We describe innovation in terms of a generalized branching process. Each new invention pairs with any existing one to produce a number of offspring, which is Poisson distributed with mean p. Existing inventions die with probability p/τ at each generation. In contrast with mean field results, no phase transition occurs; the chance for survival is finite for all p>0. For τ=∞, surviving processes exhibit a bottleneck before exploding superexponentially—a growth consistent with a law of accelerating returns. This behavior persists for finite τ. We analyze, in detail, the asymptotic behavior as p→0.
%0 Journal Article
%1 Sood2010Interacting
%A Sood, Vishal
%A Mathieu, Myléne
%A Shreim, Amer
%A Grassberger, Peter
%A Paczuski, Maya
%D 2010
%I American Physical Society
%J Physical Review Letters
%K model, sussidiario cascades
%N 17
%P 178701+
%R 10.1103/physrevlett.105.178701
%T Interacting Branching Process as a Simple Model of Innovation
%U http://dx.doi.org/10.1103/physrevlett.105.178701
%V 105
%X We describe innovation in terms of a generalized branching process. Each new invention pairs with any existing one to produce a number of offspring, which is Poisson distributed with mean p. Existing inventions die with probability p/τ at each generation. In contrast with mean field results, no phase transition occurs; the chance for survival is finite for all p>0. For τ=∞, surviving processes exhibit a bottleneck before exploding superexponentially—a growth consistent with a law of accelerating returns. This behavior persists for finite τ. We analyze, in detail, the asymptotic behavior as p→0.
@article{Sood2010Interacting,
abstract = {{We describe innovation in terms of a generalized branching process. Each new invention pairs with any existing one to produce a number of offspring, which is Poisson distributed with mean p. Existing inventions die with probability p/τ at each generation. In contrast with mean field results, no phase transition occurs; the chance for survival is finite for all p>0. For τ=∞, surviving processes exhibit a bottleneck before exploding superexponentially—a growth consistent with a law of accelerating returns. This behavior persists for finite τ. We analyze, in detail, the asymptotic behavior as p→0.}},
added-at = {2019-06-10T14:53:09.000+0200},
author = {Sood, Vishal and Mathieu, Myl\'{e}ne and Shreim, Amer and Grassberger, Peter and Paczuski, Maya},
biburl = {https://www.bibsonomy.org/bibtex/2430decb3ac57027784b1d456ef8f93f0/nonancourt},
citeulike-article-id = {8044888},
citeulike-linkout-0 = {http://dx.doi.org/10.1103/physrevlett.105.178701},
citeulike-linkout-1 = {http://link.aps.org/abstract/PRL/v105/i17/e178701},
citeulike-linkout-2 = {http://link.aps.org/pdf/PRL/v105/i17/e178701},
doi = {10.1103/physrevlett.105.178701},
interhash = {ac5fc02d70b770084210e8c218b28554},
intrahash = {430decb3ac57027784b1d456ef8f93f0},
journal = {Physical Review Letters},
keywords = {model, sussidiario cascades},
month = oct,
number = 17,
pages = {178701+},
posted-at = {2010-10-18 17:26:15},
priority = {2},
publisher = {American Physical Society},
timestamp = {2019-07-31T12:52:15.000+0200},
title = {{Interacting Branching Process as a Simple Model of Innovation}},
url = {http://dx.doi.org/10.1103/physrevlett.105.178701},
volume = 105,
year = 2010
}