Abstract: A label-free detection and characterization system includes an optical source; an optical path arranged to be optically coupled to the optical source; an optical resonator disposed proximate the optical path along a side of the optical path, the optical resonator having an optical whispering-gallery mode and being optically coupled to the optical path through an evanescent field to excite the optical whispering-gallery mode; an optical receiver arranged to be optically coupled to the optical path. The optical source is frequency locked to a resonance frequency of the optical resonator and provides light sufficiently intense to provide four-wave mixing while being coupled with the optical resonator resulting in a comb spectrum received by the optical receiver. The comb spectrum provides characteristic changes in the presence of a substance in contact with the optical resonator to provide detection and characterization of the substance.

Abstract: An optical microtoroid resonator including one or more nanoparticles attached to a surface of the resonator and capable of receiving an input signal from afar-field source (via free-space transmission) and outputting light propagating within the optical apparatus. A method for coupling light into and out of an optical resonator using a nanoparticle or nanoparticles to interface with spatially separated far-field optical elements.

Abstract: An optical microtoroid resonator including one or more nanoparticles attached to a surface of the resonator and capable of receiving an input signal from a far-field source (via free-space transmission) and outputting light propagating within the optical apparatus. A method for coupling light into and out of an optical resonator using a nanoparticle or nanoparticles to interface with spatially separated far-field optical elements.

Abstract: A label-free detection and characterization system includes an optical source; an optical path arranged to be optically coupled to the optical source; an optical resonator disposed proximate the optical path along a side of the optical path, the optical resonator having an optical whispering-gallery mode and being optically coupled to the optical path through an evanescent field to excite the optical whispering-gallery mode; an optical receiver arranged to be optically coupled to the optical path. The optical source is frequency locked to a resonance frequency of the optical resonator and provides light sufficiently intense to provide four-wave mixing while being coupled with the optical resonator resulting in a comb spectrum received by the optical receiver. The comb spectrum provides characteristic changes in the presence of a substance in contact with the optical resonator to provide detection and characterization of the substance.

Abstract: An optical microtoroid resonator including one or more nanoparticles attached to a surface of the resonator and capable of receiving an input signal from a far-field source (via free-space transmission) and outputting light propagating within the optical apparatus. A method for coupling light into and out of an optical resonator using a nanoparticle or nanoparticles to interface with spatially separated far-field optical elements.

Abstract: Systems and methods are provided for detecting one or more particles such as individual unlabeled molecules or single nanoparticles. In examples described herein, optical energy is introduced into a microtoroid or other microcavity to generate an evanescent field. The microcavity has a functionalized outer surface that has been functionalized with a chemically or biologically active substance such as an antibody, antigen or protein. An indication of a particle bound to the functionalized outer surface of the microcavity is then detected based on a reactive interaction between the particle and the evanescent field while using frequency locking, balanced detection and various filtering techniques. The frequency locking, balanced detection and filtering techniques reduce the signal-to-noise ratio (SNR) of the detection system so that single nanoparticles (e.g. 2.5 nanometers (nm) in radius) and individual molecules (e.g. 15.5 kilo-Dalton (kDa) in size) can be detected in aqueous solution in some examples.

Abstract: Systems and methods are provided for detecting one or more particles such as individual unlabeled molecules or single nanoparticles. In examples described herein, optical energy is introduced into a microtoroid or other microcavity to generate an evanescent field. The microcavity has a functionalized outer surface that has been functionalized with a chemically or biologically active substance such as an antibody, antigen or protein. An indication of a particle bound to the functionalized outer surface of the microcavity is then detected based on a reactive interaction between the particle and the evanescent field while using frequency locking, balanced detection and various filtering techniques. The frequency locking, balanced detection and filtering techniques reduce the signal-to-noise ratio (SNR) of the detection system so that single nanoparticles (e.g. 2.5 nanometers (nm) in radius) and individual molecules (e.g. 15.5 kilo-Dalton (kDa) in size) can be detected in aqueous solution in some examples.

Abstract: Systems and methods are provided for detecting one or more particles such as individual unlabeled molecules or single nanoparticles. In examples described herein, optical energy is introduced into a microtoroid or other microcavity to generate an evanescent field. The microcavity has a functionalized outer surface that has been functionalized with a chemically or biologically active substance such as an antibody, antigen or protein. An indication of a particle bound to the functionalized outer surface of the microcavity is then detected based on a reactive interaction between the particle and the evanescent field while using frequency locking, balanced detection and various filtering techniques. The frequency locking, balanced detection and filtering techniques reduce the signal-to-noise ratio (SNR) of the detection system so that single nanoparticles (e.g. 2.5 nanometers (nm) in radius) and individual molecules (e.g. 15.5 kilo-Dalton (kDa) in size) can be detected in aqueous solution in some examples.

Abstract: Systems and methods are provided for detecting one or more particles such as individual unlabeled molecules or single nanoparticles. In examples described herein, optical energy is introduced into a microtoroid or other microcavity to generate an evanescent field. The microcavity has a functionalized outer surface that has been functionalized with a chemically or biologically active substance such as an antibody, antigen or protein. An indication of a particle bound to the functionalized outer surface of the microcavity is then detected based on a reactive interaction between the particle and the evanescent field while using frequency locking, balanced detection and various filtering techniques. The frequency locking, balanced detection and filtering techniques reduce the signal-to-noise ratio (SNR) of the detection system so that single nanoparticles (e.g. 2.5 nanometers (nm) in radius) and individual molecules (e.g. 15.5 kilo-Dalton (kDa) in size) can be detected in aqueous solution in some examples.

Abstract: Resonant sensors and molecule detection methods utilizing split frequency. Optical energy is introduced into a microcavity, such as a toroid-shaped or spherical microcavity. A portion of the optical energy is backscattered and interacts with the introduced optical energy to form first and second modes of optical energy at respective first and second frequencies, also referred to as split frequency or mode doublets. One or more molecules bind to an outer surface of the microcavity and interact with an evanescent field of optical energy resonating within the microcavity. Binding of one or more molecules to the outer surface is detected based at least in part upon a change of the split frequency relative to a baseline split frequency.

Abstract: Resonant sensors and molecule detection methods utilizing split frequency. Optical energy is introduced into a microcavity, such as a toroid-shaped or spherical microcavity. A portion of the optical energy is backscattered and interacts with the introduced optical energy to form first and second modes of optical energy at respective first and second frequencies, also referred to as split frequency or mode doublets. One or more molecules bind to an outer surface of the microcavity and interact with an evanescent field of optical energy resonating within the microcavity. Binding of one or more molecules to the outer surface is detected based at least in part upon a change of the split frequency relative to a baseline split frequency.