A. V. Prozorkevich
Saratov State University
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Featured researches published by A. V. Prozorkevich.
International Journal of Modern Physics E-nuclear Physics | 1998
Sebastian M. Schmidt; D. Blaschke; G. Röpke; S. A. Smolyansky; A. V. Prozorkevich; V. D. Toneev
A quantum kinetic equation has been derived for the description of pair production in a time-dependent homogeneous electric field
Physical Review Letters | 2006
D. Blaschke; A. V. Prozorkevich; Craig D. Roberts; Sebastian M. Schmidt; S. A. Smolyansky
E(t)
Physical Review D | 1999
Sebastian M. Schmidt; D. Blaschke; G. Ropke; A. V. Prozorkevich; S. A. Smolyansky; V. D. Toneev
. As a source term, the Schwinger mechanism for particle creation is incorporated. Possible particle production due to collisions and collisional damping are neglected. The main result is a closed kinetic equation of the non-Markovian type. In the low density approximation, the source term is reduced to the leading part of the well known Schwinger formula for the probability of pair creation. We compare the formula obtained with other approaches and discuss the differences.
European Physical Journal C | 2001
D. V. Vinnik; A. V. Prozorkevich; S. A. Smolyansky; V. D. Toneev; M. B. Hecht; Craig D. Roberts; S. M. Schmidt
Electron-positron pair creation in a standing wave is explored using a parameter-free quantum kinetic equation. Field strengths and frequencies corresponding to modern optical lasers induce a material polarization of the QED vacuum, which may be characterized as a plasma of e+e- quasiparticle pairs with a density of approximately 10(20) cm-3. The plasma vanishes almost completely when the laser field is zero, leaving a very small residual pair density n(r) which is the true manifestation of vacuum decay. The average pair density per period is proportional to the laser intensity but independent of the frequency nu. The density of residual pairs also grows with laser intensity but n(r) proportional to nu(2). With optical lasers at the forefront of the current generation, these dynamical QED vacuum effects can plausibly generate 5-10 observable two-photon annihilation events per laser pulse.
International Journal of Modern Physics A | 2005
V. N. Pervushin; V. V. Skokov; A. V. Reichel; S. A. Smolyansky; A. V. Prozorkevich
We analyze a quantum kinetic equation describing both boson and fermion pair production and explore analytically and numerically the solution of the non-Markovian kinetic equation. In the Markovian limit of the kinetic equation we find an analytical solution for the single particle distribution function of bosons and fermions. The numerical investigation for a homogeneous, constant electric field shows an enhancement (bosons) or a suppression (fermions) of the pair creation rate according to the symmetry character of the produced particles. For strong fields non-Markovian effects are important while they disappear for weak fields. Hence it is sufficient to apply the low density limit for weak fields but necessary to take into account memory effects for strong fields.
European Physical Journal D | 2009
D. Blaschke; A. V. Prozorkevich; G. Röpke; Craig D. Roberts; S. M. Schmidt; D. S. Shkirmanov; S. A. Smolyansky
Aspects of the formation and equilibration of a quark-gluon plasma are explored using a quantum kinetic equation, which involves a non-Markovian, Abelian source term for quark and antiquark production and, for the collision term, a relaxation time approximation that defines a time-dependent quasi-equilibrium temperature and collective velocity. The strong Abelian field is determined via the simultaneous solution of Maxwells equation. A particular feature of this approach is the appearance of plasma oscillations in all thermodynamic observables. Their presence can lead to a sharp increase in the time-integrated dilepton yield.
Physics of Particles and Nuclei | 2008
Andrey V. Filatov; A. V. Prozorkevich; S. A. Smolyansky; V. D. Toneev
The oscillator representation is used for the nonperturbative description of vacuum particle creation in a strong time-dependent electric field in the framework of scalar QED. It is shown that the method can be more effective for the derivation of the quantum kinetic equation (KE) in comparison with the Bogoliubov method of time-dependent canonical transformations. This KE is used for the investigation of vacuum creation in periodical linear and circular polarized electric fields and also in the case of the presence of a constant magnetic field, including the back reaction problem. In particular, these examples are applied for a model illustration of some features of vacuum creation of electron–positron plasma within the planned experiments on the X-ray free electron lasers.
High Energy Density Physics | 2010
G. Gregori; D. Blaschke; P.P. Rajeev; H. Chen; Rosemary Clarke; T. Huffman; C. D. Murphy; A. V. Prozorkevich; Craig D. Roberts; G. Röpke; Sebastian M. Schmidt; S. A. Smolyansky; S.C. Wilks; R. Bingham
AbstractWe consider the possibility of experimental verification of vacuum e+e- pair creation at the focus of two counter-propagating optical laser beams with intensities 1020–10
Physics of Atomic Nuclei | 2001
D. V. Vinnik; V. A. Mizerny; A. V. Prozorkevich; S. A. Smolyansky; V. D. Toneev
^{22}~{\rm W/cm}^2
Contributions To Plasma Physics | 2013
D. Blaschke; B. Kämpfer; A. D. Panferov; A. V. Prozorkevich; S. A. Smolyansky
, achievable with present-day petawatt lasers, and approaching the Schwinger limit: 10