The present disclosure relates generally to surface modification technology, and more particularly to a method and apparatus for producing a feature having a surface roughness in a substrate.
Plasmas can be generally described as ionized gases that are employed industrially for materials processing. For example, in the microelectronics industry, plasmas have been implemented in the transfer of fine patterns to a substrate surface for device fabrication by the combination of lithography followed by dry etching. Conventional lithography generally employs a resist mask formed through a series of processes, such as spin coating of a resist film, the soft and hard baking of the film, exposure of the film to photons, electrons, or ion beams, and finally the development of the film. The processes related to the resist mask and vacuum set-up may constitute a substantial portion of the device production cost. Moreover, the use of resist masks imposes limitations on the resulting etch profile, the etch selectivity, and the substrate geometry that may be employed for patterning.
A microplasma-based method and apparatus for producing a feature having a surface roughness in a substrate are described herein. Preferably, the feature has a roughness of about 10 nm or greater and a width of about 300 nm or less. A plurality of the features (e.g., an ordered array of such features) may be produced in the substrate, if desired. The substrate including the one or more features may be suited for use as a substrate in surface-enhanced Raman scattering (SERS) analysis of biochemical substances.
According to a first embodiment, the apparatus includes a conductive first electrode disposed in opposition to a conductive second electrode, where the first and second electrodes are spaced apart from each other by a distance adapted for generating a microplasma therebetween. The second electrode is a substrate, and the first electrode and the substrate are configured for relative motion in at least two opposing directions. A feature comprising a surface roughness of greater than about 10 nm is formed in the substrate when the microplasma is generated.
According to a second embodiment, the apparatus includes a conductive first electrode disposed in opposition to a conductive second electrode, where the first and second electrodes are spaced apart from each other by a distance adapted for generating a microplasma therebetween, and also a stage configured to provide relative motion of the first and second electrodes in at least two opposing directions. A feature comprising a surface roughness of greater than about 10 nm is formed in a substrate when the microplasma is generated. The relative motion of the first and second electrodes allows an array of the features to be formed.
According to a third embodiment, the apparatus includes a conductive hollow electrode including a cavity extending therethrough from a first opening to a second opening, and a conductive counter electrode disposed in opposition to the conductive hollow electrode, where the counter electrode is spaced apart from the second opening of the hollow electrode by a distance adapted for generating a microplasma therebetween. A feature having a surface roughness of greater than about 10 nm is formed in the counter electrode when the microplasma is generated.
According to a fourth embodiment, the apparatus includes: a conductive hollow electrode including a cavity extending therethrough from a first opening to a second opening; a conductive counter electrode disposed in opposition to the conductive hollow electrode, where the conductive counter electrode is spaced apart from the second opening of the hollow electrode by a distance adapted for generating a microplasma therebetween; and also a stage configured to provide relative motion of the hollow electrode and the counter electrode in a direction parallel to a surface of the counter electrode. A feature comprising a surface roughness of greater than about 10 nm is formed in the counter electrode when the microplasma is generated. The relative motion of the hollow electrode and the counter electrode allows a plurality of the features to be formed in the counter electrode.
According to a first embodiment, the method includes generating a microplasma between a conductive first electrode and a conductive second electrode, where the first and second electrodes are spaced apart a distance adapted for generating a microplasma therebetween and the second electrode is a substrate, and forming a feature in the substrate, the feature comprising a surface roughness of greater than about 10 nm and having a lateral dimension of about 300 microns or less.
According to a second embodiment, the method includes: generating a microplasma between a conductive first electrode and a conductive second electrode, where the first and second electrodes are spaced apart a distance adapted for generating a microplasma therebetween and the second electrode is a substrate; forming a feature in the substrate, where the feature has a surface roughness of greater than about 10 nm; inducing relative motion of the first and second electrodes in a direction parallel to a surface of the substrate so that the first and second electrodes take on a new relative position; generating a microplasma between the first and second electrodes at the new relative position; and forming a new feature in the substrate, where the new feature has a surface roughness of greater than about 10 nm. Preferably, moving to the new relative position and generating the microplasma between the hollow electrode and counter electrode are carried out multiple times to form an array of features in the substrate.
According to a third embodiment, the method includes: providing a conductive hollow electrode including a cavity extending therethrough from a first opening to a second opening; providing a conductive counter electrode in opposition to the conductive hollow electrode, where the counter electrode is spaced apart from the second opening of the hollow electrode by a distance adapted for generating a microplasma therebetween; generating a microplasma between the second opening of the hollow electrode and the counter electrode; and forming a feature in the counter electrode, where the feature has a surface roughness of greater than about 10 nm, thereby producing a substrate for surface-enhanced Raman scattering.
According to a fourth embodiment, the method includes: providing a conductive hollow electrode including a cavity extending therethrough from a first opening to a second opening; providing a conductive counter electrode in opposition to the conductive hollow electrode, where the counter electrode is spaced apart from the second opening of the hollow electrode by a distance adapted for generating a microplasma therebetween; generating a microplasma between the hollow electrode and the counter electrode at the first position; forming a feature in the counter electrode, the feature comprising a surface roughness of greater than about 10 nm; inducing relative motion of the hollow electrode and the counter electrode in a direction parallel to a surface of the counter electrode so that the hollow electrode and the counter electrode take on a new relative position; generating a microplasma between the hollow electrode and the counter electrode at the new relative position; and forming a new feature in the counter electrode, where the new feature has a surface roughness of greater than about 10 nm. Preferably, moving to the new relative position and generating the microplasma between the hollow electrode and counter electrode are carried out multiple times to form a plurality of features in the counter electrode, thereby producing a substrate for surface-enhanced Raman scattering.
A nonlithographic, direct patterning process based on a rastered, atmospheric pressure microplasma source is described herein for producing one or more features having a surface roughness in a substrate. The process is believed to be particularly suitable for the fabrication of low-cost, sensitive, highly reproducible, and stable substrates for surface-enhanced Raman scattering (SERS). Direct patterning using a microplasma may eliminate the need for resist masks, which are generally expensive to fabricate. Although conventional lithographic methods may be capable of producing smaller feature sizes than microplasmas, the inventors have recognized that the latter may be sufficient and advantageous for SERS-active substrate fabrication, where larger structures have been shown to exhibit significant enhancement factors.
According to a preferred embodiment, a metallic thin film (e.g., silver (Ag) supported on glass) is patterned using an argon (Ar) microplasma source coupled with a numerically controlled stage. Localized physical sputtering of the metallic film by the microplasma creates depressions or other localized features that may amplify the Raman scattering intensities from a test molecule (e.g., crystal violet (CV)) by a factor of 108-1010. Raman spectra of CV deposited in the features can be detected down to picomolar concentration levels on patterned Ag/glass substrates, indicating a significant enhancement over bare substrates.
A schematic of the setup used for nonlithographic pattern transfer is illustrated in
An inert gas such as argon or helium is flowed through the capillary tube 10 at a rate of between about 100-500 SCCM, where SCCM denotes cubic centimeters per minute at standard temperature and pressure (STP). One or more reactive gases may also be employed. In a typical experiment, a microplasma 20 is formed at ambient conditions with an argon gas flow rate of about 500 SCCM, which is set by a mass flow controller 25. Typically, a negatively biased DC power supply (e.g., Keithley, Inc. model 246) 30 operates the discharge with a current-limiting resistor in series with the microplasma 20. A voltage of 400 V and a current of 5 mA, for example, are suitable for generating the microplasma 20. The microplasma 20 extends from the capillary tube opening 10′ in a direction perpendicular to a grounded substrate 15, which may be, for example, a conductive silver-coated glass slide obtained from Kevley, Inc. The distance between the capillary tube 10 and the substrate 15 is typically about 6 mm or less, and may be about 2.5 mm or less. U.S. Pat. No. 6,700,329, which is hereby incorporated by reference in its entirety, discloses details related to such microplasma sources and their use in generating microdischarges.
The hollow cathode 10 and the substrate 15 are configured for relative motion in at least two opposing directions. The substrate 15 may be attached to a stage 35 controlled by a pair of numerically controlled stepper motors to provide motion in the x- and y-directions, as shown in
During microplasma generation, a feature (e.g., a depression having a particular depth) 40 is formed in the silver film through Ar ion and neutral collisions with the substrate surface that result in sputtering of the silver atoms. Generally, the feature 40 may be formed in a single location after about two to about eight minutes of sputtering. For example, the feature 40 may be formed after about four to about six minutes of sputtering. The depth of the feature (depression) 40 may be controlled by the duration of sputtering. The feature may extend partway or entirely through the metal film.
The feature may be a discrete or continuous structure, such as an indentation, hole, line or curve. Preferably, the feature is a localized feature having an average width of about 500 microns or less. For example, the average width of the feature may range from about 50 microns to about 500 microns. More preferably, the average width of the feature is about 300 microns or less. Even more preferably, the average width is about 200 microns or less, and may be about 100 microns or less. According to one embodiment, the average width is in the range of from about 100 microns to about 200 microns. In the case of an indentation or a hole, the width of the feature may correspond to a diameter. A continuous feature (e.g., a line or curve) may have a length that is considerably larger than its width. For example, lines or curves of millimeters or centimeters in length may be fabricated using the microplasma apparatus described herein. Such features are obtained by moving the substrate in the x and/or y direction while the plasma is being generated.
Surprisingly, the feature contains nanoscale bumps or irregularities and thus has a measurable surface roughness. The inventors believe the surface roughness may be advantageous for SERS analysis. Preferably, the surface roughness of the feature is greater than about 10 nm, on average. For example, the average surface roughness may be about 20 nm or greater, or about 50 nm or greater. The feature may also show surface roughness on the microscale (e.g., about 100 nm or greater). For the fabrication of SERS substrates, it may be advantageous for the surface roughness to be about 100 nm or less, on average. According to several embodiments, the average surface roughness of the feature may range from about 10 nm to about 300 nm, from about 30 nm to about 150 nm, or from about 50 nm to 100 nm. The inventors believe that the surface roughness may be created by the redeposition of sputtered material in the feature during microplasma generation.
More than one feature may be formed in the substrate. According to one embodiment, a plurality of the features may be formed. The features may be arranged in a regular array, as shown for example in
It is of interest to correlate the morphology (e.g., surface roughness) of silver films including the above-described features with SERS signal enhancement. Raman spectroscopy is a label-free optical detection technique for chemicals and biomolecules. A Raman spectrum provides an optical fingerprint of chemicals and biomolecules, although conventional Raman detection is limited by extremely low efficiency of scattering. In surface enhanced Raman scattering (SERS), the surface area of the substrate is increased and thus the optical cross-section for scattering increases. A discussion of SERS can be found in M. Moskovits, “Surface-Enhanced Spectroscopy,” Reviews of Modern Physics, 1985, vol. 57, pp. 783-826, which is hereby incorporated by reference in its entirety. Traditionally, SERS substrates have been based on colloidal silver or gold nanoparticles or thin films deposited on silicon or polymer substrates.
Micro-Raman spectroscopy was performed at room temperature using a Jobin-Yvon Horiba LabRam system with a He—Ne laser with an excitation frequency of 633 nm. CV 10B dissolved in methanol was used as a test molecule. Solutions were placed on the substrates in a 200 micron-thick well covered by a glass cover slip to prevent solvent evaporation. To obtain spectra, a 17 mW laser beam with a 2 micron spot size and 4 micron depth of field was passed through the cover slip and focused on the substrate surface. For the patterned samples, Raman spectra were acquired from different spots in the sputtered hole.
Since the SERS enhancement is not a linear process, the enhancement factor is estimated by comparing the Raman scattering intensities of the methanol peak at 1035 cm−1 and a CV peak at 1176 cm−1. The SERS enhancement factor can be calculated from the ratio of (ICV/NCV)/(IMeOH/NmeOH), where ICV and IMeOH denote the integrated intensities of the bands for CV and methanol, respectively, and NCV and NMeOH represent the corresponding number of CV and methanol molecules excited by the laser beam. It is assumed that all methanol molecules from the probed volume, defined by a diameter equal to the beam spot size and length equal to the depth of field, contribute to the methanol Raman peak, while CV molecules from only a thin layer of thickness near the substrate surface, approximated to be between 10 nm and 300 nm, contribute to the SERS signal. Based on this approach and the data in
To detect varying concentrations of CV, a series of solutions was introduced on the same substrate with thorough washing by methanol between loadings. The Raman spectra in
The existence of “hot spots” or variation in the SERS enhancement on a patterned substrate was determined by scanning the laser beam over an area of 300×300 square microns in 10 micron steps to obtain intensity maps. A false color SERS intensity map for a sputtered hole is shown in
The inventors have developed a simple and reproducible method to fabricate SERS-active substrates by nonlithographic patterning using a numerically-controlled tool for generating a microplasma. The tool enables microscale features, such as arrays of holes, to be carved into metal (e.g., silver) films, thus dramatically altering the density of SERS-active sites in the films. The technique is scalable and may allow mass production of identical SERS substrates for a wide array of chemical, biomedical, and environmental applications.
Although the present invention has been described in considerable detail with reference to certain embodiments thereof, other embodiments are possible without departing from the present invention. The spirit and scope of the appended claims should not be limited, therefore, to the description of the preferred embodiments contained herein. All embodiments that come within the meaning of the claims, either literally or by equivalence, are intended to be embraced therein. Furthermore, the advantages described above are not necessarily the only advantages of the invention, and it is not necessarily expected that all of the described advantages will be achieved with every embodiment of the invention.
The present patent document claims the benefit of the filing date under 35 U.S.C. §119(e) of U.S. Provisional Patent Application Ser. No. 61/036,297, which was filed on Mar. 13, 2008, and is hereby incorporated by reference in its entirety.
Number | Date | Country | |
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61036297 | Mar 2008 | US |