Campanile probe

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SEM image of a campanile probe. Campanile probe2.jpg
SEM image of a campanile probe.
SEM image of a campanile probe. Campanile probe3.jpg
SEM image of a campanile probe.
False-color SEM image of the Campanile near-field probe fabricated on the edge of an optical fiber using nanoimprint. Nanoimprinted-campanile-probe.png
False-color SEM image of the Campanile near-field probe fabricated on the edge of an optical fiber using nanoimprint.
Comparison of photoluminescence maps recorded from a molybdenum disulfide flake using a campanile probe (top) and conventional confocal microscopy (bottom). Scale bars: 1 mm. Campanile probe vs confocal PL maps.jpg
Comparison of photoluminescence maps recorded from a molybdenum disulfide flake using a campanile probe (top) and conventional confocal microscopy (bottom). Scale bars: 1 μm.

In near-field scanning optical microscopy the campanile probe is a tapered optical probe with a shape of a campanile (a square pyramid). It is made of an optically transparent dielectric, typically silica, and its two facets are coated with a metal, typically gold. At the probe tip, the metal-coated facets are separated by a gap of a few tens of nanometers, which determines the spatial resolution of the probe. Such a probe design allows collecting optical signals, usually photoluminescence (PL) or Raman scattering, with a subwavelength resolution, breaking the diffraction limit. [1] [3]

The campanile probe is attached to an optical fiber, which both provides a laser excitation of the studied sample and collects the measured signal. The probe is rastered over the sample with a standard scanning probe microscopy scanner, keeping the distance to the sample surface at a few nanometers. [1] Contrary to the traditional (circular) near-field probes, the campanile probe has no cut-off frequency and is insensitive to the spatial mode of the optical near field. Hence its application is not limited to thin-film samples. [3] Another advantage of the campanile probe is a high signal collection efficiency, which exceeds 90%. [4]

Campanile probes are typically fabricated as follows: a standard cylindrical single-mode optical fiber is etched with hydrofluoric acid to create a conical tip with a radius of ca. 100 nm. Then a square pyramid is carved on the tip using focused ion beam (FIB) milling, and its two facets are coated with a metal by shadow evaporation. A nanometer gap is the opened on the tip by FIB. [3] Alternative fabrication method uses nanoimprint lithography to replicate campanile pyramid from a mold. This approach significantly increases fabrication speed. [2]

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Scanning probe microscopy (SPM) is a branch of microscopy that forms images of surfaces using a physical probe that scans the specimen. SPM was founded in 1981, with the invention of the scanning tunneling microscope, an instrument for imaging surfaces at the atomic level. The first successful scanning tunneling microscope experiment was done by Gerd Binnig and Heinrich Rohrer. The key to their success was using a feedback loop to regulate gap distance between the sample and the probe.

Cathodoluminescence microscope

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Dip pen nanolithography (DPN) is a scanning probe lithography technique where an atomic force microscope (AFM) tip is used to create patterns directly on a range of substances with a variety of inks. A common example of this technique is exemplified by the use of alkane thiolates to imprint onto a gold surface. This technique allows surface patterning on scales of under 100 nanometers. DPN is the nanotechnology analog of the dip pen, where the tip of an atomic force microscope cantilever acts as a "pen," which is coated with a chemical compound or mixture acting as an "ink," and put in contact with a substrate, the "paper."

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Near-field scanning optical microscope

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Scanning electrochemical microscopy (SECM) is a technique within the broader class of scanning probe microscopy (SPM) that is used to measure the local electrochemical behavior of liquid/solid, liquid/gas and liquid/liquid interfaces. Initial characterization of the technique was credited to University of Texas electrochemist, Allen J. Bard, in 1989. Since then, the theoretical underpinnings have matured to allow widespread use of the technique in chemistry, biology and materials science. Spatially resolved electrochemical signals can be acquired by measuring the current at an ultramicroelectrode (UME) tip as a function of precise tip position over a substrate region of interest. Interpretation of the SECM signal is based on the concept of diffusion-limited current. Two-dimensional raster scan information can be compiled to generate images of surface reactivity and chemical kinetics.

AFM-IR Infrared microscopy technique

AFM-IR is one of a family of techniques that are derived from a combination of two parent instrumental techniques; infrared spectroscopy and scanning probe microscopy (SPM). The term was first used to denote a method that combined a tuneable free electron laser with an atomic force microscope equipped with a sharp probe that measured the local absorption of infrared light by a sample; it required that the sample be coupled to an infrared-transparent prism and be less than 1μm thick. It improved the spatial resolution of photothermal AFM-based techniques from microns to circa 100 nm.

Tip-enhanced Raman spectroscopy is a specialist approach to surface-enhanced Raman spectroscopy (SERS) in which enhancement of Raman scattering occurs only at the point of a near atomically sharp pin, typically coated with gold.

The operation of a photon scanning tunneling microscope (PSTM) is analogous to the operation of an electron scanning tunneling microscope (ESTM), with the primary distinction being that PSTM involves tunneling of photons instead of electrons from the sample surface to the probe tip. A beam of light is focused on a prism at an angle greater than the critical angle of the refractive medium in order to induce total internal reflection (TIR) within the prism. Although the beam of light is not propagated through the surface of the refractive prism under TIR, an evanescent field of light is still present at the surface.

A probe tip in scanning microscopy is a very sharp object made from metal or other materials, like a sewing needle with a point at one end with nano or sub-nanometer order of dimension. It can interact with up to one molecule or atom of a given surface of a sample that can reveal authentic properties of the surface such as morphology, topography, mapping and electrical properties of a single atom or molecule on the surface of the sample.

References

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