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Extra resources for Modern Aspects of Bulk Crystal, Thin Film Prep.
2005). Femtosecond pulse generation with a diodepumped Yb3+:YVO4 laser. 10, pp. 1150-1152, ISSN 0146-9592 Krupke W. (2000). Ytterbium solid-state lasers-the first decade. 6, pp. , Sandrock T. & Huber G. (1997). Spectroscopy, excited-state absorption and stimulated emission in Pr3+-doped Gd2SiO5 and Y2SiO5 crystals. 1, pp. , Aggarwal, R. & Fan T. (1991). Room-temperature diodepumped Yb:YAG laser. , Su L. & Xu J. (2007). Diodepumped Yb:GSO femtosecond laser. 5, pp. , Su L. & Xu J. (2006). Efficient diodepumped Yb:Gd2SiO5 laser.
Speiser J. (2007). Fifteen Years of Work on Thin-Disk Lasers: Results and Scaling Laws. , Petermann K. & Peters V. (2004). Passively mode-locked Yb:Lu2O3 laser. 14, pp. , Thomas J. (2001). Lu2SiO5 by singlecrystal X-ray and neutron diffraction. 6, pp. , Viana B. & Vivien D. (2002). Determination of laser parameters of ytterbium-doped oxide crystalline materials. 10, pp. 2365-2375. , (2001). 1-2, pp. 358-362, ISSN 0168-9002 Keller U. (2003). Recent developments in compact ultrafast lasers. 6950, pp.
The emission bandwidth FWHM of Yb:LSO crystal is appropriately 73nm which is much larger than that of Yb:YSO and Yb:GSO crystal. Although Yb:LSO possessed the largest σem around 1004nm, 34 Modern Aspects of Bulk Crystal and Thin Film Preparation the reabsorption losses was consequently strong which would detrimentally affect laser action. 4×10-21 cm2 containing the smallest thermal populating as well as the least re-absorption losses. In the case of 1032nm, the emission cross section is large enough to obtain low threshold and high efficient laser operation.