9 results about "Electronic states" patented technology

An electronic state splitter for atoms comprises an atom supplier, an atom movement path, a probe laser source, and a magnetic field generator. The atom supplier supplies atoms moving at a constant velocity along the atom movement path. The probe laser source supplies a probe laser propagating in the atom movement path in the same direction as or opposite to the motion of the atoms on the same axis as the atom movement path. The magnetic field generator generates a magnetic field orthogonal to the atom movement path in the atom movement path to mix the wave function of the clock upper state with the electronic state allowing electric dipole transitions, allowing pulsed excitation of clock transitions by the probe laser uniform in time and space. Accordingly, continuous spectroscopy of atomic transitions and frequency control of the probe laser are possible, which improves the stability of the atomic clock.

The invention relates to a magnetic field sensor (1) with an NV diamond (2), an excitation light source (3) configured to emit an excitation beam (4) for exciting electronic states of the NV diamond (2), and arranged such that the excitation beam (4) emitted by it can generate an electric field within the NV diamond (2), a detector (5) arranged and configured to detect fluorescence radiation that the NV diamond (2) can emit as a result of irradiation with the excitation radiation (4), a microwave structure (6) arranged and configured to generate a microwave field within the NV diamond (2) for manipulating spin states of the NV diamond (2), a magnetic field generating device (7) configured to generate an internal, static magnetic field within the NV diamond (2), and comprising at least one permanent magnet (8), and a hood (10). and a base plate (11),which are arranged to form a closed chamber (12). The NV diamond (2), the excitation light source (3), the detector (5), and the microwave structure (6) are arranged within the closed chamber (12). The hood (10) has at least one recess (13) for receiving the at least one permanent magnet (8, 9).

The invention relates to a magnetic field sensor (1) having an NV diamond (2), an excitation light source (3), which is designed to emit an excitation beam (4) for exciting electronic states of the NV diamond (2) and which is arranged such that the excitation beam (4) emitted thereby can generate an electric field within the NV diamond (2), a detector (5), which is arranged and designed to detect fluorescence radiation which the NV diamond (2) can emit as a result of irradiation with the excitation radiation (4), a microwave structure (6), which is arranged and designed to generate a microwave field within the NV diamond (2) in order to manipulate spin states of the NV diamond (2), a magnetic field generating device (7), which is designed to generate an internal, static magnetic field within the NV diamond (2) and which comprises at least one permanent magnet (8), and a hood (10) and a base plate (11), which are arranged such that they form a closed chamber (12). The NV diamond (2), the excitation light source (3), the detector (5) and the microwave structure (6) are arranged within the closed chamber (12). The hood (10) has at least one recess (13) for receiving the at least one permanent magnet (8, 9).

The atomic electronic state separator (1) of the present invention includes: an atomic supply unit (11), an atomic movement path (12), a probe laser source (13), and a magnetic field generating unit (M). The atomic supply unit (11) supplies atoms that move in the atomic movement path (12) at a certain speed. The probe laser source (13) supplies a probe laser that propagates coaxially with the atomic movement path (12) in a direction opposite to or the same as the direction of atomic movement. The magnetic field generating unit (M) generates a magnetic field orthogonal to the atomic movement path (12) in the atomic movement path (12) and mixes it with the wave function of the electronic state that allows electric dipole transitions, thereby enabling pulse excitation of clock transitions based on the same probe laser in time and space. Alternatively, a magnetic shielding member can pulse excite clock transitions by shielding the magnetic field applied in the atomic movement path (12) and spatially changing the Zeeman frequency shift, thereby enabling pulse excitation of clock transitions by the same probe laser in time and space. As a result, it is possible to continuously perform spectral analysis of atomic transitions and frequency control of the detection laser, thereby improving the stability of the atomic clock.

Quantum mechanical systems, such as for instance electronic states in molecules or solid bodies, can be simulated using quantum computers. However, at present quantum computers only provide a limited quantity of qubits for the calculation. This deficiency is attributable to unsolved problems in connection with inherent noise and scalability, with the result that quantum computers currently only enable simulations of small quantum systems. A method simulates and evaluates an electronic system with a continuous spectral density on the basis of the interruption of the quantum simulation by measurements. The quantum simulation is interrupted to read the qubits, the qubit measurements are stored in a classical parity register and restored to the qubits, and the simulation is continued after the restore.

The utility model belongs to the technical field of low-voltage electrical appliances, and discloses an automatic transfer switching device and a dual-power supply device. The automatic transfer switching equipment comprises a shell, a display window is arranged on the shell, a contact system, an indicating structure, a rotating shaft, an operating mechanism and an electronic state indicating device are arranged in the shell, the indicating structure, the rotating shaft and the electronic state indicating device are arranged in the shell, and the operating mechanism drives the rotating shaft to rotate. When the moving contact is switched among a power supply I state, a power supply II state and a double-open state, the rotating shaft drives the indicating structure to rotate to a corresponding position so as to trigger a corresponding position of the electronic state indicating device and enable a corresponding indicating area to directly face a display window. A worker can conveniently identify whether the power supply II or the power supply I is used at the moment according to the information of the indication area observed from the display window, and the working stability of the automatic change-over switch is effectively guaranteed.

The invention discloses a high-entropy alloy composite coating with matched high and low atomic numbers and a preparation method of the high-entropy alloy composite coating, and belongs to the technical field of functional materials and preparation of the functional materials. The problem that an existing high-entropy alloy composite coating has a weak radiation depletion region is solved. Light atoms with small atomic sizes are doped in metal gaps in a gap filling mode through cooperation of high atomic numbers and low atomic numbers, electrons are effectively prevented from directly penetrating through energy loss gaps in the gaps, and therefore the shielding performance of the light atoms on high-energy electrons is improved; and the influence of a radiation depletion weak region of the existing high-entropy alloy on the radiation shielding efficiency is made up. The doping of the light atoms can influence the state of electrons around the metal, so that the electrons can form a denser electron region around the light atoms, the collision probability of the electrons in unit cells is increased, the maximization of non-elastic collision of extranuclear electrons is realized, and the protection performance of the composite material on the electrons is further improved; therefore, the tolerance of the device in high-energy electrons is improved.

This physical quantity calculation method comprises: a step (S12) for acquiring data indicating an electronic state of a material calculated on the basis of an arrangement of atoms constituting the material; a step (S14) for adjusting a parameter indicating a Fermi level in the acquired data; and a step (S18) for calculating a physical quantity indicating a physical property of the material on the basis of the acquired data and the adjusted parameter indicating the Fermi level.

A spin sensor configured from one diamond particle having a maximum diameter of 0.01 [mu] m or more and less than 10 [mu] m, the diamond particle having a center of color, the electronic state of the center of color having a spin ground state level of spin zero and a spin excitation level of spin + / -1, the spin transverse relaxation time T2 of the diamond particles is 180 nsec or more.