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The encyclopedia covers this topic well: with a long overview article on laser material processing and specialized articles on
A regenerative amplifier is a device which is used for strong amplification of light pulses, usually with ultrashort pulse durations in the picosecond or femtosecond domain (→ ultrafast amplifiers). Multiple passes through the laser gain medium (nearly always a solid-state medium) are achieved by placing the gain medium in an optical resonator, together with an optical switch, which is usually realized with an electro-optic modulator and a polarizer. The number of round trips in the resonator can be controlled with the optical switch, and it can be very large, so that a very high overall amplification factor (gain) is achieved.
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For some applications, it is important to keep the energy of any satellite pulses very low, i.e. to achieve a high pulse contrast. Such satellite pulses can occur in various ways, e.g. via imperfect switching of the Pockels cell or parasitic reflections in the amplifier. An additional pulse picker may be used to suppress pre- and post-pulses.
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The duration of the amplified pulses may be increased due to the limited gain bandwidth of the amplifier medium, which reduces the pulse bandwidth. This so-called gain narrowing effect may be reduced by inserting a properly designed spectral filter in the amplifier, which makes the net gain spectrum wider and more flat, but reduces the power conversion efficiency.
It is common to combine both approaches: a regenerative amplifier provides the high gain, and a final multipass amplifier stage boosts the energy (→ amplifier chains, ultrafast amplifiers).
This operation principle makes it possible to achieve very high gain and thus pulse energies in the millijoule range with amplifiers of moderate size, or even higher energies with larger devices. Typical pulse repetition rates are of the order of 1 kHz, although repetition rates of hundreds of kHz are sometimes possible. The highest pulse energies are achieved at lower repetition rates.
Note that the seed laser, normally a mode-locked laser, may have a much higher pulse repetition rate of e.g. 80 MHz; only a small number of the generated seed pulses is used by the amplifier. A separate pulse picker is in principle not required, since the regenerative amplifier itself can “pick” an input pulse when required, but one may want to improve the suppression of additional pulses.
Applications of regenerative amplifiers include laser material processing (e.g. cutting of metals with millijoule pulse energies) and scientific experiments e.g. in high-intensity physics, such as high harmonic generation.
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Regeneratively amplified picosecond lasers deliver high-energy pulses with durations < 30 ps and > 2 MW peak power at 1064 nm with variable repetition rates from single shot to 10 kHz. They feature a unique synchronization capability with unsurpassed 3.5 ps timing jitter for pulses on demand. Optional wavelengths at 532 nm, 355 nm and 266 nm are available collinearly or as multiple output beams. The power consumption is < 30 W. The air-cooling and compact design attribute to the competitive advantages. Numerous applications include micromachining of metal and non-metal materials, semiconductor wafer inspection, carving, nonlinear optics and ultrafast spectroscopy.
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At least in femtosecond devices, the chromatic dispersion introduced by the Pockels cell (in addition to that from the gain medium and other components) has to be carefully compensated. Nonlinear effects may also occur; these can be effectively suppressed with the methods of chirped-pulse amplification or divided-pulse amplification. If this is not done, the obtainable pulse energy may be limited by nonlinear effects or even optical damage phenomena.
Pulse injection and ejection require the use of a Pockels cell and a Pockels cell driver with a short switching time (well below the resonator round-trip time) and precision. These requirements are substantially more challenging than those for simple Q switching of a laser, for example.
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The power conversion efficiency of a regenerative amplifier can be severely reduced by the effect of intracavity losses (particularly in the electro-optic switch). Note that the sensitivity to such losses is particularly high in cases with low round-trip gain because this increases the number of resonator round trips required to achieve a certain overall amplification factor.
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For high repetition rates (e.g. tens of kilohertz or higher), the amplifier gain medium is usually pumped continuously. For lower repetition rates (particularly for pulse periods well above the upper-state lifetime), pulsed pumping (e.g. with a Q-switched laser) is preferable. A common configuration is to use a frequency-doubled YAG laser to pump a regenerative Ti:sapphire amplifier.
The software RP Fiber Power can be used for analyzing and optimizing regenerative amplifiers – not only based on fibers, but also with bulk laser crystals. As an example, see a case study.
A possible alternative to a regenerative amplifier is a multipass amplifier, where multiple passes (each time with a slightly different propagation direction) are arranged with a set of mirrors. That approach does not require a fast modulator, but becomes complicated (also in terms of alignment) if the number of passes through the gain medium is high.
As a rule of thumb, a multipass amplifier may be more appropriate for very high pulse energies if a limited gain is required ( because the input pulse energy is already relatively high), whereas a regenerative amplifier is more suitable for very high gains.
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Note that although a pulse makes multiple passes in a regenerative amplifier, the term multipass amplifier is often reserved for a device where a fixed number of passes is obtained – not with an optical switch, but just according to the geometric beam path. It would be more natural, though, to consider a regenerative amplifier as one type of multipass amplifier.
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Regenerative amplifiers can also have a reduced gain and power efficiency due to a finite lower-state lifetime, leading to a significant population in the lower laser level during amplification of a pulse, and thus to reabsorption on the laser transition. That problem occurs primarily in amplifiers for very short pulses, but not with chirped-pulse amplification, where the pulse duration within the amplifier is relatively large.
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Another technique for reaching high pulse energies, although not nearly as high as with regenerative amplifiers, is cavity dumping of a mode-locked laser. That technique is particularly suitable for very high pulse repetition rates of several megahertz.
Cite:M. N. Polyanskiy. Refractiveindex.info database of optical constants. Sci. Data 11, 94 (2024)https://doi.org/10.1038/s41597-023-02898-2
Book Air Au-Ag (Gold-silver alloy) Cu-Zn (Copper-zinc alloy, Brass) Nb-Sn (Niobium-tin alloy) Ni-Fe (Nickel-iron alloy, Permalloy) Pd-H (Palladium-hydrogen alloy, Palladium hydride) V-Ga (Vanadium-gallium alloy) V-H (Vanadium-hydrogen alloy, Vanadium hydride) Zr-H (Zirconium-hydrogen alloy, Zirconium hydride) AlAs-GaAs (Aluminium gallium arsenide, AlGaAs) AlSb-GaSb (Aluminium gallium antimonide, AlGaSb) AlN-Al2O3 (Aluminium oxynitride, ALON) GaAs-InAs (Gallium indium arsenide, GaInAs, InGaAs) GaP-InP (Gallium indium phosphide, GaInP) GaAs-InAs-GaP-InP (Gallium indium arsenide phosphide, GaInAsP) Si-Ge (Silicon-germanium, SiGe) AuAl2 (Gold-aluminium intermetallic, Purple plague) PtAl2 (Platinum-aluminium intermetallic) AgGaS2-AgInS2 HfO2-Y2O3 (Hafnium dioxide - Yttrium oxide) In2O3-SnO2 (Indium tin oxide, ITO) TlBr-TlCl (Thallium bromo-chloride, KRS-6) TlBr-TlI (Thallium bromo-iodide, KRS-5) ZnO-CdO (Zinc cadmium oxide, ZnCdO) ZrO2-Y2O3 (Yttria-stabilized zirconia, YSZ) Si:InP (Silicon-doped indium phosphide) Mg:LiTaO3 (Magnesium-doped lithium tantalate) Nb:RbTiOPO4 (Niobium-doped rubidium titanyl phosphate, Nb:RTP) Al:ZnO (Aluminium-doped zinc oxide, AZO) Si-O (Non-stoichiometric silicon oxide) Franckeite Hydrogenated amorphous carbon (C8H8)n-(C3H3N)m (Styrene-acrylonitrile, SAN) C6H4S4:C12H4N4 (Tetrathiafulvalene:tetracyanoquinodimethane, TTF:TCNQ) PTB7:PC71BM P3HT:PC61BM PEDOT:PSS PBDB-T:ITIC H2O:C3H5(OH)3 (Water:Glycerol) D2O:C3H5(OH)3 (Heavy water:Glycerol) Cu:C12H4N4 (Copper:tetracyanoquinodimethane, Cu:TCNQ ) Li:C12H4N4 (Lithium:tetracyanoquinodimethane, Li:TCNQ ) CR-39 EVASKY S87 EVASKY S88 Kapton NAS-21 Optorez 1330 Pharmacoat 606 (Hydroxypropyl methylcellulose, HPMC) Surlyn A-1601 Zeonex E48R 5CB (4-pentyl-4'-cyanobiphenyl) 5PCH (4-trans-pentylcyclohexylcyanobenzene) E7 E44 MLC-6241-000 MLC-6608 MLC-9200-000 MLC-9200-100 TL-216 Biodisel BK matching liquid Fused silica matching liquid Acrylic matching liquid Leica Type F Olympus IMMOIL-F30CC Sigma Aldrich M5904 Loctite 3526 Norland NOA 61 Norland NOA 170 Norland NOA 1348 Eukitt FluorSave Microchem 8.5 mEL copolymer resist Microchem 495 PMMA resist Microchem 950 PMMA resist Microchem SU-8 2000 Microchem SU-8 3000 Micro resist EpoClad Micro resist EpoCore Micro resist ma-N 405 : ma-T 1050, 1:1 Micro resist ma-N 1407 Nanoscribe IP-S Nanoscribe IP-Dip CH3NH3PbBr3 (Methylammonium lead tribromide, MAPbBr3) CH3NH3PbCl3 (Methylammonium lead tribromide, MAPbCl3) CH3NH3PbI3 (Methylammonium lead iodide, MAPbI3) Cs2AgBiBr6 (Cesium silver bismuth bromide, CABB) CsPbBr3 (Cesium lead tribromide) CsPbCl3 (Cesium lead trichloride) CsPbI3 (Cesium lead triiodide) CsPb(Br,Cl)3 (Cesium lead tribromide - Cesium lead trichloride) 2D HOIP (Hybrid organic-inorganic perovskite) CdSe/ZnCdS (Cadmium selenide / zinc cadmium sulfide core/shell) Therminol VP-1 Blood Adipose tissue (body fat) Liver Colon DNA Acetylene soot Propanee soot Diesel soot Montmorillonite Kaolinite Illite Bombyx mori (silkworm) silk Antheraea mylitta silk Samia ricini (eri silkworm) silk Antheraea assamensis silk Metamaterials
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For high pulse repetition rates, it can happen that the pulse amplification process exhibits strong fluctuations. Bifurcations with period doubling can also occur, where the pulse energy first alternates between two values, later four or even eight values. For further increased repetition rates, this can lead into deterministic chaos [8, 9, 12]. Fig 2 shows a numerical example case.
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A common gain medium for regenerative amplifiers is Ti:sapphire, which has a broad gain bandwidth and high thermal conductivity. Other gain media, e.g. doped with ytterbium or neodymium, are suitable for diode pumping and have a good energy storage capability due to their long upper-state lifetimes, but the generated pulses are longer (typically hundreds of femtoseconds or more) due to the smaller gain bandwidth.
Definition: optical amplifiers with a resonator in which a light pulse can do multiple round trips before being coupled out
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