This disclosure relates to light homogenizing elements for illumination systems. More particularly, this disclosure relates to light homogenizing elements that deliver a highly uniform distribution of light at an image plane of an illumination systems. Most particularly, this disclosure relates to light homogenizing elements that include a lens array with a plurality of lenslets in which an aperture of at least one lenslet is masked to correct for non-uniformities in the light field incident to the lens array.
Projection systems, and microlithography projection systems, in particular, require a uniform field of electro-magnetic energy to illuminate an object such as a mask or spatial light modulator. This energy is then transferred by an optical system to illuminate a wafer or create an image in some other location. If the field is not uniform the exposure of the image will not be uniform.
Many current microlithography illuminators use a low-pressure mercury arc lamp to generate 365 nm light. The large lamps and their associated utilities are expensive, inefficient, and can cause potential safety problems. Moving from a lamp source to a light emitting diode (LED) source makes improvements on all of these fronts. These LEDs can be placed in an array and homogenized to create a uniform field of light at the reticle plane. The LED dies are made in a semiconductor manufacturing process, which results in repeatable structures and patterns for making the die.
There are several possible methods of uniformizing the LEDs. The two most efficient methods are with a pair of lens arrays or a kaleidoscope, also known as a light tunnel or integrating bar. Each method has advantages and disadvantages. A disadvantage to a lens array solution is that odd order non-uniformities cannot be uniformized in a lens array solution. There are also manufacturing variations that can create subtle and slight variations in the uniformity that cannot be compensated for in traditional lens array or light tunnel illuminators. For example, variations in coatings on lens elements will change the transmission as a function of the field, and this has an impact on the final uniformity. Microlithography systems, in particular, have extremely tight tolerances on the uniformity of the light field so that microelectronic circuitry is printed consistently on the wafer.
If an array of LEDs is used as a source and all LEDs are oriented in the same clocking position, a tilt to the irradiance pattern will be presented to the illumination system. Since the tilt is an odd function, the lens array cannot correct the non-uniformity. It can be minimized by creating a lens array with smaller and more lens elements, but this approach can be very expensive and difficult to manufacture. If a more conventional source is used, there are still non-uniformities created by imperfections in the illumination system. One method that also has been used to correct non-uniformities is use of an optical apodizer. An optical apodizer is a window with a variable coating that is placed just before the uniform plane. The variable coating has a variable transmission function that reduces transmission in high energy areas to create a more uniform light field. These optical apodizers are difficult and expensive to make, and are usually used only to correct rotationally symmetric non-uniformities.
Therefore, there is a need for a low-cost method for fixing residual non-uniformities in light fields caused by light source anomalies or manufacturing variations in projection illumination systems.
Light homogenizing elements are described. The light homogenizing elements include lens arrays with corrective features designed to improve the uniformity of light fields produced by optical sources. The corrective features include masks placed at selected positions of selected lenslets in a lens array. The corrective features block or reduce the transmission of light through the lens array at the selected position to correct for spatial or angular non-uniformities in a light field produced by an optical source. The light field exiting the corrected lens array has greater uniformity than the light field entering the lens array. Preferred lens arrays include fly's eye arrays. Illumination systems that include a corrected lens array coupled to a light source produce highly uniform light fields. Applications include microlithography.
The present disclosure extends to:
The present disclosure extends to:
The present disclosure extends to:
Microlithography is a widely used process in the patterning of silicon wafers in the semiconductor industry. In microlithography, a pattern on a reticle is transferred to a photoresist on a wafer to define a pattern for a microelectronic circuit. The apparatus used to perform microlithography includes an illumination system and a projection system. The illumination system includes a light source and an optical system. The optical system produces a light field from the light source and directs it to the reticle. A surface of the reticle includes features that modify the light field (e.g. through diffraction) to produce a patterned light field. The patterned light field is directed to the projection system, which includes optical elements that direct the patterned light field to a photoresist. The pattern of the light field determines the areas of the photoresist that are exposed to the light field. Subsequent development of the photoresist creates a contrast between exposed and unexposed areas to define a pattern for a microelectronic circuit.
As features sizes for microelectronic circuits decrease, there is a need for greater precision in the microlithography process. Spatial and angular uniformity of the light field incident to the reticle surface is critical to achieving faithful transfer of the reticle pattern to the wafer. Variability in the output of the light source is a significant contributor to non-uniformities in the light field produced by the illumination system. Light sources used in illumination systems include lamps, light emitting diodes, and lasers. Variabilities in light sources include spatial and angular deviations in the light field. Spatial deviations correspond to non-uniformity in the intensity or power of the light field over the cross-section of the light field and angular deviations refer to non-uniformities in divergence of the light field over the cross-section of the light field. Manufacturing variability or imperfections in other optical elements present in the illumination system and alignment errors also contribute to non-uniformities in the light field. Non-uniformities in the light field are replicated at the reticle and ultimately transferred to the photoresist to create imperfections in the patterned microelectronic circuit formed on the wafer.
One strategy for improving the uniformity of the light field of an illumination system is to incorporate a light homogenizing element in the optical system. The light homogenizing element is operatively coupled to the light source of the illumination system. Light produced by the light source is directed to the light homogenizing element. Light enters the light homogenizing element at one or more apertures, passes through the light homogenizing element, and exits the light homogenizing element. Light homogenizing elements are optical elements that suppress variability in a light field by mixing light rays that deviate in space or angle to provide a homogenized light field with averaged spatial and angular characteristics having greater uniformity. Common light homogenizing elements include integrator rods and lens arrays. Illumination systems with light homogenizing elements provide light fields with greater uniformity. There remains, however, a need for further improvements in the uniformity of light fields produced by illumination systems. As used herein, “uniformity” of a light field refers to uniformity in irradiance at an imaging field plane, where irradiance is defined as power per unit area and is typically expressed in units of mW/cm2.
The present disclosure is directed to lens arrays with improved performance. A lens array is an optical element that consists of a two-dimensional array of lenses. The individual lenses of a lens array are referred to herein as lenslets. The surfaces through which light enters and exits a lenslet are referred to herein as apertures. The lenslets are integrated to form a monolithic lens array. A monolithic lens array can be formed from a single substrate (e.g. piece of glass) through selective removal of material to form the individual lenslets in an intended pattern or configuration. Alternatively, the individual lenslets can be formed separately and combined (e.g. fused) into a monolithic assembly. Embodiments of lens arrays include fly's eye arrays. Lens arrays are designed to transmit a single wavelength, multiple wavelength, or over a continuous range of wavelengths. The wavelength(s) transmitted by a lens array are referred to herein as the operating wavelength(s) of the lens array. Representative operating wavelengths include infrared (750 nm-2000 nm), visible (400 nm-750 nm), and ultraviolet wavelengths (100 nm-400 nm). Lens arrays are constructed of materials suitable for transmitting operating wavelength(s) needed for a particular application. Representative materials for lens arrays include glass, silica glass, doped silica glass, and fluoride crystals. Fluoride crystals include CaF2 and MgF2.
In various aspects, the cross-section of lenslets is square, rectangular, circular, elliptical, oval, round, or polygonal (e.g. hexagonal). The shape of the lenslet determines the shape of the light field and is selected according to the intended application of an illumination system. The lenslet apertures have surfaces that are powered or plano. Powered apertures have surfaces that are concave, convex, spherical, aspherical, or anamorphic. Opposing apertures of a lenslet are the same or different in shape or power. In various aspects, opposing apertures of a lenslet are both plano, both powered, or a combination of powered and plano. In one embodiment, the lens array is a fly's eye array.
In one embodiment, the illumination system includes two or more lens arrays.
In one embodiment, lens array 230 is conjugate to homogenization plane 280 and lens array 240 is conjugate to the pupil of the illumination system. In a preferred embodiment, lens arrays 230 and 240 are equivalent. The light source 210 is imaged by condenser lens 220 and lens array 230 so that the aperture of each lenslet in lens array 240 is filled by an image of light source 210. The aperture of each lenslet of lens array 230 is magnified and imaged to homogenization plane 280. The irradiance at homogenization plane 280 is the summation of the energy from all lenslets of lens array 230. Since the images of the lenslets are superimposed, a highly uniform distribution of irradiance is created.
The distribution of irradiance at homogenization plane 280 has an average irradiance, a maximum irradiance and a minimum irradiance. Uniformity of the distribution of irradiance is assessed as a difference between the maximum irradiance and the minimum irradiance. The difference between the maximum irradiance and the minimum irradiance is less than 20% of the average irradiance, or less than 10% of the average irradiance, or less than 5% of the average irradiance, or less than 1% of the average irradiance.
In the example depicted in
Although improved light field uniformity results from inclusion of one or more lenses in the optical path of an illumination system, further improvements are needed. As noted above, manufacturing variability and imperfections in optical components (e.g. condenser lens 220 and combiner lens 250) introduce localized non-uniformities that are difficult to correct. Further complications arise from variabilities in the light source. In the limit of a light source that is uniform both spatially and angularly, no correction of non-uniformities in the light field is required. Actual light sources, however, are not uniform in space and angle. Lamps have filaments that extend over distances of millimeters or centimeters and variability in the composition, durability, or power distribution over the length leads to variabilities in the light field produced. LEDs also have finite light-generating areas that are subject to variability. Similarly, laser light is not perfectly collimated and exhibits variability in divergence and uniformity (angular and spatial). Non-uniformities in the light field produced by an optical source become more pronounced when multiple light devices are combined and integrated. To achieve higher irradiance, for example, it is common to bundle LEDs to form an LED array and to use the LED array as a light source in an optical system. Manufacturing variability in the production of LEDs leads to differences in the characteristics of the individual LEDs in an array. There may also be systematic non-uniformities in the irradiance distribution of the LED dies. Variability in operating conditions (e.g. fluctuations in the delivery of power or irregularities in supporting electronic components) also lead to differences in the characteristics of the individual LEDs in an array. The light field produced by an LED array exhibits non-uniformities due to differences in light fields generated by the individual LEDs in an array, or similar non-uniformities in each LED, and these non-uniformities are a function of position in the LED array. Such non-uniformities are difficult to correct and are specific to a particular LED array. If, for example, an LED array reaches its operating lifetime and needs to be replaced, the replacement LED array will likely produce a light field with non-uniformities that differ in degree, type, and spatial position than the non-uniformities in the light field produced by the original LED array. Such variations require significant and expensive adjustments in downstream optical elements to effect corrections.
The present disclosure provides lens arrays with corrective features designed to further improve the uniformity of light fields in optical systems. The corrective features are selectively placed at localized positions within a lens array to compensate for localized non-uniformities in light field. The corrective features are preferably features placed on or near the surface of an aperture of one or more lenslets of a lens array, where the surface features reduce transmission through the lenslet. In one embodiment, the corrective features are in direct contact with the surface of the aperture. In a preferred embodiment, the corrective features are spaced apart from the surface of the aperture and positioned in close proximity to the surface of the aperture. In this embodiment, a gap is present between the corrective feature and the surface of the aperture, but the corrective feature is positioned sufficiently close to the surface of the aperture to reduce transmittance through the lenslet. Mechanical mounts are used to position corrective features in close proximity to the surface of an aperture. In one embodiment, the corrected portion of an aperture or a surface is a shadow of a corrective feature positioned in close proximity to the aperture or surface.
A lenslet with a corrective feature is referred to herein as a corrected lenslet, the portion of a lenslet or lens array covered by the corrective feature is referred to herein as the corrected portion of the lenslet or lens array, and a lens array with at least one corrected lenslet is referred to herein as a corrected lens array. An aperture or surface having a corrective feature is referred to herein as a corrected aperture or corrected surface, respectively. When the corrective feature is a mask, the terms masked lenslet, masked lens assembly, and masked portions are also used herein. A lenslet lacking a corrective feature is referred to herein as an uncorrected lenslet. Portions of a lenslet or lens array lacking a corrective feature are referred to herein as uncorrected portions. An aperture or surface lacking a corrective feature is referred to herein as a corrected aperture or corrected surface, respectively. The lens array includes one or a plurality of corrected lenslets. The lens array optionally also includes one or a plurality of uncorrected lenslets.
The corrected portion is defined by the corrective feature. When the corrective feature is in direct contact with a lenslet, the corrected portion of the lenslet coincides with the corrective feature. When the corrective feature is spaced apart from the lenslet, the corrected portion of the lenslet comprises or coincides with a shadow of the corrective feature on the surface of an aperture of the lenslet.
In one embodiment, the corrective features are masks made from a material that is opaque or partially opaque to the wavelength(s) of light passing through the lens array. The opaque material absorbs and/or reflects the wavelength(s) of light passing through the lens array to reduce transmittance. Representative materials for masks include metals (e.g. aluminum or stainless steel) and transparent substrates coated with an interference coating designed to reduce transmittance to a controlled degree. As used herein, a transparent substrate is a substrate with at least 90%/mm transmittance at an operating wavelength. In one embodiment, the mask is perforated and includes a hole or pattern of holes to permit partial transmittance of the light field through the mask. The holes are arranged randomly or in a pattern in a surrounding material. The surrounding material is opaque or translucent. The holes are uniform in size or variable in size. In another embodiment, the mask is made from a material translucent to the operating wavelength of the lens array.
The thickness, configuration, and/or composition of the mask material is selected to block light passing through the corrected portion of the lens array (0% transmittance) or to reduce transmittance through the corrected portion relative to uncorrected portions to a controlled degree. Transmittance of the operating wavelength(s) through a corrected portion of a lens array is less than 50%, or less than 30%, or less than 10%, or less than 5%, or less than 1% of the transmittance of the operating wavelength(s) through uncorrected portions of the lens array. Transmittance of the operating wavelength(s) through uncorrected portion of the lens array is greater than 80%/mm, or greater than 90%/mm, or greater than 95%/mm, where mm refers to millimeter of distance in the direction of propagation of the operating wavelength(s) through the lens array. The location of the masks is selected to regulate transmittance through the lens array and to compensate for localized variations in intensity or irradiance across the light field. Spatial and angular non-uniformities are correctable with the present lens arrays.
The corrective features at least partially cover at least one aperture of at least one lenslet in a lens array. The corrective feature is placed at or near the aperture of a lenslet.
Although the lens arrays depicted in
By way of example and referring to
Lens array 240 is conjugate to the pupil of the illumination system 200. The pupil is the angular distribution of the energy as it focuses onto homogenization plane 280. In some applications, the centroid of the angular distribution is important. Modification of lens array 230 with a corrective feature can change the centroid of the angular distribution of the light field at homogenization plane 280. The variation of the centroid of the angular distribution accompanying a modification of lens array 230 with a corrective feature can be reduced by including a corrective feature complementary to corrective feature 430 with lens array 230. The complementary corrective feature is located at a position opposite to corrective feature 430 and acts to reduce irradiance from the opposite side of the light field entering lens array 400. Corrective feature 440 is complementary to corrective feature 430. The reduction of irradiance by corrective feature 440 counteracts the variation of angular centroid caused by corrective feature 430 to maintain a centroid position at homogenization plane 280 that closely approximates the centroid of the light field incident to lens array 400. The complementary corrective feature has the same or different shape or transmittance than the corrective feature. As defined herein, a complementary corrective feature is a feature that fully or partially compensates for variation in the centroid of the angular distribution of the light field resulting from a corrective feature. In one embodiment, the positions of the corrective feature and its complement are symmetric about the center of the pupil or symmetric about the center of lens array 240.
To further illustrate in reference to
Processes for adding corrective features to form corrected lenslets include designing a mask (perforated or unperforated) having a particular size, shape, and coating, and mechanically mounting the mask in close proximity to an aperture at a predetermined location of a lens array to enable correction of the light field passing through the aperture. This process can be repeated for each lenslet for which correction is desired. Interference films configured to reduce the transmittance of an operating wavelength can be formed on transparent substrates using materials and techniques known in the art (e.g. PVD, CVD).
To determine placement of corrective features, one can assemble the optical system, characterize the uniformity of the light field at a particular point along the optical pathway, determine the positions in the light field requiring correction, and correspondingly place corrective features at selected positions of the lens array to compensate for non-uniformities. In
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Those skilled in the art will appreciate that the methods and designs described above have additional applications and that the relevant applications are not limited to those specifically recited above. Also, the present invention may be embodied in other specific forms without departing from the essential characteristics as described herein. The embodiments described above are to be considered in all respects as illustrative only and not restrictive in any manner.
This application claims the benefit of priority to U.S. Provisional Application Ser. No. 62/690,398 filed on Jun. 27, 2018, the content of which is relied upon and incorporated herein by reference in its entirety.
Number | Date | Country | |
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62690398 | Jun 2018 | US |