摘要:
The application relates to methods for producing islands of functionality within nanoscale apertures. Islands of functionality can be produced by growing an aperture constriction layer from the walls, functionalizing the exposed base of the aperture, then removing the aperture constriction layer. The aperture constriction layer can be produced, for example, by anodically growing an oxide layer onto a cladding through which the aperture extends. The islands of functionality can be used to bind a single molecule of interest, such as an enzyme within the nanoscale aperture.
摘要:
The application relates to improved optical containment structures, methods of manufacture and use, and systems for employing same. The optical containment structures generally comprise zero-mode waveguide structures having non-reflective walls. The non-reflective walls allow the preparation of optical containment regions in which the optical containment dimensions can be decoupled from the solution containment dimensions. The application also relates to methods for producing islands of functionality within nanoscale apertures.
摘要:
The application relates to methods for producing islands of functionality within nanoscale apertures. Islands of functionality can be produced by growing an aperture constriction layer from the walls, functionalizing the exposed base of the aperture, then removing the aperture constriction layer. The aperture constriction layer can be produced, for example, by anodically growing an oxide layer onto a cladding through which the aperture extends. The islands of functionality can be used to bind a single molecule of interest, such as an enzyme within the nanoscale aperture.
摘要:
The application relates to improved optical containment structures, methods of manufacture and use, and systems for employing same. The optical containment structures generally comprise zero-mode waveguide structures having non-reflective walls. The non-reflective walls allow the preparation of optical containment regions in which the optical containment dimensions can be decoupled from the solution containment dimensions. The application also relates to methods for producing islands of functionality within nanoscale apertures.
摘要:
Photonic crystal sensors may be created from two and three dimensional photonic crystals by introducing defects. The localization of the optical field in the defect region affords the ability to sense small volumes of analyte.
摘要:
An apparatus and method for measuring a target environmental variable (TEV) that employs a film-bulk acoustic resonator with motion plate. The film-bulk acoustic resonator (FBAR) includes an acoustic reflector formed in an FBAR wafer and a surface. A first electrode is formed on the surface of the acoustic reflector and has a surface. A piezoelectric layer is formed on the surface of the first electrode and has a surface. A second electrode is formed on the surface of the piezoelectric layer. A motion plate is suspended in space at a predetermined distance relative to the surface of the second electrode and is capacitively coupled to the FBAR.
摘要:
A humidity sensor that includes a resonant structure and a structure for altering a resonant frequency of the resonant structure in response to a change in humidity. The structures of a humidity sensor according to the present teachings may be formed in relatively small form factors and are well suited to remote applications and providing mechanisms for compensating for temperature drift.
摘要:
A photonic crystal sensor adapted for single nanoparticle detection is disclosed. Very small single particles and single molecules may be detected. The sensors may be adapted to allow differential measurements.
摘要:
Photonic crystal sensors may be created from two and three dimensional photonic crystals by introducing defects. The localization of the optical field in the defect region affords the ability to sense small volumes of analyte.
摘要:
The external cavity laser includes a resonant cavity defined at one end by a Bragg reflector and a gain medium located in the optical cavity. Coupled to the Bragg reflector is an actuator that changes the pitch of the Bragg reflector and, hence, the wavelength at which the optical cavity is resonant. The wavelength of the light generated by the external cavity laser can therefore be tuned by a single control signal applied to the actuator.