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Self-action of a point charge in classical electrodynamics charge. Thus, the problem of mass renormalization is avoided. An exact relativistic expression

Renormalization on noncommutative torus determine, for the particular cases d=2 and d=4, the counterterms required by one-loop renormalization. We

Nuclear spin-lattice relaxation dispersion and segment diffusion in entangled polymers. Renormalized Rouse formalism-volume forces were taken into account in the frame of the renormalized Rouse approach [K. S. Schweizer, J. Chem

Numerical study of dynamical properties of entangled polymer melts in terms of renormalized rouse modelsThe dynamic properties of n-renormalized Rouse models (n = 1, 2) were numerically investigated

Numerical study of dynamical properties of entangled polymer melts in terms of renormalized rouse modelsThe dynamic properties of n-renormalized Rouse models (n = 1, 2) were numerically investigated

Nuclear spin-lattice relaxation dispersion and segment diffusion in entangled polymers. Renormalized Rouse formalism-volume forces were taken into account in the frame of the renormalized Rouse approach [K. S. Schweizer, J. Chem

Electroweak radiative corrections for polarized Møller scattering at one loop and beyond in two different renormalization schemes: on-shell and constrained differential renormalization. Also we

Renormalization of static self-potentialRenormalization of static self-potential

Numerical study of dynamical properties of entangled polymer melts in terms of renormalized rouse modelsThe dynamic properties of n-renormalized Rouse models (n = 1, 2) were numerically investigated

Numerical study of dynamical properties of entangled polymer melts in terms of renormalized rouse modelsThe dynamic properties of n-renormalized Rouse models (n = 1, 2) were numerically investigated

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