Saturated absorption and reverse saturated absorption of Cu:SiO2 at λ = 532 nm. Ganeev, R. A, Ryasnyansky, A. I, Stepanov, A. L, & Usmanov, T. physica status solidi (b), 241(3):R1--R4, March, 2004.
Saturated absorption and reverse saturated absorption of Cu:SiO2 at λ = 532 nm [link]Paper  doi  abstract   bibtex   
Nonlinear absorption in copper-doped silicate glasses was investigated by the Z-scan technique using second harmonic radiation of a Nd:YAG laser (λ = 532 nm, τ = 55 ps). The simultaneous influence of saturated and reverse saturated nonlinear absorption processes was analyzed. The nonlinear absorption coefficient and the saturation intensity of copper-doped glasses at laser intensity of 5.4 × 109 W cm−2 were measured to be 6 × 10−6 cm W−1 and 4.3 × 108 W cm−2, respectively. (© 2004 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)
@article{ganeev_saturated_2004,
	title = {Saturated absorption and reverse saturated absorption of {Cu}:{SiO}2 at λ = 532 nm},
	volume = {241},
	issn = {1521-3951},
	shorttitle = {Saturated absorption and reverse saturated absorption of {Cu}},
	url = {http://onlinelibrary.wiley.com/doi/10.1002/pssb.200309025/abstract},
	doi = {10.1002/pssb.200309025},
	abstract = {Nonlinear absorption in copper-doped silicate glasses was investigated by the Z-scan technique using second harmonic radiation of a Nd:YAG laser (λ = 532 nm, τ = 55 ps). The simultaneous influence of saturated and reverse saturated nonlinear absorption processes was analyzed. The nonlinear absorption coefficient and the saturation intensity of copper-doped glasses at laser intensity of 5.4 × 109 W cm−2 were measured to be 6 × 10−6 cm W−1 and 4.3 × 108 W cm−2, respectively. (© 2004 WILEY-VCH Verlag GmbH \& Co. KGaA, Weinheim)},
	language = {en},
	number = {3},
	urldate = {2011-11-11TZ},
	journal = {physica status solidi (b)},
	author = {Ganeev, R. A and Ryasnyansky, A. I and Stepanov, A. L and Usmanov, T.},
	month = mar,
	year = {2004},
	keywords = {42.65.An, 42.70 Jk, 78.20.Ci},
	pages = {R1--R4}
}
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