2015
DOI: 10.1063/1.4932997
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High-flux low-divergence positron beam generation from ultra-intense laser irradiated a tapered hollow target

Abstract: By using two-dimensional particle-in-cell simulations, we demonstrate high-flux dense positrons generation by irradiating an ultra-intense laser pulse onto a tapered hollow target. By using a laser with an intensity of 4 × 1023 W/cm2, it is shown that the Breit-Wheeler process dominates the positron production during the laser-target interaction and a positron beam with a total number >1015 is obtained, which is increased by five orders of magnitude than in the previous work at the same laser intensity.… Show more

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Cited by 20 publications
(12 citation statements)
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“…In the direct way, laser irradiates a target directly to generate positrons, such as the multi-photon BW (Breit-Wheeler) process [11]. First, photon radiation can be described as e + mγ l → e + γ r on behalf of an energetic electron (e) interacting with laser photons (γ l ) to radiate a high-energy gamma photon (γ r ) [12,13]. Second, the BW process is initiated to generate positrons when these radiated gamma photons further interact with laser photons, which is γ r + nγ l → e + e + .…”
Section: Open Access Edited Bymentioning
confidence: 99%
“…In the direct way, laser irradiates a target directly to generate positrons, such as the multi-photon BW (Breit-Wheeler) process [11]. First, photon radiation can be described as e + mγ l → e + γ r on behalf of an energetic electron (e) interacting with laser photons (γ l ) to radiate a high-energy gamma photon (γ r ) [12,13]. Second, the BW process is initiated to generate positrons when these radiated gamma photons further interact with laser photons, which is γ r + nγ l → e + e + .…”
Section: Open Access Edited Bymentioning
confidence: 99%
“…3. The positron production of conical hollow targets can be increased by 5 orders of magnitude at the same laser intensity [19]. The composite target composed of nitrogen and gaseous aluminium can increase the yield of electronpositron pairs [20].…”
Section: The Influence Of Laser-plasma Interaction On the Qed Effectmentioning
confidence: 99%
“…[14,15] When the plasma is irradiated by such intense laser pulses, quantum electrodynamics (QED) effects become important, [16,17] and ultrarelativistic dense plasma can be produced. As one of the fundamental QED effects, electron-positron ( e − e + ) pair plasma production is highly concerned worldwide, [18][19][20][21][22][23] which is potentially interesting for a wide range of applications, such as particle physics, [24] plasma physics, [25] and laboratory astrophysics. [26] It is demonstrated experimentally that e − e + pair plasmas can be produced via the Bethe-Heitler (BH) process from picosecond-class laser pulses (with intensities of 10 18 W/cm 2 -10 20 W/cm 2 ) interacting with mm-thick high-Z target.…”
Section: Introductionmentioning
confidence: 99%