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Direct generation of optical bottle beams from a tightly focused end-pumped solid-state laser

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Abstract

We demonstrate that various optical bottle beams can be directly generated from a tightly focused end-pumped Nd:YVO4 laser. By controlling the size of pump beam and intracavity aperture in a planoconcave cavity, we obtain well contrasting optical bottles with semiconfocal, 1/3-, and 1/5-degenerate cavity configurations. These beams result, respectively, from the superposition of the fundamental mode and the corresponding lowest degenerate transverse eigenmode, which is in-phase at their beam waists. Unlike that of our previous simulation model, this new observation is universal; it is suitable for any kind of gain media in tightly end-pumped lasers.

©2004 Optical Society of America

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Figures (4)

Fig. 1.
Fig. 1. Intensity patterns and their corresponding three-dimensional profiles. (a) Out-of-phase summing up LG00 and LG20 modes at beam waist, (b–d) in-phase adding LG00 and LG20, LG00 and LG30, as well as LG00 and LG50 modes, where W0 is the beam waist, and zR is the Rayleigh length.
Fig. 2.
Fig. 2. Radial intensity patterns of the optical bottle generated from a laser operated with the 1/4-degenerate cavity at various distances from the transform lens, which is indicated above the photographs, where zR is the Rayleigh range.
Fig. 3.
Fig. 3. Calculated radial intensity distributions and the experimentally observed beam profiles. The calculated transverse profile of LG00+LG20 is at z=zR and of LG00+LG30 at z=zR/√3 that correspond to the photographs taken at 1/4 and 1/3 degeneracy, respectively.
Fig. 4.
Fig. 4. Depth of optical bottle versus different pumping size and corresponding calculated profiles at 1/5 degeneracy. The CCD images in (a–c) are the beam patterns when the laser is operated with pump size of 30 μm, 20 μm, and 15 μm, respectively. (d) The calculated profile of LG00+LG20 is at z=0.324 zR.
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