dE/dx is an unsuitable quantity to deal with PID, what is needed are straggling functions. The theory and understanding needed for PID will be presented. Instrumental effects must also be calculated and understood. 1 Introduction. 1.1 General concepts The concept dE/dx representing the mean rate of energy loss in an absorber [1] is used inappropriately in the description of the physics of most high energy particle detectors. Consider Fig. 1 which gives the probability density function (p.d.f.) f(∆) for energy losses ∆ of particles 1 with βγ = 3.
Particle identification in intermediate heavy-ion collisions, using a modern 4 pi detector which con...
Recent theoretical results have led to improvements in formulas for dE=dx, particularly in the regim...
Proton-deuteron identification at energies between 2.5 MeV and 6 MeV has been studied as a function ...
Particle identification, PID, is of crucial importance in most experiments. The requirement can rang...
The performance of existing or nearly completed detectors for particle identification by using the r...
Ionization losses - dE/dx - in CMD-3 drift chamber describe charged particle track. dE/dx value help...
This paper deals with two major particle identification methods: dE/dx and Cherenkov detection. In t...
A particle identification method is presented, in which calculations of AE energy losses are stored ...
The Photoproduction of neutral kaons off a deuteron target has been investigated at the Tohoku Unive...
We review some basic features of dE/dx particle identification that are relevant to high energy phys...
The particle identification capabilities of the ALICE experiment are unique among the four major LHC...
Some complementary methods are proposed for an identification of charged particles based on $dE/dx$ ...
Equipping an experiment at FCC-ee with particle identification (PID) capabilities, in particular the...
We performed a calculation of the energy loss dE/dx and the primary ionization density dN/dx for a c...
Particle IDentification (PID) is fundamental to particle physics experiments. This paper reviews PID...
Particle identification in intermediate heavy-ion collisions, using a modern 4 pi detector which con...
Recent theoretical results have led to improvements in formulas for dE=dx, particularly in the regim...
Proton-deuteron identification at energies between 2.5 MeV and 6 MeV has been studied as a function ...
Particle identification, PID, is of crucial importance in most experiments. The requirement can rang...
The performance of existing or nearly completed detectors for particle identification by using the r...
Ionization losses - dE/dx - in CMD-3 drift chamber describe charged particle track. dE/dx value help...
This paper deals with two major particle identification methods: dE/dx and Cherenkov detection. In t...
A particle identification method is presented, in which calculations of AE energy losses are stored ...
The Photoproduction of neutral kaons off a deuteron target has been investigated at the Tohoku Unive...
We review some basic features of dE/dx particle identification that are relevant to high energy phys...
The particle identification capabilities of the ALICE experiment are unique among the four major LHC...
Some complementary methods are proposed for an identification of charged particles based on $dE/dx$ ...
Equipping an experiment at FCC-ee with particle identification (PID) capabilities, in particular the...
We performed a calculation of the energy loss dE/dx and the primary ionization density dN/dx for a c...
Particle IDentification (PID) is fundamental to particle physics experiments. This paper reviews PID...
Particle identification in intermediate heavy-ion collisions, using a modern 4 pi detector which con...
Recent theoretical results have led to improvements in formulas for dE=dx, particularly in the regim...
Proton-deuteron identification at energies between 2.5 MeV and 6 MeV has been studied as a function ...