Abstract:
The present invention relates to a method for separating and enriching stable isotopes in gas phase using the principles of high field asymmetric waveform ion mobility spectrometry, substantially at atmospheric pressure (760 torr) and substantially at room temperature (298 K). Specifically, the method of the present invention may be used to separate and enrich isotopes of chlorine. Electrospray ionization may be used to generate a gaseous mixture of ions and the ion beam exiting the high field asymmetric waveform ion mobility spectrometer may be sampled into a mass spectrometer for isotope identification.
Abstract:
A liquid chromatograph mass spectrometer includes a solvent removing tube, a first ion lens and a second ion lens. Voltages applied to the solvent removing tube, and the first and second ion lenses corresponding to each mass number of a standard sample are studied in advance so that efficiencies of passing ions become best. A voltage scanning pattern is made based on the impressed voltages, and stored in a memory portion. When a scanning measurement is carried out, a control portion controls a current voltage source and a high frequency voltage source according to the voltage scanning pattern, synchronizing with the scanning of the impressed voltage to the quadrupole filter. As a result of the control, an objective ion which is generated by being atomized from a nozzle may effectively pass through the entrance of a quadrupole filter.
Abstract:
An Atmospheric Pressure Ion (API) source is configured for Electrospray (ES) and Atmospheric Pressure Chemical Ionization (APCI) operating modes. The API source includes a multipurpose heater assembly mounted in the API source chamber. The multipurpose heater supplies heat to the API chamber endplate, bath gas and entrance end of the capillary orifice into vacuum as well as supplying electrical connections to the API source elements. An additional heater is configured at the exit end of the capillary orifice into vacuum. With this configuration, the bath gas, endplate and capillary entrance temperature can be set independent of gas flow rate. The capillary exit and entrance temperatures can be set independently as well. The multipurpose endplate heater combined with the capillary exit heater allows the optimization of API source performance over a wide range of operating conditions and analytical applications.
Abstract:
A high voltage ion propulsion field is applied across the length of an ion mobility spectrometer that is divided by a barrier wall into a desolvation region and a drift tube. A plume of ions and solvent is electrosprayed into the desolvation region, and ions are propelled from the desolvation region through the drift tube to an ion target. Drift gas flows through the drift tube in the opposite direction to oppose the ion flow. A portal in the barrier wall permits ions to move from the desolvation region into the drift tube, and restricts flow of drift gas from the drift tube into the desolvation region. The resulting drift gas velocity increase effects desolvation without requiring elevated temperature or decreased pressure. An ion gate is located near the portal and an aperture grid is located near the ion target. The drift gas flow rate is varied to change the ionization spectra to alter selectivity.
Abstract:
There is described an interface for delivering ions generated in an ion source into a mass analyzer in a chamber under vacuum pressure. In particular, the interface employs two consecutive ion guides operated to dissociate adduct ions formed in the ion source or high pressure regions of the interface between the ion source and the mass analyzer, thus improving the limit of detection or limit of quantitation of the mass analyzer by increasing the analyte ion current.
Abstract:
A method in which cutting of small droplets, neutral particles or photons through to a slit provided between a differential pumping portion and a mass analysis portion is combined with slight deflection of ions just before introduction of the ions into the mass analysis portion so that noises are greatly reduced without reduction of signals to thereby improve the signal-to-noise ratio which is an index of detecting sensitivity or lower limit.
Abstract:
A method of analyzing an analyte contained in a plasma, in inductively coupled plasma mass spectrometry (ICP-MS). A sample of the plasma is drawn through an orifice in a sampler, then skimmed in a skimmer orifice, and the skimmed sample is directed at supersonic velocity onto a blunt reducer having a small orifice therein, forming a shock wave on the reducer. Gas in the shock wave is sampled through an offset aperture in the reducer into a vacuum chamber containing ion optics and a mass spectrometer. This reduces space charge effects, thus reducing mass bias and also reducing the mass dependency of matrix effects. Since the region between the skimmer and the reducer can operate at about 0.1 Torr, which is the same pressure as that produced by the roughing pump which backs the high vacuum pump for the vacuum chamber, a single common pump can be used for both purposes, thus reducing the hardware needed. In a simplified version, the skimmer can be replaced by a small beam blocking finger which extends across a line of sight between the sampler and reducer orifices and occludes the reducer orifice from the sampler orifice.
Abstract:
A method of analyzing an analyte contained in a plasma, in inductively coupled plasma mass spectrometry (ICP-MS). A sample of the plasma is drawn through an orifice in a sampler. The sample is then skimmed in a skimmer orifice, and the skimmed sample is directed at supersonic velocity onto a blunt reducer having a small orifice therein, forming a shock wave on the reducer. Gas in the shock wave is sampled through an offset aperture in the reducer into a vacuum chamber containing ion optics and a mass spectrometer. Because the gas sampled through the skimmer and reducer orifices is substantially neutral (ions and free electrons are in close proximity), and also because the reducer orifice is very small, space charge effects are reduced, thus reducing mass bias and also reducing the mass dependency of matrix effects. Separation of ions from free electrons and focusing of ions into the mass spectrometer largely occurs in and downstream of the ion optics in the vacuum chamber. Since the region between the skimmer and the reducer can operate at about 0.1 Torr, which is the same pressure as that produced by the roughing pump which backs the high vacuum pump for the vacuum chamber, a single common pump can be used for both purposes, thus reducing the hardware needed.
Abstract:
Improved techniques are provided for forming ionized molecules from electrosprayed droplets for analysis by a mass spectrometer. A high voltage is applied to a capillary tube for spraying droplets at substantially atmospheric pressure or above, and the electrosprayed droplets contain sample solute of interest and solvent. The electrosprayed droplets are passed into an ion generating chamber which is maintained at a pressure in the range of from 0.2 Torr to 10 Torr. The walls of the ion generating chamber are controllably heated to a temperature which will desolvate the droplets and produce ionized molecules of interest for analysis by the mass spectrometer. The electrospray technique does not rely upon a countercurrent heated gas flow, and provides a particularly simple and inexpensive means to couple electrospray ionization to either quadrupole or magnetic mass analyzers.
Abstract:
An intra-microspray ICP torch for use in conjunction with spectographic analysis generates a high temperature ionized gas in a plasma region at one end of the torch, and includes a preshaped tube mounted within the torch, with a first end of the tube terminating adjacent the plasma region, and a nebulizer mounted to a second end of the tube. The preshaped tube has at least one set of impactors that define at least two chambers, the impactors blocking the line of sight between adjacent chambers. The nebulizer propels a pressurized aerosol/sample mixture at the impactors, toward the plasma region. The impactors divert the mixture as it travels from chamber to chamber toward the plasma region, causing a filtering effect that promotes passage to the plasma region of sample particles having a size of about 15 microns or less, thereby resulting in optimum spectrographic clarity.