Properties of the electron-positron plasma created from a vacuum in a strong laser field: Quasiparticle excitations

被引:25
作者
Blaschke, D. B. [1 ,2 ,3 ]
Kaempfer, B. [4 ,5 ]
Schmidt, S. M. [6 ,7 ,8 ]
Panferov, A. D. [9 ]
Prozorkevich, A. V. [10 ]
Smolyansky, S. A. [10 ]
机构
[1] Univ Wroclaw, Inst Theoret Phys, PL-50204 Wroclaw, Poland
[2] Joint Inst Nucl Res, Bogoliubov Lab Theoret Phys, RU-141980 Dubna, Russia
[3] Univ Bielefeld, Fak Phys, D-33615 Bielefeld, Germany
[4] Helmholtz Zentrum Dresden Rossendorf, D-01314 Dresden, Germany
[5] Tech Univ Dresden, Inst Theoret Phys, D-01062 Dresden, Germany
[6] Forschungszentrum Julich, Inst Adv Simulat, D-52425 Julich, Germany
[7] JARA, D-52425 Julich, Germany
[8] Rhein Westfal TH Aachen, Phys Zentrum, Phys Inst B 3, D-52056 Aachen, Germany
[9] Saratov NG Chernyshevskii State Univ, Dept Math, RU-410026 Saratov, Russia
[10] Saratov NG Chernyshevskii State Univ, Dept Phys, RU-410026 Saratov, Russia
来源
PHYSICAL REVIEW D | 2013年 / 88卷 / 04期
关键词
PAIR PRODUCTION; RADIATION;
D O I
10.1103/PhysRevD.88.045017
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Solutions of a kinetic equation are investigated which describe, on a nonperturbative basis, the vacuum creation of quasiparticle electron-positron pairs due to a strong laser field. The dependence of the quasiparticle electron (positron) distribution function and the particle number density is explored in a wide range of the laser radiation parameters, i.e., the wavelength lambda and amplitude of electric field strength E-0. Three domains are found: the domain of vacuum polarization effects where the density of the e(-)e(+) pairs is small (the "calm valley") and two accumulation domains in which the production rate of the e(-)e(+) pairs is strongly increased and the e(-)e(+) pair density can reach a significant value (the short wavelength domain and the strong field one). In particular, the obtained results point to a complicated short-distance electromagnetic structure of the physical vacuum in the domain of short wavelengths lambda less than or similar to lambda(acc) = pi/m. For moderately strong fields E-0 less than or similar to E-c = m(2)/e, the accumulation regime can be realized where a plasma with a high density of e(-)e(+) quasiparticles can be achieved. In this domain of the field strengths and in the whole investigated range of wavelengths, an observation of the dynamical Schwinger effect can be facilitated.
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页数:12
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