A non-resonance photo-neutralizer for negative ion-based neutral beam injectors. The non-resonance photo-neutralizer utilizes a nonresonant photon accumulation, wherein the path of a photon becomes tangled and trapped in a certain space region, i.e., the photon trap. The trap is preferably formed by two smooth mirror surfaces facing each other with at least one of the mirrors being concave. In its simplest form, the trap is elliptical. A confinement region is a region near a family of normals, which are common to both mirror surfaces. The photons with a sufficiently small angle of deviation from the nearest common normal are confined. Depending on specific conditions, the shape of the mirror surface may be one of spherical, elliptical, cylindrical, or toroidal geometry, or a combination thereof.

A non-resonance photo-neutralizer for negative ion-based neutral beam injectors. The non-resonance photo-neutralizer utilizes a nonresonant photon accumulation, wherein the path of a photon becomes tangled and trapped in a certain space region, i.e., the photon trap. The trap is preferably formed by two smooth mirror surfaces facing each other with at least one of the mirrors being concave. In its simplest form, the trap is elliptical. A confinement region is a region near a family of normals, which are common to both mirror surfaces. The photons with a sufficiently small angle of deviation from the nearest common normal are confined. Depending on specific conditions, the shape of the mirror surface may be one of spherical, elliptical, cylindrical, or toroidal geometry, or a combination thereof.

Aspects of the present disclosure describe an atomic oven including a cathode, an anode that comprises a source material, and a power supply that provides a voltage between the cathode and the anode, wherein applying the voltage causes multiple electrons from the cathode to ablate the source material from the anode or locally heat the anode to cause source material to evaporate from the anode and, in both case, to produce a stream of ablated or evaporated particles that passes through an opening in the cathode.

Aspects of the present disclosure describe an atomic oven including a cathode, an anode that comprises a source material, and a power supply that provides a voltage between the cathode and the anode, wherein applying the voltage causes multiple electrons from the cathode to ablate the source material from the anode or locally heat the anode to cause source material to evaporate from the anode and, in both case, to produce a stream of ablated or evaporated particles that passes through an opening in the cathode.

An imaging system utilizing atomic atoms is provided. The system may include a neutral atom source configured to generate a beam of neutral atoms. The system may also include an ionizer configured to collect neutral atoms scattered from the surface of a sample. The ionizer may also be configured to ionize the collected neutral atoms. The system may also include a selector configured to receive ions from the ionizer and selectively filter received ions. The system may also include one or more optical elements configured to direct selected ions to a detector. The detector may be configured to generate one or more images of the surface of the sample based on the received ions.

By heating a high-temperature bath with a heater, atomic gas is generated in the high-temperature bath from an atomic source. A magneto-optical trap is realized by a laser beam reflected by a right-angled conical mirror and a magnetic field formed by a magnetic field generator, and the atomic gas is confined by using the magneto-optical trap and cooled. The cooled atoms are output from an opening to the outside of a slow atom beam generator by a laser beam, which is a push laser beam. A slow atomic beam is thereby formed.

By heating a high-temperature bath with a heater, atomic gas is generated in the high-temperature bath from an atomic source. A magneto-optical trap is realized by a laser beam reflected by a right-angled conical mirror and a magnetic field formed by a magnetic field generator, and the atomic gas is confined by using the magneto-optical trap and cooled. The cooled atoms are output from an opening to the outside of a slow atom beam generator by a laser beam, which is a push laser beam. A slow atomic beam is thereby formed.

Embodiments herein described using a matched filter in a measurement device that includes an atomic sensor with a co-sensor. In one embodiment, the matched filter is a non-causal filter. Embodiments herein also describe a method for producing a matched filter by determining a filter transfer function from the transfer functions of the atomic sensor and the co-sensor. The method can be used to produce a matched filter that is non-causal but can also generate a causal filter for time sensitive applications.

Embodiments herein described using a matched filter in a measurement device that includes an atomic sensor with a co-sensor. In one embodiment, the matched filter is a non-causal filter. Embodiments herein also describe a method for producing a matched filter by determining a filter transfer function from the transfer functions of the atomic sensor and the co-sensor. The method can be used to produce a matched filter that is non-causal but can also generate a causal filter for time sensitive applications.

An ion throughput pump (ITP) includes a pump inlet configured to communicate with a vacuum chamber; an ionization source fluidly communicating with the vacuum chamber via the pump inlet and configured for ionizing gas species received from the vacuum chamber; a pump outlet; ion optics configured for accelerating ions produced by the ionization source toward the pump outlet; and a roughing pump stage configured for receiving the ions from the ionization source, producing neutral species from the ions, and pumping the neutral species through the pump outlet.