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Andriy Kostyuk

Publications and source records attributed to Andriy Kostyuk.

12 recordsLinked to original sources
arXiv2019

Comment on 'Simulation of ultra-relativistic electrons and positrons channeling in crystals with MBN Explorer'

The snapshot model of crystal atoms was implemented in the Monte Carlo code ChaS (Channeling Simulator) and is being successfully used for simulation of ultrarelativistic particle channeling. The model was criticized by Sushko et al. (J. Comp. Phys. 252 (2013) 404-418) who claim that it overestimates the mean scattering angle in a single projectile-atom collision. As a matter of fact, no evidence that would support this claim can be found in the mentioned publication. Moreover, the snapshot model and the model suggested by Sushko et al. yield essentially the same value of the mean scattering angle. Contrary to the claim of Sushko et al., the target electrons can be considered as fixed-position scatterer, corrections due to their finite mass and nonzero initial velocity have a negligible impact on the channeling of light projectiles (electrons and positrons). In contrast to the snapshot model, the model preferred by Sushko et al. does not take into account incoherent scattering of the projectile by crystal electrons. This explains why the two models predict different values of the dechanneling length. The claim that the snapshot model underestimates the dechanneling length is unfounded. In actual fact, this model is in good agreement with experimental data.

physics.acc-ph↗
arXiv2019

Comment on `Radiation from multi-GeV electrons and positrons in periodically bent silicon crystal'

Simulations of electron and positron channelling in a crystalline undulator with a small amplitude and a short period (A Kostyuk, Phys. Rev. Lett. 110 (2013) 115503) were repeated by V G Bezchastnov, A V Korol and A V Solov'yov (J. Phys. B: At. Mol. Opt. Phys. 47 (2014) 195401)for the same parameter set but using another computer code, MBN Explorer, which implements a different model of projectile scattering by crystal atoms. The authors of the latter paper claim that their approach, in contrast to the one of the former paper, allows them to observe short-period undulator oscillations in plots of simulated trajectories. In fact, the undulator oscillations become visible on trajectory segments which have a small amplitude of channelling oscillations. This is equally true for both approaches. The claim of Bezchastnov et al. that their model is "more accurate" is unfounded. Moreover, there are indications of severe mistakes in their calculations: the phases of undulator oscillations in the trajectories obtained with MBN Explorer are inconsistent with each other and with well established properties of forced oscillations.

physics.acc-ph↗
arXiv2017

Planar Channeling of 855 MeV Electrons in Silicon: Monte-Carlo Simulations

A new Monte Carlo code for the simulation of the channeling of ultrarelativistic charged projectiles in single crystals is presented. A detailed description of the underlying physical model and the computation algorithm is given. First results obtained with the code for the channeling of 855 MeV electrons in Silicon crystal are presented. The dechanneling lengths for (100), (110) and (111) crystallographic planes are estimated. In order to verify the code, the dependence of the intensity of the channeling radiation on the crystal dimension along the beam direction is calculated. A good agreement of the obtained results with recent experimental data is observed.

physics.acc-ph↗
arXiv2017

Strained Layer Crystalline Undulator

Ultrarelativistic charged particles are predicted to emit hard electromagnetic radiation of undulator type while being channeled in a crystal with periodically bent crystallographic planes. The recently proposed crystalline undulator with the bending amplitude smaller than the distance between the bent planes and the bending period shorter than the period of channeling oscillations is far superior to what was proposed previously. In the same time, it is more challenging from the technical point of view because its bending period has to be in the sub-micron range. It is shown that a mixed crystal of silicon-germanium with properly varying germanium fraction can have the necessary bending parameters. Moreover, it is predicted to be stable against misfit dislocations.

physics.acc-ph↗
arXiv2013

Crystalline Undulator with a Small Amplitude and a Short Period

The crystalline undulator is a single crystal with periodically bent crystallographic planes. If ultrarelativistic charged particles channel through such a crystal, they emit hard radiation of undulator type. A crystalline undulator with a bending amplitude smaller than the distance between the bent planes and a bending period shorter than the period of channeling oscillations is proposed. Heretofore, it was believed that such a range of bending parameters was unsuitable for a crystalline undulator. This point of view is refuted. In fact, the undulator with a small amplitude and a short period is far superior to what was proposed previously. It requires much lower beam energy for production of photons of the same frequency. Such an undulator allows for a larger effective number of undulator periods. It is predicted to emit intense undulator radiation in the forward direction with a narrow spectral distribution and a lower and softer background. The undulator effect is seen for both positron and electron beams. Using positrons is, however, preferable because they enable one to obtain higher intensity of the undulator radiation with lower background.

physics.optics↗
arXiv2013

Recent Progress in the Theory of the Crystalline Undulator

If an ultrarelativistic charged particle channels inside a single crystal with periodically bent crystallographic planes, it emits hard electromagnetic radiation of the undulator type. Due to similarity of its physical principles to the ordinary (magnetic) undulator, such a device is termed as the crystalline undulator. Recent development of a new Monte Carlo code ChaS made possible a detailed simulation of particle channeling and radiation emission in periodically bent crystals. According to recent findings, energy of the electron beam below 1 GeV is sufficient to observe the undulator effect in a periodically bent crystal. Even more exciting results were obtained for a crystalline undulator whose bending period is shorter than the period of the channeling oscillations and the bending amplitude is smaller than the width of the planar channel. Such a crystalline undulator is far superior to what was proposed previously. It allows for a large effective number of undulator periods. Therefore, it is predicted to emit intense undulator radiation in the forward direction. A narrow undulator peak is seen for both positron and electron beams. Using positrons is, however, more desirable because in this case the intensity of the undulator radiation is higher while the background is lower.

physics.acc-ph↗
arXiv2013

B_c meson enhancement and the momentum dependence in Pb+Pb collisions at LHC energy

B_c meson production in Pb+Pb collisions at sqrt{s}=2.76 A TeV is surveyed in both a statistical coalescence model and a transport model. The nuclear modification factor R_{AA} is predicted to be between 2 and 18 in the most central collisions, which can help to confirm the regeneration mechanism. In addition, the momentum dependence is also investigated as given by the transport model. A strong suppression of the transverse momentum is found in central collisions accompanying the enhancement in yield. The spectrum and elliptic flow of B_c are also discussed.

nucl-th↗
arXiv2008

Stable propagation of a modulated particle beam in a crystal channel

The propagation of a modulated beam of charged particles in a planar crystal channel is investigated. It is demonstrated that the beam preserves its modulation at sufficiently large penetration depths to ensure the feasibility of using a crystalline undulator as a coherent source of hard X rays. This finding is a crucial milestone in developing a new type of lasers radiating in the hard X ray and gamma ray range.

physics.acc-ph↗
arXiv2008

One-dimensional Model of a Gamma Klystron

A new scheme for amplification of coherent gamma rays is proposed. The key elements are crystalline undulators - single crystals with periodically bent crystallographic planes exposed to a high energy beam of charged particles undergoing channeling inside the crystals. The scheme consists of two such crystals separated by a vacuum gap. The beam passes the crystals successively. The particles perform undulator motion inside the crystals following the periodic shape of the crystallographic planes. Gamma rays passing the crystals parallel to the beam get amplified due to interaction with the particles inside the crystals. The term `gamma klystron' is proposed for the scheme because its operational principles are similar to those of the optical klystron. A more simple one-crystal scheme is considered as well for the sake of comparison. It is shown that the gamma ray amplification in the klystron scheme can be reached at considerably lower particle densities than in the one-crystal scheme, provided that the gap between the crystals is sufficiently large.

physics.acc-ph↗
arXiv2005

Double, Triple and Hidden Charm Production in the Statistical Coalescence Model

The production of particles with double, triple and hidden charm in heavy ion collisions is studied in the framework of the statistical coalescence model. According to the postulates of the model, the charm quark-antiquark pairs are created at the initial stage of a heavy ion reaction in hard parton collisions. The amount of charm is assumed to be unchanged at later stages. The charm (anti)quarks are distributed among different hadron species at hadronization according to the laws of statistical physics. Several approaches to the statistical treatment of charm hadronization are considered. The grand canonical approach is appropriate for systems containing large number of charm (anti)quarks. The exact charm conservation and Poissonian fluctuations of the number of charm quark-antiquark pairs should be taken into account, if the average number of these pairs is of oder of unity or smaller. The charm hadronization in a subsystem of a larger system is discussed. It is explained why the canonical approach is not appropriate for the description of charm hadronization. The obtained formulas can be used to calculate the production of charm in heavy ion collisions in a wide energy range.

nucl-th↗