A mass spectrometer comprises: a first ion optical device in a relatively low gas pressure region; a second ion optical device in a relatively high gas pressure region, the first and second ion optical devices receiving respective RF voltages from respective RF power supplies for generating respective RF fields that confine ions in respective trapping regions of the ion optical devices; and a gas conductance restriction, restricting gas flow from the relatively high gas pressure region to the relatively low gas pressure region, the gas conductance restriction having an aperture to allow ions to pass from the second to the first ion optical device. The first and second RF power supplies are independent to allow the RF voltages for generating the first RF field to have a different amplitude from the RF voltages for generating the second RF field.

A method of manufacturing a multipole device includes the steps of: (a) forming an intermediate device by assembling a plurality of components including a plurality of precursor multipole electrodes, wherein the plurality of precursor multipole electrodes in the assembled device extend along and are distributed around a central axis; (b) forming a multipole device from the intermediate device by machining the precursor multipole electrodes within the intermediate device to provide a plurality of multipole electrodes having a predetermined spatial relationship; wherein a first component of the multipole device that includes a multipole electrode is attached non-permanently to a second component of the multipole device, the first component including a first alignment formation, and the second component including a second alignment portion configured to engage with the first alignment formation on the first component so as to facilitate alignment of the first component and the second component when the first component and the second component are attached, thereby allowing the first component to be detached from and then reattached to the second component while retaining the predetermined spatial relationship between the plurality of multipole electrodes.

A mass spectrometer includes a first vacuum chamber, which is provided with an atmospheric pressure interface communicating with an external atmospheric pressure environment and to a first vacuum pump, the range of working pressure P1 of the first vacuum chamber being P1>30 mbar; a second vacuum chamber, which is connected to the first vacuum chamber by means of a vacuum interface to receive the analyte from the first vacuum chamber and to a second vacuum pump, the range of working pressure P2 of the second vacuum chamber being 0.5 mbar≤P2≤30 mbar; and a third vacuum chamber, which is connected to the second vacuum chamber by means of a vacuum interface to receive the analyte from the second vacuum chamber and to a third vacuum pump, the first vacuum pump or the second vacuum pump being used as a forepump of the third vacuum pump.

To provide a mass spectrometer for higher ion permeation efficiency. In a mass spectrometer to transfer ions generated in an ion source 101 to a detector 106 through a vacuum chamber equipped with electrodes, the vacuum chamber includes a first vacuum chamber 107 and a second vacuum chamber 108 communicated by a pore 104 and an air flow containing ions introduced from the ion source 101 into the first vacuum chamber 107 is separated to an air flow 704 and an ion flow 703 by an ion guide 103 in the first vacuum chamber 107. The first vacuum chamber 107 has a current plate 113 to reduce mixing of the separated air flow 704 and ion flow 703.

Methods and systems for analyzing ions in a magnetic ion trap are provided herein. In accordance with various aspects of the present teachings, the methods and systems described herein enable Fourier transform ion cyclotron resonance mass spectrometry across relatively narrow gap magnetic fields substantially perpendicular to the axis along which the ions are injected into the ion trap. As a result, smaller, less expensive magnets can be used to produce the high-intensity, uniform magnetic fields utilized in high performance FT-ICR/MS applications. Accordingly, the present teachings enable permanent magnets (as well as electromagnets) to generate these magnetic fields, potentially reducing the cost, size, and/or complexity of the systems described herein relative to conventional FT-ICR systems.

Ions are injected into an orbital electrostatic trap. An ejection potential is applied to an ion storage device, to cause ions stored in the ion storage device to be ejected towards the orbital electrostatic trap. Synchronous injection potentials are applied to a central electrode of the orbital electrostatic trap and a deflector electrode associated with the orbital electrostatic trap, to cause the ions ejected from the ion storage device to be captured by the electrostatic trap such that they orbit the central electrode. Application of the ejection potential and application of the synchronous injection potentials are each started at respective different times, the difference in times being selected based on desired values of mass-to-charge ratios of ions to be captured by the orbital electrostatic trap.

An ion guide device includes a plurality of ring electrodes disposed in parallel, wherein each ring electrode includes at least 4 electrode units separated from each other, a channel for ion transmission is formed inside the plurality of ring electrodes, and an arrangement direction of the plurality of ring electrodes defines an axial direction of ion transmission; an radio-frequency voltage source, for applying out-of-phase radio-frequency voltages on the neighboring electrode units belonging to the same ring electrode, and applying in-phase radio frequency voltages on a neighboring electrode units along the axial direction, thereby forming an radio-frequency multipole field that confine ions in the ion guide device; and a direct-current voltage source, wherein the ions are transmitted off-axis and focused to a position closer to an inner surface of the ring electrode under a combined action of the radio-frequency voltage and the direct-current voltage.

In one aspect, an ion guide assembly for use in a mass spectrometry system is disclosed, which comprises a first plurality of multipole rods that are arranged to allow passage of ions therebetween, a second plurality of multipole rods that are arranged to allow passage of ions therebetween, and a board disposed between the first and second plurality of rods, the board comprising an ion lens. The first and second plurality of rods are coupled to the board, and the rods of the first plurality of rods are pairwise aligned with, and coupled to, rods of the second plurality of rods.

A device includes a first surface, a second surface and a controller. The second surface is adjacent to the first surface. The first and the second surfaces define a first ion channel therebetween. The first ion channel extends along a first direction. The second surface includes a first plurality of electrodes including a first electrode and a second electrode spaced apart from the first electrode along a second direction lateral to the first direction. The first plurality of electrodes extends along the first direction. The first electrode is configured to receive a first voltage signal and generate at least a portion of a pseudopotential that inhibits ions in the first ion channel from approaching the second surface. The second plurality of electrodes is located between the first electrode and the second electrode and arranged along the first direction. The second plurality of electrodes are configured to receive a second voltage signal to generate a first traveling drive potential that travels along the first direction. The first traveling drive potential is configured to guide ions along the first ion channel. The device further includes a controller electrically coupled to the first and the second surface. The controller is configured to generate the first voltage signal and the second voltage signal.

Certain configurations of devices are described herein that include DC multipoles that are effective to direct ions. In some instances, the devices include a first multipole configured to provide a DC electric field effective to direct first ions of an entering particle beam along a first exit trajectory that is substantially orthogonal to an entry trajectory of the particle beam. The devices may also include a second multipole configured to provide a DC electric field effective to direct the received first ions from the first multipole along a second exit trajectory that is substantially orthogonal to the first exit trajectory.