1,341 research outputs found

    Zel'dovich states with very small mass and charge in nonlinear electrodynamics coupled to gravity

    Full text link
    It is shown that in non-linear electrodynamics (in particular, Born-Infeld one) in the framework of general relativity there exist "weakly singular" configurations such that (i) the proper mass M is finite in spite of divergences of the energy density, (ii) the electric charge q and Schwarzschild mass m ~ q can be made as small as one likes, (iv) all field and energy distributions are concentrated in the core region. This region has an almost zero surface area but a finite longitudinal size L=2M. Such configurations can be viewed as a new version of a classical analogue of an elementary particle.Comment: 11 pages. 1 reference added. To appear in Grav. Cosm

    Bunch-excited wakefield in dielectric waveguide with hollow plasma channel

    Full text link
    Wakefield excitation by a single relativistic electron bunch in a plasma-dielectric accelerating structure has been studied both analytically and numerically. The structure represents a dielectric-loaded cylindrical metal waveguide, which has partially plasma-filled channel (the hollow plasma channel) to transport charged particles. Assuming the linear regime of excitation, analytical expressions have been derived for the longitudinal and radial wakefields generated by a finite-size electron bunch. Axial profiles of wakefield component amplitudes have been studied, and their mode and spectrum analyses have been performed. Furthermore, the electron bunch-driven wakefield excitation has been PIC-simulated numerically for the quasi-linear regime. The comparative analysis of the data resulting from analytical studies and the ones obtained by numerical simulation has demonstrated qualitative agreement between the results

    Parity violating cylindrical shell in the framework of QED

    Full text link
    We present calculations of Casimir energy (CE) in a system of quantized electromagnetic (EM) field interacting with an infinite circular cylindrical shell (which we call `the defect'). Interaction is described in the only QFT-consistent way by Chern-Simon action concentrated on the defect, with a single coupling constant aa. For regularization of UV divergencies of the theory we use % physically motivated Pauli-Villars regularization of the free EM action. The divergencies are extracted as a polynomial in regularization mass MM, and they renormalize classical part of the surface action. We reveal the dependence of CE on the coupling constant aa. Corresponding Casimir force is attractive for all values of aa. For aβ†’βˆža\to\infty we reproduce the known results for CE for perfectly conducting cylindrical shell first obtained by DeRaad and Milton.Comment: Typos corrected. Some references adde

    The banding in serpentinites and its influence on character of talc-magnesite and magnesite mineralization (natural and experimental data)

    Get PDF
    The geological setting of some banded talc-magnesite ores and magnesites was studied in the field (Urals, Russia; Finland, East Iran). Talc-magnesite and magnesite ores occur in ultramafic rocks. Experimental methods were used in order to determine the influence of physico-mechanical parameters on the formation of banded structures in talc-magnesite rocks and magnesites. Experiments were carried out with axial compression up to 10 kbar and confining pressure 2, 4, 6 and 8 kbars at room temperature. The samples were chemically analyzed using a Philips Analytical PW 2400 authomatic XRF Spectrometer and a scanning electron microscope (SEM). Some analyses were made with a "Camebax SX-50" electron microprobe, using an accelerating voltage of 20 kilovolts for all elements with a sample current of 20 nanoamps. X-ray method for phase identification was used. Structure peculiarities of rocks prior to the experiment and after were studied by optical methods in polished sections and thin sections. It was shown, that banding in talc-magnesite stone and magnesites are inherited from banded serpentinites and can affect on distribution and composition rock-forming minerals

    The behaviours of Mg and Ca in some types of ultramaphic alkaline melts in the presence of H 2 O at high temperature and pressure (the experimental data)

    Get PDF
    The sample has been investigated, which was composed of olivine-melilite rock from the south-western part of the Kugda intrusion, situated in the eastern margin of the Maimecha-Kotuiskay alkaline- ultramaphic province (northern part of Siberia platform). The experiments were carried out using a high-pressure apparatus of the "piston-cylinder" type. The pressure was 5-15 kb and the temperature -800-1250 0 C. The water content in the system was 3 and 9 wt. All experiments were carried out in hermetically sealed Pt or Au ampoules. The samples were chemically analyzed using a scanning electron microscope (SEM). Besides, the chemical composition of the experimental phases was determined by means of more than 40 electron microprobe in 20 experimental samples. For phase identification the X-ray method was used too. The structural peculiarities of rocks and mineral compositions were studied by optical methods in polished and thin sections prior and after the experiment. It was shown that at pressures above 7.5-8 kb the olivine-melilite melt is separated into two melts: pyroxenite and melilite. Most part of Mg in this system was concentrated in a high temperature phase of diopside type. The remaining melt was depleted of Mg and enriched by Ca. The mineralization vapour practically did not contain Mg. The main components of the mineralization vapour were Ca, Na, Si and Fe

    ВлияниС рСлаксационных процСссов ΠΏΡ€ΠΈ Π΄Π΅Ρ„ΠΎΡ€ΠΌΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠΈ Π½Π° элСктричСскоС сопротивлСниС ΠΏΠΎΠ»ΠΈΠΏΡ€ΠΎΠΏΠΈΠ»Π΅Π½ΠΎΠ²Ρ‹Ρ… ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡ‚ΠΎΠ² с тСхничСским ΡƒΠ³Π»Π΅Ρ€ΠΎΠ΄ΠΎΠΌ

    Get PDF
    Objectives. To study the relationship between bending deformation and the change in the electrical resistance of carbon black polypropylene composites.Methods. Conductive polypropylene composites filled with carbon black UM-76 were investigated. The samples were deformed and kept under constant bending at temperatures of 20–155 Β°C.Results. The deformation of the samples led to a reversible increase in their electrical resistance, while subsequent holding of the samples in the deformed state was accompanied by an exponential drop in their electrical resistance. The average times and activation energies of the electrical relaxation of the deformed polypropylene composites were calculated (30–32 kJ/mol) and compared with similar characteristics of polyethylene composites (15–16 kJ/mol).Conclusions. The electrical resistance relaxation of deformed carbon black polypropylene composites at elevated temperatures is similar to their stress relaxation. The average times and activation energies of the electrical relaxation of deformed polypropylene composites are comparable with similar data on their mechanical relaxation. It was found that these electrical and mechanical phenomena are based on the same underlying physical processes.Π¦Π΅Π»ΠΈ. Π Π°Π±ΠΎΡ‚Π° посвящСна ΠΈΠ·ΡƒΡ‡Π΅Π½ΠΈΡŽ влияния Π΄Π΅Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΠΈ ΠΈΠ·Π³ΠΈΠ±Π° ΠΏΡ€ΠΈ ΠΏΠΎΠ²Ρ‹ΡˆΠ΅Π½Π½Ρ‹Ρ… Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π°Ρ… Π½Π° ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ элСктричСского сопротивлСния элСктропроводящих ΠΏΠΎΠ»ΠΈΠΏΡ€ΠΎΠΏΠΈΠ»Π΅Π½ΠΎΠ²Ρ‹Ρ… ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡ‚ΠΎΠ², Π½Π°ΠΏΠΎΠ»Π½Π΅Π½Π½Ρ‹Ρ… тСхничСским ΡƒΠ³Π»Π΅Ρ€ΠΎΠ΄ΠΎΠΌ.ΠœΠ΅Ρ‚ΠΎΠ΄Ρ‹. ИсслСдовались ΠΏΠΎΠ»ΠΈΠΏΡ€ΠΎΠΏΠΈΠ»Π΅Π½ΠΎΠ²Ρ‹Π΅ ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡ‚Ρ‹ с тСхничСским ΡƒΠ³Π»Π΅Ρ€ΠΎΠ΄ΠΎΠΌ УМ-76. ΠžΠ±Ρ€Π°Π·Ρ†Ρ‹ изгибались ΠΈ Π²Ρ‹Π΄Π΅Ρ€ΠΆΠΈΠ²Π°Π»ΠΈΡΡŒ ΠΏΡ€ΠΈ Π·Π°Π΄Π°Π½Π½ΠΎΠΌ ΠΏΡ€ΠΎΠ³ΠΈΠ±Π΅ Π² ΠΈΠ½Ρ‚Π΅Ρ€Π²Π°Π»Π΅ 20–155 Β°C.Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹. ΠŸΡ€ΠΈ Π΄Π΅Ρ„ΠΎΡ€ΠΌΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠΈ ΠΎΠ±Ρ€Π°Π·Ρ†ΠΎΠ² наблюдался ΠΎΠ±Ρ€Π°Ρ‚ΠΈΠΌΡ‹ΠΉ рост элСктричСского сопротивлСния. ΠŸΠΎΡΠ»Π΅Π΄ΡƒΡŽΡ‰Π°Ρ Π²Ρ‹Π΄Π΅Ρ€ΠΆΠΊΠ° ΠΎΠ±Ρ€Π°Π·Ρ†ΠΎΠ² Π² Π΄Π΅Ρ„ΠΎΡ€ΠΌΠΈΡ€ΠΎΠ²Π°Π½Π½ΠΎΠΌ состоянии ΡΠΎΠΏΡ€ΠΎΠ²ΠΎΠΆΠ΄Π°Π»Π°ΡΡŒ ΡΠΊΡΠΏΠΎΠ½Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½Ρ‹ΠΌ ΠΏΠ°Π΄Π΅Π½ΠΈΠ΅ΠΌ ΠΈΡ… элСктричСского сопротивлСния. Π‘Ρ‹Π»ΠΈ рассчитаны срСдниС Π²Ρ€Π΅ΠΌΠ΅Π½Π° ΠΈ энСргия Π°ΠΊΡ‚ΠΈΠ²Π°Ρ†ΠΈΠΈ элСктричСской рСлаксации Π΄Π΅Ρ„ΠΎΡ€ΠΌΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹Ρ… ΠΏΠΎΠ»ΠΈΠΏΡ€ΠΎΠΏΠΈΠ»Π΅Π½ΠΎΠ²Ρ‹Ρ… ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡ‚ΠΎΠ² (30–32 ΠΊΠ”ΠΆ/моль), Π° Ρ‚Π°ΠΊΠΆΠ΅ ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½ΠΎ ΠΈΡ… сравнСниС с Π°Π½Π°Π»ΠΎΠ³ΠΈΡ‡Π½Ρ‹ΠΌΠΈ характСристиками полиэтилСновых ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡ‚ΠΎΠ² (ΠΎΠΊΠΎΠ»ΠΎ 14–16 ΠΊΠ”ΠΆ/моль).Π’Ρ‹Π²ΠΎΠ΄Ρ‹. ΠŸΡ€ΠΈ мСханичСском Π΄Π΅Ρ„ΠΎΡ€ΠΌΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠΈ элСктропроводящих ΠΏΠΎΠ»ΠΈΠΏΡ€ΠΎΠΏΠΈΠ»Π΅Π½ΠΎΠ²Ρ‹Ρ… ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡ‚ΠΎΠ² с тСхничСским ΡƒΠ³Π»Π΅Ρ€ΠΎΠ΄ΠΎΠΌ, Π² Ρ‚ΠΎΠΌ числС ΠΏΡ€ΠΈ ΠΏΠΎΠ²Ρ‹ΡˆΠ΅Π½Π½Ρ‹Ρ… Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π°Ρ…, Ρ…Π°Ρ€Π°ΠΊΡ‚Π΅Ρ€ рСлаксации элСктричСского сопротивлСния Π°Π½Π°Π»ΠΎΠ³ΠΈΡ‡Π΅Π½ Ρ…Π°Ρ€Π°ΠΊΡ‚Π΅Ρ€Ρƒ рСлаксации мСханичСского напряТСния. Π‘Ρ€Π΅Π΄Π½ΠΈΠ΅ Π²Ρ€Π΅ΠΌΠ΅Π½Π° ΠΈ энСргия Π°ΠΊΡ‚ΠΈΠ²Π°Ρ†ΠΈΠΈ элСктричСской рСлаксации Π΄Π΅Ρ„ΠΎΡ€ΠΌΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹Ρ… ΠΏΠΎΠ»ΠΈΠΏΡ€ΠΎΠΏΠΈΠ»Π΅Π½ΠΎΠ²Ρ‹Ρ… ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡ‚ΠΎΠ² сопоставимы с Π°Π½Π°Π»ΠΎΠ³ΠΈΡ‡Π½Ρ‹ΠΌΠΈ показатСлями для мСханичСской рСлаксации. Π­Ρ‚ΠΎ ΡƒΠΊΠ°Π·Ρ‹Π²Π°Π΅Ρ‚ Π½Π° ΠΎΠ±Ρ‰ΠΈΠΉ ΠΌΠ΅Ρ…Π°Π½ΠΈΠ·ΠΌ этих процСссов

    Hadron and Quark Form Factors in the Relativistic Harmonic Oscillator Model

    Full text link
    Nucleon, pion and quark form factors are studied within the relativistic harmonic oscillator model including the quark spin. It is shown that the nucleon charge, magnetic and axial form factors and the pion charge form factor can be explained with one oscillator parameter if one accounts for the scaling rule and the size of the constituent quarks.Comment: 9 pages, Latex, 3 postscript figures, DFTT 8/9

    The Boltzmann equation for colourless plasmons in hot QCD plasma. Semiclassical approximation

    Full text link
    Within the framework of the semiclassical approximation, we derive the Boltzmann equation describing the dynamics of colorless plasmons in a hot QCD plasma. The probability of the plasmon-plasmon scattering at the leading order in the coupling constant is obtained. This probability is gauge-independent at least in the class of the covariant and temporal gauges. It is noted that the structure of the scattering kernel possesses important qualitative difference from the corresponding one in the Abelian plasma, in spite of the fact that we focused our study on the colorless soft excitations. It is shown that four-plasmon decay is suppressed by the power of gg relative to the process of nonlinear scattering of plasmons by thermal particles at the soft momentum scale. It is stated that the former process becomes important in going to the ultrasoft region of the momentum scale.Comment: 41, LaTeX, minor changes, identical to published versio

    Quark-antiquark composite systems: the Bethe-Salpeter equation in the spectral-integration technique

    Get PDF
    The Bethe-Salpeter equations for the light-quark composite systems, q q-bar, are written in terms of spectral integrals. For the q q-bar -mesons characterized by the mass M, spin J and radial quantum number n, the equations are presented for the following (n,M^2)-trajectories: pi_J, eta_J, a_J, f_J, rho_J, omega_J, h_J and b_J.Comment: 42 pages, 5 figures, typos correcte
    • …
    corecore