2022
DOI: 10.1109/lpt.2022.3196276
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All-Fiber Chirped-Pulse Amplifier Emitting 670 fs Pulses With 92 MW Peak Power

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Cited by 10 publications
(5 citation statements)
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“…However, it is better to study the operation of SGF amplifiers and SCF amplifiers at higher energy and average power levels. As recently, an all-fiber CPA system emiting140 µJ (61.8 µJ after compression of 670 fs) amplified pulse by using the amplifier with 21 cm intensively Yb-doped SGF which has a core diameter of just 14 µm is demonstrated [21], this result has exhibited the big potential of the SGF not only in higher energy pulse amplification but also in the high damage threshold. A large dispersionmanaged monolithic all-fiber chirped pulse amplification system by using SGF as main amplifier for high-energy femtosecond laser generation was also demonstrated, and a record pulse energy of 170 µJ with pulse durations of 781 fs was achieved [22].…”
Section: Resultsmentioning
confidence: 88%
“…However, it is better to study the operation of SGF amplifiers and SCF amplifiers at higher energy and average power levels. As recently, an all-fiber CPA system emiting140 µJ (61.8 µJ after compression of 670 fs) amplified pulse by using the amplifier with 21 cm intensively Yb-doped SGF which has a core diameter of just 14 µm is demonstrated [21], this result has exhibited the big potential of the SGF not only in higher energy pulse amplification but also in the high damage threshold. A large dispersionmanaged monolithic all-fiber chirped pulse amplification system by using SGF as main amplifier for high-energy femtosecond laser generation was also demonstrated, and a record pulse energy of 170 µJ with pulse durations of 781 fs was achieved [22].…”
Section: Resultsmentioning
confidence: 88%
“…In [9], there is a large pedestal in autocorrelation trace of the pulses, which we attribute to the presence of high-order modes (HOM). Similar amplifier design, but with a perfectly single-mode propagation regime, was demonstrated by our group in [10]. In this case, an input core diameter of an LMA tapered fiber was reduced down to 14 µm, which allowed us to achieve the first HOM cut-off of 0.95 µm relative to a Ge-doped pedestal surrounding the core.…”
Section: Introductionmentioning
confidence: 81%
“…Thus, the previously obtained absorption from the cla at the level of 24 dB/m and a wavelength of 976 nm can be increased only by usi design of fiber with a pedestal [12,29], which in turn actually excludes the possib creating a polarization-maintaining fiber. In addition, in the case of increasing abso from the cladding, the thermal load per unit length of the fiber increases significantl leads to a sharp decrease in the maximum average output power that can be ext from the amplifier based on such a fiber [29] and, as a consequence, significantly the scope of application of such amplifiers. Thus, the ytterbium concentration and ometric dimensions of the core and cladding of the tapered fiber used in [17,26] app be close to optimal.…”
Section: Tapered Fiber Designmentioning
confidence: 99%
“…In addition, in the case of increasing absorption from the cladding, the thermal load per unit length of the fiber increases significantly. This leads to a sharp decrease in the maximum average output power that can be extracted from the amplifier based on such a fiber [29] and, as a consequence, significantly limits the scope of application of such amplifiers. Thus, the ytterbium concentration and the geometric dimensions of the core and cladding of the tapered fiber used in [17,26] appear to be close to optimal.…”
Section: Tapered Fiber Designmentioning
confidence: 99%