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{{short description|Interacting particle system}}
In [[probability theory]], the '''asymmetric simple exclusion process (ASEP)''' is an [[interacting particle system]] introduced in 1970 by [[Frank Spitzer]].<ref>{{Cite
| | year=1970 | title=Interaction of Markov Processes | journal=[[Advances in Mathematics]] | volume=5 | issue=2 | pages=246–290 | doi=10.1016/0001-8708(70)90034-4 | doi-access=free}}</ref> Many articles have been published on it in the physics and mathematics literature since then, and it has become a "default stochastic model for transport phenomena".<ref>{{cite journal|last=Yau|first=H.T.|author-link=Horng-Tzer Yau |title=(log t)^2/3 law of the two dimensional asymmetric simple exclusion process|journal=Ann. Math. |year=2004|volume=159|pages=377–405|
The process with parameters <math>p, q \geqslant 0,\, p + q = 1</math> is a continuous-time [[Markov process]] on <math>S = \lbrace 0, 1\rbrace^{\mathbb{Z}}</math>,
the 1s being thought of as particles and the 0s as
with probability <math>p</math> and one site to the left with probability <math>q</math>. However, the jump is performed only if there is no particle at the target site. Otherwise, nothing happens and the particle waits another exponential time. All particles are doing this independently of each other.
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==References==
*{{Citation
| last1=Tracy | first1=C. A. | author1-link = Craig Tracy
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| volume=290 |issue=1 | pages=129–154
| doi=10.1007/s00220-009-0761-0
|arxiv = 0807.1713 |bibcode = 2009CMaPh.290..129T | s2cid=14730756 }}.
*{{Citation
| last1=Bertini | first1=L.
| last2=Giacomin | first2=G.
| year=
| title=Stochastic Burgers and KPZ equations from particle systems
| journal=[[Communications in Mathematical Physics]]
| volume=183 |issue=3 | pages=571–607
| s2cid=122139894
}}.
[[Category:Statistical mechanics]]
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