PROCESS FOR SURFACE AND FLUID CLEANING

Abstract: A cleaning system which utilizes surface tension forces (4) and phase changes. The surface (21) to be cleaned is submerged within a vessel (30), and the vessel pressure is increased. Rapid depressurization causes bubbles (12) to form around undesired particulate matter (13) on the surface (14) of the article, the bubbles (12) rising to the surface of the liquid (27), thereby cleaning the article. A second embodiment applies a cleaning fluid (52) to the surface of the article (49) and freezes the fluid (52), thereby reducing the adhesion force between the surface and the particulates. The surface is subsequently heated, and the particulate matter is removed through the medium of the cleaning fluid (52).

Description: PROCESS FOR SURFACE AND FLUID CLEANING Background of the Invention Field of the Invention This application relates to new and novel methods f cleaning both surfaces and liquids. More particularly, t present invention concerns methods of removing smal particulate matter from surfaces, and from fluids in whic such particles may be suspended. Description of Related Technology Cleaning techniques are as varied as the contaminant and media to be cleaned. Precision cleaning has taken o great importance in recent years due to the necessity i certain fields, such as computer disks and integrated circui manufacture, where the removal of microscopic particulat matter is essential to assure the basic efficacy of th device or manufacturing process. For example, in th manufacture of silicon wafers as used in the integrate circuit industry, a rejection rate of 20 to 30 percent can b caused solely by the presence of particulate matter on th surface of the wafers. Various methods have been employed in the field o precision cleaning, including ultrasonics, megasonics wiping, brush scrubbing, low pressure surfactant spraying high pressure jet spraying, etching and centrifugal spraying Each of these methods will now be briefly discussed. In ultrasonic cleaning, a part is immersed in a suitabl liquid medium and sonicated or agitated at a high frequenc (18 to 120 kilohertz). This usually lasts for severa minutes, and then the part is rinsed and dried. Cavitatio occurs when microscopic bubbles form in the liquid medium an then violently collapse or implode, mechanically scouring th part to be cleaned and displacing and loosening th contaminants. There are many advantages to ultrasoni cleaning. It is fast, effective and safe to use. It requires less heat than other cleaning methods, and when used properly it can vigorously clean delicate parts without harming surface finishes. Also, there is no need to dismantle assemblies. Disadvantages of ultrasonic cleaning include its complexity and the generation of noise. In fact, ultrasonic cleaning makes so much noise at frequencies lower than 20 kilohertz that a 40 kilohertz frequency is recommended even though it is less efficient. Megasonic cleaning is another cleaning method whic consists of basically the same steps as ultrasonic cleaning: immersion, agitation or sonication, rinsing and drying. Th major difference between the two is that while ultrasoni frequencies range from 18 to 120 kilohertz, megasoni frequencies are in the range of 0.8 to 1 megahertz with inpu power densities ranging from 5 to 10 watts per centimeter. Whereas the cleaning action in ultrasonic cleaning comes fro cavitation, the cleaning action in megasonic cleaning come from high pressure waves pushing and tugging at contaminant lodged on a part's surface. There are many advantages t megasonic cleaning. It causes almost no scratches, breakag or chipping since substrates are not transferred or subjecte to any mechanical stress. It is three to four times mor productive than scrubbing or chemical cleaning at an equal o lower investment cost and produces superior wafe cleanliness. Megasonic cleaning consumes only about a eighth the amount of chemical solvents when compared t conventional chemical cleaning, and megasonic cleaners hav low maintenance and are simpler to automate. Megasoni cleaners are also able to use more chemically active cleanin solutions such as hydrogen peroxide and amonium hydroxide. Megasonic cleaning also has some disadvantages. Fo example, the solvent system must be adapted to the particula contaminant-substrate bonding and the transducer matrix i not a commercial item. Cleaning solutions such as stron hydrofluoric acid cannot be used, and a substrate containe must be designed to minimize obstruction to the megasoni beam . Although it may not be as efficient as sonic cleanin wiping is another successful cleaning method. It is a inefficient but effective method of particle removal that i commonly used to clean optical surfaces. Besides the amoun of time it takes, a major drawback to wiping is tha particles can be deposited from the tissue or the solven being used. Wiping is also unable to reach irregular surfac geometries and the results depend on the wiper's skill an attention to detail. A related method of cleaning is brush scrubbing. In th brush scrubbing method, the brush never actually touches th surface being cleaned due to the hydrophilic nature of th brush. There is always the film of the scrubbing solutio between the brush and the surface. The hydrophilic brus will only remove contaminants from hydrophobic surfaces Surfaces that are hydrophilic are more difficult to clea because suspended contaminants can precipitate onto them There are several factors which contribute to making brus scrubbing ineffective. First, the aqueous neutral detergen solutions used with scrubbers can leave behind thin nylo films. When used with chemically active cleaning solutions rapid corrosion can occur. If this is true, chemica cleaning is then also required, and this inevitabl introduces more particles. Another problem can arise whe brushes become infested with dirt particles and debris fro surface breakage or chipping. When this happens, the brushe themselves can become sources of contamination and scratches Finally, scrubbers are sequential in operation and can onl clean one part, and often only one side, at a time. Unlike brush scrubbing, low pressure surfactant sprayin relies on chemical means to remove particles. Its succes depends on the effectiveness of the detergent that it sprays The pressure of the jet itself, which can vary from 5 ps (34.5 kPa) to 80 psi (552 kPa), is not nearly enough b itself to remove particles. Therefore, the compatability o the detergent with the contaminant and the surface i crucial. Detergents are surfactants which function b reducing the surface tension of water. They remove soil through emulsification and by concentrating at wate interfaces. At high concentrations, detergent solutions for micelles. Micelles occur when the detergent carbon chai forms a low polarity region that is stabilized by having th polar ends in contact with the water. The cleansing actio occurs because the lowered water surface tension allows th detergent to penetrate and the micelles to dissolve grease and oils by taking them into the carbon regions. High pressure jet cleaning operates under very differen principles than surfactant spraying. It works when the shea force it exerts is greater than the adhesion force holding particle to a surface. The method consists of a hig velocity jet of liquid sweeping across a surface at pressure of 100 to 4,000 psi (690 to 27,580 kPa) . The main advantag of high pressure jet scrubbing is that it is able to remov microscopic debris from difficult surface geometries such a depressions and circuit corners. Etching is one of the most common cleaning methods used It is a chemical cleaning method that consists of dissolvin unwanted substances on a surface and is not as severe to t surface as a mechanical means of surface treatment. Etchin is closely related to acid cleaning and is one of the mos important procedures in microelectronic device fabricatio Etching is performed as a sequential purification process i which oxidation and dissolution of residual or organi impurities in certain metal contaminants occurs in a mixtur of water, hydrogen peroxide and ammonia peroxide. A soluti of hydrogen peroxide and hydrochloric acid is used to remo heavy metals and to prevent displacement replating fr solution by forming soluble complexes with the resulti ions. These solutions are chosen because they are complete volatile. They are also less hazardous than other possib cleaning mixtures and present no disposal problems. Th method works because at a high pH, hydrogen peroxi solutions are effective at removing organic contaminants oxidation and at a low pH they are effective at desorbi metal contaminants by complexing. This technique i particularly useful in cleaning silicon device wafers, quart tubes, and parts used in semiconductor processing. Centrifugal spray cleaning is an effective cleanin alternative to chemical immersion processes. It is commonl used for cleaning wafers. The wafers are enclosed in sealed chamber purged with nitrogen. As the wafers spin they are subjected to a series of continuous fine sprays o reagent solutions, including a hot aqueous solution o hydrogen peroxide and ammonium hydroxide, an aqueous solutio of hydrochloric acid and hydrogen peroxide, and high purit water. Recontamination is prevented by arranging the spray so that each wafer is continuously exposed to fres solutions. Wafers are sprayed at 2,500 psi (17,240 kPa) After the wafers have been sprayed, they are dried wit nitrogen. Centrifugal spray cleaning relies on centrifuga force, shear force and solvency. A commercial apparatus for cleaning semiconductor wafer is disclosed in U.S. Pat. No. 4,186,032, issued to Ham. I this device, super-heated steam is passed over the surface o the wafer, the condensate being permitted to form and dri off the wafer and drying being accomplished by heating chamber to a temperature in excess of 100°C. Note that thi apparatus is limited to cleaning loose foreign surface matte and chemical impurities. The following chart presents the current state of th art of methods for surface particle removal: CLEANING LOWER LIMIT GENERAL METHOD MECHANISM PARTICLE SIZE CHARACTERISTICS ultrasonic cavitation 25 microns frequency range of 18 to 100 kilohertz; may damage surface megasonic high pressure 0.2 microns frequency range waves eight-tenths to one megahertz; 15 minutes duration wiping sheer 5 microns time-consuming brush mechanical 0.5 microns does not work scrubbing and sheer well on hydro¬ philic surface low mechanical 0.2 microns pressure range pressure and of 5 to 80 spray detergency pounds per inch; relatively time-consuming high sheer 0.2 microns pressure range pressure of 100 to 4,000 spray pounds per square inch; relatively slow; can damage surface Each of the cleaning methods heretofore discussed ha required either the use of an active mechanical component, the use of special chemical solutions, or labor intensiv human participation in order to achieve a satisfactory leve of effectiveness. Furthermore, each cleaning metho discussed is limited to a particular class of media to b cleaned, and, given the stringent requirements of certai industries, the absolute cleaning effectiveness of eac method is not yet at a uniform, commercially acceptabl level. Summary of the Invention Our invention is intended to remove particles tha reside on the surfaces of solid objects or which may b suspended in liquid solutions. The invention is particularl applicable to the semiconductor and computer industries wher cleanliness is of the utmost importance in the manufacturin of such devices as semiconductor integrated circuit chips disk drives, and other sophisticated electrical or mechanica components. For example, in the manufacture of semi-conduct wafers, the current yield in commercial operations is oft only on the order of 20 to 30%. A yield of 50% would considered quite high. A major reason for the low yield commercial semi-conductor wafer manufacture is the inabili to achieve uniform and consistent cleanliness during t manufacturing process. For example, on many semi-conduct devices, the dimensions between adjacent paths of the circu may be only on the order of one micron, and can often go low as 0.25 microns in some experimental devices. A hum hair typically has a diameter of 70 microns, and so one m readily realize that even the smallest particles may beco lodged in integrated circuitry devices and thereby cau irreparable damage. The invention also has applications in the manufacturi of precision optical components such as mirrors, lense lasers and other components whose surfaces must be kept cle to prevent a scattering of light and the degradation performance. Other applications of the invention may found in the pharmaceutical and biotechnology industri where particulate matter must be removed from surfaces liquids during the manufacturing process. The miner processing industry is another field where particulate matt must frequently be separated from the liquid in which t particles are suspended. Accordingly, the present invention discloses nov methods and apparatus for cleaning surfaces and fluids. In one embodiment, the surface to be cleaned, such as silicon or gallium arsenide semiconductor wafer used in th manufacture of semiconductor integrated circuit chips, i immersed in a liquid, such as water housed in a vessel. gas, such as carbon dioxide, is then introduced into th vessel and the pressure of the gas is increased. The ga will dissolve in the liquid, with the amount of gas dissolve increasing with increasing pressure. By increasing the ga pressure to a sufficiently high level, a given amount of th gas can be caused to dissolve in the liquid. After some tim has elapsed, during which time the gas has dissolved into th liquid, a valve in the vessel is opened, substantiall instantaneously, in order to relieve the gas pressure. Th sudden drop in gas pressure causes the dissolved gas in th liquid to form bubbles. Since the formation of a gas bubbl in the liquid will require a nucleus around which a gas ca form, particles immersed in the liquid will serve as nucle for bubble formation. As bubbles form around the particle in the liquid and grow in size, the buoyant force wil increase. Eventually the bubble will detach from the surfac and ascend in the liquid, carrying the particle with it t the top of the liquid surface. By this means, the particle will be detached from the surface of the object to be cleane and congregate at the surface of the liquid. Brief Description of the Drawings Figure 1 is a schematic drawing of an apparatus fo surface cleaning constructed according to the principles o the present invention; Figure 2 is a second embodiment of an apparatu constructed according to the principles of the presen invention; Figure 3 is a schematic diagram illustrating bubbl formation under a particle according to the principles of th present invention; Figure 4 is a schematic diagram illustrating bubbl formation around the particle according to the principles o the present invention; Figure 5 is a schematic diagram of a liquid cleanin system constructed according to the principles of the presen invention; Figure 6 is a schematic diagram showing forces acting o a gas bubble as utilized in the present invention; Figure 7 is a schematic diagram depicting an alternat method and apparatus for cleaning wafer surfaces; Figure 8 is a cross-sectional view depicting th mechanics of particle removal as utilized by the metho depicted in Figure 7; Figure 9 is a schematic view depicting the adhesio distance between a particle and a surface during a phas change; Figure 10 is a schematic diagram of an apparatus fo cleaning a single wafer using the method depicted in Figur 7; Figure 11 is a schematic diagram of a system fo cleaning a wafer utilizing a spindle; and Figure 12 depicts a method of cleaning a cassette o wafers utilizing a rotating spindle. Detailed Description of the Preferred Embodiments The relevant fluid dynamics relationships utilized b the present invention can best be visualized by reference t Figures 3, 4 and 6. Referring particularly to Figure 6, -th relationship between bubble size and gas pressure can b discerned. The gas bubble shown generally at 1 is internall supported by a uniform pressure, signified by arrows 2 having a value of p. The bubble 1 has a radius 3, having value of r. The size of the bubble 1 is constrained by th action of surface tension forces 4, having a value of f which are uniformly exerted on bubble 1 by the liquid i which bubble 1 resides. Normally, the pressure p exerted b the gas inside the bubble 1 will be at equilibrium with th surface tension forces f exerted by the liquid, and th bubble 1 will have a constant radius r. The bubble 1 wil grow in size only when the pressure force is higher than th surface tension force. The minimum value of p which must b achieved in order to achieve bubble growth is given by th equation: where r is the radius of bubble 1 and f is the surfac tension of the liquid. By rearranging the terms of equatio 1, the value of p is given by the equation: p = 2__ = 4f . (2) r d where d is the diameter of the bubble 1. Equation 2 als permits calculation of the diameter of the particle aroun which the gas bubble 1 can form. Table 1 shows the values o particle diameter d and pressure p for bubble formatio within liquid water, where f equals 72 dynes per centimeter. Table I RELATIONSHIP BETWEEN PARTICLE DIAMETER (d) AND GAS PRESSURE (p) FOR BUBBLE FORMATION d (micrometers) o ( ps i ) / ( kPa ) 10.00 8 . 4 ( 58 ) 1.00 84 . 0 ( 579 ) 0.10 840 . 0 ( 5 , 792 ) 0.05 1 , 680 . 0 ( 11 , 580 ) The actual mechanism of particle formation is bes viewed with reference to Figures 3 and 4. In Figure 3, single bubble 5, having a left lobe 5a and a right lobe 5 is seen to first form in the space between the particle 6 a the surface 7. The relatively high gas pressure within t bubble then pushes the particle 6 away from the surface thereby overcoming the adhesion force between the partic and the surface. The pressure force, p, is shown by arro 8. In addition to the pressure forces 8, there is also t surface tension forces, f, shown by arrows 9 which a tangentially to the surface of particle 6 and which also a in a direction that would tend to lift the particle 6 aw from surface 7. By this means, the particle 6 is detach and removed from the surface 7 by means of resultant force acting to overcome the adhesion force 11. A second mechanism of bubble formation is shown Figure 4, where a bubble 12 first forms around a particle 1 The particle 13 then attaches itself to the bubble 12, t particle 13 becoming separated from the surface 14 as t bubble 12 detaches itself from the surface 14 and ris within the liquid. In either mechanism, the particle i separated from the surface (7 or 14) and carried by th bubble (6 or 12) to the surface (15 or 16) of the liquid Note that in Figure 4, the surface tension force 17 (whic creates a resultant force 20) assists in transmitting th buoyant force 18 to particle 13, thereby overcoming surfac adhesion force 19. The precise manner in which bubbles form in a liqui will vary depending on the surface tension of the liquid an the surface properties of the particle. A hydrophobi particle surface will probably cause the bubble to for differently than a hydrophilic particle surface. However regardless of the manner in which the bubble is formed, th force exerted by the bubble on the particle will be hig enough to cause the particle to be separated from th surface, provided, of course, that a sufficiently hig initial gas pressure is used. Apparatus suitable for exploiting these relationships t accomplish the cleaning of a surface or a liquid is shown i Figures 1, 2 and 5. Referring particularly to Figure 1, a apparatus is shown which may be useful for cleaning a article 21, such as a wafer or a magnetic memory disk as use in computers. The article 21 is first placed in a pressur vessel 22. Deionized and filtered water or some othe suitable cleaning fluid is then introduced into the vessel 2 through valve 23 until the article 21 is completel submerged. A gas under pressure, such as carbon dioxide, i then bubbled through the liquid by opening a valve 24 unti the desired pressure is reached. The system is allowed t operate until a sufficient amount of gas is dissolved in th liquid. Pressure relief valve 25 is then quickly opened reducing the pressure in the vessel and allowing bubbles t form around the particles to lift the particles away from th surface of article 21. The liquid 27 may then be draine through valve 28, carrying away the particles which are no suspended in the liquid 27. If the article 21 needs to b dried, dry nitrogen, air or some other gas can be admitte into the vessel 22 by opening valve 29 until the water o cleaning fluid has evaporated. The vessel cover 30 can the be opened and the article 21 removed. In the apparatus shown in Figure 2, the part 31 to b cleaned is first placed in a vessel 32. The system is firs pressurized by opening valve 33 until the vessel 32 i completely filled with a gas, such as carbon dioxide, unti the desired pressure is reached. Next, deionized a filtered water or some other suitable cleaning fluid i sprayed into the vessel through the spray nozzle 34, whic may be accomplished by opening valve 35. By spraying t fluid into the vessel, numerous droplets 36 are formed. the droplets 36 fall through the gas, the gas is dissolve In this way the rate of dissolution of the gas into t liquid is increased. After enough liquid has been spray into the vessel 32 and the part 31 to be cleaned completely covered by the liquid, valve 37 is opene suddenly reducing the gas pressure in the vessel 32 a allowing bubbles to form around the particles. After t particles have been lifted away by the bubbles, the liquid drained by opening valve 38 and dry air or nitrogen introduced into the vessel 32 via valve 39 to dry the pa 31. In addition to the use of the invention for removi particles from surfaces, the invention can also be used remove particles suspended in a liquid. For particle remov from a liquid, the liquid will be placed in a vessel a subjected to high gas pressure. A valve will then be open and the gas pressure caused to drop quickly to some ambie condition. As the bubbles form in the liquid around t particles and rise to the surface, they will carry t particles with them to the surface where they can separated from the clean liquid remaining below. An apparatus for achieving this goal in a continuo process is shown in Figure 5. A liquid containing suspend particulate matter is represented by arrow 40. The liqu enters a vessel 41, along with a gas under pressure, the g being represented by arrow 42. As the mixture of liquid and gas 42 flows through the pressure vessel, the gas 42 dissolved in the liquid 40. The liquid 40 is then allowed expand through a restricting orifice 43. As the liquid flows through the restricting orifice 43, the pressu exerted between liquid 40 is suddenly reduced, causi bubbles 44 to form in the liquid 40. The bubbles 44 th rise to the upper portion 45 of the flowing liquid stream 4 the contaminant particles • being transported within t bubbles 44. The stream 46 can then be separated into upper stream 47 and a lower stream 48, the upper stream being removed by some conventional method and the relative clean liquid within lower stream 48 being discharg separately. The present invention is not restricted to the use water as the cleaning liquid or the use of carbon dioxide the gas. Other liquids, such as fluorocarbons, acid solvents, etc., can also be used. Gases such as nitroge oxygen, argon, helium and others would also be suitable a can be advantageous under some circumstances. In genera the gas used must have suitable solubility characteristics the liquid. Its physical and chemical properties must al be compatible with the liquid and the surface to be cleaned In particular, it may be desirable to use a sing substance such as a fluorocarbon of a suitable vap pressure/temperature relationship, in which case, t substance would first be pressurized to form a liquid in which the surface is placed. The pressure is then quick reduced. As the liquid vaporizes, bubbles form around t particles causing them to be lifted from the surface. some instances, the pressure can be raised sufficiently unt the critical point of the substance is exceeded, there forming a "super critical fluid". As the pressure reduced, the bubbles form as just described so as to lift t particles from the surface. An alternate method of cleaning particles from a surfa may be accomplished by utilizing the effect of a phase chan on the adhesion force between a particle and a surface. I particular, the process of particle removal from a surface b freezing and melting a thin layer of water on the surface ha been found to be, through laboratory experiment, quit effective. The specific mechanism involved is related to th expansion of water during the breathing process. As shown i Figure 9A, a particle 56 is adjacent to surface 57, th particle being immersed in a thin film of water 58. Curren adhesion theory predicts that a particle having a radius o 500 angstroms will be suspended from the surface 57 by distance of four angstroms. However, as shown in Figure 9B, as the water 58 freezes thereby becoming ice, the volume occupied by the wate expands, causing the particle 56 to move away from surfac 57, thereby greatly increasing the separation distanc between the particle 56 and the surface 57. In particular the distance increases from four angstroms to a distance o 49 angstroms, thereby greatly reducing the adhesion forc between the particle and the surface. The reduction an adhesion force allows the particle to be removed from th surface 57 with relative ease. A more general view of this process as applied t cleaning a surface is shown in Figure 8. In this case, th surface 57 is coated with a plurality of particles 56, whic are then coated with a layer of water 58. As the water 5 becomes ice, the particles 56 are entrapped within the ice If the surface 57 is then heated from below, the ice sheet 5 will slide away from the surface in the direction of arro 59, thereby carrying the entrapped particles with the ic sheet 58 and removing them from the surface 57. In some cases, the gas utilized may be placed under sufficiently high pressure so as to exceed the critica pressure of the gas or the liquid. Liquids and gases in suc a super critical state would be particularly suitable fo cleaning very small particles or particles that adhere ver strongly to surfaces. The specific conditions under whic such super critical fluids can be used will vary according t the liquid, gas and surface involved. An apparatus embodying this alternate method of cleanin is depicted in Figure 7. In this embodiment, the wafers 4 are supported on wafer carrier 50, the wafer carrier 50 bein housed within a suitable chamber 51. The first step in th cleaning process involves spraying water 52 into chamber 5 via nozzle 53. The wafers 49 may be submerged in the water 52, bu preferably, rather than submerging the wafers 49 in the wate 52, the water 52 is applied only to the extent necessary t coat the surface of the wafers, thereby forming a thin laye of liquid on the wafer surface. The surface of the wafer 4 is then cooled below the freezing point of water by injectin into the chamber a gas 54, such as cold air or nitrogen which is below the freezing temperature of water 52. Th circulation of gas 54 through the chamber 52 causes the laye of water 52 on the surface of wafers 49 to freeze. As the water 52 freezes, the volume occupied by th water increases, thereby pushing any particles which ma reside on the surface of wafer 49 away from the surface This lessens the adhesion force between the surface of wafe 49 and the undesired particle, thereby decreasing th resistance of the particle to removal from the surface. Once the freezing process is completed, the surface o the wafer 49 may be heated, causing the thin layer of ice t slide away from the surface, carrying the particles with it An alternate method of removing the ice would simply requir that warm water be sprayed on the wafer surface, and th particles would be flushed away with the melting ice. Fo example, as shown in Figure 7, the temperature of water 5 could be elevated, melting the ice and flushing away th particles. Finally, a gas 55, such as air or nitrogen, coul be introduced into the chamber to evaporate the water and dr the wafer surface. Experiments involving this cleanin method have shown a cleaning efficiency of 90%, that is removal of 90% of the undesired particles from the wafe surface. Many other methods may be used to accomplish th objectives of this novel cleaning method. For example, th wafer 49 could be heated by microwave energy, othe electromagnetic radiation, infrared heating, warm air, o other warm gases, or the heating step could be eliminate altogether. In the non-heating method, the freezing cycl could simply be repeated until the ice broke away from th surface of the wafer. Specifically, a thin layer of wate could be frozen on the surface as before, the surfac temperature could then be gradually reduced to a sufficientl low level until the ice became separated from the surface a a result of the difference in the coefficients of therma expansion of the ice and the substrate surface material. I this way, the entrapped particles are removed without havin to first melt the ice. The phase change cleaning method just describe involves, in the preferred embodiment, changing the wate (liquid phase) to ice (solid phase) and then back to wate (liquid phase). In some applications, other substances ca also be used. Examples of alternate substances includ methanol, ethanol and various alcohols, organic chemica compounds such as fluorocarbons and hydrocarbons, and an other substance which can be frozen and melted in a manne similar to water. Also, some agitation or spinning of th wafers might facilitate the cleaning method. Various other apparatus may be useful in carrying ou the method described herein. For example, Figure 10 shows schematic diagram of a system in which a single silicon wafe 60 is placed in a chamber 61. A source of water 62 supplie a spray 63 via nozzle 64. Cold air, nitrogen or some othe gas 65 is introduced into the chamber 61 until the water o the wafer surface freezes. Warm water is then sprayed ont the surface causing the ice to melt. The water is the drained from the chamber 61 and dry air nitrogen or som other suitable gas 66 is then introduced into the chamber t evaporate the water and dry the surface. Cooling of the ga used to freeze the water on the surface can be done b mechanical refrigeration, or by passing gaseous nitroge through a chamber containing liquid nitrogen until th temperature is reduced sufficiently to cause the freezing o water. An alternate embodiment for carrying out the sam process is shown in Figure 11. In this method, the wafer 6 is placed on a spindle 68 and rotated (as shown by arrow 69 while water 70 is sprayed onto the wafer 67. This cause only a thin layer of water to form on the surface of wafe 67. This water layer is then frozen, melted and dried a described before. Another embodiment of an apparatus utilizing the metho described herein is depicted in Figure 12. In thi apparatus, wafer cassettes 71 house individual wafers 72 The wafer cassette 71 resides within a cassette bin 73 whic in turn is housed within chamber 74. The cassette bin 73 i caused to rotate as shown by the direction of arrow 75 whil water 76 is sprayed onto the wafers 72. A plurality o nozzles 77 may be connected to any suitable liquid source 78 Freezing of the water may be accomplished by a suitable ga 79, and melting accomplished by injection of another suitabl gas 80 within chamber 74. The invention is not to be limited to the specifi construction or arrangement of parts shown, but the device and methods as described above may be widely modified withi the scope of the invention. The above described method is not limited to cleanin semi-conductor wafers alone. It can be used to clean man surfaces, including computer disk drive surfaces, plasti wafer carriers, precision mechanical, electrical and optica parts, all of which can be readily cleaned by the method described. In applying the water to the surface according to th method disclosed, the water must actually wet the surface t be cleaned. If wetting is incomplete, air bubbles could b entrapped between the liquid and the surface, thereb resulting in incomplete cleaning. However, this can b easily remedied by adding a small amount of a surface activ agent such as detergent to improve the wettability of th surface. Other chemicals, such as an acid, can also be adde to both improve the wettability of the surface and to remov other surface contaminants while undergoing particle remova by the process described.

Claims: WE CLAIM : 1. A method for cleaning a surface of an articl comprising: (a) placing the article within a pressure vesse the pressure vessel having a pressure relief valve; (b) introducing a cleaning fluid within t pressure valve, such that the cleaning fluid submerges t surface of the article; (c) introducing a gas into the cleaning fluid, t gas tending to pressurize the pressure vessel to a fir pressure; (d) activating the pressure relief valve such th a second pressure is established within the pressure vesse the second pressure having a lower value than the fir pressure, the activation of the pressure relief valve causi a substantially instantaneous decline from the first pressu to the second pressure within the pressure vessel such th bubbles are spontaneously formed around contaminants on t surface, the bubbles tending to remove the contaminants fr the surface, the contaminants thereby becoming suspended the cleaning fluid; and (e) draining the cleaning fluid from the pressu vessel, thereby removing the suspended contaminants from t pressure vessel and leaving a relatively clean surface withi the pressure vessel. 2. The method of claim 1, wherein the gas is carb dioxide. 3. The method of claim 1, wherein the cleaning flui is deionized and filtered water. 4. A method for cleaning a liquid containing suspende particulate matter, comprising the steps of: (a) introducing the liquid into a pressure vessel the pressure vessel having an exit orifice; (b) introducing a gas into the pressure vessel thereby establishing a first pressure within the pressur vessel; (c) causing the liquid and the gas to exit th pressure vessel and pass through a restricting orifice, th restricting orifice having an inlet side and an outlet side the passage of the gas and the liquid through the restrictin orifice causing a pressure decrease such that a secon pressure value exists at the outlet side of the restrictin orifice, the second pressure value being less than the firs pressure value, the decrease in pressure values causing spontaneous formation of bubbles within the liquid at th outlet side of the restricting orifice, the bubbles tendin to form around the suspended particulate matter within th liquid, the bubbles tending to ascend within the liquid; (d) causing the liquid to pass into a collectio vessel, the collection vessel being divided into an uppe region and a lower region; (e) collecting the liquid within the upper regio of the collection vessel, thereby removing the bubble containing suspended particulate matter from the collectio vessel; and (f) draining the liquid from the lower region o the collection vessel, thereby removing a relatively clea liquid from the collection vessel. 5. The method of claim 4, wherein the gas is carbo dioxide. 6. A method for cleaning a surface of an article comprising the steps of: (a) placing the article within a chamber, suc that the article is supported within the chamber; (b) introducing a cleaning fluid in a liquid stat within the chamber, such that the cleaning fluid coats t surface of the article to be cleaned, thereby forming a fi on the surface to be cleaned; (c) causing the fluid to freeze on the surface the article, the freezing action lessening the adhesion for between the surface of the article and undesired particula matter on the surface of the article; and (d) heating the surface of the article such th the frozen cleaning fluid is removed from the surface of t article, the particulate matter thereby being removed fr the surface of the article through the medium of the cleani fluid. 7. A method for cleaning a surface of an articl comprising: (a) placing the article within a chamber, su that the article is supported within the chamber; (b) introducing a cleaning fluid in a liquid sta within the chamber, such that the cleaning fluid coats t surface of the article to be cleaned, thereby forming a fi on the surface to be cleaned; (c) introducing a gas into the chamber, the g having a temperature below the freezing point of the cleani point, thereby causing the fluid to freeze on the surface the article, the freezing action lessening the adhesion for between the surface of the article and undesired particula matter on the surface of the article; and (d) heating the surface of the article such th the frozen cleaning fluid is removed from the surface of t article, the particulate matter thereby being removed fro t surface of the article through the medium of the cleani fluid.

Inventors: AHN KANG-HO, LIU BENJAMIN Y H, AHN, KANG-HO, LIU, BENJAMIN, Y., H.
Applicants: UNIV MINNESOTA, REGENTS OF THE UNIVERSITY OF MINNESOTA
Application year: 1988
Main classification: B08B3
IPC codes: B08B3, B08B7, C02F1, H01L21