We calculate the force operator for a charged particle in the field of an Aharonov–Bohm flux line. Formally this is the Lorentz force, with the magnetic field operator modified to include quantum corrections due to anomalous commutation relations. For stationary states, the magnitude of the force is proportional to the product of the wavenumber k with the amplitudes of the ‘pinioned’ components...

In this article, we provide a splitting method for solving monotone inclusions in real Hilbert space involving four operators: maximally monotone, monotone-Lipschitzian, cocoercive, and monotone-continuous operator. The proposed takes advantage of the intrinsic properties each operator, generalizing forward–backward–half-forward Tseng’s algorithm with line search. At iteration, our defines step...

This paper presents an advanced telerobotic control system for a mobile robot with multisensor feedback. A telecontrol concept for various degrees of cooperation between a human operator and a mobile robot is described. With multisensor on-board the robot at the remote site can adjust its path while continuously accepting commands from the human operator. Interactive modelling that allows the m...

We introduce a new concept of general $G$-$eta$-monotone operator generalizing the general $(H,eta)$-monotone operator cite{arvar2, arvar1}, general $H-$ monotone operator cite{xiahuang} in Banach spaces, and also generalizing $G$-$eta$-monotone operator cite{zhang}, $(A, eta)$-monotone operator cite{verma2}, $A$-monotone operator cite{verma0}, $(H, eta)$-monotone operator cite{fanghuang}...

We calculate the force operator for a charged particle in the field of an Aharonov-Bohm flux line. Formally this is the Lorentz force, with the magnetic field operator modified to include quantum corrections due to anomolous commutation relations. For stationary states, the magnitude of the force is proportional to the product of the wavenumber k with the amplitudes of the 'pinioned' components...

We calculate the force operator for a charged particle in the eld of an Aharonov-Bohm ux line. Formally this is the Lorentz force, with the magnetic eld operator modiied to include quantum corrections due to anomolous commutation relations. For stationary states, the magnitude of the force is proportional to the product of the wavenumber k with the amplitudes of thèpinioned' components, the two...