Application of Statistics in Physics

Claimed by Edwin Solis (April 16th, Spring 2022)

With the development of Quantum Mechanics and Statistical Mechanics, the subject of Statistics has become quintessential for understanding the foundation of these physical theories.

Basics

Probability

Probability is the numerical description of the likelihood of an event occurring from a sample space written as a value between 0 and 1. This event is just the outcome of executing an experiment, and the sample space is just the whole set of outcomes possible from this experiment. Usually, the probability for equally likely outcomes is written mathematically as

[math]\displaystyle{ P(A)=\frac{\text{# Number of times A occurs}}{\text{# Total number of outcomes}} }[/math]

For example, for a six face fair dice, we have a sample space [math]\displaystyle{ S=\{1, 2, 3, 4, 5, 6\} }[/math], where the probability of obtaining a 3 from a dice throw is given by [math]\displaystyle{ P(X=3)=\frac{1}{6} }[/math]. Here the dice throw is the experiment while the event is the outcome of the number obtained from the dice.

Note that we then define the probability of being in the sample space [math]\displaystyle{ P(S) = 1 }[/math] as an axiom and congruent with the definition of probability.

More generally, however, we can define a probability space for an experiment with discrete outcomes as a mathematical function called probability mass function (pmf) [math]\displaystyle{ p(x) }[/math]. In the dice example, the pmf would be written as

[math]\displaystyle{ \begin{align} P(X=x) = p(x)=\begin{cases} \frac{1}{6} &\;|\;x=1,2,3,4,5,6\\ 0 &\;|\;otherwise \end{cases} \end{align} }[/math]

Now, consider an experiment as throwing a dart into a dartboard or measuring the length of a piece of rope. In both cases, we expect that there be infinitely many points where the dart can land and values of length that the rope can have. Therefore, in this case, we find ourselves with a set of continuous values inside the sample space. As there are uncountable possible non-zero probabilities for these points, we would end up with a diverging value for [math]\displaystyle{ P(S) }[/math] which goes against the definition.

Therefore, for these continuous cases, we define the mathematical function, the probability density function (pdf) [math]\displaystyle{ f(x) }[/math]. Instead of assigning a probability for an outcome to take a specific value, the pdf assigns a probability to an interval of values that the outcome could come to have.

For example, if a there is a uniform probability of a bus arriving between [math]\displaystyle{ 10:00\text{ am} \text{ and } 11:00 \text{ am} }[/math], then the pdf of arriving [math]\displaystyle{ t }[/math] minutes after [math]\displaystyle{ 10:00\text{ am} }[/math] would be written as: [math]\displaystyle{ f(x) = \begin{cases} \frac{1}{60} &\;|\;0\leq x \leq 60\\ 0 &\;|\; otherwise \end{cases} }[/math] To obtain the actual probability we integrate over the interval we desire to evaluate. So, for the probability of the bus arriving during the first 10 minutes we would have:

[math]\displaystyle{ P(0\leq X \leq 10) = \int^{10}_0{f(x)\text{d}x} = \frac{1}{6} }[/math]

Therefore, we have the following properties:

Discrete

For the pmf [math]\displaystyle{ p(x) }[/math] with [math]\displaystyle{ n }[/math] possible events,

[math]\displaystyle{ P(X=x) = p(x) }[/math]

[math]\displaystyle{ \sum^n_{i=1}P(X=x_i) = 1 }[/math]

Continuous

For the pdf [math]\displaystyle{ f(x) }[/math],

[math]\displaystyle{ P(a\lt X\lt b)=\int^b_a{f(x)\,\text{d}x} }[/math]

[math]\displaystyle{ P(-\infty\lt X\lt \infty)=\int^{\infty}_{-\infty}{f(x)\,\text{d}x}=1 }[/math]