The invention relates to a system for aligning the firing of a laser-ablation apparatus to a signal or property of an inductively-coupled-plasma mass-spectrometer apparatus. At least one kind of input unit that receives timing data from the mass-spectrometer and isolates the system. A processor configured to translate the mass cycle of the mass-spectrometer into a series of triggering signals to fire the laser. A delay circuit to retard the triggering signals by a specified duration. At least one kind of signal output unit to deliver a triggering signal to the laser. A method for configuring a system for controlling a laser in laser-ablation inductively-coupled-plasma mass-spectrometry as above. A computer program product for controlling a laser in laser-ablation inductively-coupled-plasma mass-spectrometry as above.

Provided is a method of reducing the magnitude of a quasi-static electric dipole field at the null position of an oscillating electric quadrupole field of an ion trap. The method includes trapping at least one ion in a trapping electric field. The trapping electric field includes an electric field amplitude; using an interferometry sequence including applying a first laser pulse when the trapping electric field amplitude includes a first trapping electric field amplitude; applying a second laser pulse when the trapping electric field amplitude includes a second trapping electric field amplitude different from the first electric field amplitude; and measuring a state of the ion; repeating the interferometry sequence in order to obtain a plurality of measurements of the state of the ion; determining a probability that the trapped ion changes state; and adjusting the trapping electric field based on the determined probability.

A mass spectrometer support apparatus includes a peak shape logic to determine one or more peak shapes using a calibration mass spectrum and known peak locations; and a tuning logic to adjust instrument parameters to achieve a selected peak width. A method for tuning a quadrupole-based mass spectrometer includes determining one or more peak shapes using a calibration mass spectrum and known peak locations; and adjusting instrument parameters to achieve a selected peak width.

A mass spectrometer support apparatus includes a peak shape logic to determine one or more peak shapes using a calibration mass spectrum and known peak locations; and a tuning logic to adjust instrument parameters to achieve a selected peak width. A method for tuning a quadrupole-based mass spectrometer includes determining one or more peak shapes using a calibration mass spectrum and known peak locations; and adjusting instrument parameters to achieve a selected peak width.

A method of processing ions in a mass spectrometer comprises introducing one or more precursor ions into a collision cell to fragment at least a portion of said ions, where the collision cell is configured to confine ions having m/z ratios above a selected threshold (i.e., high m/z ions). The ions are released from the collision cell and introduced into a downstream analyzer ion trap to radially confine high m/z ions. The collision cell and the analyzer ion trap are configured to confine ions having m/z ratios below said selected threshold (i.e., low m/z ions). Ions are introduced into the collision cell and undergo fragmentation. The fragment ions are released from the collision cell and introduced into the analyzer ion trap, thus loading the analyzer ion trap with both high m/z and low m/z ions. The ions are released from the analyzer ion trap and detected by a detector.

Improved multi-pass time-of-flight mass spectrometers MPTOF, either multi-reflecting (MR) or multi-turn (MT) TOF are proposed with elongated pulsed converters—either orthogonal accelerator or radially ejecting ion trap. The converter 35 is displaced from the MPTOF s-surface of isochronous ion motion in the orthogonal Y-direction. Long ion packets 38 are pulsed deflected in the transverse Y-direction and brought onto said isochronous trajectory s-surface, this way bypassing said converter. Ion packets are isochronously focused in the drift Z-direction within or immediately after the accelerator, either by isochronous trans-axial lens/wedge 68 or Fresnel lens. The accelerator is improved by the ion beam confinement within an RF quadrupolar field or within spatially alternated DC quadrupolar field. The accelerator improves the duty cycle and/or space charge capacity of MPTOF by an order of magnitude.

Provided is a mass spectrometer including: an ion generation unit configured to provide an ion generation path; an ion selection unit configured to provide an ion selection path connected to the ion generation path; a reaction unit configured to provide a reaction path connected to the ion selection path; a second ion selection unit configured to provide a second ion selection path connected to the reaction path; and an ion detection unit coupled to the second ion selection unit. The ion selection path and the reaction path extend in a first direction, and the reaction unit includes: a reaction pipe extending in the first direction to define the reaction path; and a sample inflow pipe coupled to the reaction pipe. The sample inflow pipe provides a sample inflow path connected to the reaction path, and the sample inflow path includes an inclined path. The inclined path extends to form an acute angle (α) with respect to the first direction.

Devices and methods of generating resonance excitation for an ion manipulation apparatus are provided. The ion manipulation apparatus can be operated as an ion filtration apparatus used with particle mass spectrometry system. The devices and methods can be capable of generating a resonance excitation to effect an ion filtration in a multipole apparatus. The resonance excitation is generated by mixing a radio frequency signal with a plurality of alternative current voltage signals having different frequencies. The resonance excitation can be added to at least one electrode of the multipole apparatus. The generation of mixed alternative current voltage signal is performed in a time domain, therefore no time-consuming inverse Fourier transform procedure is needed, which significantly improves an analysis speed and a throughput of the particle mass spectrometry system.

A mass spectrometer may have an ion source region including an ion generator configured to generate ions from a sample, an ion detector configured to detect ions and produce corresponding ion detection signals, an electric field-free drift region disposed between the ion source region and the ion detector through which the generated ions drift axially toward the ion detector, a plurality of spaced-apart charge detection cylinders disposed in the drift region and through which the ions drifting axially through the drift region pass, and a plurality of charge amplifiers each coupled to a different one of the plurality of charge detection cylinders and each configured to produce a charge detection signal corresponding to a magnitude of charge of one or more of the generated ions passing through a respective one of the plurality of charge detection cylinders.

The invention generally relates to methods and devices for synchronization of ion generation with cycling of a discontinuous atmospheric interface. In certain embodiments, the invention provides a system for analyzing a sample that includes a mass spectrometry probe that generates sample ions, a discontinuous atmospheric interface, and a mass analyzer, in which the system is configured such that ion formation is synchronized with cycling of the discontinuous atmospheric interface.