Chromium-doped Gain Media
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Definition: laser gain media doped with chromium ions
German: chromdotierte Verstärkermedien
- Cr2+ ions are mostly used in zinc chalcogenides such as Cr2+:ZnS, Cr2+:ZnSe, Cr2+:ZnSxSe1−x, and Cr2+:CdSe. Lasers based on these crystals can emit roughly between 1.9 and 3.5 μm and are typically pumped around 1.5–1.9 μm. Despite this huge emission bandwidth, they can have reasonably low threshold pump powers and can be diode-pumped. It is possible to passively mode-lock such lasers for generating pulses with durations well below 100 fs.
- Cr3+ ions are the active ingredients of ruby (chromium-doped aluminum oxide), the laser medium of the first laser, and alexandrite (Cr3+:BeAl2O4), an early tunable solid-state laser medium. Cr3+ ions are now mostly used in gain media such as Cr3+:LiSrAlF6 (Cr:LiSAF), Cr3+:LiCaAlF6 (Cr:LiCAF) and Cr3+:LiSrGaF6 (Cr:LiSGAF), emitting around 0.8–0.9 μm. (Such crystals are called colquiriites.) Passively mode-locked lasers based on such media can be used for pulse durations down to roughly 10 fs. Compared with titanium–sapphire lasers, such lasers can be much cheaper, because they use a red rather than a green pump source and can be operated with low pump powers, so that diode pumping is feasible. However, the output powers achievable are lower (partly because of thermal quenching effects at higher temperatures), the wavelength tuning range is smaller, and the minimum pulse duration is larger. Some rather new materials are Cr3+:LiInGeO4 (Cr:LIGO), Cr3+:LiScGeO4, and Cr3+:LiInSiO4 (Cr:LISO) [21, 23, 25]. Here, Cr3+ ions emit in a surprisingly long wavelength range between about 1.2 and 1.6 μm (which is more typical for Cr4+) and with a very large bandwidth.
- Cr4+ ions occur in media such as Cr4+:YAG, Cr4+:MgSiO4 (forsterite) and other silicates, and also in germanates, apatites and other crystal types. The emission range is e.g. ≈ 1.35–1.65 μm for Cr4+:YAG and 1.1–1.37 μm for Cr4+:MgSiO4. Pulse durations below 20 fs have been achieved e.g. with Cr4+:MgSiO4. Nd:YAG lasers are often used for pumping such Cr4+ lasers.
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|||V. Petrivevic et al., “Laser action in chromium-doped forsterite”, Appl. Phys. Lett. 52, 1040 (1988)|
|||S. A. Payne et al., “LiCaAlF6:Cr3+: a promising new solid-state laser material”, IEEE J. Quantum Electron. 24 (11), 2243 (1988)|
|||S. A. Payne et al., “Optical spectroscopy of the new laser materials, LiSrAlF6:Cr3+ and LiCaAlF6:Cr3+”, J. Lumin. 44, 167 (1989)|
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|||M. J. P. Dymott et al., “All-solid-state actively mode-locked Cr:LiSAF laser”, Opt. Lett. 19 (9), 634 (1994)|
|||Cr. R. Pollock et al., “Cr4+ lasers: present performance and prospects for new host lattices”, IEEE Sel. Top. Quantum Electron. 1 (1), 62 (1995)|
|||D. Kopf et al., “1.1-W cw Cr:LiSAF laser pumped by a 1-cm diode array”, Opt. Lett. 22 (2), 99 (1997)|
|||R. H. Page et al., “Cr2+-doped zinc chalcogenides as efficient, widely tunable mid-infrared lasers”, IEEE J. Quantum Electron. 33 (4), 609 (1997)|
|||D. Kopf et al., “High-average-power diode-pumped femtosecond Cr:LiSAF lasers”, Appl. Phys. B 65, 235 (1997)|
|||J. M. Hopkins et al., “Efficient, low-noise, SESAM-based femtosecond Cr3+:LiSrAlF6 laser”, Opt. Commun. 154, 54 (1998)|
|||T. J. Carrig et al., “Mode-locked Cr2+:ZnSe laser”, Opt. Lett. 25 (3), 168 (2000)|
|||D. J. Ripin et al., “Generation of 20-fs pulses by a prismless Cr4+:YAG laser”, Opt. Lett. 27 (1), 61 (2002)|
|||P. Wagenblast et al., “Diode-pumped 10-fs Cr3+:LiCAF laser”, Opt. Lett. 28 (18), 1713 (2003)|
|||A. Isemann and C. Fallnich, “High-power colquiriite lasers with high slope efficiencies pumped by broad-area laser diodes”, Opt. Express 11 (3), 259 (2003)|
|||E. Sorokin et al., “Ultrabroadband infrared solid-state lasers”, IEEE J. Sel. Top. Quantum Electron. 11 (3), 690 () (a review mainly concerning Cr2+ and Cr4+ lasers)|
|||M. Sharonov et al., “Near-infrared laser operation of Cr3+ centers in chromium-doped LiInGeO4 and LiScGeO4 crystals”, Opt. Lett. 30 (8), 851 (2005)|
|||U. Demirbas and A. Sennaroglu, “Intracavity-pumped Cr2+:ZnSe laser with ultrabroad tuning range between 1880 and 3100 nm”, Opt. Lett. 31 (15), 2293 (2006)|
|||M. Sharonov et al., “Continuous tunable laser operation in both the 1.31 and 1.55 μm telecommunication windows in LiIn(Si/Ge)O4 olivines doped with trivalent chromium”, Opt. Lett. 32 (24), 3489 (2007)|
|||S. B. Mirov et al., “Recent progress in transition-metal-doped II–VI mid-IR lasers”, IEEE J. Sel. Top. Quantum Electron. 13 (3), 810 ()|
|||A. Fuerbach et al., “Direct diode-pumped laser operation of Cr3+- doped LiInGeO4 crystals”, Opt. Express 15 (24), 16097 (2007)|
|||U. Demirbas et al., “Highly efficient, low-cost femtosecond Cr3+:LiCAF laser pumped by single-mode diodes”, Opt. Lett. 33 (6), 590 (2008)|
|||S. Mirov et al., “Progress in Cr2+ and Fe2+ doped mid-IR laser materials”, Laser & Photon. Rev. 4 (1), 21 (2010)|
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