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Original Articles

Registration Probabilities and Pulse-Height Distributions of Coincidences in Optical Particle Counters

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Pages 155-164 | Received 01 Apr 2003, Accepted 01 Jul 2003, Published online: 17 Aug 2010

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).

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)); R2—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).

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%.

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).

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%.

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%.

FIG. 7 Doublet pulse-height probability density functions of counter with Gaussian pulses; mean number of particles in the view volume μ=0.05: 1—counter resolution 5%, 2—counter resolution 10%, 3—counter resolution 20%, 4—counter resolution 30%.

FIG. 7 Doublet pulse-height probability density functions of counter with Gaussian pulses; mean number of particles in the view volume μ=0.05: 1—counter resolution 5%, 2—counter resolution 10%, 3—counter resolution 20%, 4—counter resolution 30%.

FIG. 8 Doublet pulse-height probability density functions of counter with Gaussian 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. 8 Doublet pulse-height probability density functions of counter with Gaussian 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%.

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