A mass spectrometer is disclosed wherein highly charged fragment ions resulting from Electron Transfer Dissociation fragmentation of parent ions are reduced in charge state within a Proton Transfer Reaction cell by reacting the fragment ions with a neutral superbase reagent gas such as Octahydropyrimidolazepine.

A mass spectrometer is disclosed wherein highly charged fragment ions resulting from Electron Transfer Dissociation fragmentation of parent ions are reduced in charge state within a Proton Transfer Reaction cell by reacting the fragment ions with a neutral superbase reagent gas such as Octahydropyrimidolazepine.

The invention relates to reducing harmonic signals in FT-ICR spectra. Since harmonic signals in quadrupolar 2ω-detection can be more abundant for the same ion motion in the ICR cell as compared to harmonic signals in classical dipolar 1ω-detection, they could hitherto not be reduced to satisfactory levels by any known method, such as gated deflection during ion introduction into, and correcting for an offset electric field axis in the ICR cell. The present disclosure foresees, in addition to other methods carried out for improving the measurement conditions as the case may be, performing the quadrupolar 2ω-detection at least twice, where the phase of the ion excitation radio frequency is turned by 180° in the second measurement. From the sum transient, a Fourier-transformed spectrum is derived. As a result, the broad band spectra of complex substance mixtures like crude oil become cleaner, and misinterpretations of false (harmonic) peaks are minimized.

A microwave microstrip resonator apparatus including a housing; a resonator within the housing; an output conductor within the housing and spaced apart from the resonator so as to define a capacitive gap therebetween; a reaction vessel configured to reside with the capacitive gap; and a power supply coupled to the resonator whereby contents within the reaction vessel are heated when energy is supplied to the resonator by the power supply. A mass spectrometer may also be coupled to an outlet end of the reaction vessel such that the contents within the reaction vessel are, simultaneously, delivered to the mass spectrometer for analysis.

A microwave microstrip resonator apparatus including a housing; a resonator within the housing; an output conductor within the housing and spaced apart from the resonator so as to define a capacitive gap therebetween; a reaction vessel configured to reside with the capacitive gap; and a power supply coupled to the resonator whereby contents within the reaction vessel are heated when energy is supplied to the resonator by the power supply. A mass spectrometer may also be coupled to an outlet end of the reaction vessel such that the contents within the reaction vessel are, simultaneously, delivered to the mass spectrometer for analysis.

A method for mass spectral analysis of molecules based on full mass spectral profile or raw scan mode data, comprising the steps of specifying the basic building blocks for the molecule; estimating initial values including trial numbers of building blocks, charge states, and possible modifications; calculating discrete isotope distributions based on elemental compositions; calculating a profile mode theoretical mass spectrum using a target mass spectrum peak shape function; performing regression analysis between acquired profile mode mass spectrum data and calculated theoretical mass spectrum data and reporting regression statistics; using regression statistics as feedbacks to update initially estimated values including trial numbers of building blocks, charge states, and possible modifications; and repeating selected step to optimize the regression statistics. A mass spectrometer operating in accordance with the method. A medium having computer readable program instructions for causing a mass spectrometer associated with a computer to operate in accordance with the method.

Provided herein are approaches for performing electrodynamic mass analysis with a radio frequency (RF) biased ion source to reduce ion beam energy spread. In some embodiments, a system may include an ion source including a power supply, the ion source operable to generate a plasma within a chamber housing, and an extraction power assembly including a first power supply and a second power supply electrically coupled with the chamber housing of the ion source, wherein the first power supply and the second power supply are operable to bias the chamber housing of the ion source with a time modulated voltage to extract an ion beam from the ion source. The system may further include an electrodynamic mass analysis (EDMA) assembly operable to receive the ion beam and perform mass analysis on the ion beam.

Provided herein are approaches for performing electrodynamic mass analysis with a radio frequency (RF) biased ion source to reduce ion beam energy spread. In some embodiments, a system may include an ion source including a power supply, the ion source operable to generate a plasma within a chamber housing, and an extraction power assembly including a first power supply and a second power supply electrically coupled with the chamber housing of the ion source, wherein the first power supply and the second power supply are operable to bias the chamber housing of the ion source with a time modulated voltage to extract an ion beam from the ion source. The system may further include an electrodynamic mass analysis (EDMA) assembly operable to receive the ion beam and perform mass analysis on the ion beam.

A device (1) for manipulating charged particles, the device comprising a series of electrodes (2, 3) that form a channel for transportation of the charged particles. A power supply unit (5, 6) provides a voltage to axially segmented bunching electrodes to create a potential well within the channel having one or more local minima between local maxima (50, 51). The well is translated along the channel. An axial extraction region (54) comprises electrodes defining an end of the channel. They receive a supply voltage to create a pseudo-potential within the channel such that the depth of the potential well varies according to the mass-to-charge ratio (m/z) of the charged particles transported therein and reduces as a local maxima of the potential well is translated axially towards the axial extraction region thereby to release the transported charged particles of different mass-to-charge ratio (m/z) at different respective times.

A charge detection mass spectrometer may include an electrostatic linear ion trap (ELIT) or orbitrap, a source of ions to supply ions to the ELIT or orbitrap, a processor operatively coupled to the ELIT or orbitrap, a display monitor coupled to the processor, and a memory having instructions stored therein executable by the processor to produce a control graphic user interface (GUI) on the display monitor, the control GUI including at least one selectable GUI element for at least one corresponding operating parameter of the ELIT or orbitrap, receive a first user command, via user interaction with the control GUI, corresponding to selection of the at least one selectable GUI element, and control the ELIT or orbitrap to control the at least one corresponding operating parameter of the ELIT or orbitrap in response to receipt of, and based on, the first user command.