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Dive into the research topics where A. V. Prozorkevich is active.

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Featured researches published by A. V. Prozorkevich.


International Journal of Modern Physics E-nuclear Physics | 1998

A Quantum kinetic equation for particle production in the Schwinger mechanism

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

Pair production and optical lasers.

D. Blaschke; A. V. Prozorkevich; Craig D. Roberts; Sebastian M. Schmidt; S. A. Smolyansky

E(t)


Physical Review D | 1999

Non-Markovian effects in strong-field pair creation

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

Plasma production and thermalisation in a strong field

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

THE KINETIC DESCRIPTION OF VACUUM PARTICLE CREATION IN THE OSCILLATOR REPRESENTATION

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

Dynamical Schwinger effect and high-intensity lasers. Realising nonperturbative QED

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

Inertial mechanism: Dynamical mass as a source of particle creation

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

A proposal for testing subcritical vacuum pair production with high power lasers

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

Kinetic description of vacuum particle production in collisions of ultrarelativistic nuclei

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

Influence of Laser Pulse Parameters on the Properties of e–e+ Plasmas Created from Vacuum

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

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D. Blaschke

National Research Nuclear University MEPhI

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V. D. Toneev

Joint Institute for Nuclear Research

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G. Röpke

University of Rostock

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Craig D. Roberts

Argonne National Laboratory

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