1. Technical Field
The present invention relates to the field of excimer lamps, and in particular to a non-oxidizing electrode arrangement for an excimer (V)UV lamp.
2. Description of Related Art
The electrodes of prior art excimer lamps which emit in the VUV spectral range are susceptible to oxidation when operated in air, leading to corrosive deterioration of the electrode material. The oxidation is particularly pronounced with ultra-violet (UV) or deep ultra-violet (VUV) light sources as the emitted UV or VUV radiation produces atomic oxygen and ozone in the very proximity of the electrodes. Both atomic oxygen and ozone are extremely strong oxidizers that will readily oxidize prior art excimer lamp electrodes. These problems can be better understood with a review of excimer lamps.
In excimer lamps, excited diatomic molecules (excimers) are generated by an electrical gas discharge in rare gases or rare gas/halogen mixtures at gas pressures of 50–5000 Torr. When the excimer decays, it generates spectrally selective, narrow-banded radiation in the VUV, UV or visible spectral range, which can be used for various photo-initiated or photo-sensitized applications for solids, liquids and gases.
One form of electrical excitation is given by dielectric barrier discharges (DBDs). In a DBD-driven excimer lamp, a high voltage is applied across a gas gap, which is separated from metallic electrodes by at least one dielectric barrier. Dielectric barriers in excimer lamps include, for instance, glass or quartz which allow the emission of the radiation generated by the excimer.
Typical efficiencies of DBD-driven excimer VUV light sources depend on the electron densities and electron energy distribution function and can be “controlled” mainly by the applied voltage frequency and shape, gas pressure, gas composition and gas gap distance. Under usual conditions (several 10 kHz AC voltage, several 100 Torr gas pressure, few mm gap spacing), the radiant efficiency of DBD-driven lamps are in the range of 1–15% efficiency. Using other excitation voltages (such as steep-rising voltage pulses), UV efficiencies in the range of 20–40% can be obtained.
The uniqueness of excimer (V)UV light sources is that nearly all of the radiation is emitted in a spectrally selectively, and relatively narrow-banded spectral region. In fact, for photo-initiated or photo-sensitized processes, the emission can be considered quasi-monochromatic. Since many photo-physical and photo-chemical processes (e.g., UV curing and bonding, lacquer hardening, polymerization, material deposition, and UV oxidation) are initiated by a specific wavelength (ideally the excimer light source will emit close to those wavelengths), these light sources can be by far more effective than high-powered light sources that usually emit into a wide spectral range.
A problem arises when UV or VUV producing excimer light sources (lamps) are intended to be operated in oxygen-containing environments such as air. This is for example the case with Xenon excimer lamp systems (emitting at 172±7 nm) that utilize the VUV radiation for photochemical cleaning of surfaces in air (or similar). In this process the VUV radiation is used to photo dissociate molecular oxygen, leading to the formation of atomic oxygen and subsequently ozone, both of which are extremely strong oxidizing agents. As the atomic oxygen and/or ozone reach the surface of the material to be cleaned, a radical reaction with the surface contaminant is initiated, leading the removal of contaminants through a process called “advanced oxidation” or “cold combustion”. Unfortunately, just as the atomic oxygen and ozone react with the surface contaminants, they also readily oxidize the electrodes. Eventually, the electrodes oxidize enough that the lamp's performance is adversely affected.
One prior art solution to prevent oxidation of the excimer lamp's electrodes is to operate the sources in a lamp housing that is flushed with an inert, oxygen-free gas (typically pure nitrogen). The lamp housing also contains a transparent window, which allows the VUV radiation to be introduced into the oxygen-containing processing gas (e.g., air) where the photochemical cleaning takes place. An example of such a system is illustrated in
While this method protects the electrodes from oxidation, the protective quartz layer 220 and the positioning of the VUV sources in the inert gas filled lamp housing also increases the minimum distance between the treatment surface 240 and the electrode 200 on the lamp surface. The intensity on the system window (i.e., the protective quartz layer) is lower than on the excimer lamp itself, and hence more powerful and expensive lamps must be used for a purged excimer (V)UV system to obtain the same result as with a bare bulb. The protective quartz layer and the purged lamp housing also add to the cost of the excimer lamps.
The following is a summary of various aspects and advantages realizable according to various embodiments of the non-oxidizing electrode arrangement for an excimer lamp according to the present invention. It is provided as an introduction to assist those skilled in the art to more rapidly assimilate the detailed discussion of the invention that ensues and does not and is not intended in any way to limit the scope of the claims that are appended hereto.
The various embodiments described below are directed to a method of forming a non-oxidizing electrode arrangement for an excimer lamp by coating an electrode of the lamp with a layer of protective media that prevents the electrode from oxidizing. The protective media should be transparent when the output radiation of the lamp is intended to pass through, where one or both of the electrodes of the excimer lamp is coated with a transparent layer of protective media (e.g., silicon oxide, magnesium fluoride, calcium fluoride) to prevent oxidation of the electrode during lamp operation. The transparent layer of protective media is pure enough to allow transmission of desired frequencies of light. The transparent layer is preferably formed as a very thin layer (e.g., approximately 1 micrometer). Any coating that prevents oxidation and still allows the transmission of the desired light frequencies can be utilized for the protective media.
When the excimer lamp is configured as a DBD lamp, where one or both of the two electrodes is formed directly on a surface of the excimer lamp by coating a dielectric surface with a conductive material (e.g., aluminum or other metal), both the electrode and the dielectric are preferably coated with the protective media. In one embodiment, the electrode is formed on the lamp surface in the shape of a mesh (or grid), where the pattern of the mesh or grid can be chosen to provide a desired level of optical transmission through the electrode. When the electrode being covered is a grid, both the conductive material and the space between the conductive material that makes up the grid are preferably coated by the protective media.
Before forming the non-oxidizing electrode arrangement on the surface of the excimer lamp, the interior of the lamp is preferably evacuated to a pressure level that is lower than the pressure level surrounding the excimer lamp at any time during the electrode formation process. Keeping the pressure surrounding the excimer lamp from exceeding the pressure within the interior of the lamp during the electrode formation process helps maintain the structure integrity of the lamp, especially when the lamp is a flat excimer lamp.
The features of the present invention are set forth with particularity in the appended claims. The present invention, both as to its organization and manner of operation, together with further advantages, may best be understood by reference to the following description, taken in connection with the accompanying drawings in which the reference numerals designate like parts throughout the figures thereof and wherein:
The following description is provided to enable any person skilled in the art to make and use the invention and sets forth the best modes contemplated by the inventors of carrying out their invention. Various modifications, however, will remain readily apparent to those skilled in the art, since the general principles of the present invention have been defined herein specifically to provide a non-oxidizing electrode arrangement for an excimer lamp.
Referring now to
In block 320, a protective layer is deposited over the electrode that separates the electrode from an environment adjacent to the excimer lamp. The electrode and/or the surface of the excimer lamp is coated with the protective layer to prevent oxidation of the electrode during lamp operation or otherwise during exposure to oxygen in the surrounding environment. The protective layer is preferably formed to be transparent to at least one desired light frequency. The present invention is intended to be utilized with any type of excimer lamp, such as those containing excimers that emit radiation in the deep ultra-violet ((V)UV), the ultra-violet (UV), or the visible spectral range. The protective layer is pure enough to allow transmission of the desired frequencies of light. In one embodiment, the silicon oxide layer is a very thin layer (e.g., approximately 1 micrometer). The protective layer preferably must possess a low permeability for oxygen and be light transmissive. The protective layer preferably comprises at least one of silicon dioxide, magnesium fluoride or calcium fluoride.
Since the protective layer protects the electrode from oxidizing molecules in the environment, conventional quartz plates and inert purge gases are not required for the excimer lamp housing. Thus, the excimer lamp is able to get closer to treatment surfaces than prior art lamps without the electrode oxidizing, and lamp efficiency (i.e., system efficiency) is improved. This is particularly advantageous with flat panel excimer lamps for irradiating large treatment surfaces at close range; however the present invention is intended to be utilized with any excimer lamp configuration, including but not limited to the excimer lamps as described in United States Patent Application Publication No. 2002/0067130, Ser. No. 09/730,185, filed Dec. 5, 2000, entitled, “Flat-Panel, Large-Area, Dielectric Barrier Discharge-Driven V(UV) Light Source,” the contents of which are hereby incorporated by reference.
Referring now to
A second electrode 450 is formed on the opposite surface 460 of the flat excimer lamp 400 and may similarly be covered with a protective layer 470. The protective layer 470 may also be composed of the same substance as protective layer 430; however, in some embodiments, different substances are used to form the two protective layers.
In another preferred embodiment, at least one of the electrodes formed on the surface of the excimer lamp is formed in the shape of a mesh (or grid), as illustrated in
The second electrode 450 that is formed on the opposite surface 460 of excimer lamp may comprise any type of electrode configuration. In one preferred embodiment, the second electrode is not directly applied to the surface of the lamp. For example, a flat, conductive surface (e.g., a polished aluminum disk) may be positioned against the opposite surface 460 that acts as the second electrode 450. In other preferred embodiments, the second electrode 450 is also applied deposited on the opposite surface 460 of the lamp in similar fashion as any of the above-described deposition techniques for the first electrode 410. The second electrode 450 may be formed without gaps (i.e., as a continuous solid piece) or may be grid-shaped.
Flat excimer lamps are structurally sound when the pressure outside the lamp is higher than the pressure inside the lamp. However, flat excimer lamps are not as structurally sound when that pressure difference is eliminated or reversed. This can be problematic during excimer lamp formation, because many of the formation steps and deposition processes are performed in a relative vacuum. Thus, when the pressure in the environment outside the lamp is reduced to form the electrodes and protective layer, the lamp could fracture.
To avoid the pressure differential problem, before the electrode is formed on the surface of the flat excimer lamp, the interior of the lamp is evacuated to a pressure level that does not exceed the pressure level of the environment surrounding the flat excimer lamp at any time during the electrode formation process. The interior pressure of the excimer lamp is preferably maintained at a level lower than external pressure of the excimer lamp. For example, in one embodiment, the interior of the lamp is evacuated to a pressure level of less than 10−2 torr (preferably lower than this pressure level), and the pressure level outside the lamp when the electrode is formed is approximately 1–20 torr.
At block 730, the electrodes are formed on the lamp. At block 740, a protective layer is placed over the electrodes. At block 750, the exterior pressure is returned to atmospheric level. In some embodiments, the order of blocks 740 and 750 are reversed. At block 760, the lamp is filled with the desired fill gas. At block 770, the lamp is sealed.
The different structures of the non-oxidizing electrode arrangement for an excimer lamp of the present invention are described separately in each of the above embodiments. However, it is the full intention of the inventors of the present invention that the separate aspects of each embodiment described herein may be combined with the other embodiments described herein. Those skilled in the art will appreciate that various adaptations and modifications of the just described preferred embodiment can be configured without departing from the scope and spirit of the invention. Therefore, it is to be understood that, within the scope of the appended claims, the invention may be practiced other than as specifically described herein.
This application is a continuation of U.S. Provisional Patent Application Ser. No. 60/474,010, filed on May 29, 2003, entitled, “Non-Oxidizing Electrode Arrangement for Excimer V(UV) Lamps.”
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