English

The double domain structure of pair contact process with diffusion

Statistical Mechanics 2007-05-23 v3

Abstract

We investigate the domain structure of pair contact process with diffusion (PCPD). PCPD is a stochastic reaction-diffusion model which evolves by the competition of two binary reactions, 2A3A2A \to 3A and 2A02A \to 0. In addition, each particle diffuses isotropically, which leads to the bidirectional coupling between solitary particles and pairs. The coupling from pairs to solitary particles is linear, while the opposite coupling is quadratic. The spreading domain formed from localized activities in vacuum consists of two regions, the coupled region of size RpR_p where pairs and solitary particles coexist and the uncoupled region of size RUR_U where only solitary particles exist respectively. As the size of the whole domain RR is given as R=Rp+RUR=R_p + R_U, RpR_p and RUR_U are the basic length scales of PCPD. At criticality, RpR_p and RUR_U scale as Rpt1/ZpR_p \sim t^{1/Z_p} and RUt1/ZUR_U \sim t^{1/Z_U} with ZU>ZpZ_U > Z_p. We estimate Zp=1.61(1)Z_p =1.61(1) and ZU=1.768(8)Z_U =1.768(8). Hence, the correction to the scaling of RR, Q=RU/RpQ=R_U /R_p extremely slowly decays, which makes it practically impossible to identify the asymptotic scaling behavior of RR. In addition to the generic feature of the bidirectional coupling, the double domain structure is another reason for the extremely slow approach to the asymptotic scaling regime of PCPD.

Keywords

Cite

@article{arxiv.cond-mat/0701315,
  title  = {The double domain structure of pair contact process with diffusion},
  author = {Sungchul Kwon and Yup Kim},
  journal= {arXiv preprint arXiv:cond-mat/0701315},
  year   = {2007}
}

Comments

5 pages and 5 figures

R2 v1 2026-07-22T11:42:04.370Z