30 research outputs found

    Reflection of a Rayleigh wave from the edge of a wedge in oblique incidence

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    The reflection of a Rayleigh wave from the edge of a sharp elastic wedge in oblique incidence is aaalyzed. It is shown that the nature of the angular dependence of the modulus of the reflection coeffrcient is strongly affected by the phase shift of the symmetric field mode associated with reflection from a caustic. The results are tested experimentally

    Directivity patterns of a spark source of acoustic waves in a solid

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    The direcrional characteristics of a spark source of acoustic waves in a solid are studied experimentally' The angular dependence of the ampiituJes of longitudinal and shear waves and of Rayleigh surface waves is inuestigated for two principal discharge geometries. A qualitative interpretation of the observed dependences is given

    First results of dust injection in T-10 plasma

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    First results of T-10 injection experiments of the carbon dust particles with 2-10 mm diameter and 40-300 m/s velocity are presented. Different scenarios of the dust injection were tested. The dust particles ablation was studied. An approach for determination of a dust particle penetration length was developed. Measured penetration depths (3-7 cm) are compared with the simulation by the ablation model. The mm range of the separate dust particle diameters derived from the ablation data was close to sizes of the dust injected assuming that an acceleration of the separate particle is similar to the large carbon pellet in the pellet injector.ΠŸΡ€Π΅Π΄ΡΡ‚Π°Π²Π»Π΅Π½ΠΎ ΠΏΠ΅Ρ€ΡˆΡ– Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΈ СкспСримСнтів ΠΏΠΎ Ρ–Π½ΠΆΠ΅ΠΊΡ†Ρ–Ρ— Π²ΡƒΠ³Π»Π΅Ρ†Π΅Π²ΠΈΡ… ΠΏΠΈΠ»ΠΎΠ²ΠΈΡ… часток Π΄Ρ–Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠΌ 2-10 ΠΌΠΊΠΌ Π·Ρ– ΡˆΠ²ΠΈΠ΄ΠΊΠΎΡΡ‚ΡΠΌΠΈ 40-300 ΠΌ/с Ρƒ Π’-10. ΠŸΡ€ΠΎΡ‚Π΅ΡΡ‚ΠΎΠ²Π°Π½ΠΎ Ρ€Ρ–Π·Π½Ρ– сцСнарії Ρ–Π½ΠΆΠ΅ΠΊΡ†Ρ–Ρ— ΠΏΠΈΠ»Ρƒ. ДослідТСно Π²ΠΈΠΏΠ°Ρ€ ΠΏΠΈΠ»ΠΎΠ²ΠΈΡ… часток. Π ΠΎΠ·Ρ€ΠΎΠ±Π»Π΅Π½ΠΎ ΠΏΡ€ΠΈΠ±Π»ΠΈΠ·Π½Ρƒ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΠΊΡƒ визначСння Π³Π»ΠΈΠ±ΠΈΠ½ΠΈ проникнСння ΠΏΠΈΠ»ΠΎΠ²ΠΈΡ… часток. ΠžΠ±ΠΌΡ–Ρ€ΡΠ½Ρ– Π³Π»ΠΈΠ±ΠΈΠ½ΠΈ проникнСння (3-7 см) ΠΏΠΎΡ€Ρ–Π²Π½ΡŽΠ²Π°Π»ΠΈΡΡ Π· Ρ€ΠΎΠ·Ρ€Π°Ρ…ΡƒΠ½ΠΊΠ°ΠΌΠΈ ΠΏΠΎ ΠΌΠΎΠ΄Π΅Π»Ρ– Π²ΠΈΠΏΠ°Ρ€Ρƒ. ΠžΡ†Ρ–Π½Π΅Π½Ρ– ΠΌΡ–ΠΊΡ€ΠΎΠ½Π½Ρ– Π΄Ρ–Π°ΠΌΠ΅Ρ‚Ρ€ΠΈ часток, ΠΎΡ‚Ρ€ΠΈΠΌΠ°Π½Ρ– Π· Π΄Π°Π½ΠΈΡ… ΠΏΠΎ Π²ΠΈΠΏΠ°Ρ€Ρƒ, Ρ” близькими Π΄ΠΎ Ρ€ΠΎΠ·ΠΌΡ–Ρ€Ρ–Π² Ρ–Π½ΠΆΠ΅ΠΊΡ‚ΠΎΠ²Π°Π½ΠΎΠ³ΠΎ ΠΏΠΈΠ»Ρƒ, Ρƒ ΠΏΡ€ΠΈΠΏΡƒΡ‰Π΅Π½Π½Ρ– Ρ‚ΠΎΠ³ΠΎ, Ρ‰ΠΎ ΠΎΠΊΡ€Π΅ΠΌΡ– частки ΠΏΡ€ΠΈΡΠΊΠΎΡ€ΡŽΡŽΡ‚ΡŒΡΡ Ρ‚Π°ΠΊ само, як Ρ– ΠΏΡ€ΠΈ Ρ–Π½ΠΆΠ΅ΠΊΡ†Ρ–Ρ— Π²Π΅Π»ΠΈΠΊΠΈΡ… ΠΏΠ΅Π»Π΅Ρ‚Ρ–Π².ΠŸΡ€Π΅Π΄ΡΡ‚Π°Π²Π»Π΅Π½Ρ‹ ΠΏΠ΅Ρ€Π²Ρ‹Π΅ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ экспСримСнтов ΠΏΠΎ ΠΈΠ½ΠΆΠ΅ΠΊΡ†ΠΈΠΈ ΡƒΠ³Π»Π΅Ρ€ΠΎΠ΄Π½Ρ‹Ρ… ΠΏΡ‹Π»Π΅Π²Ρ‹Ρ… частиц Π΄ΠΈΠ°ΠΌΠ΅Ρ‚Ρ€ΠΎΠΌ 2-10 ΠΌΠΊΠΌ со скоростями 40-300 ΠΌ/с Π² Π’-10. ΠŸΡ€ΠΎΡ‚Π΅ΡΡ‚ΠΈΡ€ΠΎΠ²Π°Π½Ρ‹ Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Π΅ сцСнарии ΠΈΠ½ΠΆΠ΅ΠΊΡ†ΠΈΠΈ ΠΏΡ‹Π»ΠΈ. ИсслСдовано испарСниС ΠΏΡ‹Π»Π΅Π²Ρ‹Ρ… частиц. Π Π°Π·Ρ€Π°Π±ΠΎΡ‚Π°Π½Π° ΠΏΡ€ΠΈΠ±Π»ΠΈΠ·ΠΈΡ‚Π΅Π»ΡŒΠ½Π°Ρ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΠΊΠ° опрСдСлСния Π³Π»ΡƒΠ±ΠΈΠ½Ρ‹ проникновСния ΠΏΡ‹Π»Π΅Π²Ρ‹Ρ… частиц. Π˜Π·ΠΌΠ΅Ρ€Π΅Π½Π½Ρ‹Π΅ Π³Π»ΡƒΠ±ΠΈΠ½Ρ‹ проникновСния (3-7 см) ΡΡ€Π°Π²Π½ΠΈΠ²Π°Π»ΠΈΡΡŒ с расчСтами ΠΏΠΎ ΠΌΠΎΠ΄Π΅Π»ΠΈ испарСния. ΠžΡ†Π΅Π½Π΅Π½Π½Ρ‹Π΅ ΠΌΠΈΠΊΡ€ΠΎΠ½Π½Ρ‹Π΅ Π΄ΠΈΠ°ΠΌΠ΅Ρ‚Ρ€Ρ‹ частиц, ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Π΅ ΠΈΠ· Π΄Π°Π½Π½Ρ‹Ρ… ΠΏΠΎ ΠΈΡΠΏΠ°Ρ€Π΅Π½ΠΈΡŽ, Π±Π»ΠΈΠ·ΠΊΠΈ ΠΊ Ρ€Π°Π·ΠΌΠ΅Ρ€Π°ΠΌ ΠΈΠ½ΠΆΠ΅ΠΊΡ‚ΠΈΡ€ΠΎΠ²Π°Π½Π½ΠΎΠΉ ΠΏΡ‹Π»ΠΈ, Π² ΠΏΡ€Π΅Π΄ΠΏΠΎΠ»ΠΎΠΆΠ΅Π½ΠΈΠΈ Ρ‚ΠΎΠ³ΠΎ, Ρ‡Ρ‚ΠΎ ΠΎΡ‚Π΄Π΅Π»ΡŒΠ½Ρ‹Π΅ частицы ΡƒΡΠΊΠΎΡ€ΡΡŽΡ‚ΡΡ Ρ‚Π°ΠΊ ΠΆΠ΅, ΠΊΠ°ΠΊ ΠΈ ΠΏΡ€ΠΈ ΠΈΠ½ΠΆΠ΅ΠΊΡ†ΠΈΠΈ ΠΊΡ€ΡƒΠΏΠ½Ρ‹Ρ… ΠΏΠ΅Π»Π»Π΅Ρ‚ΠΎΠ²

    Elliptic flow in Pb+Pb collisions at sqrt{s_{NN}} = 2.76 TeV: hybrid model assessment of the first data

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    We analyze the elliptic flow parameter v_2 in Pb+Pb collisions at sqrt{s_{NN}} = 2.76 TeV and in Au+Au collisions at sqrt{s_{NN}} =200 GeV using a hybrid model in which the evolution of the quark gluon plasma is described by ideal hydrodynamics with a state-of-the-art lattice QCD equation of state, and the subsequent hadronic stage by a hadron cascade model. For initial conditions, we employ Monte-Carlo versions of the Glauber and the Kharzeev-Levin-Nardi models and compare results with each other. We demonstrate that the differential elliptic flow v_2(p_T) hardly changes when the collision energy increases, whereas the integrated v_2 increases due to the enhancement of mean transverse momentum. The amount of increase of both v_2 and mean p_T depends significantly on the model of initialization.Comment: 5 pages, 5 figure

    Comissioning of the linear accelerator-injector at the TNK facility

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    The industrial storage facility has been developed and manufactured at the Budker INP SB RAS. It contains an 80 MeV electron linear accelerator-injector and two electron storage rings: the lesser 450 MeV booster ring and the main 2.5 GeV storage ring. In 2002, the work on the accelerator assembling was begun. On December, 25 this year the accelerator was started up, and the current at the linear accelerator output was obtained. The linear accelerator schematic together with a description of the 6 meter long accelerating DAW structure which operates at 2.8 GHz, are presented in the paper. The first results of the accelerator start-up are as follows: the accelerated electron current of ~50 mA with the energy of ~55...60 MeV.Π’Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³Ρ–Ρ‡Π½ΠΈΠΉ Π½Π°ΠΊΠΎΠΏΠΈΡ‡ΡƒΠ²Π°Π»ΡŒΠ½ΠΈΠΉ комплСкс Π±ΡƒΠ² спроСктований Ρ– Π²ΠΈΠ³ΠΎΡ‚ΠΎΠ²Π»Π΅Π½ΠΈΠΉ Ρƒ Π†Π―Π€ Ρ–ΠΌ. Π“.Π†. Π‘ΡƒΠ΄ΠΊΠ΅Ρ€Π° Π‘Π’ РАН. Π’Ρ–Π½ ΠΌΡ–ΡΡ‚ΠΈΡ‚ΡŒ Ρƒ собі інТСктор–лінійний ΠΏΡ€ΠΈΡΠΊΠΎΡ€ΡŽΠ²Π°Ρ‡ Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Ρ–Π² Π· Π΅Π½Π΅Ρ€Π³Ρ–Ρ”ΡŽ Π΄ΠΎ 80 ΠœΠ΅Π’ Ρ– Π΄Π²Π° Π½Π°ΠΊΠΎΠΏΠΈΡ‡ΡƒΠ²Π°Ρ‡Ρ– Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Ρ–Π²: ΠΌΠ°Π»ΠΈΠΉ накопичувач–бустСр Π½Π° Π΅Π½Π΅Ρ€Π³Ρ–ΡŽ 450 ΠœΠ΅Π’ Ρ– основний Π½Π°ΠΊΠΎΠΏΠΈΡ‡ΡƒΠ²Π°Ρ‡ Π½Π° Π΅Π½Π΅Ρ€Π³Ρ–ΡŽ 2.5 Π“Π΅Π’. ΠŸΡ€ΠΈΠ²ΠΎΠ΄ΡΡ‚ΡŒΡΡ Ρ„ΡƒΠ½ΠΊΡ†Ρ–ΠΎΠ½Π°Π»ΡŒΠ½Π° схСма Π»Ρ–Π½Ρ–ΠΉΠ½ΠΎΠ³ΠΎ ΠΏΡ€ΠΈΡΠΊΠΎΡ€ΡŽΠ²Π°Ρ‡Π° ΠΉ опис конструкції ΠΏΡ€ΠΈΡΠΊΠΎΡ€ΡŽΡŽΡ‡ΠΎΡ— структури Ρ–Π· шайбами Ρ– Π΄Ρ–Π°Ρ„Ρ€Π°Π³ΠΌΠ°ΠΌΠΈ довТиною 6 ΠΌ, Ρ‰ΠΎ ΠΏΡ€Π°Ρ†ΡŽΡ” Π½Π° частоті 2.8 Π“Π“Ρ†.ΠŸΡ€Π΅Π΄ΡΡ‚Π°Π²Π»Π΅Π½ΠΎ ΠΏΠ΅Ρ€ΡˆΡ– Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΈ запуску ΠΏΡ€ΠΈΡΠΊΠΎΡ€ΡŽΠ²Π°Ρ‡Π°: ΠΎΡ‚Ρ€ΠΈΠΌΠ°Π½ΠΈΠΉ прискорСний струм Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Ρ–Π² ~50 мА Π· Π΅Π½Π΅Ρ€Π³Ρ–Ρ”ΡŽ ~(55...60) ΠœΠ΅Π’.ВСхнологичСский Π½Π°ΠΊΠΎΠΏΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹ΠΉ комплСкс Π±Ρ‹Π» спроСктирован ΠΈ ΠΈΠ·Π³ΠΎΡ‚ΠΎΠ²Π»Π΅Π½ Π² ИЯЀ ΠΈΠΌ. Π“.И. Π‘ΡƒΠ΄ΠΊΠ΅Ρ€Π° БО РАН. Он Π²ΠΊΠ»ΡŽΡ‡Π°Π΅Ρ‚ Π² сСбя инТСктор–линСйный ΡƒΡΠΊΠΎΡ€ΠΈΡ‚Π΅Π»ΡŒ элСктронов с энСргиСй Π΄ΠΎ 80 ΠœΡΠ’ ΠΈ Π΄Π²Π° накопитСля элСктронов: ΠΌΠ°Π»Ρ‹ΠΉ Π½Π°ΠΊΠΎΠΏΠΈΡ‚Π΅Π»ΡŒβ€“Π±ΡƒΡΡ‚Π΅Ρ€ Π½Π° ΡΠ½Π΅Ρ€Π³ΠΈΡŽ 450 ΠœΡΠ’ ΠΈ основной Π½Π°ΠΊΠΎΠΏΠΈΡ‚Π΅Π»ΡŒ Π½Π° ΡΠ½Π΅Ρ€Π³ΠΈΡŽ 2.5 ГэВ. ΠŸΡ€ΠΈΠ²ΠΎΠ΄ΡΡ‚ΡΡ Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΎΠ½Π°Π»ΡŒΠ½Π°Ρ схСма Π»ΠΈΠ½Π΅ΠΉΠ½ΠΎΠ³ΠΎ ускоритСля ΠΈ описаниС конструкции ΡƒΡΠΊΠΎΡ€ΡΡŽΡ‰Π΅ΠΉ структуры с шайбами ΠΈ Π΄ΠΈΠ°Ρ„Ρ€Π°Π³ΠΌΠ°ΠΌΠΈ Π΄Π»ΠΈΠ½ΠΎΠΉ 6 ΠΌΠ΅Ρ‚Ρ€ΠΎΠ², Ρ€Π°Π±ΠΎΡ‚Π°ΡŽΡ‰Π΅ΠΉ Π½Π° частотС 2.8 Π“Π“Ρ†. ΠŸΡ€Π΅Π΄ΡΡ‚Π°Π²Π»Π΅Π½Ρ‹ ΠΏΠ΅Ρ€Π²Ρ‹Π΅ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ запуска ускоритСля: ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½ ускорСнный Ρ‚ΠΎΠΊ элСктронов ~50 ΠΌA с энСргиСй ~(55...60) ΠœΡΠ’

    Nucleosomes in gene regulation: theoretical approaches

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    This work reviews current theoretical approaches of biophysics and bioinformatics for the description of nucleosome arrangements in chromatin and transcription factor binding to nucleosomal organized DNA. The role of nucleosomes in gene regulation is discussed from molecular-mechanistic and biological point of view. In addition to classical problems of this field, actual questions of epigenetic regulation are discussed. The authors selected for discussion what seem to be the most interesting concepts and hypotheses. Mathematical approaches are described in a simplified language to attract attention to the most important directions of this field

    Efficient excitation of Rayleigh waves by a strong shock wave initiated by a spark in air

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    Efficient excitation of Rayleigh waves by a strong shock wave initiated by a spark in ai

    Waveforms of acoustic pulses generated in a solid by a spark discharge

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    The waveforms of longitudinal and Rayleigh wave pulses generated in a glass sample by a spark discharge are measured
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