A mass spectrometer is disclosed comprising an ion optics device housing having one or more external electrical connectors (1719) provided thereon. An ion optics device (301) is arranged inside the ion optics device housing, the ion optics device (301) comprising one or more electrodes for manipulating ions, the one or more electrodes being electrically connected to the one or more external electrical connectors (1719) provided on the ion optics device housing. A voltage supply housing (1717) is provided having one or more external electrical connectors provided thereon. One or more voltage supplies are arranged inside the voltage supply housing (1717), the one or more voltage supplies being in electrical communication with the one or more external electrical connectors provided on the voltage supply housing. The one or more external electrical connectors provided on the voltage supply housing are directly physically and electrically connected to the one or more external electrical connectors (1719) provided on the ion optics device housing.

The present disclosure provides a gas analysis device and a method for detecting sample gas. The gas analysis device includes: an ion mobility spectrometer including an ion mobility tube, an ion gate, a plurality of electrodes, a suppression grid, and a Faraday plate sequentially disposed in the ion mobility tube, wherein the Faraday plate is configured to receive sample ions discharged from the suppression grid, and the Faraday plate is provided with a through hole; a mass spectrometer; a gate valve disposed between the Faraday plate and an ion inlet of the mass spectrometer; and a controller configured to control an opening or closing of the gate valve to allow the sample ions discharged from the suppression grid to flow into the mass spectrometer through the through hole of the Faraday plate when the gate valve is opened.

Pole electrodes (150) are disclosed for use in an ion reaction apparatus, e.g., an electron induced dissociation cell, to reduce fouling due to polymer build-up and increase the useful lifetime of such electrodes. To reduce fouling, the novel pole electrode designs include a X-shaped aperture (160) in lieu of the conventional central circular aperture. The pole electrodes are particularly useful in systems having a plurality of branched electrodes (152) defining a first axis for controlled passage of charged ions and a transverse axis for passage of an electron beam. The pole electrodes are adapted for disposition between an electron source and the branched electrodes to provide an aperture for passage of an electron beam while also impeding escape of ions and reaction products from the apparatus. The X-shaped aperture eliminates or reduces the portion of the pole electrode surface that is most prone to fouling by polymeric build-up.

A mass spectrometry method comprises: (1) introducing ions and gas into an first electrode section of an ion transport apparatus through a slot of an ion transfer tube, the ion tunnel section comprising a first longitudinal axis that is contained within a slot plane of the ion transfer tube, the first longitudinal axis not intersecting an outlet of the ion transfer tube, wherein the apparatus further comprises: (a) a second electrode section configured to receive the ions from the first electrode section and comprising a second longitudinal axis that is not coincident with the first longitudinal axis; and (b) an ion outlet aperture; (2) providing voltages to electrodes of the ion transport apparatus that urge the ions to migrate towards the first longitudinal axis within the first electrode section; and (3) exhausting gas through a port that is offset from the ion outlet aperture.

A method of introducing and ejecting ions from an ion entry/exit device (4) is disclosed. The ion entry/exit device (4) has at least two arrays of electrodes (20,22). The device is operated in a first mode wherein DC potentials are successively applied to successive electrodes of at least one of the electrode arrays ((20,22) in a first direction such that a potential barrier moves along the at least one array in the first direction and drives ions into and/or out of the device in the first direction. The device is also operated in a second mode, wherein DC potentials are successively applied to successive electrodes of at least one of the electrode arrays (20,22) in a second, different direction such that a potential barrier moves along the array in the second direction and drives ions into and/or out of the device in the second direction. The device provides a single, relatively simple device for manipulating ions in multiple directions. For example, the device may be used to load ions into or eject ions from an ion mobility separator in a first direction, and may then be used to cause ions to move through the ion mobility separator in the second direction so as to cause the ions to separate.

A pulsed accelerator for a Time of Flight mass spectrometers comprising a set of parallel electrodes. The accelerator is inclined at an oblique angle to the incoming ion beam defined by the ratio of the incoming ion beam velocity spreads axial and transverse to the beam. Additionally a deflection electrode is included to deflect unwanted ions away from the detector during the fill cycle of the accelerator.

A method of determining one or more interference parameters for a particular peak of an isotopic distribution corresponding to a precursor molecule in MS scan data is provided. The MS scan data comprises a plurality of peaks. Each peak has a mass-to-charge ratio and a relative abundance. The isotopic distribution comprises a subset of the plurality of peaks. The one or more interference parameters comprises a peak purity, p.sub.i, for the particular peak. The method comprises determining that there are no interfering peaks relevant to the isotopic distribution and determining that the peak purity, p.sub.i, for the particular peak should be a maximum purity value. Alternatively, the method comprises identifying one or more interfering peaks from the MS scan data, wherein the one or more interfering peaks do not belong to the subset of peaks of the isotopic distribution, and determining the peak purity, p.sub.i, for the particular peak based on: the relative abundance, I.sub.i, of the particular peak, and the relative abundance of the one or more interfering peaks.

A voltage supply for a mass analyser is provided. The voltage supply comprises a voltage source, a first voltage output, a second voltage output, and a voltage divider network. The first voltage output is configured to provide a first voltage to a first electrode of the mass analyser, wherein the first electrode of the mass analyser has a first mass shift per volt perturbation. The second voltage output is configured to provide a second voltage to a second electrode of the mass analyser, wherein the second electrode of the mass analyser has a second mass shift per volt perturbation. The second mass shift per volt perturbation opposes the first mass shift per volt perturbation. The voltage divider network comprises a first resistor and a second resistor. The first resistor is configured to define the first voltage, the first resistor having a first temperature coefficient. The second resistor is configured to define the second voltage, the second resistor having a second temperature coefficient. The second temperature coefficient is selected based on the first and second mass shift per volt perturbations and the first temperature coefficient such that a first mass shift associated with the first electrode is compensated by a second mass shift associated with the second electrode.

A voltage supply for a mass analyser is provided. The voltage supply comprises a voltage source, a first voltage output, a second voltage output, and a voltage divider network. The first voltage output is configured to provide a first voltage to a first electrode of the mass analyser, wherein the first electrode of the mass analyser has a first mass shift per volt perturbation. The second voltage output is configured to provide a second voltage to a second electrode of the mass analyser, wherein the second electrode of the mass analyser has a second mass shift per volt perturbation. The second mass shift per volt perturbation opposes the first mass shift per volt perturbation. The voltage divider network comprises a first resistor and a second resistor. The first resistor is configured to define the first voltage, the first resistor having a first temperature coefficient. The second resistor is configured to define the second voltage, the second resistor having a second temperature coefficient. The second temperature coefficient is selected based on the first and second mass shift per volt perturbations and the first temperature coefficient such that a first mass shift associated with the first electrode is compensated by a second mass shift associated with the second electrode.

An ion confinement device (2) comprising: a plurality of electrodes arranged and configured for confining ions when an AC or RF voltage is applied thereto; and at least one inductive ballast (10a,10b), each ballast connected to at least some of said electrodes so as to form a resonator circuit therewith.