Temporal-space-transforming pulse-shaping system with a knife-edge apparatus for a high-energy laser facility

For the first time to our knowledge, in a high-energy laser facility with an output energy of 454.37 J, by using a temporal-space-transforming pulse-shaping system with our own design of a knife-edge apparatus, we obtained a quasi-square laser pulse. (c) 2005 Optical Society of America.

Fabricación y reparación de geometrías complejas mediante aporte por laser.

El láser cladding es una tecnología en alza. Mediante la energía de una radiación láser, se crea un baño fundido de material que, combinado con la inyección de material en polvo a través de una boquilla y controlando el movimiento a través de la programación de una plataforma cinemática, ofrece la posibilidad de fabricar una geometría determinada mediante la adición de material. Se trata, sin embargo, de un proceso complejo en el que intervienen gran cantidad de fenómenos físicos y resulta complicado obtener un buen resultado en trayectorias complejas. En el presente trabajo se ha tratado el proceso de fabricación de una geometría compleja tipo álabe de turbina. Para ello, se ha comenzado por llevar a cabo una revisión bibliográfica, posteriormente, se han llevado a cabo una serie de ensayos experimentales para la determinación de parámetros de proceso, y finalmente, se ha desarrollado una estrategia de aporte original para estructuras tipo álabe que permite garantizar la estabilidad del proceso. En base a los resultados satisfactorios obtenidos, se ha concluido que mediante la aplicación de la nueva estrategia es posible la generación de geometrías complejas con alto grado de estabilidad.

Single mode Er-doped pi-phase-shifted distributed feedback fibre grating laser

A novel method incorporating the shielded method and the post-processing method has been proposed to fabricate the pi-phase-shilted fibre grating. Then an Er-doped pi-phase-shifted distributed feedback fibre grating laser has been fabricated using the grating. The laser threshold is 20 mW. When pumped with 90 mW light at 980 nm, the laser gives an output of 1.1 mW. Its signal-to-noise ratio is better than 60 dB. It is demonstrated that the laser is single mode operation by means of a Fabry-Perot scanning interferometer.

Fields of apertured polychromatic laser beams with Gaussian and Hermite-Gaussian transverse modes

Starting from the Huygens-Fresnel diffraction integral, the field expressions of apertured polychromatic laser beams with Gaussian and Hermite-Gaussian transverse modes are derived. Influence of the bandwidth on the intensity distributions of the laser beams is analyzed. It is found that when the bandwidth increases, the amplitudes and numbers of the intensity spikes decrease and beam uniformity is improved in the near field and the width of transverse intensity distribution of the apertured beams decreases in the far field. Thus, the smoothing and narrowing effects can be achieved by increasing the bandwidth. Also, these effects are found in the laser beams with Hermite-Gaussian transverse modes as the bandwidth increases.(c) 2006 Elsevier Ltd. All rights reserved.

Smoothing the side lobes of a focused pattern by spectral dispersion in the broadband laser

Starting from the Huygens-Fresnel diffraction integral, the propagation equations of a broadband laser passing through a dispersive lens and a dispersive wedge are derived. Smoothing effect on the side lobes of the focused pattern is achieved as the broadband laser passes through the lens because of the spectral dispersion of the lens. By inserting a dispersive wedge behind the lens, better smoothing effect is realized because a relative position shift between focused patterns of different frequency components is generated due to the spectral dispersion of the wedge. Smoothing effect on the side lobe is obtained even with small bandwidth of the broadband laser as the wedge is used. (c) 2006 Elsevier GmbH. All rights reserved.