The present disclosure includes a mass spectrometry apparatus for analyzing an analyte sample, which comprises: an ion source from which a quantity of analyte ions from the analyte sample may be sourced for providing an ion beam; a mass analyzer serving to filter the analyte ions of the ion beam based on their mass-to-charge ratio; a first detector unit for analyzing the ions of the ion beam; and a second detector unit being based on the time-of-flight principle and comprising a second detector for analyzing the ions of the ion beam. The present disclosure further includes a method for analyzing an analyte sample using a mass spectrometry apparatus according to the present disclosure.

The use of multiple ion chains in a single ion trap for quantum information processing (QIP) systems is described. Each chain can have its own set of laser beams with which to implement and operate quantum gates within that chain, where each chain may therefore correspond to a single quantum computing register or core. Operations can be performed in parallel across all of these chains as they can be treated independently from each other. To implement and operate quantum gates between different chains, neighboring chains are merged into a single, larger chain, in which one can perform quantum gates between any of the ions in the larger chain. The combined chains can then be separated again by another shuttling event as needed. To implement and operate quantum gates between ions which do not occupy neighboring chains, swap gates can be used via a sequence of intervening chains.

In an ion trap chip, an RF electrode for producing a radio-frequency ion-trapping electric field is formed in one of a plurality of metallization layers formed on a substrate and separated from each other by intermetal dielectric. At least two spans of the RF electrode are suspended between support pillars over a void defined within one or more layers of intermetal dielectric. For each span that is suspended between a first and a second support pillar, an area A.sub.Total and an area A.sub.Supported are defined. A.sub.Total is the total electrode area from an initial edge of the first support pillar to an initial edge of the second support pillar. A.sub.Supported is the electrode area directly underlain by the first support pillar. In each span that is suspended from a first support pillar to a second support pillar, A.sub.Supported is not more than one-half of A.sub.Total.

The disclosure features mass spectrometry systems and methods that include an ion source, an ion trap, a detector subsystem featuring first and second detector elements, and a controller electrically connected to the ion source, the ion trap, and the detector subsystem and configured so that during operation of the system, the controller: applies an electrical signal to the ion source to generate positively and negatively charged particles from sample particles in the system; applies an electrical signal to the ion trap to eject a plurality of particles from the ion trap through a common aperture of the ion trap, and determines information about the sample particles based on first and second electrical signals generated by the ejected particles.

A mass spectrometer collision cell system, comprising: a gas containment vessel comprising an internal chamber having ion inlet and ion outlet ends and a cross-sectional area, A.sub.chamber; a gas inlet aperture; first and second gas outlet apertures that are disposed at or proximal to the ion inlet and outlet ends, respectively, and that have respective outlet aperture cross-sectional areas, A.sub.aperture1 and A.sub.aperture2, and an average outlet aperture cross-sectional area, A.sub.aperture.sup.ave; a longitudinal axis of the chamber extending from the ion inlet end to the ion outlet end and having a length, L.sub.chamber; and a set of multipole rod electrodes, at least a portion of each multipole rod electrode being within the chamber, wherein the values of A.sub.chamber, L.sub.chamber and A.sub.aperture.sup.ave are such that the combined gas conductance of the chamber and the gas outlet apertures is not greater than 95 percent of the gas conductance of the gas outlet apertures alone.

An ionizer 1 including an ionization chamber 10, a sample gas introduction port 14 provided in the ionization chamber 10 for introducing sample gas, an electron beam emitting section 11 which emits an electron beam toward the ionization chamber 10, electron beam passage openings 10a and 10b which are formed on a path of the electron beam emitted from the electron beam emitting section 11 on a wall of the ionization chamber 10 and has a length in a direction of the path longer than a width of a cross section orthogonal to the direction, and an ion outlet 10c provided in the ionization chamber 10 for emitting an ion of the sample gas generated by irradiation with the electron beam, and a mass spectrometer 60 including the ionizer 1.

A method for correcting mass spectral m/z values comprises: detecting mass spectra for different amounts of sample ions within an ion trapping mass analyzer; evaluating an observable difference of relative m/z shift from the detected mass spectra of at least two of the different amounts of ions induced by space charge; evaluating a visible total charge Q.sub.v and/or the difference of a visible total charge Q.sub.v from the detected mass spectra; determining, from the evaluated observable differences of relative m/z shift and the evaluated visible total charges Q.sub.v and/or differences of the visible total charge Q.sub.v, a slope of a linear correlation between relative m/z shift and visible total charge Q.sub.v; determining a relative m/z shift of sample ions detected in a mass spectrum by multiplying visible total charge Q.sub.v with the determined slope; and correcting the m/z values in the mass spectrum using its determined relative m/z shift.

The present invention relates to the technical field of mass spectra. Disclosed are a novel ion storage system and method based on a quadrupole-ion trap tandem mass spectrometry. The system sequentially comprises a heating capillary, a tube lens, a skimmer, a first ion guide, a second ion guide, a quadrupole mass analyzer, an ion trap mass analyzer, and a detector; a first lens is provided between the first ion guide and the second ion guide; a second lens and a third lens are provided between the second ion guide and the quadrupole mass analyzer, wherein operation modes of the first ion guide and the second ion guide comprise an ion transmission mode and an ion storage mode. Compared with conventional time sequence control methods, more ions are stored during the same time according to the present invention, thereby improving the sensitivity of the instrument.

Systems and methods are disclosed for utilizing an ion mobility cell to improve desolvation prior to interaction with a hydrogen-deuterium exchange reagent, thereby improving the accuracy of the HDX data generated by MS and reducing the effects of conformational changes that can occur with increased temperatures.

Systems and methods are disclosed for utilizing an ion mobility cell to improve desolvation prior to interaction with a hydrogen-deuterium exchange reagent, thereby improving the accuracy of the HDX data generated by MS and reducing the effects of conformational changes that can occur with increased temperatures.