Elongation of orthogonal accelerators is assisted by ion spatial transverse confinement within novel confinement means, formed by spatial alternation of electrostatic quadrupolar field (22). Contrary to prior art RF confinement means, the static means provide mass independent confinement and may be readily switched. Spatial confinement defines ion beam (29) position, prevents surfaces charging, assists forming wedge and bend fields, and allows axial fields in the region of pulsed ion extraction, this way improving the ion beam admission at higher energies and the spatial focusing of ion packets in multi-reflecting, multi-turn and singly reflecting TOF MS or electrostatic traps.

Even if vibration is applied to an electrode, a connector section is not separated due to urge of a spring section by using a mass spectrometer that includes an electrode (plate-like electrode); a power source section that supplies electric power to the electrode with a predetermined voltage and/or current; a connection line formed of a conductive wire rod having elasticity for electrically connecting the electrode and the power source section; a connector section provided at one end of the connection line; a seat provided in the electrode to be contacted with the connector section; a fixation section provided in the connection line to be fixed to the power source section; and a spring section formed between the connector section and the fixation section of the connection line or in the connector section and for urging the connector section to the seat.

Systems and methods are disclosed for ion injection into an electrostatic trap. Various aspects of this disclosure provide a mass spectrometer system including a primary ion path including a plurality of quadrupoles; and a secondary ion path coupled to the primary ion path utilizing turning elements. The secondary ion path may include an electrostatic linear ion trap (ELIT), the ELIT being operable to analyze ions diverted from the primary ion path and return them to the primary ion path. The primary ion path may include a time-of-flight mass analyzer. The secondary ion path may be bi-directional. Ions may travel in a first direction when coupled into the secondary ion path using a first turning element in the primary ion path and may travel in a second direction when coupled into the secondary ion path utilizing a second turning element in the primary ion path. The secondary ion path may include a collision quadrupole.

A Time of Flight analyser comprising a flight tube (160) and a reflectron (170), wherein the reflectron comprises a stack of electrodes (172) that are compressed against the flight tube such that they remain parallel to each other under compression.

A multi-pass time-of-flight mass spectrometer is disclosed having an elongated orthogonal accelerator (30). The orthogonal accelerator (30) has electrodes (31) that are transparent to the ions so that ions that are reflected or turned back towards it are able to pass through the orthogonal accelerator (30). The electrodes (31) of the orthogonal accelerator (30) may be pulsed from ground potential in order to avoid the reflected or turned ion packets being defocused. The spectrometer has a high duty cycle and/or space charge capacity of pulsed conversion.

The invention relates to the operation of an energy-focusing and solid-angle-focusing reflector for time-of-flight mass spectrometers with pulsed ion acceleration into a flight tube, e.g. from an ion source with ionization by matrix-assisted laser desorption (MALDI). The objective of the invention is to generate high mass resolution in wide mass ranges up to high masses above eight kilodaltons by varying at least one operating voltage on one of the diaphragms of the reflector which can be varied according to a suitable time function during the spectrum acquisition. It may also be advantageous to adapt the operation of the accelerating voltages in the starting region of the ions accordingly. These measures make it possible to achieve a mass resolution much higher than R=100,000 in a wide mass range extending up to and above eight kilodaltons.

An assembly for a mass spectrometer, comprising a housing (106) and a Time of Flight analyser (110), wherein the housing (106) is configured to enclose at least the Time of Flight analyser (110), and the Time of Flight analyser comprises a pusher assembly (120) and a flight tube (160), wherein the Time of Flight mass analyser (110) is cantilevered from the housing.

A mass spectrometer comprising: a vacuum chamber; and an ion inlet assembly for transmitting analyte ions into the vacuum chamber; wherein the spectrometer is configured to operate in a cooling mode in which it selectively controls one or more gas flow to the ion inlet assembly for actively cooling the ion inlet assembly.

A mass spectrometer comprising: a vacuum housing comprising a first vacuum chamber having a first gas exhaust port; a gas pump (1700) having a first gas inlet port connected to the first gas exhaust port (H1) by a first gas conduit for evacuating the first vacuum chamber; and a first apertured cover (2010) arranged over the first gas exhaust port (H1) or first gas inlet port, or in the first gas conduit therebetween.

An analytical device includes: a mass spectrometry unit that separates ions based on flight time and detects the ions having been separated; an analysis unit that creates data corresponding to a spectrum in which an intensity of the ions having been detected and the flight time or m/z corresponding to the flight time are associated; a peak width calculation unit that calculates a first peak width at a first intensity and a second peak width at a second intensity different from the first intensity for at least one peak in the spectrum; and an adjustment unit that performs an adjustment of the mass spectrometry unit based on the first peak width and the second peak width.