Abstract:
A mass spectrometer and method of mass spectrometry in which polyatomic and doubly charged ion interferences are attenuated by establishing an electron population through which a beam of particles containing elemental sample ions and the interfering ions is passed such that the interfering ions preferentially undergo ion-electron recombination and thus dissociation to remove a significant number of the interfering ions. Means (30 or 32) for providing a population of electrons (34 or 36) in an ICP-MS (22) may comprise a magnetic field means such as an electric coil, or an electron generating device. The population of electrons has an electron number density (>10 11 cm -3 to 10 14 cm -3 ), a free electron energy (>0.01eV to
Abstract translation:通过建立电子群减少多原子和双电荷离子干扰的质谱仪和质谱法,通过该质谱仪将含有元素样品离子和干扰离子的粒子束通过,使得干扰离子优先进行离子电子重组 并因此解离以除去大量的干扰离子。 用于在ICP-MS(22)中提供电子群体(34或36)的装置(30或32)可以包括诸如电线圈或电子产生装置的磁场装置。 电子数量的电子数密度(> 10 11 cm -3 -3 10 -10 cm -3),自由电子能量(> 0.01eV至<5eV)处于较低的区域 压力(<10Torr),使得对于通过电子群的离子的预定路径长度(1-4cm),干扰离子将优先通过解离复合过程而衰减。 离子束(40)然后通过质量分析器(42),并且通过离子检测器(44)检测已经根据其质荷比分离的离子。
Abstract:
Provided is an orthogonal acceleration time-of-flight mass spectrometer in which an ion injected into an orthogonal acceleration area is accelerated in a direction orthogonal to a direction of the injection and thereby ejected into a flight space, and a mass-to-charge ratio of the ion is determined based on a time of flight of the ion. The mass spectrometer includes: an ion transport electrode (241) for transporting an ion into the orthogonal acceleration area; an orthogonal acceleration electrode (242) for orthogonally accelerating an ion injected into the orthogonal acceleration area; a flight-path-defining electrode (246) including a flight tube; a storage section (41) in which applied-voltage information which is a set of information concerning levels of voltages applied to the orthogonal acceleration electrode (241), the ion transport electrode, and the flight-path-defining electrode is stored, where an applied voltage whose level changes depending on an ion-ejection period is related to at least one of the electrodes; and a voltage supplier (44) for applying voltages to the aforementioned one of the electrodes.
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:
In order to provide a thermionic emission filament capable of ensuring a long life and improving an analysis accuracy of a mass spectrometer using the thermionic emission filament, in the thermionic emission filament (211) including a core member (211A) through which electric current flows and an electron emitting layer (211B) which is formed so as to cover a surface of the core member (211A), the electron emitting layer (211B) is configured to have denseness for substantial gas-tight integrity.
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.
Abstract:
Mass spectrometry is performed utilizing an electron ionization (EI) source. The EI source ionizes a sample at different electron energies, including below and above 70 eV. The EI source may be utilized for soft ionization as well as hard ionization. The value of the electron energy may be selected so as to favor the formation of molecular ions or other ions of high analytical value. The ion source may be an axial ion source.
Abstract:
A plurality of molecular components contained in a gas are to be ionized together at the same time by the PI method. For example, a plurality of molecular components contained in a gas generated at a certain instant are accurately analyzed in real-time based on the PI method. A gas analyzer includes a gas conveyor 4 that conveys a gas generated from a sample S in a sample chamber R0 to an analysis chamber R1, an ionizer 19 that ionizes the gas, a quadrupole filter 21 that separates ions for each mass-to-charge ratio, and an ion detector 22 that detects the separated ions. The ionizer 19 has an ionizing region provided near a gas outlet of the gas conveyor 4 and a lamp 33A that applies light to the ionizing region. Since the lamp 33A emits light having an light directivity lower than that of laser light and traveling in a spreading manner, the gas having entered the ionizing region in the ionizer 19 receives light irradiation in a wide range, and a plurality of gas components therein are ionized.
Abstract:
A method of fabricating miniature quadrupole electrostatic mass filter has been previously described. The electrodes are metallised cylinders, mounted in grooves etched in oxidised silicon substrates, which are held apart at the correct spacing by cylindrical spacer rods. This invention concerns an ion source mounted on extensions of the spacer rods, which project beyond the mass filter. The ion source consists of a cold-cathode electron emitter, which emits electrons with energies sufficient to cause impact ionisation, and electrostatic optics suitable for coupling the ion flux into the mass filter. Methods of constructing a single self-aligned electron source and a similar dual source are described. Arrangements for mounting the electron source and the ion coupling lens so that the electron and ion beams travel at right angles to one another for efficient separation are described. A method of fabricating a self-aligned one-dimensional einzel electrostatic lens from metallised cylinders mounted in the silicon substrates using etched grooves is described. A method of fabricating a-self-aligned two-dimensional einzel lens from metal plates is also described.
Abstract:
An x-ray source for use in an electron spectrometer comprises a cathode filament (23), focussing means (28,29) and a target (24) which is part of the vacuum chamber housing (10) of the electron spectrometer. The housing (10) itself acts as an anode. By forming the target as part of the vacuum housing, the spectrometer may be more economically and compactly constructed. The target may also comprise part of the energy analysing system associated with the spectrometer.
Abstract:
An ion source (30) for a static gas mass spectrometer is described. The ion source (30) comprises: a source block (310) defining a volume V to receive a sample gas G; an electron source (320) in fluid communication with the source block (310) and configured to provide a flux of electrons E therein for ionising the sample gas G; a set of electrodes (330), including a first electrode (330A), disposed between the electron source (320) and the source block (310); and a controller (not shown) configured to control a voltage applied to the first electrode (330A) to attenuate the flux of the electrons E into the source block (310) during a first time period following receiving of the sample gas G in the source block (310) and to permit the flux of the electrons E into the source block (310) during a second time period following the first time period.