2010
DOI: 10.1364/ol.35.002052
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Power scaling of a high-repetition-rate enhancement cavity

Abstract: A passive optical resonator is used to enhance the power of a pulsed 78 MHz repetition rate Yb laser providing 200 fs pulses. We find limitations relating to the achievable time-averaged and peak power, which we distinguish by varying the duration of the input pulses. An intracavity average power of 18 kW is generated with close to Fourier-limited pulses of 10 W average power. Beyond this power level, intensity-related effects lead to resonator instabilities, which can be removed by chirping the seed laser pul… Show more

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Cited by 91 publications
(54 citation statements)
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“…Potential intensity-related limitations are mitigated due to the long pulse durations of the stretched CPA pulses, which, in principle, should allow for much higher pulse energies in a loaded cavity than fs-or ps-pulses did in the past. 30 A schematic drawing of the basic concept is depicted in Figure 1a. For their temporal stacking, the pulses are coupled into a cavity with a length corresponding to the repetition rate f rep of the incident pulse train, which is typically on the order of 10 MHz.…”
Section: Methodsmentioning
confidence: 99%
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“…Potential intensity-related limitations are mitigated due to the long pulse durations of the stretched CPA pulses, which, in principle, should allow for much higher pulse energies in a loaded cavity than fs-or ps-pulses did in the past. 30 A schematic drawing of the basic concept is depicted in Figure 1a. For their temporal stacking, the pulses are coupled into a cavity with a length corresponding to the repetition rate f rep of the incident pulse train, which is typically on the order of 10 MHz.…”
Section: Methodsmentioning
confidence: 99%
“…Steady-state is reached when the energy coupled to the cavity balances exactly the roundtrip losses L. Typically, a power enhancement of a few orders of magnitude can be achieved. 30,36 However, before this state is reached, in the SnD concept the intracavity pulse is coupled out via a switch faster than 1/f rep and at a switching rate f switch before the next stacking period begins, i.e., the cavity is operated in a non-steady-state regime.…”
Section: Methodsmentioning
confidence: 99%
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“…Optical damage is among the challenges towards scaling up the power of such systems. Moreover, their output is often intensified further in regenerative amplifiers [13], optical parametric amplification (OPA) stages [14], and inside enhancement cavities [15,16]. The latter can reach average intracavity power of several tens of kW, which is limited by the damage threshold of optical coatings [15,17].…”
Section: Introductionmentioning
confidence: 99%
“…Femtosecond ECs, seeded by Ti:Sa-based lasers were first demonstrated in 2005 [6,7]. More recently, advances in Yb-based fiber laser technology enabled reaching higher circulating powers in ECs [5,8], resulting in higher photon energies and higher XUV average powers. However, due to the narrower gain bandwidth of Yb-doped active materials, these systems operate with pulse durations significantly longer than 100 fs.…”
Section: Introductionmentioning
confidence: 99%