An orbitrap may include elongated inner and outer electrodes, wherein the inner and outer electrodes each define two axially spaced apart electrode halves with a central transverse plane extending through the electrodes also passing between both sets of electrode halves, a cavity defined radially about and axially along the inner electrode between the two inner electrode halves and the two outer electrode halves, means for establishing an electric field configured to trap an ion in the cavity and to cause the trapped ion to rotate about, and oscillate axially along, the inner electrode, wherein the rotating and oscillating ion induces charges on the inner and outer electrode halves, and charge detection circuitry configured to detect the charges induced on the inner and on outer electrode halves, and to combine the detected charges for each oscillation to produce a measured ion charge signal.

Disclosed are methods for improving compound detection and characterization. Methods for characterizing a sample are disclosed. The methods can include providing a sample to a liquid chromatography system capable of sample separation to generate sample components; analyzing sample components by multiplexed targeted selected ion monitoring (SIM) to generate an inclusion list; and performing iterative mass spectral data-dependent acquisition (DDA) from the inclusion list, to identify individual sample components thereby characterizing the sample. In one example, multiplexed targeted SIMs and iterative MS2 DDA acquisition is used to increase robust compound identification for cell culture medium analysis.

An interface transports ions from a first pressure environment to a lower pressure analysis instrument and may include a first region pumped to a second pressure less than the first pressure, a first ion funnel disposed in the first region, a first ion carpet in the first region opposite an ion outlet end of the first ion funnel, a second region pumped to a third pressure less than the second pressure and greater than the instrument pressure, a second ion funnel disposed in the second region and a second ion carpet in the second region opposite an ion outlet end of the second ion funnel. Ions from the environment pass sequentially through the first and second ion funnels and into the analysis instrument. Each of the first and second ion funnels define a tapered axial passageway therethrough each defining a respective virtual jet disrupter therein.

A mass spectrometer comprises: an ion source that generates ions having an initial range of mass-to-charge ratios; an auxiliary ion detector, downstream from the ion source that receives a plurality of first ion samples derived from the ions generated by the ion source and determines a respective ion current measurement for each of the plurality of first ion samples; a mass analyzer, downstream from the ion source that receives a second ion sample derived from the ions generated by the ion source and to generate mass spectral data by mass analysis of the second ion sample; and an output stage that establishes an abundance measurement associated with at least some of the ions generated by the ion source based on the ion current measurements determined by the auxiliary ion detector.

An instrument for separating ions may include an ion source in a first pressure environment at a first pressure and configured to generate ions from a sample, an ion separation instrument, controlled to an instrument pressure that is less than the first pressure, and configured to separate ions as a function of at least one molecular characteristic and an interface, controlled to a second pressure less than the first pressure and greater than the instrument pressure, for transporting the generated ions from the first pressure environment into the ion separation instrument operating at the instrument pressure. The interface may include a sealed ion funnel defining an axial passageway therethrough, and an ion carpet sealed to the first ion funnel. A portion of the axial passageway tapers from a first cross-sectional area to a reduced cross-sectional area such that the tapered axial passageway defining a virtual jet disrupter therein.

Disclosed are methods for improving compound detection and characterization. Methods for characterizing a sample are disclosed. The methods can include providing a sample to a liquid chromatography system capable of sample separation to generate sample components; analyzing sample components by multiplexed targeted selected ion monitoring (SIM) to generate an inclusion list; and performing iterative mass spectral data-dependent acquisition (DDA) from the inclusion list, to identify individual sample components thereby characterizing the sample. In one example, multiplexed targeted SIMs and iterative MS2 DDA acquisition is used to increase robust compound identification for cell culture medium analysis.

There is provided a method of identifying spurious peaks in a mass spectrum produced from a time-varying transient signal detected in a mass spectrometer. The method comprises the steps of generating, using a regularized inversion algorithm having one or more adjustable parameters, a first mass spectrum from the time-varying transient signal, according to a first set of values of said one or more adjustable parameters. Generating, using the regularized inversion algorithm, one or more perturbed mass spectra from the transient signal, according to one or more respective perturbed versions of the first set of values. Identifying one or more spurious peaks in the first mass spectrum by comparing the first mass spectrum with at least one of the perturbed mass spectra. There are also provided corresponding systems and computer readable media.

There is disclosed a method for eliminating an added crosstalk signal from a measured data signal, which is generated by an image current. There is further disclosed a signal processing unit for carrying out the method. There is still further disclosed a mass spectrometer and a mass analyser comprising the signal processing unit for carrying out the method. There is yet still further disclosed a Fourier transform mass spectrometer configured to eliminate the added crosstalk signal from a measured data signal.

A charge detection mass spectrometer may include an electrostatic linear ion trap (ELIT) or an orbitrap, an ion source to supply ions thereto, at least one amplifier operatively coupled to the ELIT or orbitrap, a processor coupled to ELIT or orbitrap and to the amplifier(s), and processor programmed to control the ELIT or orbitrap as part of a trapping event to attempt to trap therein a single ion supplied by the ion source, to record ion measurement information based on output signals produced by the amplifier(s) over a duration of the trapping event, to determine, based on the measurement information, whether the control of the ELIT or orbitrap resulted in trapping of a single ion, no ion or multiple ions, and to compute an ion mass or mass-to-charge ratio from the measurement information only if a single ion was trapped during the trapping event.

An orbitrap may include elongated inner and outer electrodes, wherein the inner and outer electrodes each define two axially spaced apart electrode halves with a central transverse plane extending through the electrodes also passing between both sets of electrode halves, a cavity defined radially about and axially along the inner electrode between the two inner electrode halves and the two outer electrode halves, means for establishing an electric field configured to trap an ion in the cavity and to cause the trapped ion to rotate about, and oscillate axially along, the inner electrode, wherein the rotating and oscillating ion induces charges on the inner and outer electrode halves, and charge detection circuitry configured to detect the charges induced on the inner and on outer electrode halves, and to combine the detected charges for each oscillation to produce a measured ion charge signal.