Coherent Laser Beam Combining 2013
DOI: 10.1002/9783527652778.ch08
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Coherent Beam Combining of Pulsed Fiber Amplifiers in the Long‐Pulse Regime (Nano‐ to Microseconds)

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Cited by 4 publications
(5 citation statements)
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“…According to [36], the typical optical turbulence coherence time is on the order of 1 to 10 ms (cutoff frequency ranging from 100 Hz to 1 kHz). On the other hand, the accumulated phase noise of fiber amplifiers is up to 𝑓 = 10 kHz [9]. In order to properly sample the phase noise and distinguish the contribution of different channels, the tagging frequencies must fit within an octave and should be spaced by at least ~10 × 𝑓 .…”
Section: Fiber Amplifiers and Optical Headmentioning
confidence: 99%
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“…According to [36], the typical optical turbulence coherence time is on the order of 1 to 10 ms (cutoff frequency ranging from 100 Hz to 1 kHz). On the other hand, the accumulated phase noise of fiber amplifiers is up to 𝑓 = 10 kHz [9]. In order to properly sample the phase noise and distinguish the contribution of different channels, the tagging frequencies must fit within an octave and should be spaced by at least ~10 × 𝑓 .…”
Section: Fiber Amplifiers and Optical Headmentioning
confidence: 99%
“…In order to properly sample the phase noise and distinguish the contribution of different channels, the tagging frequencies must fit within an octave and should be spaced by at least ~10 × 𝑓 . This leads to tagging frequencies ranging from 𝐹 = 10 × 𝑁 × 𝑓 = 0.6 MHz to 𝐹 = 10 × (2𝑁 − 2) × 𝑓 = 1 MHz with 𝑁 = 6 and 𝑓 = 10 kHz [9]. The effective bandwidth of the control loop is 30 kHz.…”
Section: Fiber Amplifiers and Optical Headmentioning
confidence: 99%
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“…[11][12][13][14][15] A challenge in pulse fiber laser development for remote sensing is to address ASE and NLOEs while retaining the primary fiber benefits of low SWaP, good BQ, and overall ruggedness and reliability. Achieving such performance in fiber is generally viewed as challenging as it requires containment of amplified spontaneous emission (ASE) and mitigation of in-fiber nonlinear optical effects (NLOEs).…”
Section: Introductionmentioning
confidence: 99%
“…Phase control is a key technique in CBC, which aims to compensate phase errors and achieve the phase locking of the combined lasers. According to the method of phase information detecting, active phase-control techniques can be divided into two categories [1]: direct phase-locking techniques such as the heterodyne detection phase-control technique [2,3], shearing interferometer method [4], and Hänsch-Couillaud detector method [5,6]; and indirect phaselocking techniques such as the stochastic parallel gradient descent algorithm [7][8][9][10] and single/multi-frequency dithering techniques [11][12][13][14][15][16][17][18].…”
mentioning
confidence: 99%