Figures & data
FIG. 1 Measured concentration dependency on loading: a—in accordance with EquationEquation (3); b—in accordance with Pisani and Thomson's EquationEquation (5).
![FIG. 1 Measured concentration dependency on loading: a—in accordance with EquationEquation (3); b—in accordance with Pisani and Thomson's EquationEquation (5).](/cms/asset/71c1a614-482e-415f-b01a-3eb0cfac8735/uast_a_9705865_o_f0001g.gif)
FIG. 2 Doublet registration probability for two types of particle counters: R 2—for counter with the choice of the first maximum of a photodetector's signal for counting (EquationEquation (11)); R′2—for counter with the choice of the global maximum of a photodetector's signal for counting (numerical calculation).
![FIG. 2 Doublet registration probability for two types of particle counters: R 2—for counter with the choice of the first maximum of a photodetector's signal for counting (EquationEquation (11)); R′2—for counter with the choice of the global maximum of a photodetector's signal for counting (numerical calculation).](/cms/asset/e8b27e86-acd3-43b0-9f0e-0f4843de1be4/uast_a_9705865_o_f0002g.gif)
FIG. 3 Pulse-height probability density functions for counter with square response pulses; mean number of particles in the view volume μ=1; bold line—counter resolution 10%; dotted line—counter resolution 20%.
![FIG. 3 Pulse-height probability density functions for counter with square response pulses; mean number of particles in the view volume μ=1; bold line—counter resolution 10%; dotted line—counter resolution 20%.](/cms/asset/1952bab8-dc6a-48d7-9e8d-c926baa494ff/uast_a_9705865_o_f0003g.gif)
FIG. 4 Isosceles triangular pulse approximation: (a) CPC counter photodetector pulse, (b) superposition of two isosceles triangular pulses for z < τ/2, (c) superposition of two isosceles triangular pulses for z > τ/2 (see the text).
![FIG. 4 Isosceles triangular pulse approximation: (a) CPC counter photodetector pulse, (b) superposition of two isosceles triangular pulses for z < τ/2, (c) superposition of two isosceles triangular pulses for z > τ/2 (see the text).](/cms/asset/b8a81e24-895d-4557-81f5-8639d9f289c1/uast_a_9705865_o_f0004g.gif)
FIG. 5 Doublet pulse-height probability density functions of counter with isosceles triangular pulses; mean number of particles in the view volume μ=1: 1—counter resolution 5%, 2—counter resolution 10%, 3—counter resolution 20%, 4—counter resolution 30%.
![FIG. 5 Doublet pulse-height probability density functions of counter with isosceles triangular pulses; mean number of particles in the view volume μ=1: 1—counter resolution 5%, 2—counter resolution 10%, 3—counter resolution 20%, 4—counter resolution 30%.](/cms/asset/e74e7507-29a1-45d2-9b0d-eae02c112bcd/uast_a_9705865_o_f0005g.gif)
FIG. 6 Doublet pulse-height probability density functions of counter with isosceles triangular pulses; mean number of particles in the view volume μ=3: 1—counter resolution 5%, 2—counter resolution 10%, 3—counter resolution 20%, 4—counter resolution 30%.
![FIG. 6 Doublet pulse-height probability density functions of counter with isosceles triangular pulses; mean number of particles in the view volume μ=3: 1—counter resolution 5%, 2—counter resolution 10%, 3—counter resolution 20%, 4—counter resolution 30%.](/cms/asset/4e24269a-63c6-428f-9e90-078c34578de9/uast_a_9705865_o_f0006g.gif)