537 research outputs found

    Observable effects caused by vacuum pair creation in the field of high-power optical lasers

    Full text link
    We consider the possibility of an experimental proof of vacuum e+e- pair creation in the focus of two counter-propagating optical laser beams with an intensity of the order of 10^20 - 10^22 W/cm^2. Our approach is based on the collisionless kinetic equation for the distribution function of the e+e- pairs with the source term for particle production. As a possible experimental signal of vacuum pair production we consider the refraction of a high-frequency probe laser beam by the produced e+e- plasma to be observed by an interference filter. The generation of higher harmonics of the laser frequency in the self-consistent electric field is also investigated.Comment: 7 pages, 7 figures; typos corrected, Eq.(16) corrected, reference adde

    From Coulomb excitation cross sections to non-resonant astrophysical rates in three-body systems: 17^{17}Ne case

    Get PDF
    Coulomb and nuclear dissociation of 17^{17}Ne on light and heavy targets are studied theoretically. The dipole E1 strength function is determined in a broad energy range including energies of astrophysical interest. Dependence of the strength function on different parameters of the 17^{17}Ne ground state structure and continuum dynamics is analyzed in a three-body model. The discovered dependence plays an important role for studies of the strength functions for the three-body E1 dissociation and radiative capture. The constraints on the [s2]/[d2][s^2]/[d^2] configuration mixing in 17^{17}Ne and on pp-wave interaction in the 15^{15}O+pp channel are imposed based on experimental data for 17^{17}Ne Coulomb dissociation on heavy target.Comment: 12 pages, 13 figure

    Long-Time Asymptotics of Perturbed Finite-Gap Korteweg-de Vries Solutions

    Full text link
    We apply the method of nonlinear steepest descent to compute the long-time asymptotics of solutions of the Korteweg--de Vries equation which are decaying perturbations of a quasi-periodic finite-gap background solution. We compute a nonlinear dispersion relation and show that the x/tx/t plane splits into g+1g+1 soliton regions which are interlaced by g+1g+1 oscillatory regions, where g+1g+1 is the number of spectral gaps. In the soliton regions the solution is asymptotically given by a number of solitons travelling on top of finite-gap solutions which are in the same isospectral class as the background solution. In the oscillatory region the solution can be described by a modulated finite-gap solution plus a decaying dispersive tail. The modulation is given by phase transition on the isospectral torus and is, together with the dispersive tail, explicitly characterized in terms of Abelian integrals on the underlying hyperelliptic curve.Comment: 45 pages. arXiv admin note: substantial text overlap with arXiv:0705.034

    КоксованиС высоковязкой ΠΎΠ±Π²ΠΎΠ΄Π½Π΅Π½Π½ΠΎΠΉ Π½Π΅Ρ„Ρ‚ΠΈ

    Get PDF
    Objectives. A characteristic feature of oil production is an increase in the volume of highviscosity bituminous oil. In Russia, technologies based on the use of water vapor are used for their extraction. The use of such technologies leads to a large amount of water in the product stream from the production well. Preparation of oil for processing involves its stabilization, desalination, and dewatering. Since the densities of the extracted oil and the water contained in it are comparable, traditional preparation schemes for processing of high-viscosity bituminous oil are ineffective. One of the possible solutions to the problem involving such oil in the fuel, energy, and petrochemical balance is to use a coking process at the first stage of its processing. This aim can be achieved by studying the influence of the process conditions of coking high-viscosity water-containing oil on the yield and characteristics of the resulting products.Methods. Coking of oil with a density of 1.0200 g/cm3 at 50 Β°C and with 18 wt % water content was carried out in a laboratory installation in a β€œcube.” A hollow cylindrical apparatus was used as a reactor and was placed in a furnace. The temperature and pressure in the reactor were maintained at 500–700 Β°C and 0.10–0.35 MPa, respectively.Results. An increase in the coking process temperature results in an increase in the amount of gaseous products, a decrease in the amount of the coke generated, and a higher dependence of the amount of liquid products on temperature with a maximum yield at 550–600 Β°C. The process temperature also affects the composition of liquid products. At a lower temperature, the amount of gasoline and kerosene fractions in liquid products is higher. With an increase in pressure, a higher amount of gaseous products, coke, and low-molecular-weight hydrocarbon fractions in liquid products could also be obtained. The characteristics of the coke produced in the coking process are similar to those of commercially produced grades. It is noted that when coking water-containing oil, up to 98% of the emulsion water goes with liquid products, and the remaining amount of water remains in the formed coke.Conclusions. Results showed the possible application of the coking process at the initial stage of processing high-viscosity bituminous oil. In this case, the dewatering stage is significantly simplified since the technological scheme of delayed coking allows the separation of the gasoline fraction from water. Β Π¦Π΅Π»ΠΈ. ВозрастаниС Π΄ΠΎΠ»ΠΈ высоковязкой ΠΈ Π±ΠΈΡ‚ΡƒΠΌΠΈΠ½ΠΎΠ·Π½ΠΎΠΉ Π½Π΅Ρ„Ρ‚ΠΈ являСтся Ρ…Π°Ρ€Π°ΠΊΡ‚Π΅Ρ€Π½ΠΎΠΉ ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡ‚ΡŒΡŽ соврСмСнной Π½Π΅Ρ„Ρ‚Π΅Π΄ΠΎΠ±Ρ‹Ρ‡ΠΈ. Π’ России ΠΏΡ€ΠΈ Π΅Π΅ Π΄ΠΎΠ±Ρ‹Ρ‡Π΅ ΠΏΡ€ΠΈΠΌΠ΅Π½ΡΡŽΡ‚ Ρ‚Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ, основанныС Π½Π° использовании водяного ΠΏΠ°Ρ€Π°. ΠŸΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ Ρ‚Π°ΠΊΠΈΡ… Ρ‚Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ ΠΏΡ€ΠΈΠ²ΠΎΠ΄ΠΈΡ‚ ΠΊ Ρ‚ΠΎΠΌΡƒ, Ρ‡Ρ‚ΠΎ ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚ΠΎΠ²Ρ‹ΠΉ ΠΏΠΎΡ‚ΠΎΠΊ, выходящий ΠΈΠ· Π΄ΠΎΠ±Ρ‹Π²Π°ΡŽΡ‰Π΅ΠΉ скваТины, ΠΌΠΎΠΆΠ΅Ρ‚ ΡΠΎΠ΄Π΅Ρ€ΠΆΠ°Ρ‚ΡŒ большоС количСство Π²ΠΎΠ΄Ρ‹. ΠŸΠΎΠ΄Π³ΠΎΡ‚ΠΎΠ²ΠΊΠ° Π½Π΅Ρ„Ρ‚ΠΈ ΠΊ ΠΏΠ΅Ρ€Π΅Ρ€Π°Π±ΠΎΡ‚ΠΊΠ΅ ΠΏΡ€Π΅Π΄ΠΏΠΎΠ»Π°Π³Π°Π΅Ρ‚ Π΅Π΅ ΡΡ‚Π°Π±ΠΈΠ»ΠΈΠ·Π°Ρ†ΠΈΡŽ, обСссоливаниС ΠΈ ΠΎΠ±Π΅Π·Π²ΠΎΠΆΠΈΠ²Π°Π½ΠΈΠ΅. ВслСдствиС Ρ‚ΠΎΠ³ΠΎ, Ρ‡Ρ‚ΠΎ ΠΏΠ»ΠΎΡ‚Π½ΠΎΡΡ‚ΡŒ Π΄ΠΎΠ±Ρ‹Π²Π°Π΅ΠΌΠΎΠΉ Π½Π΅Ρ„Ρ‚ΠΈ ΠΈ содСрТащСйся Π² Π½Π΅ΠΉ Π²ΠΎΠ΄Ρ‹ сопоставимы, Ρ‚Ρ€Π°Π΄ΠΈΡ†ΠΈΠΎΠ½Π½Ρ‹Π΅ схСмы ΠΏΠΎΠ΄Π³ΠΎΡ‚ΠΎΠ²ΠΊΠΈ ΠΊ ΠΏΠ΅Ρ€Π΅Ρ€Π°Π±ΠΎΡ‚ΠΊΠ΅ высоковязкой ΠΈ Π±ΠΈΡ‚ΡƒΠΌΠΈΠ½ΠΎΠ·Π½ΠΎΠΉ Π½Π΅Ρ„Ρ‚ΠΈ ΡΠ²Π»ΡΡŽΡ‚ΡΡ малоэффСктивными. Одним ΠΈΠ· Π²ΠΎΠ·ΠΌΠΎΠΆΠ½Ρ‹Ρ… Ρ€Π΅ΡˆΠ΅Π½ΠΈΠΉ ΠΏΡ€ΠΎΠ±Π»Π΅ΠΌΡ‹ вовлСчСния Ρ‚Π°ΠΊΠΎΠΉ Π½Π΅Ρ„Ρ‚ΠΈ Π² Ρ‚ΠΎΠΏΠ»ΠΈΠ²Π½ΠΎ-энСргСтичСский ΠΈ нСфтСхимичСский баланс являСтся использованиС Π½Π° ΠΏΠ΅Ρ€Π²ΠΎΠΌ этапС Π΅Π΅ ΠΏΠ΅Ρ€Π΅Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ процСсса коксования. Для Ρ€Π΅Π°Π»ΠΈΠ·Π°Ρ†ΠΈΠΈ этой ΠΈΠ΄Π΅ΠΈ Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΠΎ ΠΈΠ·ΡƒΡ‡ΠΈΡ‚ΡŒ влияниС условий коксования высоковязкой ΠΎΠ±Π²ΠΎΠ΄Π½Π΅Π½Π½ΠΎΠΉ Π½Π΅Ρ„Ρ‚ΠΈ Π½Π° Π²Ρ‹Ρ…ΠΎΠ΄ ΠΈ характСристики ΠΎΠ±Ρ€Π°Π·ΡƒΡŽΡ‰ΠΈΡ…ΡΡ ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚ΠΎΠ².ΠœΠ΅Ρ‚ΠΎΠ΄Ρ‹. ΠžΠ±ΡŠΠ΅ΠΊΡ‚ΠΎΠΌ исслСдования Π±Ρ‹Π»Π° Π½Π΅Ρ„Ρ‚ΡŒ с ΠΏΠ»ΠΎΡ‚Π½ΠΎΡΡ‚ΡŒΡŽ ΠΏΡ€ΠΈ 50 Β°Π‘ 1.0200 Π³/см³, содСрТащая 18 мас. % Π²ΠΎΠ΄Ρ‹. КоксованиС ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ Π½Π° Π»Π°Π±ΠΎΡ€Π°Ρ‚ΠΎΡ€Π½ΠΎΠΉ установкС Π² Β«ΠΊΡƒΠ±Π΅Β». Π’ качСствС Ρ€Π΅Π°ΠΊΡ‚ΠΎΡ€Π° использовался пустотСлый цилиндричСский Π°ΠΏΠΏΠ°Ρ€Π°Ρ‚, Ρ€Π°Π·ΠΌΠ΅Ρ‰Π°Π΅ΠΌΡ‹ΠΉ Π² ΠΏΠ΅Ρ‡ΠΈ. Π’Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π° Π² Ρ€Π΅Π°ΠΊΡ‚ΠΎΡ€Π΅ Π²Π°Ρ€ΡŒΠΈΡ€ΠΎΠ²Π°Π»Π°ΡΡŒ ΠΎΡ‚ 500 Π΄ΠΎ 700 Β°Π‘, Π΄Π°Π²Π»Π΅Π½ΠΈΠ΅ ΠΎΡ‚ 0.10 Π΄ΠΎ 0.35 МПа.Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹. ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½Π½Ρ‹Π΅ исслСдования ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΈ, Ρ‡Ρ‚ΠΎ ΠΏΡ€ΠΈ возрастании Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρ‹ коксования Π²Ρ‹Ρ…ΠΎΠ΄ Π³Π°Π·ΠΎΠΎΠ±Ρ€Π°Π·Π½Ρ‹Ρ… ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚ΠΎΠ² увСличиваСтся, ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½ΠΈΠ΅ кокса ΡƒΠΌΠ΅Π½ΡŒΡˆΠ°Π΅Ρ‚ΡΡ, Π° Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡ‚ΡŒ Π²Ρ‹Ρ…ΠΎΠ΄Π° ΠΆΠΈΠ΄ΠΊΠΈΡ… ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚ΠΎΠ² ΠΈΠΌΠ΅Π΅Ρ‚ ΡΠΊΡΡ‚Ρ€Π΅ΠΌΠ°Π»ΡŒΠ½Ρ‹ΠΉ Ρ…Π°Ρ€Π°ΠΊΡ‚Π΅Ρ€ с максимумом Π² области Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€ 550–600 Β°C. Π’Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π° процСсса влияСт Π½Π° состав ΠΆΠΈΠ΄ΠΊΠΈΡ… ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚ΠΎΠ². ΠŸΡ€ΠΈ Π±ΠΎΠ»Π΅Π΅ Π½ΠΈΠ·ΠΊΠΎΠΉ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π΅ Π² ΠΆΠΈΠ΄ΠΊΠΈΡ… ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚Π°Ρ… Π²Ρ‹ΡˆΠ΅ содСрТаниС Π±Π΅Π½Π·ΠΈΠ½ΠΎΠ²ΠΎΠΉ ΠΈ кСросиновой Ρ„Ρ€Π°ΠΊΡ†ΠΈΠΉ. ΠŸΠΎΠ²Ρ‹ΡˆΠ΅Π½ΠΈΠ΅ давлСния ΠΏΡ€ΠΈΠ²ΠΎΠ΄ΠΈΡ‚ ΠΊ Π²ΠΎΠ·Ρ€Π°ΡΡ‚Π°Π½ΠΈΡŽ Π²Ρ‹Ρ…ΠΎΠ΄Π° Π³Π°Π·ΠΎΠΎΠ±Ρ€Π°Π·Π½Ρ‹Ρ… ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚ΠΎΠ², кокса ΠΈ содСрТания Π² ΠΆΠΈΠ΄ΠΊΠΈΡ… ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚Π°Ρ… низкомолСкулярныхфракций ΡƒΠ³Π»Π΅Π²ΠΎΠ΄ΠΎΡ€ΠΎΠ΄ΠΎΠ². ΠžΠ±Ρ€Π°Π·ΡƒΡŽΡ‰ΠΈΠΉΡΡ Π² процСссС кокс ΠΏΠΎ своим характСристикам Π±Π»ΠΈΠ·ΠΎΠΊ ΠΊ ΠΏΡ€ΠΎΠΌΡ‹ΡˆΠ»Π΅Π½Π½ΠΎ выпускаСмым ΠΌΠ°Ρ€ΠΊΠ°ΠΌ. ΠžΡ‚ΠΌΠ΅Ρ‡Π΅Π½ΠΎ, Ρ‡Ρ‚ΠΎ ΠΏΡ€ΠΈ коксовании ΠΎΠ±Π²ΠΎΠ΄Π½Π΅Π½Π½ΠΎΠΉ Π½Π΅Ρ„Ρ‚ΠΈ Π΄ΠΎ 98% Π²ΠΎΠ΄Π½ΠΎΠΉ ΡΠΌΡƒΠ»ΡŒΡΠΈΠΈ ΡƒΡ…ΠΎΠ΄ΠΈΡ‚ с ΠΆΠΈΠ΄ΠΊΠΈΠΌΠΈ ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚Π°ΠΌΠΈ коксования, ΠΈ лишь нСбольшоС количСство Π²ΠΎΠ΄Ρ‹ остаСтся Π² ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π²ΡˆΠ΅ΠΌΡΡ коксС.Π’Ρ‹Π²ΠΎΠ΄Ρ‹. ΠŸΡ€Π΅Π΄ΡΡ‚Π°Π²Π»Π΅Π½Π½Ρ‹Π΅ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ ΠΏΠΎΠΊΠ°Π·Ρ‹Π²Π°ΡŽΡ‚ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡ‚ΡŒ использования процСсса коксования Π½Π° Π½Π°Ρ‡Π°Π»ΡŒΠ½ΠΎΠΌ этапС ΠΏΠ΅Ρ€Π΅Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ высоковязкой ΠΈ Π±ΠΈΡ‚ΡƒΠΌΠΈΠ½ΠΎΠ·Π½ΠΎΠΉ Π½Π΅Ρ„Ρ‚ΠΈ. Π’ этом случаС сущСствСнно упрощаСтся ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½ΠΈΠ΅ стадии Π΅Π΅ обСзвоТивания, Ρ‚Π°ΠΊ ΠΊΠ°ΠΊ Π² тСхнологичСской схСмС Π·Π°ΠΌΠ΅Π΄Π»Π΅Π½Π½ΠΎΠ³ΠΎ коксования прСдусмотрСно ΠΎΡ‚Π΄Π΅Π»Π΅Π½ΠΈΠ΅ Π±Π΅Π½Π·ΠΈΠ½ΠΎΠ²ΠΎΠΉ Ρ„Ρ€Π°ΠΊΡ†ΠΈΠΈ ΠΎΡ‚ Π²ΠΎΠ΄Ρ‹.

    Laser acceleration of ion beams

    Get PDF
    We consider methods of charged particle acceleration by means of high-intensity lasers. As an application we discuss a laser booster for heavy ion beams provided, e.g. by the Dubna nuclotron. Simple estimates show that a cascade of crossed laser beams would be necessary to provide additional acceleration to gold ions of the order of GeV/nucleon.Comment: 4 pages, 4 figures, Talk at the Helmholtz International Summer School "Dense Matter in heavy Ion Collisions and Astrophysics", August 21 - September 1, 2006, JINR Dubna, Russia; v2, misprints correcte

    Current state and prospects of protoplast technology and potato somatic hybridization (review)

    Get PDF
    Wild Solanum species have often been used as sources of important agricultural traits, including resistance to various diseases, pests, and abiotic factors. However, their large-scale use in potato breeding is limited by complex barriers of sexual incompatibility with Solanum tuberosum. Fusion of protoplasts enzymatically isolated from somatic cells is one of the approaches to overcoming sexual incompatibility. The diverse nuclear and cytoplasmic traits exhibited by potato somatic hybrids provide new genetic material for breeding programs, which is confirmed by the creation of a large number of somatic hybrids of cultivated potatoes with wild Solanum species. The research in development of somatic potato hybrids by means of protoplast fusion has been carried out for more than 40 years already. In this review, the prospects for the use of this technology in modern potato breeding are considered. Genomic, transcriptomic, and proteomic studies provide further insight into the fundamental processes underlying the somatic hybrids formation, such as cell wall formation, chromosomal rearrangements in fusion products, regeneration, and also make a significant contribution to understanding the processes of genome stabilization. Improvement in the methods of molecular screening of both genome and cytoplasm also contributes to the expansion of the field of application of somatic hybrids in breeding. Finally, it has been shown that somatic hybridization promotes the introgression of important agricultural traits, primarily resistance to pathogens
    • …
    corecore