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Jevgenijs Kaupuzs

Publications and source records attributed to Jevgenijs Kaupuzs.

2 recordsLinked to original sources

Corrections to scaling in the 2D phi^4 model: Monte Carlo results and some related problems

Monte Carlo (MC) simulations have been performed to refine the estimation of the correction-to-scaling exponent $ω$ in the 2D $φ^4$ model, which belongs to one of the most fundamental universality classes. If corrections have the form $\propto L^{-ω}$, then we find $ω=1.546(30)$ and $ω=1.509(14)$ as the best estimates. These are obtained from the finite-size scaling of the susceptibility data in the range of linear lattice sizes $L \in [128,2048]$ at the critical value of the Binder cumulant and from the scaling of the corresponding pseudocritical couplings within $L \in [64,2048]$. These values agree with several other MC estimates at the assumption of the power-law corrections and are comparable with the known results of the $ε$-expansion. In addition, we have tested the consistency with the scaling corrections of the form $\propto L^{-4/3}$, $\propto L^{-4/3} \ln L$ and $\propto L^{-4/3} /\ln L$, which might be expected from some considerations of the renormalization group and Coulomb gas model. The latter option is consistent with our MC data. Our MC results served as a basis for a critical reconsideration of some earlier theoretical conjectures and scaling assumptions. In particular, we have corrected and refined our previous analysis by grouping Feynman diagrams. The renewed analysis gives $ω\approx 4-d-2 η$ as some approximation for spatial dimensions $d<4$, or $ω\approx 1.5$ in two dimensions.

cond-mat.stat-mech↗

Probabilistic Description of Traffic Breakdowns

We analyze the characteristic features of traffic breakdown. To describe this phenomenon we apply to the probabilistic model regarding the jam emergence as the formation of a large car cluster on highway. In these terms the breakdown occurs through the formation of a certain critical nucleus in the metastable vehicle flow, which enables us to confine ourselves to one cluster model. We assume that, first, the growth of the car cluster is governed by attachment of cars to the cluster whose rate is mainly determined by the mean headway distance between the car in the vehicle flow and, may be, also by the headway distance in the cluster. Second, the cluster dissolution is determined by the car escape from the cluster whose rate depends on the cluster size directly. The latter is justified using the available experimental data for the correlation properties of the synchronized mode. We write the appropriate master equation converted then into the Fokker-Plank equation for the cluster distribution function and analyze the formation of the critical car cluster due to the climb over a certain potential barrier. The further cluster growth irreversibly gives rise to the jam formation. Numerical estimates of the obtained characteristics and the experimental data of the traffic breakdown are compared. In particular, we draw a conclusion that the characteristic intrinsic time scale of the breakdown phenomenon should be about one minute and explain the case why the traffic volume interval inside which traffic breakdown is observed is sufficiently wide.

cond-mat.soft↗