A concept for multiterawatt fibre lasers based on coherent pulse stacking in passive cavities

Since the advent of femtosecond lasers, performance improvements have constantly impacted on existing applications and enabled novel applications. However, one performance feature bearing the potential of a quantum leap for high-field applications is still not available: the simultaneous emission of extremely high peak and average powers. Emerging applications such as laser particle acceleration require exactly this performance regime and, therefore, challenge laser technology at large. On the one hand, canonical bulk systems can provide pulse peak powers in the multi-terawatt to petawatt range, while on the other hand, advanced solid-state-laser concepts such as the thin disk, slab or fibre are well known for their high efficiency and their ability to emit high average powers in the kilowatt range with excellent beam quality. In this contribution, a compact laser system capable of simultaneously providing high peak and average powers with high wall-plug efficiency is proposed and analysed. The concept is based on the temporal coherent combination (pulse stacking) of a pulse train emitted from a high-repetition-rate femtosecond laser system in a passive enhancement cavity. Thus, the pulse energy is increased at the cost of the repetition rate while almost preserving the average power. The concept relies on a fast switching element for dumping the enhanced pulse out of the cavity. The switch constitutes the key challenge of our proposal. Addressing this challenge could, for the first time, allow the highly efficient dumping of joule-class pulses at megawatt average power levels and lead to unprecedented laser parameters. Coherent pulse stacking may allow compact fibre-laser systems to be used in laser-based particle accelerators, report scientists in Germany. Such accelerators require lasers that can simultaneously provide exceedingly high peak and average powers—a tall order indeed. Now, Sven Breitkopf and co-workers propose that it could be achieved by employing temporal coherent combination of a pulse train emitted by a high-repetition-rate femtosecond fibre laser in a passive cavity. Following pulse stacking, a fast switching element dumps the enhanced high-peak power pulse from the cavity. Although this process increases the pulse peak power at the expense of a lower repetition rate, it retains a high average power. Ultimately, the scheme could lead to Joule-class pulses with terawatt peak powers and megawatt average powers.

[1]  T. Tajima,et al.  Laser Electron Accelerator , 1979 .

[2]  S. Döbert SLAC-PUB-10463 May 2004 RF-Breakdown in High-Frequency Accelerators , 2004 .

[3]  Gerard Mourou,et al.  Compression of amplified chirped optical pulses , 1985 .

[4]  Ferenc Krausz,et al.  Large-mode enhancement cavities. , 2013, Optics express.

[5]  L. A. Lompré,et al.  Multiple-harmonic conversion of 1064 nm radiation in rare gases , 1988 .

[6]  Wolfgang Sandner,et al.  Photoinjector drive laser of the FLASH FEL. , 2011, Optics express.

[7]  A. Tünnermann,et al.  Michelson interferometer with diffractively-coupled arm resonators in second-order Littrow configuration. , 2012, Optics express.

[8]  Tino Eidam,et al.  530 W, 1.3 mJ, four-channel coherently combined femtosecond fiber chirped-pulse amplification system. , 2013, Optics letters.

[9]  Wim Leemans The BErkeley Lab Laser Accelerator (BELLA): A 10 GeV Laser Plasma Accelerator , 2010 .

[10]  M Rosenbluh,et al.  Pulse picking by phase-coherent additive pulse generation in an external cavity. , 2003, Optics letters.

[11]  T. Fan,et al.  Coherent beam combining and phase noise measurements of ytterbium fiber amplifiers. , 2004, Optics letters.

[12]  Jens Limpert,et al.  The future is fibre accelerators , 2013, Nature Photonics.

[13]  L. Pinard,et al.  External cavity enhancement of picosecond pulses with 28,000 cavity finesse. , 2013, Applied optics.

[14]  T. Gottschall,et al.  58 mJ burst comprising ultrashort pulses with homogenous energy level from an Yb-doped fiber amplifier. , 2012, Optics letters.

[15]  S. Hooker,et al.  Developments in laser-driven plasma accelerators , 2013, Nature Photonics.

[16]  Arnaud Brignon,et al.  Collective coherent phase combining of 64 fibers. , 2011, Optics express.

[17]  Cesar Jauregui,et al.  Yb-doped large-pitch fibres: effective single-mode operation based on higher-order mode delocalisation , 2012, Light: Science & Applications.

[18]  Cesar Jauregui,et al.  High-power fibre lasers , 2013 .

[19]  Jens Limpert,et al.  Basic considerations on coherent combining of ultrashort laser pulses. , 2011, Optics express.

[20]  Matthias Golling,et al.  275 W average output power from a femtosecond thin disk oscillator operated in a vacuum environment. , 2012, Optics express.

[21]  H. Hoffmann,et al.  Compact diode-pumped 1.1 kW Yb:YAG Innoslab femtosecond amplifier. , 2010, Optics letters.

[22]  Jun Ye,et al.  Femtosecond pulse amplification by coherent addition in a passive optical cavity. , 2002, Optics letters.

[23]  S. Dobert RF breakdown in high frequency accelerator , 2004, Conference Record of the Twenty-Sixth International Power Modulator Symposium, 2004 and 2004 High-Voltage Workshop..

[24]  Cesar Jauregui,et al.  Fiber chirped-pulse amplification system emitting 3.8 GW peak power. , 2011, Optics express.

[25]  B. Visentin,et al.  Gamma rays produced by intra-cavity inverse Compton scattering of a storage ring free-electron laser , 1999 .

[26]  Jens Limpert,et al.  88 W 0.5 mJ femtosecond laser pulses from two coherently combined fiber amplifiers. , 2011, Optics letters.

[27]  Tino Eidam,et al.  Femtosecond fiber CPA system emitting 830 W average output power. , 2010, Optics letters.

[28]  Cesar Jauregui,et al.  Analysis of passively combined divided-pulse amplification as an energy-scaling concept. , 2013, Optics express.

[29]  M Hanna,et al.  Passive coherent combination of two ultrafast rod type fiber chirped pulse amplifiers. , 2012, Optics letters.

[30]  Stephan Polachowski,et al.  Chopper system for time resolved experiments with synchrotron radiation. , 2009, The Review of scientific instruments.

[31]  Yoann Zaouter,et al.  Femtosecond fiber chirped- and divided-pulse amplification system. , 2013, Optics letters.

[32]  Shian Zhou,et al.  Divided-pulse Amplification of Ultrashort Pulses , 2006, 2007 Conference on Lasers and Electro-Optics (CLEO).

[33]  Joshua E. Rothenberg,et al.  Perturbative analysis of coherent combining efficiency with mismatched lasers. , 2010, Optics express.

[34]  Thomas Udem,et al.  A frequency comb in the extreme ultraviolet , 2005, Nature.

[35]  T. Eidam,et al.  Megawatt-scale average-power ultrashort pulses in an enhancement cavity. , 2014, Optics letters.

[36]  T. Fan Laser beam combining for high-power, high-radiance sources , 2005, IEEE Journal of Selected Topics in Quantum Electronics.

[37]  Jun Ye,et al.  Phase-coherent frequency combs in the vacuum ultraviolet via high-harmonic generation inside a femtosecond enhancement cavity. , 2005, Physical review letters.

[38]  Jens Limpert,et al.  Coherently combined fiber laser system delivering 120 μJ femtosecond pulses. , 2011, Optics letters.

[39]  Tino Eidam,et al.  Compact high-repetition-rate source of coherent 100 eV radiation , 2013, Nature Photonics.

[40]  Eric Esarey,et al.  Laser-driven plasma-wave electron accelerators , 2009 .

[41]  Tino Eidam,et al.  Power scaling of a high-repetition-rate enhancement cavity. , 2010, Optics letters.