Difference between revisions of "Poisson Statistics"

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== Background ==
 
== Background ==
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The Poisson distribution can characterize random events that occur at a well-defined average rate. It is widely used in atomic and sub-atomic physics. The Poisson distribution is effective in a variety of statistical applications. The most common involve event probabilities, but several assumptions must hold true: i) the rate at which random events
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occur does not change for the duration of the measurement; ii) the occurrence of one event does not change the likelihood of another event; iii) events occur at a slow enough rate that they can be individually distinguished.
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In this experiment, Poisson statistics will be used to analyze random radioactive decay events that occur in a defined time interval. A decay occurs an integer k number of times in the interval, including possibly not at all <math>\hat{S} = \hat{\sigma}_+ +\hat{\sigma}_-</math>. The average number of events expected in a defined time interval is λ, known as the event rate. Given λ,
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the probability of observing k events in the time interval is :
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[http://www.unm.edu/~mph/307/Poisson_UNM2.pdf Experiment Instructions (pdf)]
 
[http://www.unm.edu/~mph/307/Poisson_UNM2.pdf Experiment Instructions (pdf)]
 
  
 
== Background Reading ==
 
== Background Reading ==

Revision as of 21:24, 3 February 2020

Background

The Poisson distribution can characterize random events that occur at a well-defined average rate. It is widely used in atomic and sub-atomic physics. The Poisson distribution is effective in a variety of statistical applications. The most common involve event probabilities, but several assumptions must hold true: i) the rate at which random events occur does not change for the duration of the measurement; ii) the occurrence of one event does not change the likelihood of another event; iii) events occur at a slow enough rate that they can be individually distinguished.

In this experiment, Poisson statistics will be used to analyze random radioactive decay events that occur in a defined time interval. A decay occurs an integer k number of times in the interval, including possibly not at all Failed to parse (Missing <code>texvc</code> executable. Please see math/README to configure.): \hat{S} = \hat{\sigma}_+ +\hat{\sigma}_- . The average number of events expected in a defined time interval is λ, known as the event rate. Given λ, the probability of observing k events in the time interval is :


Experiment Instructions (pdf)

Background Reading

The Poisson Distribution


History

Experiment set up and verified by Martin Hoeferkamp, January 2020