1. Field of the Invention
The invention relates to methods and apparatus for processing wafer-shaped articles, and more particularly to methods and apparatus for megasonic cleaning of wafer-shaped articles.
2. Description of Related Art
Removal of particulate contaminants from a semiconductor substrate can be accomplished by ultrasonic cleaning. When the frequency of ultrasound is close to or above 1,000 kHz (1 MHz) it is often referred to as “megasonic”, and the term ultrasonic as used herein encompasses megasonic.
Commonly-owned application U.S. 2012/0073596 (corresponding to WO 2012/038933) describes improved techniques for ultrasonic cleaning of substrates, in which a bubble generator creates bubbles in a treatment fluid by a controlled decrease in pressure. This allows ultrasonic energy to be applied to the fluid at energy levels lower than those required to induce cavitation in the fluid.
However, there remains a need to improve megasonic cleaning techniques so as to more reliably remove nanoparticulate contamination without damaging the workpiece being processed, and without generating unacceptable cleaning patterns such as result from a non-uniform removal of contaminants. Shorter process times are also desired, as well as techniques that permit extending the process window and reducing the amount of control loops.
It is accordingly an object of the present invention to produce a method and apparatus for treating articles that overcomes, at least in part, the disadvantages of the conventional art.
In one aspect, the present invention relates to an apparatus for processing wafer-shaped articles, comprising a chuck having a chuck body that is driven in rotation about an axis, and holding elements projecting from the chuck body and configured to position a lower surface of a wafer-shaped article a predetermined distance from the chuck body. The lower surface is preferably the device side of a semiconductor wafer. An acoustic resonator assembly is non-rotatably mounted on the chuck adjacent the chuck body such the acoustic resonator assembly is positioned between the chuck body and a wafer-shaped article when a wafer-shaped article is positioned by the holding elements at the predetermined distance from the chuck body.
In preferred embodiments of the apparatus according to the present invention, the chuck body is mounted for rotation about a stationary central shaft, and the acoustic resonator assembly is mounted in a cantilevered manner with a proximal end fastened to the central shaft and a distal end positioned above a peripheral region of the chuck body.
In preferred embodiments of the apparatus according to the present invention, the acoustic resonator assembly comprises a source of ultrasonic energy positioned so as to vibrate a fluid medium adjacent the article.
In preferred embodiments of the apparatus according to the present invention, a bubble generator is configured to produce a treatment fluid comprising a dispersion of gas bubbles having diameters ranging from 0.4 μm to 12 μm in a treatment liquid, the bubble generator being positioned adjacent the source of ultrasonic energy.
In preferred embodiments of the apparatus according to the present invention, the bubble generator is integrated into the acoustic resonator assembly.
In preferred embodiments of the apparatus according to the present invention, the holding elements are positioned and configured to hold a semiconductor wafer having a diameter of 300 or 450 mm.
In preferred embodiments of the apparatus according to the present invention, the source of ultrasonic energy is configured to generate an acoustic interference pattern in a treatment fluid comprising regions of pressure amplitude minima and maxima at an interface of the treatment fluid and a wafer-shaped article.
In preferred embodiments of the apparatus according to the present invention, the acoustic resonator assembly comprises a housing having an inlet opening for receiving a treatment fluid, a plurality of injection orifices or an injection slit provided in the housing, and a resonator positioned so as to generate an acoustic interference pattern adjacent the predetermined position.
In preferred embodiments of the apparatus according to the present invention, the acoustic resonator assembly is spaced from the predetermined position by 0.1 mm to about 10 mm.
In preferred embodiments of the apparatus according to the present invention, the acoustic resonator assembly comprises inlets communicating with supplies of at least three different treatment fluids.
In preferred embodiments of the apparatus according to the present invention, a second bubble generator is positioned so as to be spaced by 0.1 mm to about 10 mm from an upper surface of a wafer-shaped article positioned on the holding elements.
In preferred embodiments of the apparatus according to the present invention, the second bubble generator and a second source of ultrasonic energy are integrated in a second acoustic resonator assembly.
In another aspect, the present invention relates to a method for treating wafer-shaped articles, comprising positioning a wafer-shaped article on holding elements projecting from a chuck body of a chuck, rotating the chuck body and the wafer-shaped article about an axis of rotation and contacting a surface of the wafer-shaped article facing the chuck body with an ultrasonically energized treatment fluid comprising a dispersion of gas bubbles in a liquid. An acoustic resonator assembly is non-rotatably mounted on the chuck adjacent the chuck body such the acoustic resonator assembly is positioned between the chuck body and the wafer-shaped article.
In preferred embodiments of the method according to the present invention, the surface of the wafer-shaped article facing the chuck body is contacted with another treatment gas or liquid dispensed from the acoustic resonator assembly before or after the contacting step.
In preferred embodiments of the apparatus according to the present invention, a surface of the wafer-shaped article facing away from the chuck body is contacted with an ultrasonically energized treatment fluid comprising a dispersion of gas bubbles in a liquid.
The invention will be more fully understood from the following detailed description of various preferred embodiments thereof, which are given by way of non-limiting example, and taken with reference to the accompanying drawings, in which:
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Although not shown in the figures, the spin chuck may be surrounded by a process chamber, which may be a multi-level process chamber as described in commonly-owned U.S. Pat. No. 7,837,803 (corresponding to WO 2004/084278). The spin chuck can be positioned at the selected level by moving the chuck axially relative to the stationary surrounding chamber, or by moving the surrounding chamber axially relative to the axially-stationary chuck, as described in connection with
A wafer W is held with its lower surface a predetermined distance from the chuck body 10, by a series of gripping pins 12 that project upwardly from the chuck body 10. Gripping pins 12 are driven in concert by a ring gear 16, from an open position in which the upper eccentric gripping portions of pins 12 are positioned radially outwardly of the wafer edge, to a closed position in which the eccentric gripping portions engage the wafer edge. A given chuck will typically be designed to accommodate wafers of a specified standard diameter, and it is preferred that the present chuck be configured to hold a semiconductor wafer whose diameter is 300 mm or 450 mm, or whose diameter varies from those values within the tolerances specified in the applicable standard.
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The structured solid element could be made out of aluminum, sapphire, silicon or quartz, or any other suitable material. The grooves 22 may be exposed, or may be covered by a plastic or polymer coating. The thickness of this coating is preferably between 1 μm and 100 μm.
The resulting acoustic interference pattern forms alternating regions of pressure amplitude maxima and minima within the liquid and at the solid-liquid interface at the wafer W. If bubbles are injected in the developed acoustic field, they will be sorted, depending on their size, towards the pressure amplitude maxima and minima. In a relatively weak acoustic field, a bubble driven below resonance (which means that the driving frequency of the imposed ultrasound field is below the fundamental resonance frequency of the bubble (calculated by the Minnaert equation)) moves to the pressure amplitude maximum. The bubbles typically grow due to coalescence in the pressure maxima until they reach the critical size given by the Minnaert equation they will start moving towards a pressure amplitude minimum.
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Furthermore, it has been found that operating in an acoustic pressure range of from 10−3 bar to 103 bar allows to manage (in combination with the selected operational frequency) the bubble activity, which allows bubbles to create surface modes, surface instabilities, volumetric oscillations even leading to heavy collapsing bubbles, and therefore can create acoustic streaming, shear stress or enrich the liquid-solid interface with one or more gaseous components.
Besides the in situ heterogeneous nucleation of bubbles in the liquid, it is especially beneficial to inject bubbles directly in to the liquid, which allows to operate at acoustic pressure below the cavitation threshold (typically lower than 1 bar). Furthermore, bubble size distribution and content of the bubbles can be more easily tuned towards the targeted application.
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Although as noted above the openings 24 have a diameter from about 50 μm to about 500 μm, and preferably between 100 and 350 μm, the bubbles that come out of solution upon the treatment fluid passing through these openings are much smaller. In particular, the bubble size distribution in the treatment fluid is preferably such that 90% of the bubbles have a bubble diameter d wherein 0.8*ds≦d≦1.2*ds, where ds is a selected number in the range of about 0.5 μm to about 10 μm, and preferably less than about 5 μm.
Although the bubbles are created by the pressure drop as the treatment liquid passes through openings 24, rather than by nucleation induced by the megasonic radiation, the size to which the bubbles grow is nevertheless a function of the wavelength of the megasonic radiation emitted by the resonator. For example, when the resonator generates megasonic radiation of 1 MHz, this corresponds to a wavelength λ=1.48 mm, which in turn leads to ds=λ/500, and a bubble diameter of about 3 μm. The preferred ranges of bubble diameters for use in the present method and apparatus are 0.4-12 μm, preferably 1-8 μm, and more preferably 2-5 μm.
If the openings 24 were substantially smaller, for example on the order of the bubble diameter, then greater pressure would be required to force the treatment fluid through the openings 24. That higher pressure would cause the bubbles to come out of solution at a point more distant from the resonator, and would thereby inhibit the efficacy of the megasonic cleaning or render the bubbles ineffective altogether. The gap between the resonator and the wafer can be filled via supply connection 36. Connection 32 is preferably used for nitrogen gas supply.
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