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1.
Opt Lett ; 42(4): 683-686, 2017 Feb 15.
Artigo em Inglês | MEDLINE | ID: mdl-28198839

RESUMO

We report on the parametric generation of 100 fs sub-6-cycle 40 µJ pulses with the center wavelength at 5.2 µm using a 1 ps 2.1 µm pump laser and a dispersion management scheme based on bulk material. Our optically synchronized amplifier chain consists of a Ho:YAG chirped-pulse amplifier and white-light-seeded optical parametric amplifiers providing simultaneous passive carrier-envelope phase locking of three ultrashort longwave pulses at the pump, signal, and idler wavelengths corresponding, respectively, to 2.1, 3.5, and 5.2 µm. We also demonstrate bandwidth enhancement and efficient control over nonlinear spectral phase in the regime of cascaded χ2 nonlinearity in ZnGeP2.

2.
Nature ; 537(7618): 84-88, 2016 09 01.
Artigo em Inglês | MEDLINE | ID: mdl-27409814

RESUMO

The use of femtosecond laser pulses allows precise and thermal-damage-free removal of material (ablation) with wide-ranging scientific, medical and industrial applications. However, its potential is limited by the low speeds at which material can be removed and the complexity of the associated laser technology. The complexity of the laser design arises from the need to overcome the high pulse energy threshold for efficient ablation. However, the use of more powerful lasers to increase the ablation rate results in unwanted effects such as shielding, saturation and collateral damage from heat accumulation at higher laser powers. Here we circumvent this limitation by exploiting ablation cooling, in analogy to a technique routinely used in aerospace engineering. We apply ultrafast successions (bursts) of laser pulses to ablate the target material before the residual heat deposited by previous pulses diffuses away from the processing region. Proof-of-principle experiments on various substrates demonstrate that extremely high repetition rates, which make ablation cooling possible, reduce the laser pulse energies needed for ablation and increase the efficiency of the removal process by an order of magnitude over previously used laser parameters. We also demonstrate the removal of brain tissue at two cubic millimetres per minute and dentine at three cubic millimetres per minute without any thermal damage to the bulk.


Assuntos
Temperatura Baixa , Temperatura Alta , Terapia a Laser/efeitos adversos , Terapia a Laser/métodos , Lasers/efeitos adversos , Animais , Encéfalo/cirurgia , Bovinos , Córnea/cirurgia , Dentina/cirurgia , Humanos , Terapia a Laser/instrumentação , Ratos , Fatores de Tempo
3.
Opt Lett ; 41(15): 3435-8, 2016 Aug 01.
Artigo em Inglês | MEDLINE | ID: mdl-27472587

RESUMO

We demonstrate an experimental technique for both transverse and longitudinal characterization of bunched femtosecond free electron beams. The operation principle is based on monitoring of the current of electrons that obtained an energy gain during the interaction with the synchronized optical near-field wave excited by femtosecond laser pulses. The synchronous accelerating/decelerating fields confined to the surface of a silicon nanostructure are characterized using a highly focused sub-relativistic electron beam. Here the transverse spatial resolution of 450 nm and femtosecond temporal resolution of 480 fs (sub-optical-cycle temporal regime is briefly discussed) achievable by this technique are demonstrated.

4.
Opt Lett ; 41(5): 930-3, 2016 Mar 01.
Artigo em Inglês | MEDLINE | ID: mdl-26974083

RESUMO

We present a concept of a white-light-seeded-cascaded mid-infrared (mid-IR) optical parametric amplifier (OPA) based on potassium titanyl arsenate and zinc germanium phosphate nonlinear optical crystals and producing 100-µJ level pulses centered at 5300 nm, with the spectrum supporting four-optical-cycle pulse duration. The OPA is pumped by 2090-nm master oscillator/power amplifier based on a Tm,Ho-fiber laser seeder and a Ho:YAG regenerative amplifier delivering 3.8-mJ sub-ps pulses at a repetition rate of 1 kHz. We validate that output parameters of the OPA are scalable by means of increasing the pulse energy, decreasing the pulse duration and redshifting the central wavelength.


Assuntos
Arseniatos , Hólmio , Raios Infravermelhos , Lasers de Estado Sólido , Fenômenos Ópticos , Fosfatos , Túlio
5.
Opt Lett ; 40(15): 3520-3, 2015 Aug 01.
Artigo em Inglês | MEDLINE | ID: mdl-26258347

RESUMO

We report on a compact all-polarization-maintaining 2.05-µm chirped pulse fiber amplifier system emitting pulses at up to 1-MW peak power level at 371-fs pulse duration. The seed pulse repetition rate provided by an inhouse-built oscillator is reduced to around 1 MHz using a pulse picker. In combination with a two stage fiber amplifier, output pulse energies up to 570 nJ are obtained without the need of a high-power large-mode area amplifier. Both temporal stretching and compression of the chirped pulse amplifier design are achieved using a single chirped volume Bragg grating.

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