Abstract:
In a mass spectrometer utilizing an atmospheric pressure ion source, the amount of un-vaporized droplets that reach a mass spectrometric section is reduced. A mass spectrometer comprises: an ionization section for ionizing a sample at substantially atmospheric pressure; a first and a second intermediate pressure section in which the pressure is maintained lower than the pressure in said ionization section; a high vacuum section in which the pressure is maintained lower than the pressure in said intermediate pressure section and in which a mass spectrometric means for subjecting ions to mass spectrometry is disposed; a first pore electrode disposed between said ionization section and said first intermediate pressure section; an intermediate pore electrode disposed between said first intermediate pressure section and said second intermediate pressure section; and a second pore electrode disposed between said second intermediate pressure section and said high vacuum section. A first converging electrode is provided in the first intermediate pressure section, the first converging electrode having an opening towards the first pore electrode and another opening towards the intermediate pore electrode. The opening towards the first pore electrode has a larger diameter than the opening towards the intermediate pore electrode, such that the first converging electrode has a tapered shape.
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:
A mass spectrometer in which, in order to reduce noise due to other particles (large charge droplets, neutral particles, photons, or the like), the orbit of ions and the orbit of other particles are separated from each other in the inside of a mass analysis region so as to make it possible to prevent the other particles from reaching an ion detection region without using any deflector.
Abstract:
In the operation of a ion trap mass spectrometer, a high temperature gas at about 300.degree. C. is introduced as a buffer gas. As a result, water molecules absorbed on the inner wall of the quadrupole electrodes of the ion trap mass spectrometer are desorbed and evacuated. Further, the quadrupole electrodes themselves and vacuum chamber are also heated. As the high temperature gas is introduced into the ion trap space, the time necessary for evacuating the ion trap space is shortened and the noise during the measurement time is effectively reduced. During the measurement time, the temperature is controlled to be low, and the thermal degradation of the sample is prevented.
Abstract:
A novel atmospheric pressure ionization device for the transport of charged particle produced by at atmospheric pressure to a mass analyzer includes a liquid shield between the particle source and the sample inlet into the mass analyzer. The liquid shield may be in the form of a disk with a central aperture and acts as a spray splitter and aerofocusing device which increases the flow rate of a liquid sample into the analyzer. The mass analyzer is located in a high vacuum region and an intermediate low vacuum region is provided between the sample inlet and the analyzer. An ion optical system includes electrostatic lens assemblies in said vacuum regions for transporting charged particles from the inlet to the analyzer.
Abstract:
An interface for a mass spectrometer system is provided. The interface can include an inner ceramic tube fabricated from a first ceramic material and an outer tube fabricated from a second ceramic material surrounding the inner ceramic tube. The inner ceramic tube can have high electrical resistivity and high thermal conductivity and the intermediate ceramic tube can have an electrical resistivity that is at least an order of magnitude higher than the electrical resistivity of the first ceramic material and a thermal conductivity that is at least an order of magnitude higher than the thermal conductivity of the first ceramic material.
Abstract:
An interface for a mass spectrometer system is provided. The interface can include an inner ceramic tube fabricated from a first ceramic material and an outer tube fabricated from a second ceramic material surrounding the inner ceramic tube. The inner ceramic tube can have high electrical resistivity and high thermal conductivity and the intermediate ceramic tube can have an electrical resistivity that is at least an order of magnitude higher than the electrical resistivity of the first ceramic material and a thermal conductivity that is at least an order of magnitude higher than the thermal conductivity of the first ceramic material.
Abstract:
Amass spectrometer or ion mobility spectrometer is disclosed comprising: an ion block(2)for receiving ions;a heater (8) for heating the ion block(2); a vacuum housing(6); and an interface block (4) arranged between the ion block (2) and the vacuum housing(6); wherein the interface block (4) is formed from a polymer. The polymer interface block (4) inhibits the heat transfer from the ion block (2) to the vacuum housing(6) and also electrically isolates the ion block (2) and vacuum housing(6). The interface block (4) further comprises at least one conduit (12) through the body of the interface block (4). This enables gas to be transmitted through the interface block (4) to the ion block (2), and also enables the interface block (4) to be cooled.
Abstract:
A system and method for mass spectrometry including a curtain gas chamber defined by a curtain plate having an aperture for receiving ions from an ion source and an orifice plate having an inlet into a mass spectrometer. At least one barrier separates the curtain chamber into a first curtain gas chamber region and a second curtain gas chamber region. At least one gas source provides a gas inflow into the second curtain gas chamber region and a gas outflow into the first curtain gas chamber region, a portion of the gas outflow directed out of the aperture. A heating element heats the gas inflow, a portion of the heated gas inflow directed into the inlet of the mass spectrometer wherein the portion of the heated gas inflow can be at a substantially higher temperature than the portion of the gas outflow.
Abstract:
An Atmospheric Pressure Ion (API) source (1) operates Electrospray (ES) and Atmospheric Pressure Chemical Ionization (APCI) modes. The API source (1) includes a multipurpose heater assembly (10) mounted in an API source chamber (6). The multipurpose heater assembly (10) supplies heat to an API chamber endplate (8), a bath gas, and an entrance end (24) of a capillary orifice (28) into vacuum. An additional heater (15) is at the exit end (32) of the capillary (11) into vacuum. The bath gas, endplate (8) and capillary entrance (24) temperature can set independent of gas flow rate.