An electromagnet assembly suitable for mass spectrometer comprising one yoke; and two pole pieces; the pole pieces being comprised in a vacuum chamber and being separated from each other by a pole piece gap defining a passage for the charged particles to be deflected; the yoke forming a bridge over the two pole pieces thus defining a magnetic circuit. The electromagnet assembly further comprises one electrical circuit for generating a magnetic flux in the magnetic circuit, the electrical circuit being included in the yoke. The electromagnet assembly is remarkable in that the pole pieces are electrically insulated from the electrical circuit and from the yoke by first electrical insulating means and are electrically insulated from the vacuum chamber.

An electromagnet assembly suitable for mass spectrometer comprising one yoke; and two pole pieces; the pole pieces being comprised in a vacuum chamber and being separated from each other by a pole piece gap defining a passage for the charged particles to be deflected; the yoke forming a bridge over the two pole pieces thus defining a magnetic circuit. The electromagnet assembly further comprises one electrical circuit for generating a magnetic flux in the magnetic circuit, the electrical circuit being included in the yoke. The electromagnet assembly is remarkable in that the pole pieces are electrically insulated from the electrical circuit and from the yoke by first electrical insulating means and are electrically insulated from the vacuum chamber.

Disclosed is a He-3 detector arrangement that generally comprises a mass spectrometer that has an intake funnel configured to receive (sniff out) He-3 through an intake port directly from an open environment. The intake funnel is configured to direct the He-3 into the mass spectrometer. The arrangement further comprises a heating element configured to liberate the He-3 from regolith via heat. A mobile carrier is configured to position the intake port the regolith to obtain samples of the He-3.

Disclosed is a He-3 detector arrangement that generally comprises a mass spectrometer that has an intake funnel configured to receive (sniff out) He-3 through an intake port directly from an open environment. The intake funnel is configured to direct the He-3 into the mass spectrometer. The arrangement further comprises a heating element configured to liberate the He-3 from regolith via heat. A mobile carrier is configured to position the intake port the regolith to obtain samples of the He-3.

An ion implantation system has an ion source forming an ion beam. An mass analyzer defines and varies a mass analyzed beam along a beam path. A moveable mass resolving aperture assembly has a resolving aperture whose position is selectively varied in response to the variation of the beam path by the mass analyzer. A deflecting deceleration element positioned selectively deflects the beam path and selectively decelerate the mass analyzed beam. A controller selectively operates the ion implantation system in both a drift mode and decel mode. The controller passes the mass analyzed beam along a first path through the resolving aperture without deflection or deceleration in the drift mode and deflects and decelerates the beam along a second path in the decel mode. The position of the resolving aperture is selectively varied based on the variation in the beam path through the mass analyzer and the deflecting deceleration element.

An ion implantation system has an ion source forming an ion beam. An mass analyzer defines and varies a mass analyzed beam along a beam path. A moveable mass resolving aperture assembly has a resolving aperture whose position is selectively varied in response to the variation of the beam path by the mass analyzer. A deflecting deceleration element positioned selectively deflects the beam path and selectively decelerate the mass analyzed beam. A controller selectively operates the ion implantation system in both a drift mode and decel mode. The controller passes the mass analyzed beam along a first path through the resolving aperture without deflection or deceleration in the drift mode and deflects and decelerates the beam along a second path in the decel mode. The position of the resolving aperture is selectively varied based on the variation in the beam path through the mass analyzer and the deflecting deceleration element.

A low power mass spectrometer assembly includes at least an ionization component, an electrostatic analyzer, a lens assembly, a magnet assembly and at least one detector located in a same plane as the entrance to the magnet assembly for detecting the deflected sample ions and/or fragments of sample ions, including ions or ion fragments indicative of the Vitamin D metabolite within the sample.

A low power mass spectrometer assembly includes at least an ionization component, an electrostatic analyzer, a lens assembly, a magnet assembly and at least one detector located in a same plane as the entrance to the magnet assembly for detecting the deflected sample ions and/or fragments of sample ions, including ions or ion fragments indicative of the Vitamin D metabolite within the sample.

An analyzer includes: an ionizer unit that ionizes molecules to be analyzed; a filter unit that selectively passes ions generated by the ionizer unit; and a detection unit that detects ions that have passed the filter unit. The detection unit includes a plurality of detection elements disposed in a matrix, and the analyzer further includes a first reconfiguration unit that switches between detection patterns including detection elements to be enabled for detection out of the plurality of detection elements. The ionizer unit includes a plurality of ion sources, and the analyzer further includes a driving control unit that switches the connections of the plurality of ion sources based on changes in characteristics of the ion sources.

Systems and methods are provided for time-of-flight analysis of a continuous beam of ions by a detector array. A sample is ionized using an ion source to produce a continuous beam of ions. An electric field is applied to the continuous beam of ions using an accelerator to produce an accelerated beam of ions. A rotating magnetic and/or electric field is applied to the accelerated beam to separate ions with different mass-to-charge ratios over an area of a two-dimensional detector using a deflector located between the accelerator and the two-dimensional detector. An arrival time and a two-dimensional arrival position of each ion of the accelerated beam are recorded using the two-dimensional detector. Alternatively, an electric field that is periodic with time is applied in order to sweep the accelerated beam over a periodically repeating path on the two-dimensional rectangular detector.