2004
DOI: 10.1117/12.562089
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Stationary high-bandwidth beacon-tracking lasercom experiments and the evolution toward a mobile lasercom capability

Abstract: Stationary high-bandwidth experiments with a portable lasercom (laser communication) system were performed over a wide range of scintillation indices (< 0.1 to 1) at the Department of Energy's Nevada Test Site in the summer of 2003. Active alignment was performed with a quad-cell tracking detector at the transmitter transponder and a conical-scan tracking beam at the receiver transponder. During good scintillation conditions, 2-km 10-Gb/s and 11-km 2.5-Gb/s capabilities were demonstrated at error-free bit-erro… Show more

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Cited by 3 publications
(2 citation statements)
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“…Given the distance d between the Center of the Beam and the Retro, the Beam Radius W (1/e 2 , assuming a Gaussian beam), the optical Power reflected by the retro-reflector is given by : ( 2 ) Magnitude of the beam offset The amplitude of the modulation of the received power is given by the difference between the power at min distance and max distance, and we easily get: …”
Section: Theorymentioning
confidence: 99%
“…Given the distance d between the Center of the Beam and the Retro, the Beam Radius W (1/e 2 , assuming a Gaussian beam), the optical Power reflected by the retro-reflector is given by : ( 2 ) Magnitude of the beam offset The amplitude of the modulation of the received power is given by the difference between the power at min distance and max distance, and we easily get: …”
Section: Theorymentioning
confidence: 99%
“…Assuming that one can calculate the phase difference, the feedback signal has to be sent back to the other end (B), which creates a chicken and egg problem, unless one relies on out-of-band communication such as a RF link or an additional beam as proposed in prior work [3]. This question of the feedback path necessary to close the loop is addressed in section 2.…”
Section: Introductionmentioning
confidence: 99%