2004
DOI: 10.1109/lpt.2003.823103
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High-Energy Femtosecond Pulses From an Ytterbium-Doped Fiber Laser With a New Cavity Design

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Cited by 17 publications
(9 citation statements)
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“…3 A laser based on double-clad Yb fiber produced 11.8 nJ chirped pulses (110 mW average power), which were dechirped to 200 fs outside the laser. 4 This laser contained two pairs of diffraction gratings in the cavity along with an acousto-optic modulator to initiate mode locking. Much of the laser cavity is actually not fiber; the unguided propagation and low efficiency of this laser naturally counter some of the main benefits of fiber sources.…”
mentioning
confidence: 99%
“…3 A laser based on double-clad Yb fiber produced 11.8 nJ chirped pulses (110 mW average power), which were dechirped to 200 fs outside the laser. 4 This laser contained two pairs of diffraction gratings in the cavity along with an acousto-optic modulator to initiate mode locking. Much of the laser cavity is actually not fiber; the unguided propagation and low efficiency of this laser naturally counter some of the main benefits of fiber sources.…”
mentioning
confidence: 99%
“…In particular, with small net positive cavity dispersion, the pulse energy is larger than that produced in the soliton regime. Stretched pulse lasers with output energies from tens of picojoules to some nanojoules have been reported [18][19][20][21][22] before nonlinearity provokes instabilities. However, under certain circumstances nonlinearity can be advantageous.…”
Section: Compact All-fiber Femtosecond Mode-locked Lasersmentioning
confidence: 99%
“…The pulse width experiences large variations per cavity round trip, with a change in the chirp sign. Stretched-pulse lasers with output energies from tens of picojoules to some nanojoules have been reported [12][13][14]. The most fundamental limitation to pulse energy in a fiber oscillator arises from wave-breaking phenomena because of large nonlinearities.…”
Section: Pulse Shape For Normal Dispersionmentioning
confidence: 99%