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Phase transition from a free-flow phase to a jammed phase is an important feature of traffic networks. We study this transition in the case of a simple square lattice network for different values of data posting rate (ρ) by introducing a parameter p which selects a neighbour for onward data transfer depending on queued traffic. For every ρ there is a… (More)

- D Das, J Dey, A K Chandra, U Thapa, K Ismail
- Langmuir : the ACS journal of surfaces and…
- 2012

The dependence of critical micelle concentration (cmc) of sodium dioctylsulfosuccinate (AOT) on the amount of ethylene glycol (EG) in water + EG medium was reported to be unusual and different from that of other surfactants to the extent that the cmc of AOT in EG is lower than in water. It is yet to be understood why AOT behaves so in water + EG medium,… (More)

- Anjan Kumar Chandra
- Physical review. E, Statistical, nonlinear, and…
- 2012

We study the percolation transition of the geometrical clusters in the square-lattice LCCC model [a kinetic opinion exchange model introduced by Lallouache, Chakrabarti, Chakraborti, and Chakrabarti, Phys. Rev. E 82, 056112 (2010)] with the change in conviction and influencing parameter. The cluster is comprised of the adjacent sites having an opinion value… (More)

We review in details some recently proposed kinetic models of opinion dynamics. We discuss several variants including a generalised model. We provide mean field estimates for the critical points, which are numerically supported with reasonable accuracy. Using nonequilibrium relaxation techniques, we also investigate the nature of phase transitions observed… (More)

- Anjan Kumar Chandra, Subinay Dasgupta
- Physical review. E, Statistical, nonlinear, and…
- 2007

To study the ground state of an axial next-nearest-neighbor Ising chain under transverse field as a function of frustration parameter kappa and field strength Gamma, we present here two different perturbative analyses. In one, we consider the (known) ground state at kappa=0.5 and Gamma=0 as the unperturbed state and treat an increase of the field from 0 to… (More)

- Anjan Kumar Chandra, Subinay Dasgupta
- Physical review. E, Statistical, nonlinear, and…
- 2008

We consider a periodic Ising chain with nearest-neighbor and rth neighbor interaction and quench it from infinite temperature to zero temperature. The persistence probability P(t) , measured as the probability that a spin remains unflipped up to time t , is studied by computer simulation for suitable values of r . We observe that as time progresses, P(t)… (More)

- Anjan Kumar Chandra
- Journal of physics. Condensed matter : an…
- 2013

The dynamical percolation transition of the two-dimensional axial next nearest-neighbor Ising model due to a pulsed magnetic field has been studied by finite size scaling analysis (by Monte Carlo simulation) for various values of frustration parameters, pulse width and temperature (below the corresponding static transition temperature). It has been found… (More)

- A. K. Chandra, K. Kishor, P. K. Mishra, M. S. Alama
- 2016

Microfluidic devices are quite important for process industries, as these devices can intensify heat and mass transfer in two-phase reaction systems. Two-phase reaction systems, such as gas-liquid and liquid-liquid reactions with certain limitations have already been carried out in microfluidic systems by a few authors. However, these concepts are still… (More)

- Soham Biswas, Anjan Kumar Chandra, Parongama Sen
- Physical review. E, Statistical, nonlinear, and…
- 2008

We investigate the dynamics of a two-dimensional axial next-nearest-neighbor Ising model following a quench to zero temperature. The Hamiltonian is given by H= -J_(0) summation operator(L)_(i,j=1)S_(i,j)S_(i+1,j)-J_(1)summation operator_(i,j=1)(S_{i,j}S_{i,j+1}-kappaS_{i,j}S_{i,j+2}) . For kappa<1 , the system does not reach the equilibrium ground state but… (More)

- Bijoy Daga, Souvik Mondal, Anjan Kumar Chandra, Tirthankar Banerjee, Abhik Basu
- Physical review. E
- 2017

We study the totally asymmetric exclusion process (TASEP) on a nonuniform one-dimensional ring consisting of two segments having unequal hopping rates, or defects. We allow weak particle nonconservation via Langmuir kinetics (LK), which are parametrized by generic unequal attachment and detachment rates. For an extended defect, in the thermodynamic limit… (More)