Abstract:
A mass spectrometer is disclosed comprising an ion guide or ion mobility spectrometer having helical, toroidal, part-toroidal, hemitoroidal, semitoroidal or spiral ion guiding region. The ion guide may comprise a tube made from a leaky dielectric wherein an RF voltage is applied to outer electrodes in order to confine ions radially within the ion guide. A DC voltage is applied to a resistive inner layer in order to urge ions along the ion guide. Alternatively, the ion guide may comprise a plurality of electrodes each having an aperture through which ions are transmitted.
Abstract:
A mass spectrometer and method of mass spectrometry wherein charged particles in a beam undergo multiple changes of direction. A detection arrangement detects a first portion of the charged particle beam, and provides a first output based upon the intensity of the detected first portion of the charged particle beam. The detection arrangement detects a second portion of the charged particle beam that has traveled a greater path length through the mass spectrometer than the first portion of the charged particle beam, and provides a second output based upon the detected second portion of the charged particle beam. A controller adjusts the parameters of the charged particle beam and/or the detection arrangement, based upon the first output of the detection arrangement, so as to adjust the second output of the detection arrangement.
Abstract:
The present invention aims at automatically obtaining a mass spectrum over a wide mass range with a high mass resolution, without the need of the complicated determination of the number of turns or other troublesome computations due to the overtaking of ions on a loop orbit. First, a mass analysis of a target sample is performed under conditions which ensure that the overtaking of ions does not occur, to obtain a mass spectrum with a low mass resolution (S1 and S2). One or more peaks appearing on the mass spectrum are extracted based on predetermined conditions, the mass ranges corresponding to the extracted peaks are determined, and the analysis conditions which ensure that the overtaking of ions does not occur are determined for each of the mass ranges (S3 and S4). Then, in accordance with the analysis conditions, ions within a restricted mass range are selected and ejected from the ion trap to be made to fly along the loop orbit, and mass spectra with a high mass resolution are obtained (S5 and S6). The mass spectrum with a low mass spectrum and the mass spectra with a high mass resolution are eventually combined to create a mass spectrum over a wide mass range (S8).
Abstract:
A basic ion optical system (2) in which the temporal focusing of ions is ensured includes a plurality of sector-shaped electrodes (11, 12, 13, and 14), an ion injection slit (15), and an ion ejection slit (16), which are placed on the same plane. A plurality of basic ion optical systems (2) are placed in such a manner as to be mutually separated at predetermined intervals in the direction approximately orthogonal to their planes. The ion ejection slit (16) of the lower-stage basic ion optical system (2) and the ion injection slit (15) of the next-stage basic ion optical system (2) are connected to each other via another basic ion optical system (3) in which the temporal focusing of the ions is ensured. Accordingly, the flight distance can be elongated while assuredly achieving the temporal focusing of the ions as an entire ion optical system (1), and a three-dimensional space can be efficiently utilized to compactify the ion optical system (1).
Abstract:
A time of flight mass spectrometer according to the present invention includes: a) an ion source at which an ion starts flying; b) an energizer for giving a predetermined amount of energy to the ion to let the ion start flying from the ion source; c) an ion guide for forming a time-focusing flight path on which the ion flies once or repeatedly; d) a detector for detecting the ion after flying the flight path; e) an analysis controller for giving different amounts of energy to ions of the same kind using the energizer, and for measuring the values of the flight time of the ions from the ion source to the detector for the amount of energy; and f) a mass calculator for calculating or estimating the mass to charge ratio of the ion based on the difference in the values of the flight time of the ions. Since the flight time of ions on the time-focusing flight path does not depend on their kinetic energy, the difference in the flight time of an ion having two different amounts of energy gives the estimation of the mass to charge ratio of the ion. Thus, a mass spectrometry of an ion for a wide range of mass to charge ratio can be made by simply performing two measurements on the same sample. This greatly reduces the time and labor of mass analysis, and a wide range of mass spectrum can be obtained on a scarce sample on which many-time measurements are impossible.
Abstract:
A method and apparatus for time-of-flight (TOF) mass spectrometry. The apparatus improves the ion focusing properties in an orthogonal direction and permits connection with an orthogonal-acceleration ion source for improvement of sensitivity. The apparatus comprises an ion source for emitting ions in a pulsed manner, an analyzer for realizing a helical trajectory, and a detector for detecting the ions. The analyzer is composed of plural laminated toroidal electric fields to realize the helical trajectory.
Abstract:
The invention provides apparatus and methods for performing time-of-flight (TOF) mass spectrometry. A TOF mass spectrometer of the present invention comprises one or more ion focusing electric sectors. At least one of the electric sectors is associated with an ion optical element. The ion optical elements comprise at least one adjustable electrode, such that the adjustable electrode is able to modify the potential experienced by an ion entering or exiting the electric sector with which it is associated.
Abstract:
The present invention provides a time of flight mass spectrometer having a spiral flight path, whose mass resolution can be appropriately changed with respect to the analysis object or other factor without any complicated alteration or addition of the mechanical construction. In a specific form of the invention, the mass spectrometer includes deflecting electrodes 20-23 located between semi-cylindrical electrodes 11 and 12 for making ions fly along a spiral path. The deflecting electrodes 20-23 generate deflecting electric fields for shifting the ions in the axial direction of the semi-cylindrical electrodes 11 and 12. The voltage applied to the deflecting electrodes 20-23 is changed according to the mass resolution required. The deflecting electric fields are generated or removed with the change of the voltage, which makes the ions fly either along a spiral path or in the same loop orbit. The flight distance of the ions can be controlled as desired by regulating the voltage so that the ions fly in the loop orbit an appropriate number of times. Thus, the mass resolution can be arbitrarily controlled.
Abstract:
A small-sized, high-resolution, time-of-flight (TOF) mass spectrometer has a closed ion orbit formed by plural electric sectors. Ions can make plural revolutions in the closed orbit. An entrance path is formed in the closed orbit to introduce ions into the closed orbit. An exit path is formed in the closed orbit to take ions from the closed orbit. The entrance and exit paths can be formed at the exit and entrance of the electric sectors forming the closed orbit or can be positioned in the orbit between the electric sectors forming the closed orbit.
Abstract:
A time-of-flight analyzer, such as a secondary ion surface analyzer, and method are disclosed wherein a beam of charged particles is created, magnified, directed along a path to a detector, detected and the time of flight measured. An emission lens is positioned on the path to produce the magnification and an additional lens can be provided along the path to produce variable magnification. A field aperture along the path limits the size of the image and a contrast diaphragm limits the lateral ion velocity. Two or more, preferably three, particle steering analyzers are sequentially positioned along the path from the emission lens to the detector with each of the three analyzers steering the particles through substantially 90 degrees.