nonperiodic multiparticle systemAs in [7] we consider classical system of interacting particles P_1, ... , P_n on the line with only neighboring particles involved in interaction. On the contrast to [7] now periodic boundary conditions are imposed onto the system, i.e. P_1 and P_n are...
The Stokes resistance tensors (material tensors) of a multiparticle system subjected to a general shear flow depends on the spatial configuration of the particles, their shape, size and location of some arbitrarily fixed set of points locked to the particles by which their linear velocities are ...
atoms confined to a one-dimensional periodic system [18] and infinitely strong interacting atoms in one dimension described by a TG gas [17]. II. THEORETICAL BACKGROUND A. Finite basis-set expansion Consider N interacting quantum particles in one di- mension subject to an external potenti...
entanglement relies on a geometric perspective.30–32 Within this approach, one first identifies a hierarchy of non- entangled multiparticle states, also referred to as M-separable states for 2 ⩽ M ⩽ N, where N is the number of particles composing the quantum system of interest; see ...
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excitation systemelectron+positron interactionsWe propose a simple model to describe the multiparticle production in high-energy hadronic interactions. As a result of energy quantization of the excitation system formed in collisions, the model naturally explains the intermittency phenomenon as well as other...
We use a homogeneous time-dependent magnetic external fieldHext(t) of constant magnitude,Hext=5 kA m−1, to drive the system. Hence, our control space is the surface of a sphere. Each point on corresponds to a direction ofHext. For reasons that will become clear later, we can div...
A multiparticle collision dynamics algorithm is presented to simulate gas flow in nanoscopic channels with a square cross section. Special attention is given to the definition of inlet and outlet regions of the simulated system and the boundary conditions that are appropriate to describe flow through ...
As we will see, the recursion is driven by the OPE among two single-particle vertex operators and a system of multiparticle SYM equations of motion which generalize the standard description of (2.1). Throughout this paper, upper case letters from the beginning of the Latin alphabet will ...
The dynamics of a SUSY QM system is determined by a superpotential W,depending on N real coordinates (x1, . . . ,xN). For N-particle systems on a line it is natural to consider potentials with a sepa-rable centre-of-mass motion(CMM).Therefore in this paper we restrict ourselves by ...