Abstract:
We describe methods and apparatus for high-speed high-contrast imaging one-, two- and three-dimensional imaging enabled by differential interference contrast time encoded amplified microscopy of transparent media without the need for chemical staining, that are suitable for a broad range of applications from semiconductor process monitoring to blood screening. Our methods and apparatus build on a unique combination of serial time-encoded amplified microscopy (STEAM) and differential interference contrast (DIC) microscopy. These methods and apparatus are ideally suited for identification of rare diseased cells in a large population of healthy cells and have the potential to revolutionize blood analysis and pathology including identification of cancer cells, such as Circulating Tumor Cells (CTC) in early stage disease.
Abstract:
We describe methods and apparatus for high-speed high-contrast imaging one-, two- and three-dimensional imaging enabled by differential interference contrast time encoded amplified microscopy of transparent media without the need for chemical staining, that are suitable for a broad range of applications from semiconductor process monitoring to blood screening. Our methods and apparatus build on a unique combination of serial time-encoded amplified microscopy (STEAM) and differential interference contrast (DIC) microscopy. These methods and apparatus are ideally suited for identification of rare diseased cells in a large population of healthy cells and have the potential to revolutionize blood analysis and pathology including identification of cancer cells, such as Circulating Tumor Cells (CTC) in early stage disease.
Abstract:
Un método de obtención de imágenes por fluorescencia, comprendiendo el método: con un deflector acústico-óptico (22) accionado por un peine de RF (20) y un rayo láser de excitación (16), crear (82) una pluralidad de primeros haces (24) de luz con un rango de ángulos de salida y cambios de frecuencia; con un variador de frecuencia acústico-óptico (28) accionado por un tono de RF y un rayo láser (18) de excitación, crear (84) un segundo haz (30) de luz desplazado en frecuencia; combinar la pluralidad de los primeros haces (24) y el segundo haz (30) para producir una pluralidad de haces de luz (34) combinados desplazados en frecuencia; interrogar (86) simultáneamente a múltiples puntos en una muestra (46) con la pluralidad de haces de luz (34) combinados; y detectar (88) una respuesta fluorescente de la muestra por exposición a la pluralidad de haces de luz combinados.
Abstract:
Un aparato (20, 52, 88, 124, 170, 210, 250, 270) para leer patrones y detectar desplazamientos, que comprende: un medio (22, 54, 90, 126) para generar un haz de sonda pulsado de banda ancha (178); un medio (34, 66, 108, 144, 262, 340) para correlacionar mediante la transformada de Fourier del espectro de dicho haz de sonda pulsado con un dominio espacial para formar un haz óptico dispersado espacialmente (182) dirigido a un objetivo (38, 70, 110, 146, 214), en el que dicho objetivo (38, 70, 110, 146, 214) ha de ser leído; un medio (34, 66, 108, 144, 262, 34b) para formar una señal óptica de respuesta basándose en la energía óptica procedente del objetivo; un medio (40, 72, 112, 148) para la transformada de Fourier dispersiva de dicha señal óptica de respuesta para convertir dicha señal óptica de respuesta en una forma de onda en el dominio del tiempo; y un medio (42, 200, 78, 114, 154) para detectar y analizar dicha forma de onda en el dominio del tiempo para determinar patrones y/o desplazamientos dentro del objetivo que es leído.
Abstract:
An apparatus and method for measuring Raman-type spectra using optical dispersion to convert an optical spectrum into a waveform which can be detected directly in the time domain without the use of a conventional spectrometer. In the example of stimulated Raman spectroscopy, the apparatus and method exposes a sample to a chirped, pulsed probe beam and a Raman pump beam and the resulting Raman spectra is detected by an optical detector in the time domain, and analyzed. Alternatively, the Raman spectra from the probe and pump beams is chirped with a dispersive element prior to detection and analysis. Each probe pulse provides a snapshot of the Raman spectrum that is sampled in time so that neither repetitive waveforms nor static samples are required. Therefore, high speed acquisitions and high throughput assays can be conducted. To facilitate detection, these spectral signals can also be amplified using distributed Raman amplification directly in the dispersive element.
Abstract:
A system and method to chromomodally generate dispersion in light waves. The system and method may be used to control dispersive effects of an optical element such as a single-mode fiber. A light beam from the optical element is first collimated and then directed on to a spatially diffractive element where it is spatially dispersed into various chromatic frequency components. This frequency-separated light is then imparted onto a dispersion slope equalizer, and then passed into a highly multimode waveguide, where it is further dispersed. The light is then collected and focused back into an outgoing fiber-optic or other optical device.
Abstract:
An imaging flow cytometry apparatus and method which allows registering multiple locations across a cell, and/or across multiple flow channels, in parallel using radio-frequency-tagged emission (FIRE) coupled with a parallel optical detection scheme toward increasing analysis throughput. An optical source is modulated by multiple RF frequencies to produce an optical interrogation beam having a spatially distributed beat frequency. This beam is directed to one or more focused streams of cells whose responsive fluorescence, in different frequencies, is registered in parallel by an optical detector.
Abstract:
Apparatus and methods for fluorescence imaging using radiofrequency multiplexed excitation. One apparatus splits an excitation laser beam into two arms of a Mach-Zehnder interferometer. The light in the first beam is frequency shifted by an acousto-optic deflector, which is driven by a phase-engineered radiofrequency comb designed to minimize peak-to-average power ratio. This RF comb generates multiple deflected optical beams possessing a range of output angles and frequency shifts. The second beam is shifted in frequency using an acousto-optic frequency shifter. After combining at a second beam splitter, the two beams are focused to a line on the sample using a conventional laser scanning microscope lens system. The acousto-optic deflectors frequency-encode the simultaneous excitation of an entire row of pixels, which enables detection and de-multiplexing of fluorescence images using a single photomultiplier tube and digital phase-coherent signal recovery techniques.
Abstract:
A time-stretched enhanced recording scope (TiSER) is described using time stretch analog-to-digital conversion in a real-time burst mode. A chirped optical signal is modulated in response to receiving segments of an input signal. The optical signal with its modulated input signal, is stretched through an optical medium and digitized to represent the waveform segment. TiSER provides ultra-fast real-time sampling within short segment bursts of the original input signal while providing an ability to detect non-repetitive events. Methods and apparatus are also described for providing real-time information about inter-symbol information (ISI), rapidly determining bit-error rates (BER), performing time-domain reflectometry (TDR), generating eye diagrams for serial data, facilitating digital correction of data, clock recovery, optical carrier phase recovery, and otherwise increasing the speed and/or accuracy of a diverse range of high-speed signal measurement and processing activities.