1. Field of the Invention
The present invention relates to devices and methods for generating ions. More specifically, the invention relates to compact devices and methods for generating ions using a corona discharge at or near atmospheric pressure.
2. Description of the Related Art
Radioactive isotopes such as 241Am or 63Ni are commonly used as ionization sources to generate ions in a surrounding gas stream. Radioactive ionization sources have the advantage of simplicity, compactness, durability, and reliability. The regulations associated with these radioactive ionization sources, however, may render the incorporation of radioactive isotopes into a product economically unfeasible.
Electric field ionization has the advantage of simple design, relatively simple fabrication, and low power consumption. In electric field ionization, a large electric field between 107 to 108 V/m is generated between two electrodes. The large electric field accelerates any ions within the field thereby causing the accelerated ions to collide with surrounding gas molecules. The collision of an accelerated ion and a gas molecule creates an ionized molecule.
A corona discharge is a type of electric field ionization where a neutral fluid such as, for example, air is ionized near an electrode having a high electric potential gradient. Such a potential gradient is achieved by using a discharge electrode, having a small radius of curvature. The polarity of the discharge electrode determines whether the corona is a positive or negative corona. The corona has a plasma region and a unipolar region. In the plasma region, electrons avalanche to create more electron/ion pairs. In the unipolar region, the slowly moving massive (relative to the electron mass) ions move to the passive electrode, which is usually grounded. If the plasma region grows to encompass the passive electrode, a momentary spark or a continuous arc may occur. The spark or arc may damage the electrodes, produce contaminant ions, and reduce the lifetime of the ionization source. Therefore, there remains a need for devices and methods for compact ionization sources with longer lifetimes.
A compact ionization source includes first and second electrodes, each having a plurality of fingers that are interdigitated with each other. The spacing between the first and second electrodes, preferably less than 1 mm, creates a large electric field when a potential is applied across the first and second electrodes. The large electric field creates an ionization volume between the fingers of the first and second electrodes and ionizes a portion of the molecules occupying the ionization volume. The interdigitated fingers of the first and second electrodes allow for a narrow gap separating the electrodes while presenting a large flow area for ionizing molecules for downstream analysis.
One embodiment of the present invention is directed to an ionization source comprising: a first electrode having a first plurality of fingers; a second electrode having a second plurality of fingers, the first plurality of fingers being disposed between the second plurality of fingers; and a generator for applying a signal between the first and second electrodes, the signal generating an ionization volume between the first and second electrodes. In some aspects of the present invention, a distance between the first electrode and the second electrode is between 100 μm and 1 μm, preferably 60 μm and 5 μm and most preferably between 40 μm and 10 μm. In some aspects of the present invention, the ionization source further comprises a carbon nanotube layer disposed on a side of the first electrode facing a side of the second electrode. In some aspects of the present invention, the carbon nanotube layer comprises a plurality of carbon nanotubes characterized by a longitudinal axis, the longitudinal axis parallel to a surface normal of the side of the first electrode. In some aspects of the present invention, the ionization source further comprises a diamond-like coating (DLC) layer deposited on the first and second electrodes. In some aspects of the present invention, the DLC layer is comprised of tetrahedral amorphous carbon (ta-C). In some aspects of the present invention, the ta-C is n-doped.
The invention will be described by reference to the preferred and alternative embodiments thereof in conjunction with the drawings in which:
The configuration shown in
Each electrode 310, 315 includes a metal layer 320 deposited on substrate 325. The metal layers 320 may be Pt, Au, Cr, Cu, Ni, or other suitable electrode materials that may be sputtered, chemical vapor deposited or electroplated onto the substrate. The substrate is preferably silicon but may also be selected from insulator materials known in the microelectronic process arts such as, for example, glass, alumina, and quartz. An optional second metal layer 322 may be deposited on the face of the substrate opposite the first metal layer 320. In a preferred embodiment, the second metal layer 322 is held at or near the same voltage potential as the first metal layer 320.
In a preferred embodiment, electrodes 310, 315 are fabricated using deep reactive ion etching (DRIE) methods in the MEMS/semiconductor processing arts. In accordance with such methods, a metal layer 320 is first deposited on a first major surface of a continuous substrate 325. Optionally, a second metal layer 322 is then deposited on a second major surface of the substrate using photolithographic techniques. The metal layer(s) are then etched to separate electrodes 310, 315 and the substrate is etched through to define the gaps between the electrode fingers.
A voltage source 340 applies a voltage potential across the first and second electrodes, which creates an electric field in the volume 335 between the electrode fingers. The voltage is selected such that the electric field generated in volume 335 is sufficient to create an ionization region within volume 335 and ionize a portion of the molecules in the volume. The voltage source 340 may apply a DC voltage to create a corona discharge in volume 335 or may apply an RF voltage to generate a plasma in the volume.
Deflector electrode 360 may be disposed above and/or below the ionizer to drive ions from the volume 335 to another location for analysis. The “pass-through” design of ionizer 300 enables a gas to enter plenum volume 370, ionize a portion of the gas in ionizer 300, and have the ions removed to a second plenum volume 372 for downstream analysis. The “pass-through” design of ionizer 300 alternatively allows ions generated in ionizer 300 to be transported from the ionizer to the second plenum volume 372 by establishing a flow from the first plenum volume 370 to the second plenum volume 372.
Each electrode 410, 415 includes a metal layer 420 deposited on substrate 425. The metal layers 420 may be Pt, Au, Cr, Cu, Ni, or other suitable electrode materials that may be sputtered, chemical vapor deposited or electroplated onto the substrate. The substrate is preferably silicon but may also be selected from insulator materials known in the microelectronic process arts such as, for example, glass, alumina, and quartz. An optional second metal layer 422 may be deposited on the face of the substrate opposite the first metal layer 420. In a preferred embodiment, the second metal layer 422 is held at or near the same voltage potential as the first metal layer 420. In a preferred embodiment, electrodes 410, 415 are fabricated as described in conjunction with
A carbon nanotube layer 428 is disposed on the sides of the first electrode 410 facing the second electrode. In a preferred embodiment, the carbon nanotubes in layer 428 are oriented such that the axis of the carbon nanotube is generally parallel to the surface normal of the electrode side surface. The carbon nanotube layer may be fabricated in situ by biasing the electrodes and using plasma enhanced CVD methods such as those described in, for example, Chhowalla et al., “Growth process conditions of vertically aligned carbon nanotubes using plasma enhanced chemical vapor deposition,” J. Appl. Phys., vol. 90, no. 10 (November 2001), which is incorporated herein by reference.
It is believed, without being limited to a particular theory, that the small radius of curvature at the ends of the carbon nanotubes creates a large electric field concentration such that ignition of a corona occurs at a lower applied potential across the first and second electrodes.
A voltage source (not shown) similar to voltage source 340 of
Deflector electrode 460 may be disposed above and/or below the ionizer to drive ions from the volume 435 to another location for analysis. The “pass-through” design of ionizer 401 enables a gas to enter plenum volume 470, ionize a portion of the gas in ionizer 401, and have the ions removed to a second plenum volume 472 for downstream analysis. The “pass-through” design of ionizer 401 alternatively allows ions generated in ionizer 401 to be transported from the ionizer to the second plenum volume 472 by establishing a flow from the first plenum volume 470 to the second plenum volume 472.
Each electrode 510, 515 includes a metal layer 520 deposited on substrate 525. The metal layers 520 may be Pt, Au, Cr, Cu, Ni, or other suitable electrode materials that may be sputtered, chemical vapor deposited or electroplated onto the substrate. The substrate is preferably silicon but may also be selected from insulator materials known in the microelectronic process arts such as, for example, glass, alumina, and quartz. An optional second metal layer 522 may be deposited on the face of the substrate opposite the first metal layer 520. In a preferred embodiment, the second metal layer 522 is held at or near the same voltage potential as the first metal layer 520. In a preferred embodiment, electrodes 510, 515 are fabricated as described in conjunction with
A diamond-like coating (DLC) layer 529 covers the first and second electrodes 510, 515. In a preferred embodiment, the DLC layer is formed using filtered cathodic vacuum arc (FCVA) as described in Satyanarayana et al., “Field emission from tetrahedral amorphous carbon,” Appl. Phys. Lett., vol 71, no. 10, (September 1997), which is incorporated herein by reference.
It is believed that, without being limited to a particular theory, the n-doped tetrahedral amorphous carbon (ta-C) in the DLC layer results in field emission of electrons at field strengths of about 10 V/μm. The chemical inertness and high hardness of the DLC layer is believed to contribute to improving the electrode lifetime.
A voltage source (not shown) similar to voltage source 340 of
Deflector electrode 560 may be disposed above and/or below the ionizer to drive ions from the volume 535 to another location for analysis. The “pass-through” design of ionizer 502 enables a gas to enter plenum volume 570, ionize a portion of the gas in ionizer 502, and have the ions removed to a second plenum volume 572 for downstream analysis. The “pass-through” design of ionizer 502 alternatively allows ions generated in ionizer 502 to be transported from the ionizer to the second plenum volume 572 by establishing a flow from the first plenum volume 570 to the second plenum volume 572.
Having thus described at least illustrative embodiments of the invention, various modifications, and improvements will readily occur to those skilled in the art and are intended to be within the scope of the invention. Accordingly, the foregoing description is by way of example only and is not intended as limiting. The invention is limited only as defined in the following claims and the equivalents thereto.
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