vertex.