An atomic beam source includes a tubular cathode that includes an emission portion that includes an emission port through which an atomic beam can be emitted, a rod-shaped first anode disposed inside the cathode, and a rod-shaped second anode disposed inside the cathode and spaced from the first anode. At least one selected from the group consisting of a shape of the cathode, a shape of the first anode, a shape of the second anode, and a positional relationship between the cathode, the first anode, and the second anode is predetermined so that emission of sputter particles resulting from collision of cations, which have been generated by plasma between the first anode and the second anode, with at least one selected from the cathode, the first anode, and the second anode is reduced.

An atomic clock system includes a magneto-optical trap (MOT) system that traps alkali metal atoms in a cell during a trapping stage of each of sequential coherent population trapping (CPT) cycles. The system also includes an interrogation system that generates an optical difference beam comprising a first optical beam having a first frequency and a second optical beam having a second frequency different from the first frequency. The interrogation system includes a direction controller that periodically alternates a direction of the optical difference beam through the cell during a CPT interrogation stage of each of the sequential clock measurement cycles to drive CPT interrogation of the trapped alkali metal atoms. The system also includes an oscillator system that adjusts a frequency of a local oscillator based on an optical response of the CPT interrogated alkali metal atoms during a state readout stage in each of the sequential clock measurement cycles.

An atomic clock system includes a magneto-optical trap (MOT) system that traps alkali metal atoms in a cell during a trapping stage of each of sequential coherent population trapping (CPT) cycles. The system also includes an interrogation system that generates an optical difference beam comprising a first optical beam having a first frequency and a second optical beam having a second frequency different from the first frequency. The interrogation system includes a direction controller that periodically alternates a direction of the optical difference beam through the cell during a CPT interrogation stage of each of the sequential clock measurement cycles to drive CPT interrogation of the trapped alkali metal atoms. The system also includes an oscillator system that adjusts a frequency of a local oscillator based on an optical response of the CPT interrogated alkali metal atoms during a state readout stage in each of the sequential clock measurement cycles.

A bi-directional device for generating or absorbing atoms or ions. In some embodiments, the device comprises a solid-phase ion-conducting material, a first electrode positioned on a first surface of the solid-phase ion-conducting material, and a second electrode positioned on a second surface of the solid-phase ion-conducting material. The first electrode includes a plurality of triple phase boundaries, each located at an interface between the solid-phase ion-conducting material and the first electrode. A density of the triple phase boundaries is in the range of about 10.sup.4 m/m.sup.2 to about 210.sup.7 m/m.sup.2 on the first surface of the ion-conducting material. A method of operating the bi-directional device and a method of fabricating a bi-directional device are also provided.

A bi-directional device for generating or absorbing atoms or ions. In some embodiments, the device comprises a solid-phase ion-conducting material, a first electrode positioned on a first surface of the solid-phase ion-conducting material, and a second electrode positioned on a second surface of the solid-phase ion-conducting material. The first electrode includes a plurality of triple phase boundaries, each located at an interface between the solid-phase ion-conducting material and the first electrode. A density of the triple phase boundaries is in the range of about 10.sup.4 m/m.sup.2 to about 210.sup.7 m/m.sup.2 on the first surface of the ion-conducting material. A method of operating the bi-directional device and a method of fabricating a bi-directional device are also provided.

An apparatus and method provided a drug layer formed on a surface region of a medical device, the drug layer comprised of a drug deposition and a carbonized or densified layer formed from the drug deposition by irradiation on an outer surface of the drug deposition, wherein the carbonized or densified layer does not penetrate through the drug deposition and is adapted to release drug from the drug deposition at a predetermined rate.

An apparatus and method provided a drug layer formed on a surface region of a medical device, the drug layer comprised of a drug deposition and a carbonized or densified layer formed from the drug deposition by irradiation on an outer surface of the drug deposition, wherein the carbonized or densified layer does not penetrate through the drug deposition and is adapted to release drug from the drug deposition at a predetermined rate.

A negative ion-based neutral beam injector comprising a negative ion source, accelerator and neutralizer to produce about a 5 MW neutral beam with energy of about 0.50 to 1.0 MeV. The ions produced by the ion source are pre-accelerated before injection into a high energy accelerator by an electrostatic multi-aperture grid pre-accelerator, which is used to extract ion beams from the plasma and accelerate to some fraction of the required beam energy. The beam from the ion source passes through a pair of deflecting magnets, which enable the beam to shift off axis before entering the high energy accelerator. After acceleration to full energy, the beam enters the neutralizer where it is partially converted into a neutral beam. The remaining ion species are separated by a magnet and directed into electrostatic energy converters. The neutral beam passes through a gate valve and enters a plasma chamber.

A negative ion-based neutral beam injector comprising a negative ion source, accelerator and neutralizer to produce about a 5 MW neutral beam with energy of about 0.50 to 1.0 MeV. The ions produced by the ion source are pre-accelerated before injection into a high energy accelerator by an electrostatic multi-aperture grid pre-accelerator, which is used to extract ion beams from the plasma and accelerate to some fraction of the required beam energy. The beam from the ion source passes through a pair of deflecting magnets, which enable the beam to shift off axis before entering the high energy accelerator. After acceleration to full energy, the beam enters the neutralizer where it is partially converted into a neutral beam. The remaining ion species are separated by a magnet and directed into electrostatic energy converters. The neutral beam passes through a gate valve and enters a plasma chamber.

Embodiments described herein provide for a method of launching atoms in an atom interferometer. The method includes determining a direction of the total effective acceleration force on the atoms, controlling a direction of launch of the atoms for measurement in the atom interferometer based on the direction of the total effective acceleration force, and obtaining measurements from the atoms.