Abstract:
The invention relates generally to systems, methods and devices for analyzing samples and, more particularly, to systems using a mass analyzer in combination with a differential mobility spectrometer to enhance the analysis process of constituents of a sample.
Abstract:
A method and apparatus to direct ions away from their otherwise intended or parallel course. Deflectors are used to establish electric fields in regions through which ions are to pass. With such electric fields, ions may be deflected to a desired trajectory. According to the present invention, a multideflector, in the form of a series of bipolar plates spaced evenly across the ion beam path, is used as an ion deflector.
Abstract:
A band gap mass filter for separating particles of mass (M1) from particles of mass (M2) in a multi-species plasma includes a chamber defining an axis. Coils around the chamber generate an axially aligned magnetic field defined (B=B0+B1 sin ωt), with an antenna generating the sinusoidal component (B1 sin ωt) to induce an azimuthal electric field (Eθ) in the chamber. The resultant crossed electric and magnetic fields place particles M2 on unconfined orbits for collection inside the chamber, and pass the particles M1 through said chamber for separation from the particles M2. Unconfined orbits for particles M2 are determined according to an α-β plot ( α = Ω 0 2 + Ω 1 2 / 2 4 ω 2 , and β = Ω 0 Ω 1 8 ω 2 ) , where Ω0 is the cyclotron frequency for particles with mass/charge ratio M, and wherein Ω0=B0/M and Ω1=B1/M.
Abstract:
A method of separating ions includes providing a FAIMS analyzer region for separating ions, and establishing a temperature gradient across the FAIMS analyzer region to controllably affect ion focusing in the FAIMS analyzer region.
Abstract:
A method of separating ions includes providing a FAIMS analyzer region including an ion inlet orifice for providing ions thereto, and providing a sample holder along a side of the ion inlet orifice that is opposite the FAIMS analyzer. A sample material is applied to the sample holder such that sample material is disposed about first and second points along the sample holder, a distance between the first and second points being greater than a maximum dimension of the ion inlet orifice. The first point is aligned with the ion inlet orifice, and the sample material disposed about the first point is irradiated with laser light of a predetermined wavelength. Next, the sample holder is moved relative to the ion inlet so as to align the second point with the ion inlet orifice, and the sample material disposed about the second point is irradiated with laser light of a predetermined wavelength.
Abstract:
Disclosed is a method and apparatus for improving at least one of a peak separation and a signal intensity relating to an ion of interest being transmitted through an analyzer region of a FAIMS apparatus. A method according to the instant invention includes a step of introducing ions including an ion of interest into an analyzer region of a FAIMS. A flow of a doped carrier gas other than air is also provided through the analyzer region. The doped carrier gas includes a carrier gas and a trace amount of a predetermined dopant gas, the predetermined dopant gas selected for improving at least one of a peak separation and a signal intensity relating to the ion of interest relative to the peak separation and the signal intensity relating to the ion of interest in the presence of the carrier gas only. The ion of interest is selectively transmitted through the analyzer region in the presence of the doped carrier gas, and detected at a detector.
Abstract:
A time-of-flight mass analyzer having improved mass resolution without mandating a corresponding increase in instrument size is disclosed. The analyzer includes an ionizer that generates the ions that are to be analyzed. These ions are introduced to an ion flight path, at least a portion of which is aligned with a linear axis. The portion of the ion path that is aligned with the linear axis includes a region having a substantially static electric field with non-linear equipotential field lines that circumvent the linear axis. Ions either enter the substantially static electric field with a velocity component that is directed along the linear axis or have such a velocity component imparted to them once they have been trapped in the substantially static electric field. As a result of the combined effects of the linear velocity component and the non-linear field, the ions make multiple circumnavigating trips about the linear axis as they concurrently travel in the direction of the linear axis. Consequently, the ions travel along a significantly longer flight path when compared to a flight path in which the ions solely travel linearly along the axis. In one embodiment, the concurrent motions of the ions in the direction of the linear axis and along the equipotential field lines about the linear axis define a substantially helical ion trajectory. This provides a larger distance along which ions having close, but different, m/z may be separated in time thereby providing an instrument having higher resolution.
Abstract:
A semi-micro liquid chromatograph/mass spectrometer apparatus has an ion source. The space from the end portion of a flow passage of a liquid chromatograph shell to a vaporization portion is closed so as to prevent the inflow of a gas from outside the ion source into the space. Further, the nebulization and vaporization portions are joined together and heated by a common heater. Dilution of a sample to be analyzed is prevented, and high sensitivity detection becomes possible in a low velocity liquid chromatograph/mass spectrometer.
Abstract:
A gas ionizer is provided for use in a solid state mass spectrograph for analyzing a sample of gas. The gas ionizer is located in a cavity provided in a semiconductor substrate which includes an inlet for introducing the gas to be analyzed. The gas ionizer ionizes the sample of gas drawn into the cavity through the inlet to generate an ionized sample gas. The gas ionizer generates energetic particles or photons which bombard the gas to be sampled to produce ionized gas. The energetic particles or photons can be generated by reverse-bias p-n junctions, radioactive isotopes, electron discharges, point emitters, and thermionic electron emitters. A layer of cesium chloride or cesium iodide having a low work function is formed on top of the reverse-bias p-n junction gas ionizer to increase current emitted per junction area and so that the gas ionizer can be exposed to atmospheric oxygen during storage and can operate in reduced atmosphere with no additional treatments. The cesium chloride layer and the cesium iodide layer do not readily electromigrate. A fabrication process of the mass spectrograph includes using plural masks to ensure proper exposure of resist on both flat and wall surfaces of the semiconductor surface having severe topography.
Abstract:
Purely electrical or magnetic deflection systems are usually utilized in the probe-shaping part of modern electron beam tomographs in order to remove the gas ions generated in the evacuated drift tube by electron impact from the beam. The known deflection systems, however, cause an offset of the electron beam, so that this enters extra-axially into the lens element following the deflection system. In the apparatus for removing ions from an electron beam disclosed herein, a deflection unit (Wien filter) generates an E.times.B field oriented perpendicular to the beam axis that exerts strong shearing forces only on the positively charged gas ions, but does not influence the electrons. The deflection unit is essentially composed of two tube electrodes lying at a constant potential, of an electrostatic octopole deflector, and two saddle coil pairs annularly surrounding the octopole deflector. The apparatus is useful for fast electron beam tomographs, including x-ray scanners.