Abstract: A spin logic device which includes an electron confinement layer confining an electron gas in a two-dimensional area (2DEG) subtended by a direction x and a direction y, the latter perpendicular to the former. The spin logic device is configured for the 2DEG to support a persistent spin helix (PSH) formed therein with a given spin component oscillating with periodicity ? along direction x but not oscillating along direction y. Majority logic circuit of the spin logic device includes: at least one input device energizable to create respective local spin-polarizations of the 2DEG in first regions of the confinement layer. The input device is configured to detect in a second region of the confinement layer an average spin-polarization of the 2DEG diffused through resulting PSHs, wherein a projection of a distance between the second region and first regions onto direction x is equal to n?/a, n integer, a equal to 2 or 4.

Abstract: A spin logic device which includes an electron confinement layer confining an electron gas in a two-dimensional area (2DEG) subtended by a direction x and a direction y, the latter perpendicular to the former. The spin logic device is configured for the 2DEG to support a persistent spin helix (PSH) formed therein with a given spin component oscillating with periodicity ? along direction x but not oscillating along direction y. Majority logic circuit of the spin logic device includes: at least one input device energizable to create respective local spin-polarizations of the 2DEG in first regions of the confinement layer. The input device is configured to detect in a second region of the confinement layer an average spin-polarization of the 2DEG diffused through resulting PSHs, wherein a projection of a distance between the second region and first regions onto direction x is equal to n ?/a, n integer, a equal to 2 or 4.

Abstract: A topography sensor and method include a probe configured to traverse a surface to determine a topography. A stray magnetic field is disposed in proximity to the probe. A magneto-resistive sensor is configured so that the stray magnetic field passing through it changes in accordance with positional changes of the probe as the probe tip traverses the surface.

Abstract: A topography sensor and method include a probe configured to traverse a surface to determine a topography. A stray magnetic field is disposed in proximity to the probe. A magneto-resistive sensor is configured so that the stray magnetic field passing through it changes in accordance with positional changes of the probe as the probe tip traverses the surface.

Abstract: Optically coherent, two-port, serially cascaded-form optical delay line circuits can realize arbitrary signal processing functions identical to those of FIR digital filters with complex filter coefficients whilst maintaining a maximum optical transmission characteristic of 100%. The invention provides an iterative process for transitioning in a step-wise manner a filter function of an optical delay line circuit filter from a start filter function to a target filter function. The invention also describes a dynamic gain equalizer incorporating an optical delay line circuit filter.

Abstract: Optically coherent, two-port, serially cascaded-form optical delay line circuits can realize arbitrary signal processing functions identical to those of FIR digital filters with complex filter coefficients whilst maintaining a maximum optical transmission characteristic of 100%. The invention provides an iterative process for transitioning in a step-wise manner a filter function of an optical delay line circuit filter from a start filter function to a target filter function. The invention also describes a dynamic gain equalizer incorporating an optical delay line circuit filter.

Abstract: A method for manipulating a quantum system comprises at least one mobile charge carrier with a magnetic moment. The method comprises the steps or acts of applying magnetic field to the charge carrier. The magnetic is spatially non-homogeneous. The method also comprises bringing the charge carrier into an oscillatory movement along a path. The magnetic field depends on the position of the charge carrier on said path. The oscillatory movement may be caused by electrostatic interaction with gate electrodes. Due to this approach, thus, in a magnetic moment resonance process the conventional oscillating magnetic field is replaced by an oscillating electric field which is locally transformed into a magnetic field by the Coulomb interaction that displaces the charge carrier wave function within an inhomogeneous magnetic field or in and out of a magnetic field.