chromium-doped laser gain media (original) (raw)
Definition: laser gain media doped with chromium ions
Categories:
optical materials,
laser devices and laser physics
- laser gain media
- transition-metal-doped laser gain media
* chromium-doped laser gain media
* titanium-doped laser gain media
* iron-doped laser gain media
- transition-metal-doped laser gain media
Related: laser gain mediatransition-metal-doped laser gain mediaruby lasersvibronic lasersalexandrite lasers
Page views in 12 months: 536
DOI: 10.61835/ykb Cite the article: BibTex BibLaTex plain textHTML Link to this page! LinkedIn
Content quality and neutrality are maintained according to our editorial policy.
đŠ For purchasing chromium-doped laser gain media, use the RP Photonics Buyer's Guide â an expert-curated directory for finding all relevant suppliers, which also offers advanced purchasing assistance.
Contents
Chromium (chemical symbol: Cr) is a chemical element belonging to the group of transition metals. Chromium ions of different charge states (2+, 3+, 4+) are used as laser-active dopants of laser gain media:
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 ÎŒm and are typically pumped around 1.5â1.9 ÎŒm. Despite this huge emission bandwidth (for which such media are sometimes called âthe Ti:sapphire of the infraredâ), 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 [28].
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), typically emitting around 0.8â0.9 ÎŒm. (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 titaniumâsapphire 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 ÎŒm (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. â 1.35â1.65 ÎŒm for Cr4+:YAG and 1.1â1.37 ÎŒm 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.
Due to the strong electronâphonon interaction in such gain media, chromium-doped lasers are called vibronic lasers and have a large gain bandwidth.
Note that some chromium-doped crystals, in particular Cr4+:YAG, are also used as saturable absorbers in Q-switched lasers.
Frequently Asked Questions
This FAQ section was generated with AI based on the article content and has been reviewed by the articleâs author (RP).
What are chromium-doped laser gain media?
They are materials, typically crystals, where chromium ions with different charge states (Cr2+, Cr3+, or Cr4+) are added as the laser-active dopant, enabling light amplification.
Why do chromium-doped lasers typically have a broad gain bandwidth?
They are vibronic lasers, meaning there is a strong interaction between the electrons of the chromium ions and the vibrations of the host crystal lattice (phonons). This interaction broadens the energy levels, resulting in a large gain bandwidth.
What are Cr2+-doped crystals like Cr:ZnSe used for?
Cr2+-doped crystals are used to build lasers emitting in the mid-infrared spectral range, typically between 1.9 and 3.5 ”m. Their exceptionally large bandwidth allows for wide wavelength tuning and the generation of ultrashort pulses.
Which Cr3+-doped media are common, and for what applications?
Historically important media are ruby and alexandrite. Modern media like Cr:LiSAF are used for diode-pumped lasers that generate femtosecond pulses in the 0.8â0.9 ”m wavelength region.
What are the primary uses of Cr4+-doped crystals in lasers?
Cr4+-doped crystals like Cr4+:YAG or forsterite serve as gain media for lasers in the 1.1 to 1.65 ”m range. Additionally, Cr4+:YAG is widely used as a saturable absorber for passive Q-switching of other lasers.
Suppliers
Bibliography
| [1] | T. H. Maiman, âStimulated optical radiation in rubyâ, Nature 187, 194 (1960); doi:10.1038/187493a0 |
|---|---|
| [2] | R. J. Collins et al., âCoherence, narrowing, directionality, and relaxation oscillations in the light emission from rubyâ, Phys. Rev. Lett. 5 (7), 303 (1960); doi:10.1103/PhysRevLett.5.303 |
| [3] | D. Roess, âAnalysis of room temperature CW ruby lasersâ, IEEE J. Quantum Electron. 2 (4), 208 (1966); doi:10.1109/JQE.1966.1073937 |
| [4] | J. Walling et al., âTunable CW alexandrite laserâ, IEEE J. Quantum Electron. 16 (2), 120 (1980); doi:10.1109/JQE.1980.1070451 |
| [5] | J. Walling et al., âTunable alexandrite lasers: Development and performanceâ, JSTQE 21 (10), 1568 (1985); doi:10.1109/JQE.1985.1072544 |
| [6] | V. PetriveviÄ et al., âLaser action in chromium-doped forsteriteâ, Appl. Phys. Lett. 52, 1040 (1988); doi:10.1063/1.99203 |
| [7] | S. A. Payne et al., âLiCaAlF6:Cr3+: a promising new solid-state laser materialâ, IEEE J. Quantum Electron. 24 (11), 2243 (1988); doi:10.1109/3.8567 |
| [8] | S. A. Payne et al., âOptical spectroscopy of the new laser materials, LiSrAlF6:Cr3+ and LiCaAlF6:Cr3+â, J. Lumin. 44, 167 (1989); doi:10.1016/0022-2313(89)90052-5 |
| [9] | R. Scheps, âCr-doped solid-state lasers pumped by visible laser diodesâ, Opt. Mater. 1, 1 (1992); doi:10.1016/0925-3467(92)90011-B |
| [10] | M. J. P. Dymott et al., âAll-solid-state actively mode-locked Cr:LiSAF laserâ, Opt. Lett. 19 (9), 634 (1994); doi:10.1364/OL.19.000634 |
| [11] | Cr. R. Pollock et al., âCr4+ lasers: present performance and prospects for new host latticesâ, IEEE Sel. Top. Quantum Electron. 1 (1), 62 (1995); doi:10.1109/2944.468370 |
| [12] | D. Kopf et al., â1.1-W cw Cr:LiSAF laser pumped by a 1-cm diode arrayâ, Opt. Lett. 22 (2), 99 (1997); doi:10.1364/OL.22.000099 |
| [13] | R. H. Page et al., âCr2+-doped zinc chalcogenides as efficient, widely tunable mid-infrared lasersâ, IEEE J. Quantum Electron. 33 (4), 609 (1997); doi:10.1109/3.563390 |
| [14] | D. Kopf et al., âHigh-average-power diode-pumped femtosecond Cr:LiSAF lasersâ, Appl. Phys. B 65, 235 (1997); doi:10.1007/s003400050269 |
| [15] | J. M. Hopkins et al., âEfficient, low-noise, SESAM-based femtosecond Cr3+:LiSrAlF6 laserâ, Opt. Commun. 154, 54 (1998); doi:10.1016/S0030-4018(98)00312-5 |
| [16] | T. J. Carrig et al., âMode-locked Cr2+:ZnSe laserâ, Opt. Lett. 25 (3), 168 (2000); doi:10.1364/OL.25.000168 |
| [17] | D. J. Ripin et al., âGeneration of 20-fs pulses by a prismless Cr4+:YAG laserâ, Opt. Lett. 27 (1), 61 (2002); doi:10.1364/OL.27.000061 |
| [18] | P. Wagenblast et al., âDiode-pumped 10-fs Cr3+:LiCAF laserâ, Opt. Lett. 28 (18), 1713 (2003); doi:10.1364/OL.28.001713 |
| [19] | A. Isemann and C. Fallnich, âHigh-power colquiriite lasers with high slope efficiencies pumped by broad-area laser diodesâ, Opt. Express 11 (3), 259 (2003); doi:10.1364/OE.11.000259 |
| [20] | E. Sorokin et al., âUltrabroadband infrared solid-state lasersâ, JSTQE 11 (3), 690 (2005) (a review mainly concerning Cr2+ and Cr4+ lasers) |
| [21] | M. Sharonov et al., âNear-infrared laser operation of Cr3+ centers in chromium-doped LiInGeO4 and LiScGeO4 crystalsâ, Opt. Lett. 30 (8), 851 (2005); doi:10.1364/OL.30.000851 |
| [22] | U. Demirbas and A. Sennaroglu, âIntracavity-pumped Cr2+:ZnSe laser with ultrabroad tuning range between 1880 and 3100 nmâ, Opt. Lett. 31 (15), 2293 (2006); doi:10.1364/OL.31.002293 |
| [23] | M. Sharonov et al., âContinuous tunable laser operation in both the 1.31 and 1.55 ÎŒm telecommunication windows in LiIn(Si/Ge)O4 olivines doped with trivalent chromiumâ, Opt. Lett. 32 (24), 3489 (2007); doi:10.1364/OL.32.003489 |
| [24] | S. B. Mirov et al., âRecent progress in transition-metal-doped IIâVI mid-IR lasersâ, JSTQE 13 (3), 810 (2007); doi:10.1109/JSTQE.2007.896634 |
| [25] | A. Fuerbach et al., âDirect diode-pumped laser operation of Cr3+- doped LiInGeO4 crystalsâ, Opt. Express 15 (24), 16097 (2007); doi:10.1364/OE.15.016097 |
| [26] | U. Demirbas et al., âHighly efficient, low-cost femtosecond Cr3+:LiCAF laser pumped by single-mode diodesâ, Opt. Lett. 33 (6), 590 (2008); doi:10.1364/OL.33.000590 |
| [27] | S. Mirov et al., âProgress in Cr2+ and Fe2+ doped mid-IR laser materialsâ, Laser & Photon. Rev. 4 (1), 21 (2010); doi:10.1364/OME.1.000898 |
| [28] | N. Nagl et al., âDirectly diode-pumped, Kerr-lens mode-locked, few-cycle Cr:ZnSe oscillatorâ, Opt. Express 27 (17), 24445 (2019); doi:10.1364/OE.27.024445 |
| [29] | U. Demirbas, âCr:Colquiriite Lasers: Current status and challenges for further progressâ, Progress in Quantum Electronics 68, 100227 (2019); doi:10.1016/j.pquantelec.2019.100227 |
| [30] | A. Sennaroglu and Y. Morova, âDivalent (Cr2+), trivalent (Cr3+), and tetravalent (Cr4+) chromium ion-doped tunable solid-state lasers operating in the near and mid-infrared spectral regionsâ, Appl. Phys. B 128, 9 (2022); doi:10.1007/s00340-021-07735-1 |
(Suggest additional literature!)
Questions and Comments from Users
Here you can submit questions and comments. As far as they get accepted by the author, they will appear above this paragraph together with the authorâs answer. The author will decide on acceptance based on certain criteria. Essentially, the issue must be of sufficiently broad interest.
Please do not enter personal data here. (See also our privacy declaration.) If you wish to receive personal feedback or consultancy from the author, please contact him, e.g. via e-mail.
By submitting the information, you give your consent to the potential publication of your inputs on our website according to our rules. (If you later retract your consent, we will delete those inputs.) As your inputs are first reviewed by the author, they may be published with some delay.