probability axioms

{{Short description|Foundations of probability theory}}

{{Probability fundamentals}}

The standard probability axioms are the foundations of probability theory introduced by Russian mathematician Andrey Kolmogorov in 1933.{{Cite book |title=Foundations of the theory of probability |url=https://archive.org/details/foundationsofthe00kolm |last=Kolmogorov |first=Andrey |publisher=Chelsea Publishing Company |year=1950 |orig-date=1933 |location=New York, US }} These axioms remain central and have direct contributions to mathematics, the physical sciences, and real-world probability cases.{{Cite web |url=https://www.stat.berkeley.edu/~aldous/Real_World/kolmogorov.html |title=What is the significance of the Kolmogorov axioms? |last=Aldous |first=David |website=David Aldous |access-date=November 19, 2019}}

There are several other (equivalent) approaches to formalising probability. Bayesians will often motivate the Kolmogorov axioms by invoking Cox's theorem or the Dutch book arguments instead.{{Cite journal | last = Cox | first = R. T. | author-link = Richard Threlkeld Cox| doi = 10.1119/1.1990764 | title = Probability, Frequency and Reasonable Expectation | journal = American Journal of Physics | volume = 14 | pages = 1–10 | year = 1946 | issue = 1 | bibcode = 1946AmJPh..14....1C }}{{cite book|first=R. T. |last=Cox |author-link=Richard Threlkeld Cox |title=The Algebra of Probable Inference |publisher=Johns Hopkins University Press |location=Baltimore, MD |year=1961 }}

Kolmogorov axioms

The assumptions as to setting up the axioms can be summarised as follows: Let (\Omega, F, P) be a measure space such that P(E) is the probability of some event E, and P(\Omega) = 1. Then (\Omega, F, P) is a probability space, with sample space \Omega, event space F and probability measure P.

={{Anchor|Non-negativity}}First axiom =

The probability of an event is a non-negative real number:

:P(E)\in\mathbb{R}, P(E)\geq 0 \qquad \forall E \in F

where F is the event space. It follows (when combined with the second axiom) that P(E) is always finite, in contrast with more general measure theory. Theories which assign negative probability relax the first axiom.

= {{Anchor|Unitarity|Normalization}}Second axiom =

This is the assumption of unit measure: that the probability that at least one of the elementary events in the entire sample space will occur is 1.

: P(\Omega) = 1

= {{Anchor|Sigma additivity|Finite additivity|Countable additivity|Finitely additive}}Third axiom =

This is the assumption of σ-additivity:

: Any countable sequence of disjoint sets (synonymous with mutually exclusive events) E_1, E_2, \ldots satisfies

::P\left(\bigcup_{i = 1}^\infty E_i\right) = \sum_{i=1}^\infty P(E_i).

Some authors consider merely finitely additive probability spaces, in which case one just needs an algebra of sets, rather than a σ-algebra.{{Cite web|url=https://plato.stanford.edu/entries/probability-interpret/#KolProCal|title=Interpretations of Probability|last=Hájek|first=Alan|date=August 28, 2019|website=Stanford Encyclopedia of Philosophy|access-date=November 17, 2019}} Quasiprobability distributions in general relax the third axiom.

Consequences

From the Kolmogorov axioms, one can deduce other useful rules for studying probabilities. The proofs{{Cite book|title=A first course in probability|last=Ross, Sheldon M.|year=2014|isbn=978-0-321-79477-2|edition=Ninth|location=Upper Saddle River, New Jersey|pages=27, 28|oclc=827003384}}{{Cite web|url=https://dcgerard.github.io/stat234/11_proofs_from_axioms.pdf|title=Proofs from axioms|last=Gerard|first=David|date=December 9, 2017|access-date=November 20, 2019}}{{Cite web|url=http://www.maths.qmul.ac.uk/~bill/MTH4107/notesweek3_10.pdf|title=Probability (Lecture Notes - Week 3)|last=Jackson|first=Bill|date=2010|website=School of Mathematics, Queen Mary University of London|access-date=November 20, 2019}} of these rules are a very insightful procedure that illustrates the power of the third axiom, and its interaction with the prior two axioms. Four of the immediate corollaries and their proofs are shown below:

= Monotonicity =

:\quad\text{if}\quad A\subseteq B\quad\text{then}\quad P(A)\leq P(B).

If A is a subset of, or equal to B, then the probability of A is less than, or equal to the probability of B.

== ''Proof of monotonicity''<ref name=":1" /> ==

In order to verify the monotonicity property, we set E_1=A and E_2=B\setminus A, where A\subseteq B and E_i=\varnothing for i\geq 3. From the properties of the empty set (\varnothing), it is easy to see that the sets E_i are pairwise disjoint and E_1\cup E_2\cup\cdots=B. Hence, we obtain from the third axiom that

:P(A)+P(B\setminus A)+\sum_{i=3}^\infty P(E_i)=P(B).

Since, by the first axiom, the left-hand side of this equation is a series of non-negative numbers, and since it converges to P(B) which is finite, we obtain both P(A)\leq P(B) and P(\varnothing)=0.

= The probability of the empty set =

: P(\varnothing)=0.

In many cases, \varnothing is not the only event with probability 0.

== ''Proof of the probability of the empty set''==

P(\varnothing \cup \varnothing) = P(\varnothing) since \varnothing \cup \varnothing = \varnothing,

P(\varnothing)+P(\varnothing) = P(\varnothing) by applying the third axiom to the left-hand side

(note \varnothing is disjoint with itself), and so

P(\varnothing) = 0 by subtracting P(\varnothing) from each side of the equation.

= The complement rule =

P\left(A^{\complement}\right) = P(\Omega-A) = 1 - P(A)

== ''Proof of the complement rule'' ==

Given A and A^{\complement} are mutually exclusive and that A \cup A^\complement = \Omega

:

P(A \cup A^\complement)=P(A)+P(A^\complement)

... (by axiom 3)

and,

P(A \cup A^\complement)=P(\Omega)=1

... (by axiom 2)

\Rightarrow P(A)+P(A^\complement)=1

\therefore P(A^\complement)=1-P(A)

= The numeric bound =

It immediately follows from the monotonicity property that

: 0\leq P(E)\leq 1\qquad \forall E\in F.

== ''Proof of the numeric bound'' ==

Given the complement rule P(E^c)=1-P(E)

and axiom 1 P(E^c)\geq0

:

1-P(E) \geq 0

\Rightarrow 1 \geq P(E)

\therefore 0\leq P(E)\leq 1

Further consequences

Another important property is:

: P(A \cup B) = P(A) + P(B) - P(A \cap B).

This is called the addition law of probability, or the sum rule.

That is, the probability that an event in A or B will happen is the sum of the probability of an event in A and the probability of an event in B, minus the probability of an event that is in both A and B. The proof of this is as follows:

Firstly,

:P(A\cup B) = P(A) + P(B\setminus A). (by Axiom 3)

So,

:P(A \cup B) = P(A) + P(B\setminus (A \cap B)) (by B \setminus A = B\setminus (A \cap B)).

Also,

:P(B) = P(B\setminus (A \cap B)) + P(A \cap B)

and eliminating P(B\setminus (A \cap B)) from both equations gives us the desired result.

An extension of the addition law to any number of sets is the inclusion–exclusion principle.

Setting B to the complement Ac of A in the addition law gives

: P\left(A^{c}\right) = P(\Omega\setminus A) = 1 - P(A)

That is, the probability that any event will not happen (or the event's complement) is 1 minus the probability that it will.

Simple example: coin toss

Consider a single coin-toss, and assume that the coin will either land heads (H) or tails (T) (but not both). No assumption is made as to whether the coin is fair or as to whether or not any bias depends on how the coin is tossed.{{cite journal |last1=Diaconis |first1=Persi |last2=Holmes |first2=Susan |last3=Montgomery |first3=Richard |title=Dynamical Bias in the Coin Toss |journal= SIAM Review|date=2007 |volume=49 |issue=211–235 |pages=211–235 |doi=10.1137/S0036144504446436 |bibcode=2007SIAMR..49..211D |url=https://statweb.stanford.edu/~cgates/PERSI/papers/dyn_coin_07.pdf |access-date=5 January 2024}}

We may define:

: \Omega = \{H,T\}

: F = \{\varnothing, \{H\}, \{T\}, \{H,T\}\}

Kolmogorov's axioms imply that:

: P(\varnothing) = 0

The probability of neither heads nor tails, is 0.

: P(\{H,T\}^c) = 0

The probability of either heads or tails, is 1.

: P(\{H\}) + P(\{T\}) = 1

The sum of the probability of heads and the probability of tails, is 1.

See also

  • {{annotated link|Borel algebra}}
  • {{annotated link|Conditional probability}}
  • {{annotated link|Fully probabilistic design}}
  • {{annotated link|Intuitive statistics}}
  • {{annotated link|Quasiprobability}}
  • {{annotated link|Set theory}}
  • {{annotated link|Sigma-algebra|σ-algebra}}

References

{{Reflist}}

Further reading

  • {{cite book |first=Morris H. |last=DeGroot |author-link=Morris H. DeGroot |title=Probability and Statistics |location=Reading |publisher=Addison-Wesley |year=1975 |pages=[https://archive.org/details/probabilitystati0000degr/page/12 12–16] |isbn=0-201-01503-X |url=https://archive.org/details/probabilitystati0000degr/page/12 }}
  • {{cite book |first1=James R. |last1=McCord |first2=Richard M. |last2=Moroney |year=1964 |title=Introduction to Probability Theory |chapter-url=https://archive.org/details/introductiontopr00mcco |chapter-url-access=registration |chapter=Axiomatic Probability |location=New York |publisher=Macmillan |pages=[https://archive.org/details/introductiontopr00mcco/page/13 13–28] }}
  • [https://web.archive.org/web/20130923121802/http://mws.cs.ru.nl/mwiki/prob_1.html#M2 Formal definition] of probability in the Mizar system, and the [http://mmlquery.mizar.org/cgi-bin/mmlquery/emacs_search?input=(symbol+Probability+%7C+notation+%7C+constructor+%7C+occur+%7C+th)+ordered+by+number+of+ref list of theorems] formally proved about it.

{{DEFAULTSORT:Probability Axioms}}

Category:Probability theory

Category:Mathematical axioms