Spatio-temporally incremental fiber swept source

Abstract

A spatio-temporally incremental fiber sweep source includes a laser light pulse generator for generating light pulses and a fiber array of individual optical fibers. The fiber array has an input end and an output end, with the fibers at the input end receiving the light pulses substantially simultaneously. The optical fibers at the output end are arranged in a raster scan pattern, e.g., a square pattern, wherein the optical delay in each fiber is greater than the previous one in the scan pattern direction. As a result light exits the array in a completely optical two dimensional raster scan pattern. It has no moving parts, and thus no mechanical inertia, so extremely high speed scanning can be achieved.

Description

FIELD OF THE INVENTION[0001]The present invention relates to an optical fiber source for providing ultrafast inertia-free spatially-scanning laser pulses.BACKGROUND OF THE INVENTION[0002]Optical imaging has drawn great attention from various areas in the past decade, particularly industrial inspection and biomedical diagnosis. As the scientific research has gone deeper and deeper into the details of these areas, people have become more and more interested in dynamic behaviors, especially those involved in life science, e.g. hemokinesis, cytology and neurology, which provide information that may help provide a better understanding of the human body. In particular there is great interest in ultrafast dynamic diagnosis of disease and other tissue functionality. To visualize high-speed dynamic events, an optical imager is required to provide high sensitivity and high throughput. Modern photo-receivers can offer excellent sensitivity, e.g. widely-used CCD / CMOS cameras and photomultiplier...

AI Technical Summary

Benefits of technology

The present invention introduces a new laser source called 2D spatially-sweeping source (2D SS) that overcomes limitations of traditional laser sources. This new source can capture images at a faster rate of 10 s of MHz, making it ideal for applications such as flow cytometers. It can provide peak power up to the kW level, making it suitable for use in confocal microscopy. It has an ultra wide operational wavelength range and is cost-effective.

Problems solved by technology

Their imaging speed, on the other hand, is largely limited, which results in blurred images.

Typically, there are two main issues that have to be addressed for increasing the effective speed of an optical system: scanning speed and signal readout speed.

Mechanical inertia, unfortunately, limits the moving speed of these bulky stages, typically to several mm / s.

Although in the latter case, i.e., where the beam is moved, can indeed perform the video rate imaging, it is still far from the requirements for a 3D volumetric visualization of those highly dynamic objects.

In addition to the scanning speed, the readout time of the optical signal is another limitation on effectively boosting up the imaging speed, and it must be fast enough to acquire the fast scanning signal.

Traditionally, the optical signal is read out through CCD / CMOS cameras, which however exhibit an unacceptable latency and result in a slow frame rate, typically 100 Hz, and hence a long read-out time.

Unfortunately, the wavelength-swept source is a point source, and it is still necessary to perform point scanning via, e.g., galvanometer scanning, for 2D / 3D imaging.

However, it has the same issue as that of FDML, i.e., extra scanning is required.

The nature of the time-stretch, i.e., high frequency chirping, also limits the instantaneous peak power.

Thus it cannot be used for those applications requiring high peak power, for example multi-photon imaging.

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