Abstract:
A mass spectrometer includes an ionization assembly including an ionization chamber and at least one ion lens. The removable ionization assembly has a primary axis defined by the direction of an ion beam exiting the ionization assembly, and the ionization chamber and the at least one ion lens arranged along the primary axis. The mass spectrometer further includes an electron source aligned along the primary axis of the ionization assembly and a magnet assembly including a magnet. The electron source configured to provide an electron beam parallel to the primary axis. The magnet assembly movable between a first position in which the magnet is positioned to allow removal of the ion source and a second position in which the magnet is aligned with the electron source.
Abstract:
Certain configurations of an ionization source comprising a multipolar rod assembly are described. In some examples, the multipolar rod assembly can be configured to provide a magnetic field and a radio frequency field into an ion volume formed by a substantially parallel arrangement of rods of the multipolar rod assembly. The ionization source may also comprise an electron source configured to provide electrons into the ion volume of the multipolar rod assembly to ionize analyte introduced into the ion volume. Systems and methods using the ionization source are also described.
Abstract:
Apparatus (e.g., ion source), systems (e.g., residual gas analyzer), and methods provide extended life and improved analytical stability of mass spectrometers in the presence of contamination gases while achieving substantial preferential ionization of sampled gases over internal background gases. One embodiment is an ion source that includes a gas source, nozzle, electron source, and electrodes. The gas source delivers gas via the nozzle to an evacuated ionization volume and is at a higher pressure than that of the evacuated ionization volume. Gas passing through the nozzle freely expands in an ionization region of the ionization volume. The electron source emits electrons through the expanding gas in the ionization region to ionize at least a portion of the expanding gas. The electrodes create electrical fields for ion flow from the ionization region to a mass filter and are located at distances from the nozzle and oriented to limit their exposure to the gas.
Abstract:
Electron capture dissociation (ECD) is performed by transmitting an electron beam through a cell along an electron beam axis, generating plasma in the cell by energizing a gas with the electron beam, and transmitting an ion beam through the interaction region along an ion beam axis to produce fragment ions. Generating the plasma forms an interaction region in the cell spaced from and not intersecting the electron beam, and including low-energy electrons effective for ECD. The ion beam axis may be at an angle to and offset from the ion beam axis, such that the electron beam does not intersect the ion beam.
Abstract:
Exemplary metamaterial photocathodes enable detection of light from visible through long wave infrared wavelengths. Metamaterial stacks, comprising gold, silicon, and cesium-oxide, coupled to a semiconductor allow hot electrons to efficiently enter a vacuum. The hot electrons are multiplied in a multichannel plate and directly through another vacuum towards a phosphorus screen.
Abstract:
Apparatus (e.g., ion source), systems (e.g., residual gas analyzer), and methods provide extended life and improved analytical stability of mass spectrometers in the presence of contamination gases while achieving substantial preferential ionization of sampled gases over internal background gases. One embodiment is an ion source that includes a gas source, nozzle, electron source, and electrodes. The gas source delivers gas via the nozzle to an evacuated ionization volume and is at a higher pressure than that of the evacuated ionization volume. Gas passing through the nozzle freely expands in an ionization region of the ionization volume. The electron source emits electrons through the expanding gas in the ionization region to ionize at least a portion of the expanding gas. The electrodes create electrical fields for ion flow from the ionization region to a mass filter and are located at distances from the nozzle and oriented to limit their exposure to the gas.
Abstract:
The invention relates to the linear dynamic range of ion abundance measurement devices in mass spectrometers, such as time-of-flight mass spectrometers. The invention solves the problem of ion current peak saturation by producing a second ion measurement signal at an intermediate stage of amplification in a secondary electron multiplier, e.g. a signal generated between the two multichannel plates in chevron arrangement. Because saturation effects are observed only in later stages of amplification, the signal from the intermediate stage of amplification will remain linear even at high ion intensities and will remain outside saturation. In the case of a discrete dynode detector this could encompass, for example, placement of a detection grid between two dynodes near the middle of the amplification chain. The invention uses detection of the image current generated by the passing electrons.
Abstract:
Mass analyzers and methods of ion detection for a mass analyzer are provided. An electrostatic field generator provides an electrostatic field causing ion packets to oscillate along a direction. A pulse transient signal is detected over a time duration that is significantly shorter than a period of the ion oscillation or using pulse detection electrodes having a width that is significantly smaller than a span of ion harmonic motion. A harmonic transient signal is also detected. Ion intensity with respect to mass-to-charge ratio is then identified based on the pulse transient signal and the harmonic transient signal.
Abstract:
Mass analyzers and methods of ion detection for a mass analyzer are provided. An electrostatic field generator provides an electrostatic field causing ion packets to oscillate along a direction. A pulse transient signal is detected over a time duration that is significantly shorter than a period of the ion oscillation or using pulse detection electrodes having a width that is significantly smaller than a span of ion harmonic motion. A harmonic transient signal is also detected. Ion intensity with respect to mass-to-charge ratio is then identified based on the pulse transient signal and the harmonic transient signal.
Abstract:
An electron source for electron-induced dissociation in an RF-free electromagnetostatic cell for use installation in a tandem mass spectrometer is provided. An electromagnetostatic electron-induced dissociation cell may include at least one magnet having an opening disposed therein and having a longitudinal axis extending through the opening, the magnet having magnetic flux lines associated therewith, and an electron emitter having an electron emissive surface comprising a sheet, the emitter disposed about the axis at a location relative to the magnet where the electron emissive surface is substantially perpendicular to the magnetic flux lines at the electron emissive surface.