2022
DOI: 10.48550/arxiv.2203.08366
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Linear collider based on laser-plasma accelerators

Abstract: Laser-plasma accelerators (LPAs) are capable of sustaining accelerating fields of 1-100 GeV/m, 10-1000 times that of conventional RF technology, and the highest fields produced by any of the widely researched advanced accelerator concepts. Furthermore, LPAs intrinsically produce short particle bunches, 100-1000 times shorter than that of conventional RF technology, which leads to reductions in beamstrahlung and savings in overall power consumption. Furthermore, they enable novel energy recovering methods that … Show more

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Cited by 2 publications
(3 citation statements)
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“…The accelerator model works with the density 𝑛 = 10 17 𝑐𝑚 −3 and with the plasma channel which has radius of 22𝜇𝑚. The laser of the accelerator is a 6.5J, 130fs FWHM laser, and it could excite the plasma with the peak accelerating field of 6 GV/m [9]. An proper particle beams of 0.19nC (3kA beams peak current) can be obtained energy above 5 GeV with the efficiency of 20% [9].…”
Section: Electron-positron Collidermentioning
confidence: 99%
See 1 more Smart Citation
“…The accelerator model works with the density 𝑛 = 10 17 𝑐𝑚 −3 and with the plasma channel which has radius of 22𝜇𝑚. The laser of the accelerator is a 6.5J, 130fs FWHM laser, and it could excite the plasma with the peak accelerating field of 6 GV/m [9]. An proper particle beams of 0.19nC (3kA beams peak current) can be obtained energy above 5 GeV with the efficiency of 20% [9].…”
Section: Electron-positron Collidermentioning
confidence: 99%
“…The laser of the accelerator is a 6.5J, 130fs FWHM laser, and it could excite the plasma with the peak accelerating field of 6 GV/m [9]. An proper particle beams of 0.19nC (3kA beams peak current) can be obtained energy above 5 GeV with the efficiency of 20% [9]. Energy recovery operations could be performs for the energy remain in the laser as well as the plasma.…”
Section: Electron-positron Collidermentioning
confidence: 99%
“…In conventional accelerators positrons are usually produced via collisions of high energy electrons or photons with solid density high-Z foils (see, e.g., proposed [13][14][15] and operational [11] designs), accumulated in a damping ring, and then transported into the accelerator. Compact, plasma-based accelerators, however, present a set of unique requirements for accelerating positron beams efficiently [16]. The most challenging ones are achieving a low energy spread and divergence, as well as the short duration of the beam so the positrons can be efficiently captured in the plasma wakefield.…”
Section: Introductionmentioning
confidence: 99%