Abstract
Recent high-intensity laser experiments (Cole et al 2018 Phys. Rev. X 8 011020; Poder et al 2018 Phys. Rev. X 8 031004) have shown evidence of strong radiation reaction in the quantum regime. Experimental evidence of quantum effects on radiation reaction and electron–positron pair cascades has, however, proven challenging to obtain and crucially depends on maximising the quantum parameter of the electron (defined as the ratio of the electric field it feels in its rest frame to the Schwinger field). The quantum parameter can be suppressed as the electrons lose energy by radiation reaction as they traverse the initial rise in the laser intensity. As a result the shape of the intensity temporal envelope becomes important in enhancing quantum radiation reaction effects and pair cascades. Here we show that a realistic laser pulse with a faster rise time on the leading edge, achieved by skewing the temporal envelope, results in curtailing of pair yields as the peak power is reduced. We find a reduction in pair yields by orders of magnitude in contrast to only small reductions reported previously in large-scale particle-in-cell code simulations (Hojbota et al 2018 Plasma Phys. Control. Fusion 60 064004). Maximum pairs per electron are found in colliding 1.5 GeV electrons with a laser wakefield produced envelope 7.90 × 10−2 followed by a short 50 fs Gaussian envelope, 1.90 × 10−2, while it is reduced to 8.90 × 10−5, a factor of 100, for an asymmetric envelope.
Highlights
Strong field quantum electrodynamics processes can be investigated with current high power petawatt (PW) lasers, reaching intensities ∼1021 W cm−2
We have shown similar effects occurring in figure 5 as the initial electron beam energy increases, a skewed envelope gives a maximum χe of 1.0 while it is only 0.4 for the optimally compressed Gaussian pulse
We have shown that skewing the laser intensity temporal envelope, lowering the peak intensity, gives a lower electron–positron pair yield per electron 1.5 × 10−6 compared to optimally compressed 1.9 × 10−2, or in colliding an electron-beam with a pulse generated using plasma optics 7.9 × 10−2
Summary
Original content from this work may be used under the terms of the Creative Commons Attribution 4.0 licence. Any further distribution of this work must maintain attribution to the author(s) and the title of the work, journal citation and DOI. L E Bradley1,2,∗ , M J V Streeter3,4 , C D Murphy1 , C Arran1 , T G Blackburn5 , M Galletti2,6 , S P D Mangles3 and C P Ridgers1 Keywords: strong-field, quantum electrodynamics, radiation reaction, electron collisions, plasma optics, pair production
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