The present invention generally relates to nano-photolithography systems, and more particularly relates to superlens devices for nano-photolithography systems, method for fabrication of such superlens devices, and nano-photolithography system using such superlens devices.
Conventional projection photolithography systems, which are equipped with such conventional lenses, have been widely used in laboratories and in the semiconductor industry. The image resolution obtained by a conventional optical lens, however, is fundamentally limited by diffraction to approximately half of the wavelength of the light used, this limitation known as Abbe's Limit. Also, even though the resolution of a photomask could be very high, such projection photolithography setups unfortunately still suffer from this light diffraction limit when attempting to meet small size requirements.
With the advance of nanotechnology and increasing demand from various real nanotechnology applications, low-cost and high-throughput, as well as ultrahigh resolution nanofabrication techniques have become highly desirable. Currently, there are a few nanolithography techniques which have been well developed or commercially available. For example, electron beam lithography (EBL), focused ion beam (FIB) milling, x-ray lithography and dip pen lithography (DPN) are currently able to produce high-resolution nanoscale patterns. However, these techniques and the tools necessary to implement them are costly and their throughputs are very low in terms of large-scale patterning.
Nanosphere lithography (NSL) offers a low-cost method of nano-patterning and fabrication of nanostructures for the semiconductor industry and for biological and chemical analysis. NSL techniques create nanostructure arrays utilizing planar ordered nanosphere arrays as a mask. Dielectric nanospheres employed in NSL exhibit interesting optical properties, which makes NSL frequently used method for plasmonic studies. However, the shapes of NSL patterns are restricted due to nanosphere arrays being directly formed on substrate surface. Further, NSL is not applicable to many substrate materials because of the different surface properties of substrate materials. Agglomerations of nanoparticles after metal deposition are frequently a result of dislocation of nanospheres during formation of the nanosphere monolayer, thereby hindering successful lift-off of the nanosphere monolayer. These limitations make NSL only feasible for limited, specified applications.
Nanoimprinting lithography (NIL) is also a promising, effective technique for large-scale surface patterning in nanoscale. NIL offers a lower cost and higher throughput in comparison with the aforementioned nanolithography techniques. In addition, it also exhibits high resolution patterning and great flexibility in accommodating a large variety of polymer materials. These advantages make NIL tend to be an effective supplementary tool for nanofabrication of semiconductors, MEMS/NEMS devices, chemical and biological templates. Compared to commonly used projection photolithography systems in semiconductor industry, the throughput of step nanoimprinting for large area patterning is still not as high as photolithography. Some other issues related to NIL such as resist and template properties, relative complex process, accuracy and defect control also still need further investigation.
Thus, what is needed is a scalable, easily integratable nanopatterning solution for two-dimensional and three-dimensional subwavelength nanopatterning that can provide high throughput at a low cost. Furthermore, other desirable features and characteristics will become apparent from the subsequent detailed description and the appended claims, taken in conjunction with the accompanying drawings and this background of the disclosure.
According to the Detailed Description, a nano-photolithographic superlens device is provided. The nano-photolithographic superlens device includes a light permissive mask layer, a nanopatterned layer of opaque features formed on the mask layer, an intermediate layer formed on the nanopatterned layer and the mask layer, and a superlens layer formed on the intermediate layer. The intermediate layer has a predetermined thickness and is index matched to the superlens layer.
In accordance with another aspect, a method for fabrication of a nano-photolithographic superlens device is provided. The method includes the steps of providing a light permissive mask layer and forming a nanopatterned layer of opaque features on the mask layer. The method further includes the steps of forming an intermediate layer on the nanopatterned layer and the mask layer and forming a superlens layer on the intermediate layer, wherein roughness of the intermediate layer is controlled during its formation in order to provide a smooth superlens layer.
And in accordance with a further aspect, a system for nano-photolithography is provided. The system for nano-photolithography includes a light source having a predetermined light wavelength, a device to be patterned, and a photoresist layer of photoresponsive material formed on the device. The photoresponsive material is photresponsive to the predetermined light wavelength. The system further includes a superlens device in contact with the photoresist layer and including a superlens layer, a light permissive mask layer, and an intermediate layer. The superlens layer is in contact with the photoresist layer. The light source is located to radiate light at the predetermined light wavelength on the light permissive layer, the light permissive mask layer being transparent to the predetermined light wavelength. The light permissive layer also has a layer of nanopatterned opaque features formed thereon. And the intermediate layer is located between the superlens layer and the light permissive mask layer to separate them by a predetermined distance.
The accompanying figures, where like reference numerals refer to identical or functionally similar elements throughout the separate views and which together with the detailed description below are incorporated in and form part of the specification, serve to illustrate various embodiments and to explain various principles and advantages disclosed herein.
And
Skilled artisans will appreciate that elements in the figures are illustrated for simplicity and clarity and have not necessarily been depicted to scale. For example, the dimensions of some of the elements in the figures illustrating the superlens device may be exaggerated in one dimension relative to another dimension to help to improve understanding of the present and alternate embodiments. In addition the planar and perspective views of
The following detailed description is directed to various embodiments of the invention. Although one or more of these embodiments may be preferred, the embodiments disclosed should not be interpreted, or otherwise used, as limiting the scope of the disclosure, including the claims. Furthermore, there is no intention to be bound by any theory presented in the preceding background or the following detailed description. It is the intent of this disclosure to present a nano-photolithographic technology using contact optical lithography and taking advantage of the superlens effect to achieve both two-dimensional and three-dimensional nanopatterning with super-resolution and good fidelity.
Projection optical lithography has become the main lithography technology employed for high-volume semiconductor manufacturing. However, projection optical lithography is a far-field optical imaging process which has a fundamental resolution limit of λ/2, where λ is the wavelength of the light projected. Contact optical lithography is an alternative lithographic technology and by its nature is a near-field optical imaging process. By bringing the mask into contact with the photoresist layer, there is effectively no space for light waves to travel between the mask opening and the photoresist layer, except within the photoresist layer. Therefore, light waves no longer propagate as sinusoidal waves but as evanescent waves. So, such contact optical lithography can also be termed evanescent near-field optical lithography.
Thus, the sinusoidal propagating waves of scattering light from an object carry large feature information while the evanescent waves carry fine feature (subwavelength) information. The evanescent waves decay exponentially when traveling in any positive refractive index medium, which is accountable for the diffraction-limited images obtained by conventional optical lenses. A superlens is superior to conventional lenses and is able to enhance evanescent waves passing through its negative-refractive-index material, thereby creating a perfect image in either near-field or far-field by recovering a combination of evanescent and propagating waves in an image plane.
Referring to
Light 135 of a predetermined wavelength, such as ultraviolet (UV) light, is radiated from a light source (not shown) onto the superlens device 105, passing through the light permissive mask layer 110, the nanopatterned layer 115 and the intermediate layer 120 to strike the superlens layer 130. The superlens layer 130 is formed of a material having a negative refractive index (and consequently a negative permittivity) such as silver, gold or palladium and when the radiated light 135 strikes the superlens layer 130, evanescent waves are scattered and a combination of evanescent and propagating waves from the light 135 are recovered in an image plane at a substrate 140 having a patterned photoresist layer 145 formed thereon.
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In accordance with the present embodiment, the subwavelength patterning is improved and optimized by permittivity index matching between the intermediate layer 120, the superlens layer 130 and the photoresist 145. Index matching refers to the intermediate layer 120 having a permittivity substantially equal to the absolute value of the permittivity of the superlens layer 130 and the photoresist 145 at the predetermined light wavelength of the light 135 from the light source. The index matching of the permittivity of the intermediate layer 120, the superlens layer 130 and the photoresist 145 at the wavelength of the light 135 eliminates the waveguide effect well-known to those skilled in the art and the negative permittivity (and, hence, the negative refractive index) enhances evanescent waves passing therethrough, thereby creating a perfect image in either near-field or far-field by recovering a combination of evanescent and propagating waves in an image plane of the photoresist 145. Without index matching of these layers, the superlens effect would be greatly deteriorated and sub-diffraction-limit patterning would be highly difficult. Thus, it can be seen that the thin flat superlens device 105 in accordance with the present embodiment enhances evanescent wave scattering across it to achieve subwavelength patterning using common photolithography processes.
In addition to index matching, in accordance with various embodiments of the invention, the vacuum-assisted hard contact between the superlens device 105 and the photoresist layer 145 is improved by providing a smooth surface on the superlens layer 130. This improved smooth surface is maintained has a smoothness predetermined to be a root-mean-square (rms) surface roughness of less than three nanometers, which is facilitated by fabricating the intermediate layer to have an rms surface roughness of less than five nanometers.
The light permissive mask layer 110 is formed of a material transparent to the wavelength of the light 135 (e.g., UV light) such as quartz or soda lime. The opaque features 115 formed on the mask layer 110 are preferably formed of chrome (i.e., comprising chromium) and, in accordance with the present embodiment have the widths thereof and the distance between adjacent features predetermined in response to the wavelength of the light 135. Further, in accordance with the present embodiment, the intermediate layer 120 is formed of a polymer material, a dielectric material, a composite material or an organic material and preferably has a thickness between 0.1 nanometers and 100 nanometers. Additionally, the superlens layer 130 preferably has a thickness between 1 nanometer and 100 nanometers.
In accordance with another aspect of the present embodiment, three-dimensional nano-photolithography is made possible by adjusting parameters of the patterned opaque nanoscale features of the nanopatterned layer 115 formed on the mask layer 110. When all of the patterned opaque nanoscale features have consistent heights, two-dimensional nano-photolithography is performed. By varying heights for each of the opaque features, three-dimensional nano-photolithography is achievable.
Referring to
After the mask fabrication step 200, a planarizing step 205 is performed to planarize the nanopatterned layer 115. Referring to
Referring next to
Also, as mentioned above in regards to the planarizing step 205, the material of the superlens layer 130 and the material of the intermediate layer 120 are index matched by selecting the intermediate layer 120 material to have a permittivity substantially equal to the absolute value of the permittivity of the superlens layer 130 material at the wavelength of the light 135 (
In accordance with the present embodiment, three-dimensional nano-photolithography can be enabled by altering the mask fabrication step 200. If heights of the patterned opaque nanoscale features of the nanopatterned layer 115 are formed to have consistent heights, two-dimensional nano-photolithography will be performed when using the superlens device 105 in accordance with the present embodiment. On the other hand, three-dimensional nano-photolithography will be performed when using the superlens device 105 in accordance with the present embodiment if heights for each of the patterned opaque nanoscale features of the nanopatterned layer 115 are varied during formation. One method for varying the heights for each of the opaque features of the nanopatterned layer 115 during formation in accordance with the present embodiment is varying loading (such as power loading for ion milling) across the nanopatterned layer 115 during etching to achieve different heights of the opaque features.
Referring to
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In regards to
Along the x-axis 322 of the graph 320, position is plotted while normalized pattern depth is plotted along the y-axis 324. Thus, the plotting of normalized depth profile vs. position for the photoresist pattern on trace 326 and for the object features 305 on trace 328 show that nano-photolithography in accordance with the present embodiment using the superlens device 105 advantageously achieves an unprecedented sub-diffraction-limited pattern. Furthermore, the full width at half maximum (FWHM) 330 of the cross-section curve, which corresponds to the resolution of superlens device 102, has been measured at about 75 nanometers. Thus it can be seen that the superlens device 105 in accordance with the present embodiment is able to transfer 45 nanometer wide gratings of 60-nanometer half-pitch.
Referring next to
Thus, operation in accordance with the present embodiment achieves object-to-pattern resolution and fidelity much greater than prior art nano-patterning solutions. In addition, the overall design and fabrication process are completely compatible with existing semiconductor processes, making this a highly scalable, easily integratable nano-photolithographic solution. Further, the superlens device provides a robust solution for large scale fabrication (up to 12-inch wafer) of two-dimensional and three-dimensional nanostructures, which makes it extremely attractive and promising in nano-patterning applications for its low cost, high throughput and super resolution.
Index-matching between the spacer (intermediate layer 120), the superlens layer 130 and the photoresist 145 at the wavelength of the light 135 provides beneficial nano-photolithography in accordance with the present embodiment. The surface smoothness of the intermediate layer 120 and the superlens layer 130 further facilitate the subwavelength patterning in accordance with the present embodiment. The superlens device 105 design and the fabrication process in accordance with the present embodiment are simple and can be immediately integrated with existing projection photolithography systems for fabrication of two-dimensional and three-dimensional nanoscale patternings.
Accordingly, a superlens device 105 which is able to achieve super-resolution, two-dimensional and three-dimensional sub-diffraction-limit patterning by normal photolithography system, has been presented. Utilizing negative-refractive-index superlens layer 130 deposited on a smooth index-matching intermediate layer 120 to form the flat optical superlens device 105, the evanescent waves carrying the fine feature information of light scattered from opaque feature objects 115 will be enhanced to create super resolution sub-diffraction-limited patterns in the near field. The method can be extended to any existing photolithography equipment and presents a high throughput, low cost, competitive technology for nano-patterning. While several exemplary embodiments have been presented in the foregoing detailed description, it should be appreciated that a vast number of variations exist, including variations as to the materials and shapes used to form the various layers and structures 110, 115, 120, 130, 145.
It should further be appreciated that the exemplary embodiments are only examples, and are not intended to limit the scope, applicability, dimensions, or configuration of the invention in any way. Rather, the foregoing detailed description will provide those skilled in the art with a convenient road map for implementing an exemplary embodiment of the invention, it being understood that various changes may be made in the function and arrangement of elements and method of fabrication described in an exemplary embodiment without departing from the scope of the invention as set forth in the appended claims.
The present application claims priority to U.S. Patent Application No. 61/524,347, filed 17 Aug. 2011 which is incorporated by reference herein in its entirety.
Number | Date | Country | |
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61524347 | Aug 2011 | US |