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Conference on Lasers and Electro-Optics

Fast response time atomic filter at 423 nm

Y. C. Chan, Jerry A. Gelbwachs

Published May 2, 1993• 0 citations
OpenAlex

Abstract

Atomic resonance filters are optical bandpass filters that employ sharp atomic transitions to perform ultra-narrow-band (0.001 nm) filtering of light.1 Further, the bandwidth is independent of aperture size and field-of-view, These devices are designed to exclude sunlight in laser receivers. Applications include laser radar, lasercom, remote sensing, and underwater communications.

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Atomic resonance filters are optical bandpass filters that employ sharp atomic transitions to perform ultra-narrow-band (0.001 nm) filtering of light.1 Further, the bandwidth is independent of aperture size and field-of-view, These devices are designed to exclude sunlight in laser receivers. Applications include laser radar, lasercom, remote sensing, and underwater communications.
Narrow-bandwidth optical sources are readily available. However, tunable narrow-bandwidth, wide field-of-view optical filters are not available. The laser-pumped atomic vapor optical filters presented here are in principle tunable narrow-bandwidth, wide field-of-view optical filters. These filters can simultaneously provide high resolution (0.001 nm), wide field-of-view (±90°), high quantum efficiency, and electrically tunable optical filtering. These devices are ideally suited for extracting weak narrow-bandwidth signals buried in strong nonresonant optical background radiation. Potential applications of these fitters include laser communications, laser radar, detection of Raman radiation, and atomic spectroscopy.
A new resonance principle in optical filters has been utilized to simultaneously permit realization of wide field-of-view (∼2π sr) and very narrow acceptance bandwidths, approaching 0.01 Å. A light signal is transmitted through an outer bandpass filter into a resonantly absorbing atomic vapor, resulting in a fluorescence signal at a different wavelength which is transmitted through an inner bandpass filter. The outer and inner bandpass filters have no common transmission band, resulting in complete blockage of all optical signals (background noise) that are not resonantly shifted in wavelength by the intervening atomic vapor. This ’’resonance filter’’ principle is experimentally verified, and system parameters are discussed for filters utilizing potassium, rubidium, or cesium vapor at nine wavelengths between 420 and 532 nm.
Narrow bandwidth optical sources are readily available; however, tunable narrow-bandwidth, wide field-of-view optical filters are not available. Laser-excited optical filters (LEOFs) are in principle, tunable narrow-bandwidth, wide field-of-view optical filters. LEOFs can simultaneously provide high resolution (0.001 nm), wide field of-view (2π), and high quantum efficiency. These devices are ideally suited for extracting weak narrow bandwidth signals buried in strong nonresonant optical background radiation. Potential applications of these filters include remote sensing, laser communications, laser radar, detection of Raman radiation, atomic spectroscopy, etc.
An ultra-high Q isotropically sensitive optical filter or optical detector employing atomic resonance transitions. More specifically, atomic resonance transitions utilized in conjunction with two optical bandpass filters provide an optical detector having a wide field of view (.about.2.pi. steradians) and very narrow acceptance bandwidth approaching 0.01 A. A light signal to be detected is transmitted through an outer bandpass filter into a resonantly absorbing atomic vapor, the excited atomic vapor then providing a fluorescence signal at a different wavelength which is transmitted through an inner bandpass filter. The outer and inner bandpass filters have no common transmission band, thereby resulting in complete blockage of all optical signals that are not resonantly shifted in wavelength by the intervening atomic vapor. Two embodiments are disclosed, one in which the light signal raises atoms contained in the atomic vapor from the ground state to an excited state from which fluorescence occurs, and the other in which a pump laser is used to raise the atoms in the ground state to a first excited state from which the light signal then is resonantly absorbed, thereby raising the atoms to a second excited state from which fluorescence occurs. A specific application is described in which an optical detector according to the present invention can be used as an underwater detector for light from an optical transmitter which could be located in an orbiting satellite.
Narrow-bandwidth optical sources are readily available. However, tunable narrow-bandwidth wide field-of-view optical filters are not available. The laser-excited optical filters (LEOFs) presented here are in principle tunable narrow-bandwidth wide field-of-view optical filters. These filters can simultaneously provide high-resolution (0.001-nm), wide field-of-view (±90°), high-quantum-efficiency, and electrically tunable optical filtering. These devices are ideally suited for extracting weak narrow-bandwidth signals buried in strong nonresonant optical background radiation. Potential applications of these filters include laser communications, laser radar, detection of Raman radiation, and atomic spectroscopy.
An optically pumped active Ca atomic resonance filter is demonstrated, applicable to background-limited optical communications through scatter channels. In pump saturation, the filter should detect 50% of the incident 423-nm signal power with an internal photon gain of 6 and a response time of 10 micros, 2 orders of magnitude faster than a passive Ca filter. Response time of 100 micros has been demonstrated, limited by available pump power. The filter maintains the wide field of view and reduced solar background associated with atomic absorption at the Ca Fraunhofer line while permitting higher data rate communications.