On the Schwinger limit attainability with extreme power lasers

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Avalanche discharge as the Geiger Counter It can indicate on the Schwinger process provided the laser intensity required for the avalanche is small enough, I*
Colliding EM Waves: Circularly Polarized v.s. Linearly Polarized Credit: T. Shintake power emitted by electron rotating in CP wave : 2r P m c ( 1) 3 maximum frequency : e 2 2 2 4 C, 0 e e e e 0.29 max 0 3 e power emitted by electron oscillating in LP wave : r P m c ( 1) 3 maximum frequency : e 2 2 2 L, 0 e e e 2 max 0 2 e
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: , 1at I 10 e Avalanche 1/ 4 1/ 2
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 and 34: What the values of e and for the pa
Page 35 and 36: What values of e and for the parame
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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