Plasmonic nanolithography

Theory

Main article: Surface plasmon polariton

Surface plasmon polaritons are surface electromagnetic waves that propagate in between two surfaces with sign-changing permittivities. They originate from coupling of photons to plasma oscillations, quantized as plasmons. SPPs result in evanescent fields that decay perpendicularly to the interface where the propagation occurs. The dispersion relation for SPPs permits the excitation of wavelengths shorter than the free-space wavelength of the inbound light, additionally ensuring subwavelength field confinement. Nevertheless, the excitation of SPPs necessitate momentum mismatch; prism and grating coupling methods are common. For plasmonic nanolithography processes, this is achieved through surface roughness and perforations.

Methods

Plasmonic contact lithography, a modification on the evanescent near-field lithography, uses a metal photomask, on which the SPPs are excited. Similar to common photolithographic processes, photoresist is exposed to SPPs that propagate from the mask. Photomasks with holes enable grating coupling of SPPs; the fields only propagate for nanometers. Srituravanich et al. has demonstrated the lithographic process experimentally with a 2D silver hole array mask; 90 nm hole arrays were produced at 365 nm wavelength, which is beyond diffraction limit. Zayats and Smolyaninov utilized a multi-layered metal film mask to enhance the subwavelength aperture; such structures can be realized by thin film deposition methods. Bowtie apertures and nanogaps were also suggested as alternative apertures. A version of the method, named as surface plasmon interference nanolithography by Liu et al., uses SPP interference patterns. Despite offering high resolution and throughput, plasmonic contact lithography is regarded as an expensive and complex method; contamination due to contact is also a limiting factor.

Planar lens imaging nanolithography uses plasmonic lenses or negative-index superlenses, which were first proposed by John Pendry. Many superlens designs, such as Pendry's thin silver film or Fang et al.'s superlens, benefit from plasmonic excitations to focus Fourier components of incoming light beyond the diffraction limit. Chaturvedi et al. has demonstrated the imaging of a 30 nm chromium grating through silver superlens photolithography at 380 nm, while Shi et al. simulated a 20 nm lithography resolution at 193 nm wavelength with an aluminum superlens. Srituravanich et al. has developed a mechanically adjustable, hovering plasmonic lens for maskless near-field nanolithography, whereas another maskless approach by Pan et al. uses a "multi-stage plasmonic lens" for progressive coupling.

Plasmonic direct writing is a maskless form of photolithography that is based on scanning probe lithography; the method uses localized surface plasmon (LSP) enhancements from embedded plasmonic scanning probes to expose the photoresist. Wang et al. experimentally demonstrated 100 nm field confinement with this method. Kim et al. has developed a ~50 nm resolution scanning probe with a patterning speed of ~10 mm/s. Gold nanoparticles and other plasmonic nanostructures such as nanogaps have been used as masks for lithography; etching in this case can be achieved through either through photomasking principles or enhanced local heating in the vicinity of the nanostructure due to the LSP resonances. Lin et al. also used localized thermal excitations in gold nanoparticles to fabricate two-dimensional structures such as patterned graphene and molybdenum disulfide monolayers in a process termed as "optothermoplasmonic nanolithography." Photochemical effects of LSP resonances were also used as a catalyst in lithographic processes: Saito et al. demonstrated selective etching of silver nanocubes on titanium dioxide substrates by the means of plasmon-induced charge separation.

References

References

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