There is considerable ongoing effort to develop and produce low cost, high performance (high output) light emitting diodes (LEDs). Such LEDs are intended for such disparate uses as in outdoor displays, vehicle lighting, flashlights, safety signaling systems, traffic signals, lasers, medical devices and indoor lighting. LEDs are expected to replace the current incandescent bulbs or fluorescent lighting tubes if they can reach the flux intensity and low cost of current bulbs. The advantage LEDs have is very low power and heat generation for a given light intensity, small size, and extremely long life well in excess of 50,000 hrs.
These LEDs are made by metal organic chemical vapor deposition (MOCVD) using materials such as gallium-, aluminum gallium- and indium gallium nitrides and phosphides. In a process currently of significant interest, gallium nitride is deposited from a gaseous mixture of ammonia, hydrogen and trimethyl gallium. Similar, gallium nitride is being considered for “blue lasers,” i.e., lasers which emit blue light. Because blue light has a shorter wavelength than red, yellow or green light, blue lasers are anticipated to be capable of forming compact disks which will have a much higher information density than is presently the case with compact disks produced with red laser light. Gallium nitride for such blue lasers would be manufactured in the same type of ammonia/hydrogen/trimethyl gallium gaseous environment as described above for the high capacity LEDs. A high purity supply of hydrogen, ammonia, and nitrogen is essential to production of these devices.
The LEDs, blue lasers and integrated circuits are all manufactured with electron accepting p-type dopants. Such products are extremely sensitive to the presence of electron-donating n-type materials, and very small concentrations of such n-type are sufficient to deactivate the p-type dopants and impair or destroy the performance and operability of the integrated circuits, LEDs and blue lasers. Oxygen is a particularly efficient n-type material, and the presence of molecular oxygen causes lattice defects and is detrimental to the desired band gap properties in the semiconductor or laser material. Even very low concentrations of oxygen (between 10 and 100 ppb) can be sufficient to cause sufficient reduction in performance or operability (especially in wavelength control) so as to require discarding of the product after manufacture or to significantly shorten operating lifetime
Similar detrimental effects are observed with the presence of sub ppm levels of water vapor, gaseous hydrocarbons and/or carbon dioxide gas in hydride gases such as ammonia, since those materials lead to degradation of the products formed by deposition of active layers of metals or metal compounds from a hydride gas environment. Water is one of the most common and yet most difficult impurities to remove from the gases, especially hydride gasses such as ammonia. In the manufacture of the semiconductor products described above, moisture contents of the depositing gases which are in the ppm range are excessively wet. To form satisfactory products, the water content of the depositing gases must be reduced to the parts per billion (ppb) range, usually down to no more than about 100 ppb. See Whitlock et al, “High Purity Gases,” in Ruthven, ed., Encyclopedia of Separation Technology, vol. 1, pp. 987-1000 (1997).
In most high-purity product manufacturing processes, it has been conventional for hydride gases to be stored in and supplied from standard gas cylinders. The volume of gas in each such cylinder is of course limited, so that in larger scale manufacturing processes, it becomes necessary for process operators frequently to replace emptied cylinders and replace them with fresh, fall cylinders. This frequent handling and movement of heavy, awkward gas cylinders represents a safety hazard to the operators, as well as providing opportunities for gas leakage and increasing the cost of manufacturing. Also importantly, each time an empty gas cylinder is detached from the system and a new full cylinder attached, there is an opportunity for ambient contaminant gases, such as oxygen, carbon dioxide and water vapor, to enter the system, thus increasing the decontamination load on the system and accelerating the system degradation. Higher volume production may also require large banks of cylinders to be connected in parallel, increasing the probability of contamination problems, and making it very difficult to track down and replace a s contaminated cylinder. The purity of gasses delivered in these cylinders may also be compromised due to out-gassing of impurities from the cylinder walls, since the container surface area to volume ratio is higher than for bulk delivery in large containers. This same effect can change the purity of cylinder stored gasses over time as well, since out-gassing impurities can increase impurity concentrations the longer a gas is stored. As the quantity of gas in the cylinder is reduced due to consumption, the impurity levels will also increase since the impurity desorption fluxes are being accumulated in a total quantity of gas that is decreasing. Gas delivered in cylinders is generally much more expensive than gas delivered in bulk, especially for premium high purity levels in low ppb ranges. The customer will pay a significant adder for delivery, onsite storage, and pickup of cylinders from the gas company. In addition, it has become the common practice of ammonia users to change cylinders with 20% or more of the total volume of the cylinder remaining due to this concentration of impurities “at the bottom of the barrel”. Clearly, there is a need for a more economic alternative.
The industry is beginning to require gases to be supplied in large volume containers which need to be changed only at infrequent intervals (usually measured in months rather than hours, as with the individual gas cylinders). A preferred type of large volume container is the “tube trailer,” a semi-trailer which is constructed with a number of “tubes,” high capacity extended high pressure vessels, which are interconnected or operate through a common manifold. A tube trailer can be parked at a manufacturing facility and attached to the gas supply system, and will typically have sufficient gas capacity to supply the hydride gas to the facility for a period of months. Bulk hydrogen may be delivered as pressurized gas in tube trailers or as a cryogenic liquid. Liquid hydrogen requires sophisticated, expensive storage requirements and is not widely distributed throughout the world. However, even these bulk delivery systems can introduce contamination every time a new container is connected or disconnected from the plant, or the cryogenic fluid is replenished. Furthermore, contamination can be introduced in the piping systems that deliver the bulk gas to the point of use, or process tool. Removing and controlling this contamination requires the use of distributed purifiers, which may be placed at multiple locations in the distribution system. While effective in controlling contamination, this distributed purification scheme can be expensive to purchase, install, and maintain.
It would be of interest, for the flexible, low cost production of high performance LEDs and blue lasers, to manufacture high purity ammonia, hydrogen, and nitrogen from de-ionized (DI) water and standard nitrogen. Point of use production eliminates the contamination associated with delivery from bulk storage and cylinders, and the need for layers of distributed purification. De-ionized water and standard purity nitrogen are very common reagents and are universally available in all semiconductor plants. Furthermore, point of use production of high purity ammonia, hydrogen, and nitrogen from DI water is suitable for plants being set up in countries where there is limited chemical industry infrastructure, and the production of high purity gasses does not exist. However, current DI water to hydrogen POU production equipment cannot create hydrogen of a quality suitable for most semiconductor applications and as specifications for fuel cells increase, for that market as well.
It is an object of the present invention to provide a method for the manufacture of high purity ammonia, hydrogen, and nitrogen from de-ionized (DI) water and standard nitrogen. In a first embodiment of the present invention, the method comprises feeding a quantity of de-ionized water to a hydrogen generator, producing hydrogen from the deionized water, and purifying the hydrogen with a hydrogen purifier. The method further comprises producing purified nitrogen by passing standard quality nitrogen through a nitrogen purifier and, contacting the purified hydrogen and purified nitrogen with a catalyst bed, wherein a portion of the purified hydrogen purified nitrogen react to form a quantity of ammonia.
In another embodiment of the present invention, the method comprises de-gassing the de-ionized water to remove a portion of dissolved gasses, feeding the de-ionized, degassed water to a hydrogen generator, and producing hydrogen from the de-ionized, de-gassed water. The method further comprises producing a quantity of purified hydrogen by passing the hydrogen through a hydrogen purifier, producing purified nitrogen by passing standard quality nitrogen through a nitrogen purifier, compressing said the purified hydrogen and the purified nitrogen, and contacting the compressed purified hydrogen and purified nitrogen with a catalyst bed, wherein a portion of the purified hydrogen and a portion of the purified nitrogen react to form a quantity of ammonia. Purified ammonia is produced by passing the ammonia through an ammonia purifier and then delivered to a semiconductor process tool.
The present invention will be better understood when consideration is given to the following detailed description thereof. Such description makes reference to the annexed drawings, wherein:
It is an object of the present invention, useful for the flexible, low cost production of high performance IEDs and blue lasers, to provide a method for the manufacture of high purity ammonia, hydrogen, and nitrogen from de-ionized (DI) water and standard nitrogen. Point of use production eliminates the contamination associated with delivery from bulk storage and cylinders, and the need for layers of distributed purification. De-ionized water and standard purity nitrogen are very common reagents and are universally available in all semiconductor plants. Furthermore, point of use production of high purity ammonia, hydrogen, and nitrogen from DI water and standard nitrogen is suitable for plants being set up in countries where there is limited chemical industry infrastructure, and the production and distribution of ultra high purity gasses does not exist.
An alternative degassing device would be a single stage device used in combination with pre-heated DI water. The pre-heated water would facilitate the degassing of the oxygen and CO2. Pulling vacuum on the degasser would eliminate the unwanted gas from the heated DI water. Pre-heating the DI water more than about 90° C. and then degassing with a per-fluorinated membrane contactor, such as a pHasor®II manufactured by Mykrolis Corporation (Billerica, Mass.), would be a preferable embodiment. Still higher temperature DI water could be entertained, particularly if such higher temperatures improved the efficiency of the hydrogen generator.
De-gassed water 124 leaving the degasser 108 is introduced to the hydrogen generator 126. In the hydrogen generator, water is de-composed to hydrogen gas and oxygen gas by electrolytic means, as is well known to those skilled in the art. For example, a hydrogen generator 126 manufactured by Proton Energy Systems (as the HOGEN® line of hydrogen generators) may be used. Hydrogen gas produced by the generator has a typical water impurity level of less than about 5 ppm, and an oxygen impurity level of less than about ppm. These impurity levels are too high for end use and require further purification. Hydrogen delivery pressures are typically less than 14 bar. Oxygen produced by generator 126 is vented via output 128. Excess water is drained via output 134. The hydrogen output 130 is fed to input 132 of the hydrogen regenerable purifier 136. The detailed configuration of the regenerable purifiers is shown below in
The purified hydrogen output at 142 is delivered to a number of locations within process 100. It is utilized for regeneration of the nitrogen purifier 144 (at input 148), regeneration of the ammonia purifier 174 (at input 170), to compressor 156 for the production of ammonia, and for delivery to the process tool at output 172.
Nitrogen fed to the process 100 at input 104 is fed to the nitrogen regenerable purifier 144 at input 146. The detailed configuration of the regenerable purifiers is shown below in
Purified nitrogen and purified hydrogen is mixed at 153 and fed to compressor input 154. Due to the high purity requirements of the end product ammonia, compressor 156 should produce as little contamination as possible. An air driven diaphragm compressor, such as that made by Haskell, would be suitable. Other types may also be utilized, if suitable contamination levels can be maintained. Pressure levels exiting compressor 156 should be below about 100 bar, preferably in the range of about 30 to about 80 bar. The compressed nitrogen/hydrogen mixture exits the compressor at 158 and enters the ammonia reactor 162. Stoichiometric requirements for the production of pure ammonia necessitate a mole ratio of 3:1 hydrogen/nitrogen. The actual ratios may vary, depending on the conversion to ammonia and the amount of unreacted nitrogen and or hydrogen desired in the product stream. In the present invention, the product ammonia is primarily utilized for the point of use production of MOCVD films, where hydrogen and/or nitrogen are often mixed with ammonia prior to entry into the deposition chamber. The ammonia production process can therefore be tailored to the downstream CVD process, and the requirement for 100% ammonia conversion is not a strict requirement. Subsequently, the extreme conditions required by industrial ammonia production processes which include the complete separation of ammonia from unreacted hydrogen and nitrogen, and the recycle of theses gasses back to the reactor input, are not required in the present invention. Ammonia reactor 162 contains a heated catalyst bed where the hydrogen/nitrogen is reacted to form ammonia. As mentioned previously, 100% conversion to ammonia may not be required. Operating conditions of the catalyst bed would include an operating total pressure below about 100 bar, preferably in the range of about 30 to about 80 bar, most preferably about 50 bar; an operating temperature in the range of about 50 to about 400° C., preferably about 100° C. The catalyst bed 164 may comprise a standard iron oxide (magnetite) ammonia catalyst, a precious metal (platinum or palladium) promoted iron oxide catalyst, or ruthenium supported on carbon, alumina, or zeolites. These catalysts may be used alone or in combination. Other catalysts may also be used as disclosed or known in the art.
Ammonia and any unreacted nitrogen and hydrogen exit the ammonia reactor at 166 and enter the ammonia purifier 174 at input 168. The detailed configuration of the regenerable purifiers is shown below in
While various embodiments have been described above, it should be understood that they have been presented by way of example only, and not limitation. Thus, the breadth and scope of an embodiment of the present invention should not be limited by any of the above described exemplary embodiments, but should be defined only in accordance with the following claims and their equivalents.
Number | Date | Country | Kind |
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10626266 | Jul 2003 | US | national |
This application claims priority and is a continuation-in-part of U.S. application Ser. No. 10/626,266, filed Jul. 23, 2003. The entire teachings of the above application is incorporated herein by reference.
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/US04/23594 | 7/22/2004 | WO | 4/13/2006 |