On the Schwinger limit attainability with extreme power lasers

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T. Tajima, J. M. Dawson (1979) Theory LWFA Experiment
What values of e and for the parameters of FM generated EM pulse +LWFA electrons are? We assume 1 PW, a=150, 1.25 GeV (LWFA ) electron energy, ph=5 (E=2 phE 0, =4 2 ph 0): 2 2 2 1/ 2 E ( mec p0) | p0 | E 2 150 2500 e 2 e ph 10 5 E S mec 15 ES 5.110 & (in multi-photon inverse Compton scattering regime) E 1.2 5 10 2.510 3 E m c m c The number of electrons colliding with the laser pulse is about 10 6 . 2 3 S e 2 1.2 e pha e 0 2 5 5.110
Page 1 and 2: On the Schwinger limit attainabilit
Page 3 and 4: Preface The critical electric field
Page 5 and 6: Introduction
Page 7 and 8: Breit-Wheeler process of e - - e +
Page 9 and 10: We reach a limit when the nonlinear
Page 11 and 12: Laser Power to Achieve the Schwinge
Page 13 and 14: Multiple Colliding EM pulses: The s
Page 15 and 16: What is better, circular or linear
Page 17 and 18: e - - e + , -ray plasma generation
Page 19 and 20: , 1at I 10 e Avalanche 1/ 4 1/ 2
Page 21 and 22: Colliding EM Waves: Circularly Pola
Page 23 and 24: Threshold for the e - - e + Avalanc
Page 25 and 26: Bφ 1 0 1 F a TM / 2 3D EM configur
Page 27 and 28: Threshold for the e - - e + avalanc
Page 29 and 30: Towards antimatter creation in vacu
Page 31 and 32: Gamma-ray photon generation via the
Page 33: What the values of e and for the pa
Page 37 and 38: These estimations are too optimisti
Page 39 and 40: Numerical solution of the equations
Page 41: Years Parameters e a 0 e Schedule
Page 44 and 45: Linearly polarized pulses save room

On the Schwinger limit attainability with extreme power lasers

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