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Quantum Electronics

Nonlinear absorption in a Cr4+: Gd2SiO5crystal subjected to picosecond excitation

Konstantin V. Yumashev, Н. В. Кулешов, V. P. Mikhailov, V. G. Shcherbitskii, Pavel V. Prokoshin, S P Zhmako, B. I. Minkov

Published Jul 31, 1995• 4 citations
Publisher

Abstract

The optical absorption, temperature dependences of the luminescence intensity and decay time, and the transient absorption spectra of a Cr 4+ : Gd 2 SiO 5 crystal were determined by the picosecond excitation and probing method. An analysis of the results showed that the induced absorption observed in the 600–650 nm range was due to 3 T 2 ( 3 F ) → 3 T 1 ( 3 P ) transitions from the excited state. The lifetimes of the 3 T 2 ( 3 F ) and 3 T 1 ( 3 F ) levels were estimated to be 15 ns and 12 ps, respectively. The cross section for absorption from the first excited state at the wavelength of 616 nm was (1.1 ± 0.6)×10 -18 cm 2 and that for absorption from the ground state at λ = 540 nm was (2.2 ± 1.1)×10 -18 cm 2 .

DOI
10.1070/qe1995v025n07abeh000431

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The optical absorption, temperature dependences of the luminescence intensity and decay time, and the transient absorption spectra of a Cr 4+ : Gd 2 SiO 5 crystal were determined by the picosecond excitation and probing method. An analysis of the results showed that the induced absorption observed in the 600–650 nm range was due to 3 T 2 ( 3 F ) → 3 T 1 ( 3 P ) transitions from the excited state. The lifetimes of the 3 T 2 ( 3 F ) and 3 T 1 ( 3 F ) levels were estimated to be 15 ns and 12 ps, respectively. The cross section for absorption from the first excited state at the wavelength of 616 nm was (1.1 ± 0.6)×10 -18 cm 2 and that for absorption from the ground state at λ = 540 nm was (2.2 ± 1.1)×10 -18 cm 2 .
An experimental study of saturable absorption and excited-state absorption (ESA) in several inorganic saturable absorbers, Cr/sup 4+/:YAG, Cr/sup 4+/:GGG, and Cr/sup 4+/:YSGG, is presented. We provide the theoretical background of absorption characteristics in saturable absorbers that exhibit ESA, with some new results: approximate analytical solutions are proposed for the optical transmission in the case of a slow absorber, and for various light intensity conditions of spatially or temporally Gaussian beams in fast and slow absorbers. Experimentally, partial bleaching of the first excited state itself could be observed in Cr/sup 4+/:YAG at /spl lambda/=1064 nm, yielding the higher excited-state lifetime as /spl tau/*=(0.55/spl plusmn/0.1) ns. The regular transmission bleaching curve was measured in Cr/sup 4+/:GGG, for the first time in this material, yielding /spl sigma//sub ga/=(58/spl plusmn/5)/spl times/10/sup -1/ cm/sup 2/, and /spl sigma/e/sub s/=(13/spl plusmn/2)/spl times/10/sup -19/ cm/sup 2/ at /spl lambda/=1064 nm, ESA spectra were measured for the three materials between /spl sim/700 and 900 nm. All three exhibit crossing between saturable absorption at longer wavelengths and inverse saturable absorption at shorter wavelengths.
An investigation was made of the absorption spectrum of Cr 3+ ions in the ground ( 4 A 2 ) and metastable ( 2 E) states, and of the luminescence spectrum of the same ions in Y 3 Al 5 O 12 crystals at 300 and 77°K. The effective absorption cross sections were determined for the 4 A 2 state. The luminescence deexcitation time was found to be 1.5 and 9 msec at 300 and 77°K, respectively. The absorption spectrum of the 2 E state had four wide absorption bands with maxima at 16,700, 23,300, 28,600, and 40,500 cm –1 . The theoretical energy level scheme of Cr 3+ was calculated for Dq = 1725 cm –1 , G = 640 cm –1 , C = 3200 cm –1 , v = 495 cm –1 , and v' = 259 cm –1 , making an allowance for the mixing of the Γ trig S states. The experimentally observed absorption bands were attributed to specific transitions and the theoretical and experimental intensities were compared.
Abstract Excited state absorption (ESA) by Ce3+ ions in the 5d1 lowest excited state in Ce‐doped CaGa2S4 single crystal was investigated by nanosecond two‐pulse pump‐CW probe spectroscopy. The first pump pulse of 425 nm excited the 4f ground state electron to the 5d1 first excited state and the second pump pulse of 589 nm was introduced at 13 ns after the first pump in order to selectively excite the 5d1 state. Transient intensity change of the CW probe of a diode laser of 780 nm was observed. Temporal behavior of photoluminescence intensity by the 5d1 to 4f state transition was also observed under excitation of the same two‐pulse pump. The experimental results can be explained by the model of site‐dependent excited state absorption. The photoluminescence is generated from the 5d1 states of Ce3+ at two sites with different decay time, whereas the excited state absorption takes place mainly from Ce3+ at one site as well as metastable Ce2+. The model predicts that optical gain by the 5d1 to 4f transition can be achieved by Ce3+ at the other site if the populations at both the 5d1 state of Ce3+ at the site resulting in ESA and Ce2+ can be bleached by simultaneous secondary optical pumping with an IR (e.g. Nd:YAG) laser. (© 2013 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)
The differential absorption spectra of an V 3+ :Y 3 Al 5 O 12 crystal were investigated by a picosecond pump-and-probe method. An analysis of the results led to the conclusion that the induced absorption bands observed in the 850–890 and 650–770 nm ranges were due to, respectively, the 1 E ( 1 D )→ 1 T 1 ( 1 G ) and 1 E ( 1 D )→ 1 E ( 1 G ), 1 T 2 ( 1 G ) transitions in a tetrahedrally coordinated V 3+ ion. The lifetime of the 1 E ( 1 D ) level was estimated to be ~ 130 ps. Bleaching of the 3 A 2 → 3 T 1 ( 3 P ) absorption band of the tetrahedral V 3+ ion was also observed.