1. Technical Field
This invention relates generally to methods and systems for transferring ions from one gas stream or other environment to another. More specifically, this invention comprises an ion transfer device arranged to urge ions contained in a first gas stream through an ion selective aperture into a second gas stream of different composition or characteristics.
2. Description of Related Art
Ions are routinely produced by subjecting a gas stream to an energetic source. Commonly used energetic sources include radioactive isotopes, plasmas, ultraviolet light, and many others. Such sources can produce ions in an environment (e.g., ambient air), that is not compatible with an ion destination (e.g., a detector, an ion trap, a reaction region, or a deposition or neutralization site). A solution to this problem is to transfer ions from one environment (e.g., a gas stream) to another, without transferring neutral components such as water or particles, which inhibit detection or interfere with performance at the ion destination.
Transferring ions from one gas stream to another may be necessitated by a variety of objectives, such as, but not limited to, the need to remove ions from a gas stream; to move ions that were created or collected in one gas stream to another gas stream that better meets the requirements of detection or identification equipment; to move ions to a gas stream to undergo chemical and/or physical reactions to enable differentiation among ions or to produce a specific product; to move ions from a gas of erratic or changing composition, such as ambient air, to a gas stream having a fixed and stable composition; and various combinations of the above. Ion transfer may be accomplished using a variety of known techniques including the use of ion selective apertures such as those described in U.S. Pat. Nos. 6,914,243, 6,949,740, and 7,060,976, and in pending U.S. Patent Application Publication No. 2008/0296493, all of which are incorporated herein by reference in their entirety. Ion focusing at atmospheric pressure is described in U.S. Pat. Nos. 6,818,889, 6,878,930, 6,949,740, and 7,087,898, which are incorporated by reference in their entirety.
The methods and systems described herein attempt to improve upon the known and presently used devices and techniques for effecting ion transfer. Ions can be transferred from a gas stream flowing through a first conduit or tube into a second conduit or tube containing a flowing gas stream of different composition through an ion selective aperture under the influence of a potential gradient applied to electrically conductive surfaces of the aperture. The first and second tubes can be sited adjacent one another, and the ion selective aperture can form a common wall between the tubes. Gas flow rates in the first and second tubes can be independent of one another allowing a different concentration of ions in the second tube relative to the first tube. As a result, the gas composition, flow rate, and ion concentration in the second tube can be compatible with the needs of the ion destination region, such as a sensor or detector.
In one embodiment, an ion transfer device comprises a first conduit having a first gas stream, a second conduit having a second gas stream to receive the ions from the first gas stream, and an aperture layer disposed between the first conduit and the second conduit. The aperture layer has a first conductive layer proximate to the first conduit, a second conductive layer proximate to the second conduit, and an insulating layer between the first and second conductive layers. The aperture layer has one or more channels extending from the first conduit to the second conduit and through the first and second conductive layers.
In another embodiment, an ion transfer device comprises a first conduit having a first gas stream, a second conduit having a second gas stream to receive the ions from the first gas stream, a first aperture layer disposed between the first conduit and the second conduit. The first aperture layer has a first conductive layer proximate to the first conduit, a second conductive layer proximate to the second conduit, and an insulating layer between the first and second conductive layers. The insulating layer has one or more channels extending from the first conduit to the second conduit and through the first and second conductive layers. The ion transfer device also has a third conduit comprising a third gas stream to receive the ions from the second gas stream, and a second aperture layer disposed between the second conduit and the third conduit. The second aperture layer has a third conductive layer proximate to the second conduit, a fourth conductive layer proximate the third conduit, and a second insulating layer between the third and fourth conductive layers. The second insulating layer has one or more channels extending from the second conduit to the third conduit and through the third and fourth conductive layers.
In yet another embodiment, an ion transfer device comprises a first conduit comprising a first gas stream, the first conduit divided into first and second segments separated by an insulator, a second conduit comprising a second gas stream to receive the ions from the first segment; a third conduit comprising a third gas stream to receive ions from the second segment, and a first aperture layer disposed between the first segment and the second conduit. The first aperture layer has a first conductive layer proximate to the first segment, a second conductive layer proximate to the second conduit, and a first insulating layer between the first and second conductive layers. The first insulating layer has one or more channels extending from the first segment to the second conduit and through the first and second conductive layers, and a second aperture layer disposed between the second segment and the third conduit. The second aperture layer has a third conductive layer proximate to the second segment, a fourth conductive layer proximate to the third conduit, and a second insulating layer between the third and fourth conductive layers. The second insulating layer has one or more channels extending from the second segment to the third conduit and through the third and fourth conductive layers.
In another embodiment, a method for transferring ions comprises directing one or more ions from a first conduit to a second conduit through one or more channels extending through a plate between the first conduit to the second conduit; applying a voltage to a first conductive layer proximate to the first conduit and the plate; and applying a second voltage to a second conductive layer proximate to the second conduit and the plate; wherein the first voltage is different than the second voltage.
In another embodiment, a method for transferring ions comprises directing a plurality of ions from a first conduit to a second conduit through one or more channels extending through a first plate between the first conduit to the second conduit; applying a voltage to a first conductive layer proximate to the first conduit and the first plate; applying a second voltage to a second conductive layer proximate to the second conduit and the first plate, wherein the first voltage is different than the second voltage; directing the plurality of ions from the second conduit to a third conduit through one or more channels extending through a second plate between the second conduit and the third conduit; applying a third voltage to a third conductive layer proximate to the second conduit and the second plate; and applying a fourth voltage to a fourth conductive layer proximate to the second plate and the third conduit, wherein the third voltage is different than the fourth voltage.
In yet another embodiment, a method for transferring ions comprises insulating a first segment of a first conduit from a second segment of the first conduit; directing a first plurality of ions from the first segment to a second conduit through one or more channels extending through a first plate from the first segment to the second conduit; applying a voltage to a first conductive layer proximate to the first segment and the first plate; applying a second voltage to a second conductive layer proximate to the second conduit and the first plate, wherein the first voltage is different than the second voltage; directing a second plurality of ions from the second segment to a third conduit through one or more channels extending through a second plate between the second segment and the third conduit; applying a third voltage to a third conductive layer proximate to the second segment and the second plate; and applying a fourth voltage to a fourth conductive layer proximate to the second plate and the third conduit, wherein the third voltage is different than the fourth voltage.
In another embodiment, an ion transfer device comprises a first conduit comprising a first gas stream; a second conduit comprising a second gas stream to receive one or more positive ions from the first gas stream; and a first aperture layer disposed between the first conduit and the second conduit. The aperture layer comprises a first conductive layer proximate to the first conduit; a second conductive layer proximate to the second conduit; and a first insulating layer between the first and second conductive layers comprising one or more channels extending from the first conduit to the second conduit and through the first and second conductive layers. A third conduit comprises a third gas stream to receive one or more negative ions from the first conduit. A second aperture layer is disposed between the first conduit and the third conduit. The aperture layer comprises a third conductive layer proximate to the first conduit; a fourth conductive layer proximate to the third conduit; and a second insulating layer between the third and fourth conductive layers comprising one or more channels extending from the first conduit to the third conduit and through the third and fourth conductive layers. A mixing union combines the second gas stream and the third gas stream.
In yet another embodiment, an ion transfer device comprises a first conduit comprising a first gas stream and configured to receive one or more positive ions from a second conduit comprising a second gas stream and to receive one or more negative ions from a third conduit comprising a third gas stream. A first aperture layer is disposed between the first conduit and the second conduit. The aperture layer comprises a first conductive layer proximate to the first conduit; a second conductive layer proximate to the second conduit; and a first insulating layer between the first and second conductive layers comprising one or more channels extending from the first conduit to the second conduit and through the first and second conductive layers. A second aperture layer is disposed between the first conduit and the third conduit. The aperture layer comprises a third conductive layer proximate to the first conduit; a fourth conductive layer proximate to the third conduit; and a second insulating layer between the third and fourth conductive layers comprising one or more channels extending from the first conduit to the third conduit and through the third and fourth conductive layers.
Reference will now be made in detail to the preferred embodiments of the present invention, examples of which are illustrated in the accompanying drawings.
The embodiments described herein may be used in conjunction with the technology described in one or more of the following applications: U.S. Pat. No. 7,138,626, filed May 5, 2005, entitled METHOD AND SYSTEM FOR NON-CONTACT SAMPLING AND DETECTION; U.S. patent application Ser. No. 11/580,876, filed Oct. 16, 2006, entitled METHOD AND SYSTEM FOR NON-CONTACT SAMPLING AND DETECTION; U.S. patent Ser. No. 11/987,632, filed Dec. 3, 2007, entitled METHOD AND SYSTEM FOR NON-CONTACT SAMPLING AND DETECTION; U.S. patent application Ser. No. 11/455,334, filed Jun. 19, 2006, entitled SAMPLE TUBE HOLDER, U.S. patent application Ser. No. 11/544,252, filed Oct. 7, 2006, entitled REMOTE REAGENT ION GENERATOR; U.S. patent application Ser. No. 11/594,401, filed Nov. 8, 2006, entitled NON-CONTACT DETECTOR SYSTEM WITH PLASMA ION SOURCE; U.S. patent application Ser. No. 12/153,358, filed May 16, 2008, entitled METHOD AND MEANS FOR PRECISION MIXING; PCT/US2006/042863, filed Nov. 2, 2006, entitled METHOD AND DEVICE FOR NON-CONTACT SAMPLING AND DETECTION; and U.S. patent application Ser. No. 12/200,941, filed Aug. 29, 2008, entitled MINIATURE IONIZATION SOURCE; all of which are hereby incorporated by reference in their entirety.
The methods and systems described herein can transfer ions, either positive or negative or both, from one gas stream to another using electric or magnetic fields to urge ions entrained in one gas stream to move to a different gas stream.
Referring to
It is intended that although the term tube is used in the exemplary embodiments, the shape of the tube or conduit is not limited to a cylinder and may encompass any shape, size, or path. The aperture layer 130 has an insulating layer 140, which is fabricated of a non-conductive or dielectric material, such as glass, doped glass, a thermally-resistant plastic material such as VESPEL, liquid crystal polymer, fiberglass, or plastic. An electrically conductive layer or film 150 forms a first surface (e.g., an upper surface) of aperture layer 130 and a similar electrically conducting layer or film 160 forms a second surface (e.g. a lower surface) of aperture layer 130. Examples of conductive materials are gold, copper, stainless steel, silver, and platinum, among others. The preferred materials can be selected by a variety of criteria, including reactivity, ease of fabrication, cost, and commercial availability. At least one aperture or channel 170 extends through the insulating layer 140 and through the conductive layers 150, 160 to provide communication between the interior of first tube 110 and the interior of second tube 120. In a preferred embodiment, aperture layer 130 has one or more channels 170. Channels 170 may be circular, square, rectangular, or other geometric shape in cross-section and can be arranged randomly, in patterns, or in single or multiple rows. The thickness of the aperture layer 130 and the size and shape of channels 170 are not critical and may vary, but optimally are sized using the principles of fluid mechanics to minimize turbulence and mixing of gas streams at or in the channels.
Tubes 110, 120 can be positioned substantially adjacent one another having the aperture layer 130 disposed therebetween and forming a common wall between the tubes 110, 120. An electric field can be created by applying a first voltage to conductive layer 150 and a second voltage applied to conductive layer 160 that is closer to ground than the voltage applied to conductive layer 150. A voltage differential is thereby created between the two conductive layers 150, 160, as shown in
In operation, a first gas stream can flow through tube 110 and a second gas stream of different composition can flow through tube 120. Gas flow direction in tube 110 can be parallel or orthogonal to the surface of conductive layer 150. If the flow is orthogonal, the flow may be in a direction towards the conductive layer 150 and the flow of gas in tube 120 can be parallel to conductive layer 160. Also, if the gas flow direction in tube 110 is parallel to the conductive layer 150, and the flow is from left to right, then the flow direction in tube 120 can be right to left (concurrent flow) or left to right (counter flow). The movement of ions in the first gas stream flowing through tube 110 is primarily controlled by fluid mechanical principles applied to the geometry of the tube. However, those ions can be pushed or pulled through the aperture means from the gas flowing in tube 110 into the second gas stream flowing in tube 120 by superimposing an electric field onto the mechanical control of ion movement in tube 110 as the ions near the aperture layer 130 region. A combination of aerodynamic, mechanical, magnetic, and/or electrical forces can direct the ions in one direction and unwanted neutral molecules in the other direction. As ions approach the aperture layer 130, the electric field forces become dominant, which results in ion flow through channels 170 into the second gas stream flowing in tube 120. Aerodynamic forces can then become dominant, carrying ions away from the electric field.
A number of different parameters can influence or control the amount of ions transferred. Exemplary parameters include the flow rates of gases in the first tube 110 and the second tube 120; the direction of gas flow in one tube relative to the gas flow in the other tube, i.e., either concurrent or counter flow; the applied voltage differential between the two tubes 110, 120; and the cross-sectional and linear geometry of one tube relative to the other tube. For example, one or both tubes can be curved to eliminate sharp changes in ion movement direction. An arrangement where both tubes are curved away from each other, with the common point being the aperture layer 130 tangential to both tubes, can be advantageous in that the gas streams in each tube can have a tendency to stay attached to a convex surface rather than to follow a straight line. This boundary layer attachment, or Coanda effect, can reduce the possibility of significant mixing of the two gas streams in the aperture layer 130. Also, the tubes can be arranged concentrically with aperture layer 130 forming at least a portion of the inner tube wall thus permitting ion passage from the gas flowing in the inner tube into gas flowing in an annular region between the two tubes. When the first and second tubes are straight, maintenance of laminar gas flow across the aperture layer 130 also serves to minimize mixing, or cross contamination, of the gas streams on either side of the aperture layer 130.
The total gas flow rate and the gas velocities in the two tubes 110, 120 may be mandated by the requirements of other modules used in the system such as, for example, detectors or analyzers, or to avoid any significant spillover and mixing of the respective gas streams flowing through the tubes 110, 120. Gas velocity in each of the tubes 110, 120 may be set at any desired rate by changing the cross-sectional area of the tubes 110, 120, or by changing the gas flow rate in either or both of the tubes within the overall system constraints. It can also be useful to cause a small amount of spillover from one gas stream to the other. For example, the integrity of the stream receiving transferred ions can be improved, or better maintained, if a small portion of that stream is caused to flow through the channels 170 into the ion source stream by maintaining a slightly higher gas pressure in the ion receiving stream as compared to the gas pressure in the ion source stream.
The ion concentration can be varied. The ion concentration at a particular point after transfer from the first tube to the second tube can be significantly changed from the ion concentration at a point in the first tube prior to the ion transfer. The variation can be caused by appropriate manipulation of the gas flow rates in either or both of the tubes. Hence, it is possible to obtain ion concentrations in the second tube that are the same as, or lesser than, or greater than, the original ion concentration in the first tube before ion transfer. For example, in a specific time period, ions can be transferred from a high volume, fast moving gas stream in the first tube to a low volume, slow moving gas stream in the second tube. Although the total number of ions remains essentially unchanged, the resulting ion concentration in the second tube gas stream can be far higher than was the ion concentration in the first tube. If the gas stream containing the transferred ions is then passed to a sensor that measures ion concentration, the resulting sensor output signal is similarly affected as is the signal to noise ratio. Raising ion concentration in the receiving gas stream can also provide an apparent increase in the sensor sensitivity, permitting the detection of lower ion concentrations.
Sensitivity and resolution of a sensor or detector system used with the exemplary methods and systems described herein can be improved by adding dopants or other chemicals to the gas stream of the transferred ions, thereby reducing interferences. For example, dopants or chemicals include chlorides, dilute acetone, dilute ammonia, weak acids or bases, or chemicals that would neutralize interferents, while not interfering with the detection of ions of interest. Chemicals added to the gas stream containing transferred ions may also be selected to neutralize ions or to add structural elements that could enhance or amplify detection of the modified molecule. For example, acetone can be added to the conditioned stream to improve both selectivity and sensitive for some analytes. Some detectors detect neutral molecules rather than ions. Using an ion transfer device, one can separate the ions and subsequently neutralize the ions and detect them using optical spectroscopy, for example. Further, the addition of structural elements to an ion or neutral molecule, such as fluorescent tags, can significantly increase the limits of sensitivity of detection.
A number of advantages can be obtained through use of the described ion transfer methods and systems. First, the rate of flow of gas through the first tube is independent of the rate of gas flow through the second tube, and those flow rates may be independently varied as well as the composition of the gas in the different tubes. For example, the gas carried in one tube may be ambient air and the gas carried in the second tube may be a fixed composition air or other gas or gas mixture. Ion transmission from one tube to another tube can be readily accomplished by applying a bias voltage to the first and second insulating layers and, by varying the voltage, some or most of the ions carried in one gas stream may be transferred to the other gas stream. Ions may be selectively separated from other unwanted uncharged components, such as particulate matter, water, and other unwanted species. The ion concentration may be increased or decreased by maintaining different gas flow rates in one of the tubes as compared to the other. Biological species, such as proteins and toxins, can be subjected to a charging mechanism such as electrospray and thereafter can be separated from unwanted neutral molecules. The tube design can be further used to add desirable components such as taggants, quantitative standards, reactants, and the like by entraining those desirable components in the gas stream to which the ions are transferred. Also, the described ion transfer methods and systems provide an effective method for conditioning analyte ions between ion source regions and destination regions. Typical destination regions include detector systems such as mass spectrometers, ion mobility spectrometers and differential mobility spectrometers, and systems such as those for deposition, printing, or sample preparation, among others.
Referring to
In operation, ions are first transferred from the ion source gas stream in tube 210 to an ion receiving gas stream in tube 220, and are then transferred a second time into a third gas stream flowing in tube 215. This multi-step procedure ensures that the final ion receiving stream flowing in tube 215 is essentially completely free of contamination from unwanted constituents present in the ion source stream so that optimum analytical results are obtained. A similar procedure can be used to perform chemical or physical modifications of the ions that are transferred from the first conduit to another conduit. Different chemical reactions or physical changes, such as those induced by radiation, structural change, or complex formation, among others, can be caused to occur at each stage, wherein the last stage is the transfer of the ions into an environment consistent with that needed for whatever the destination of the ions can be, for example, the sensor for optimum detection.
The embodiments illustrated in
Referring to
In these exemplary embodiments, mixing of the gas streams in the different tubes can be minimized if the streams are all in laminar flow. In theory, there should be very little transfer of neutral molecules and an application of an electric field should either push or pull the ions through the ion selective apertures without carrying along neutral molecules, because the ions are under both electric field and aerodynamic forces, and the neutral molecules are under aerodynamic forces. However, depending to some degree upon the geometry of the aperture between the two tubes, a slowly turning boundary can form between the gas streams in the tubes, as shown in
Alternatively, the gas diffusion and cross-pollution illustrated in
A gas stream containing the desired ion species in admixture with unwanted contaminant molecules is caused to flow through first tube 610, and an ion-receiving gas stream of selected composition is caused to flow through the second tube 620. Referring to
Cross-contamination of the ion-receiving gas flowing in tube 620 by the ion source gas in tube 610 may be even further reduced by introducing a low-rate flow from gas source 695 into one end of enclosed space 680 and exhausting an equal volume of gas 690 at the opposite end of the enclosed space 680. The composition of the gas source 695 is preferably the same as that of the ion-receiving gas in tube 620. Further, the pressure within enclosed space 680 may be maintained slightly higher than that of the ion source gas so as to cause a minor amount of spillover from the gas in space 680 into the ion source gas stream in tube 610.
Different parameters, such as structural characteristics of the ion selective aperture, velocity and direction of gas flow, and placement of electrodes, can control the movement of ions and neutral molecules from one gas stream to another gas stream. Structural characteristics of the particular ion selective aperture employed include aperture channel size, shape, and pattern, as well as the composition and thickness of the insulating layer. Ion transfer between gas streams is also affected by the velocity of gas flow across the ion selective aperture in both the ion source stream and the ion receiving stream, as well as by the direction of flow in the source and receiving streams, either concurrent or counter-current. Placement of the electrodes used to urge ions from the source stream to the receiving stream as well as the strength of the electric fields created by the application of differing voltages to the electrodes can also affect ion movement.
The ion transfer device described herein finds particular application in the field of chemical detection, analysis, and identification of explosives and explosives residues, of drugs, of toxic industrial chemicals of all sorts, of certain biological agents, and for any other application that requires extreme detector sensitivity and identification capability. In particular, the disclosed device facilitates the detection of ions that are best collected in one environment and detected or analyzed in a different environment. The systems and methods allow for the automated collection of ions, thereby providing an increase in the sensitivity of sensors that measure concentration. Chemicals or labels can be added to the ion stream to produce ion adducts or aggregates, or tagged ions of other sorts, or to cause reactions that change ion properties to occur. Also, standards (e.g., known quantities of a specific chemical) can be applied to the ion-receiving stream for consistent use with a sensor.
In another embodiment, an ion transfer device allows for the combination or reaction of the collected ions with chemicals that produce neutral or uncharged molecules that can subsequently be detected using sensors of other types as, for example, optical spectroscopic devices and acoustic wave devices, among many others. That capability allows neutral compounds present in air, or in liquids, or on surfaces, to be converted to ions in the manner described in U.S. Pat. No. 7,138,626, which is incorporated by reference in its entirety. Ions so produced may be collected using aerodynamic or electric field means and then transferred to an environment where they can be modified or tagged to produce molecules that are altered to enhance detection in a manner that has been previously described.
One advantage of such a methodology is the immediacy of the detection and/or identification of a neutral compound or sample that can be obtained directly from the environment. The methods and systems can also be used in conjunction with existing detectors that identify and quantify neutral chemicals or other compounds. As a result, existing detectors, which presently can detect chemicals present in only vapors or gases, can detect chemicals having extremely low vapor pressures (e.g., explosives and drugs), dissolved in liquids, or present on the surfaces of a wide variety of matrices (e.g., skin, paper, textiles, building materials). For example, neutral compounds present in air, dissolved in liquids, or on solid surfaces, can be ionized in the manner described in U.S. Pat. No. 7,138,626. Those ions may then be collected using aerodynamic or electric field means, transferred to an environment where they are converted to a neutral state using the methods and systems described herein, and thereafter aerodynamically pulled into a sensor or detector that is capable of identifying specific neutral chemicals or classes of chemicals. Such sensors or detectors include, for example, those employing optical spectroscopy and spectrometry, mobility spectrometry, and variants thereof.
A sensor used with the ion transfer systems and methods can also serve to provide real-time feedback control of the environment into which the ions are transferred by automatically monitoring the level of selected background chemicals present in that environment as a function of time. The monitoring may then be used to trigger an immediate response whenever the level of the selected background chemical (e.g., water vapor) falls above or below preset limits by causing adjustment of the devices feeding chemicals or other additives into the environment.
In one embodiment, sensor 740 is a differential mobility spectrometer, such as the Sionex microDMx, which provides extremely rapid detection and identification of ions. The ion-carrying gas introduced into sensor 740 can be of fixed composition, such as air containing a very low and stable amount of water. The humidity of the gas discharging from sensor 740 may be continuously monitored by detector means 770 and, based upon its humidity level, split into two streams 785, 795. Stream 785 may be then passed through a desiccant bed, such as a molecular sieve 790, and returned to the ion receiving stream flowing in tube 720. Stream 795 may be passed to enclosed space 780 so as to keep the pressure in space 780 slightly greater than that in tube 710. Further, moisture can be added to stream 795 and past the molecular sieve 790 to achieve the desired final humidity. The composition and humidity of the ion receiving gas stream is thereby maintained resulting in optimum sensor performance.
Referring to
In operation, both polarity ions are first collected from the dual polarity ion source into tube 810 and transmitted down the tube to the ion transfer region. In this embodiment, an attractive potential for each polarity ion is formed orthogonally to the flow of gas in tube 810 in the transfer device region due to voltages applied to outer conductive layers of aperture layers 830 and 835. Positive ions are attracted through aperture layer 830 into tube 815 held at a high negative potential. Negative ions are attracted through aperture layer 835 into tube 820. Flow of conditioned gas through tubes 815 and 820 entrain the transmitted ions that are transferred across aperture layers 830 and 835, respectively. Residual neutral materials pumped from the source region are exhausted to waste 837. The ions transmitted through tubes 815, entrained in conditioned gas, are carried through dielectric member 818 to ground potential and mixed at mixing union 825 and further transmitted to the DMS for detection and analysis. The ions transmitted through tubes 820, entrained in conditioned gas, are carried through dielectric member 823 to ground potential and mixed at mixing union 825 and further transmitted to the DMS for detection and analysis. The gases exiting the DMS are purified, conditioned, and recirculated.
Referring to
In operation, both polarity ions are first collected from the dual polarity ion source into separate ion optical wells through opening 907 for positive ions and 909 for negative ions. The voltage applied to the front of the sampling tubes will determine the polarity of ions collected at bottom of the optical wells. Attraction of positive ions to sample tube 910 is accomplished by applying a negative voltage to the front of the tube. Attraction of negative ions to sample tube 915 is accomplished by applying a positive voltage to the front of the tube. Once collected at the front of the respective tubes, the ions are entrained in the flow through the tubes. In the case of positive ions in first sample tube 910, the ions are pushed up a potential barrier by flow through first dielectric tube 913 into first sample tube 912. In the case of negative ions in second sample tube 915, the ions are pushed up a potential barrier by flow through first dielectric tube 918 into first sample tube 917. Positive ions passing through sample tube 912 (held at high positive potential) are attracted through aperture layer 930 into tube 920 held at a ground potential. Negative ions passing through sample tube 917 (held at high negative potential) are attracted through aperture layer 935 into tube 920 held at a ground potential. Residual neutral materials pumped from the source region are exhausted to waste 937. The ions transmitted through tube 920, entrained in conditioned gas, are carried to the DMS for detection and analysis. The gases exiting the DMS are purified, conditioned, and recirculated.
The embodiments described above are intended to be exemplary. One skilled in the art recognizes that numerous alternative components and embodiments may be substituted for the particular examples described herein and still fall within the scope of the invention.
This application claims priority to U.S. Provisional Patent Application Ser. No. 61/009,485, filed Dec. 28, 2007, entitled ION TRANSFER DEVICE, which is hereby incorporated by reference in its entirety.
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