On the Schwinger limit attainability with extreme power lasers

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The number of electron-positron pairs produced in <strong>the</strong> focus of a single pulse or two colliding pulses I, W/cm 2 E 0/E s N e , single pulse N e , two pulses 2.5x10 26 4x10 -2 - 14 5x10 26 5.7x10 -2 - 2.6x10 7 5x10 27 0.18 25 1x10 28 0.25 3x10 7 S. S. Bulanov, N. B. Narozhny, V. D. Mur, V.S. Popov, JETP, 102, 9 (2006)
Multiple Colliding EM pulses: The scheme of interaction S. S. Bulanov, V. D. Mur, N. B. Narozhny, J. Nees, V. S. Popov, Phys. Rev. Lett. 104, 220404 (2010) A Way to Lower <strong>the</strong> Threshold of Pair Production from Vacuum N pulses N ± at W=10 kJ W(kJ) to produce one pair 2 9.0 x 10 -19 40 4 3.0 x 10 -9 20 8 4.0 10 16 1.8 x 10 3 8 24 4.2 x 10 6 5.1
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: Laser Power to Achieve the Schwinge
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 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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