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    "Π—Π΅Π»Π΅Π½ΠΈΠΉ" синтСз Π΅Ρ‚ΠΈΠ»ΠΎΠ²ΠΈΡ… СстСрів 4-гідрокси-2-оксо-1,2-Π΄ΠΈΠ³Ρ–Π΄Ρ€ΠΎΡ…Ρ–Π½ΠΎΠ»Ρ–Π½-3-ΠΊΠ°Ρ€Π±ΠΎΠ½ΠΎΠ²ΠΈΡ… кислот

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    One of the most convenient methods for obtaining ethyl of N-substituted 4-hydroxy-2-oxo-1,2-dihydroquinoline-3-carboxylates and their tricyclic analogues at present is condensation of the corresponding anilines with triethyl methanetricarboxylate. In spite of the fact that there are many methods describing the successful performance of this reaction in conditions of laboratory, but unfortunately, all of them appeared to be completely unusable for large production for a variety of reasons. The study of quality of the esters of 4-hydroxy-2-oxo-1,2-dihydroquinoline-3-carboxylic acids by HPLC has shown that all of them contain from 2.4 to 5.6% of specific admixtures of 4-hydroxy-1,2-dihydroquinolin- 2-ones. In laboratory conditions these amounts can be neglected, but for industrial manufacture they can turn into great losses. The source of admixtures of 4-hydroxy-1,2-dihydroquinolin-2-ones appearing in crude esters can be only the esters themselves. It is obvious that ester grouping is partially destroyed not in the process of separation of the final products, but during the course of the basic reaction. It has been experimentally proven that the cause of contamination of the target products with the admixtures of the corresponding 4-hydroxy-1,2-dihydroquinolin-2-ones is water, which is present in reagents. Applying the principles of Β«green chemistryΒ» the alternative for carrying out the syntheses of ethyl 4-hydroxy-2-oxo-1,2-dihydroquinoline-3-carboxylates adapted for industrial manufacture has been suggested on the basis of N-substituted anilines and triethyl methanetricarboxylate.Одним ΠΈΠ· Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ ΡƒΠ΄ΠΎΠ±Π½Ρ‹Ρ… способов получСния этиловых эфиров N-Π·Π°ΠΌΠ΅Ρ‰Ρ‘Π½Π½Ρ‹Ρ… 4-гидрокси-2-оксо-1,2-Π΄ΠΈΠ³ΠΈΠ΄Ρ€ΠΎΡ…ΠΈΠ½ΠΎΠ»ΠΈΠ½-3-ΠΊΠ°Ρ€Π±ΠΎΠ½ΠΎΠ²Ρ‹Ρ… кислот ΠΈ ΠΈΡ… трицикличСских Π°Π½Π°Π»ΠΎΠ³ΠΎΠ² Π² настоящСС врСмя остаётся кондСнсация ΡΠΎΠΎΡ‚Π²Π΅Ρ‚ΡΡ‚Π²ΡƒΡŽΡ‰ΠΈΡ… Π°Π½ΠΈΠ»ΠΈΠ½ΠΎΠ² с триэтилмСтантрикарбоксилатом. НСсмотря Π½Π° Ρ‚ΠΎ, Ρ‡Ρ‚ΠΎ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠ² ΡƒΡΠΏΠ΅ΡˆΠ½ΠΎΠ³ΠΎ провСдСния этой Ρ€Π΅Π°ΠΊΡ†ΠΈΠΈ Π² Π»Π°Π±ΠΎΡ€Π°Ρ‚ΠΎΡ€Π½Ρ‹Ρ… условиях описано достаточно ΠΌΠ½ΠΎΠ³ΠΎ, всС ΠΎΠ½ΠΈ, ΠΊ соТалСнию, ΠΏΠΎ Ρ€Π°Π·Π½Ρ‹ΠΌ ΠΏΡ€ΠΈΡ‡ΠΈΠ½Π°ΠΌ оказались ΡΠΎΠ²Π΅Ρ€ΡˆΠ΅Π½Π½ΠΎ Π½Π΅ΠΏΡ€ΠΈΠ³ΠΎΠ΄Π½Ρ‹ΠΌΠΈ для ΠΊΡ€ΡƒΠΏΠ½ΠΎΠ³ΠΎ производства. Π˜Π·ΡƒΡ‡Π΅Π½ΠΈΠ΅ качСства ΠΏΠΎΠ»ΡƒΡ‡Π°Π΅ΠΌΡ‹Ρ… слоТных эфиров 4-гидрокси-2-оксо-1,2-Π΄ΠΈΠ³ΠΈΠ΄Ρ€ΠΎΡ…ΠΈΠ½ΠΎΠ»ΠΈΠ½-3-ΠΊΠ°Ρ€Π±ΠΎΠ½ΠΎΠ²Ρ‹Ρ… кислот ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ Π’Π­Π–Π₯ ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΎ, Ρ‡Ρ‚ΠΎ всС ΠΎΠ½ΠΈ содСрТат ΠΎΡ‚ 2,4 Π΄ΠΎ 5,6% спСцифичСских примСсСй 4-гидрокси-1,2-Π΄ΠΈΠ³ΠΈΠ΄Ρ€ΠΎΡ…ΠΈΠ½ΠΎΠ»ΠΈΠ½-2-ΠΎΠ½ΠΎΠ². Π’ Π»Π°Π±ΠΎΡ€Π°Ρ‚ΠΎΡ€Π½ΠΎΠΉ ΠΏΡ€Π°ΠΊΡ‚ΠΈΠΊΠ΅ этими количСствами ΠΌΠΎΠΆΠ½ΠΎ ΠΏΡ€Π΅Π½Π΅Π±Ρ€Π΅Ρ‡ΡŒ, Π½ΠΎ для ΠΏΡ€ΠΎΠΌΡ‹ΡˆΠ»Π΅Π½Π½ΠΎΠ³ΠΎ производства ΠΎΠ½ΠΈ ΠΌΠΎΠ³ΡƒΡ‚ ΠΎΠ±Π΅Ρ€Π½ΡƒΡ‚ΡŒΡΡ Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹ΠΌΠΈ потСрями. Π˜ΡΡ‚ΠΎΡ‡Π½ΠΈΠΊΠΎΠΌ появлСния Π² Π½Π΅ΠΎΡ‡ΠΈΡ‰Π΅Π½Π½Ρ‹Ρ… эфирах примСсСй 4-гидрокси-1,2-Π΄ΠΈΠ³ΠΈΠ΄Ρ€ΠΎΡ…ΠΈΠ½ΠΎΠ»ΠΈΠ½-2-ΠΎΠ½ΠΎΠ² ΠΌΠΎΠ³ΡƒΡ‚ Π±Ρ‹Ρ‚ΡŒ Ρ‚ΠΎΠ»ΡŒΠΊΠΎ сами эти эфиры. ΠžΡ‡Π΅Π²ΠΈΠ΄Π½ΠΎ слоТноэфирная Π³Ρ€ΡƒΠΏΠΏΠΈΡ€ΠΎΠ²ΠΊΠ° частично Ρ€Π°Π·Ρ€ΡƒΡˆΠ°Π΅Ρ‚ΡΡ Π½Π΅ ΠΏΡ€ΠΈ Π²Ρ‹Π΄Π΅Π»Π΅Π½ΠΈΠΈ ΠΊΠΎΠ½Π΅Ρ‡Π½Ρ‹Ρ… ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚ΠΎΠ², Π° Π΅Ρ‰Ρ‘ Π² процСссС провСдСния основной Ρ€Π΅Π°ΠΊΡ†ΠΈΠΈ. Π­ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½ΠΎ Π΄ΠΎΠΊΠ°Π·Π°Π½ΠΎ, Ρ‡Ρ‚ΠΎ ΠΏΡ€ΠΈΡ‡ΠΈΠ½ΠΎΠΉ загрязнСния Ρ†Π΅Π»Π΅Π²Ρ‹Ρ… ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚ΠΎΠ² примСсями ΡΠΎΠΎΡ‚Π²Π΅Ρ‚ΡΡ‚Π²ΡƒΡŽΡ‰ΠΈΡ… 4-гидрокси-1,2-Π΄ΠΈΠ³ΠΈΠ΄Ρ€ΠΎΡ…ΠΈΠ½ΠΎΠ»ΠΈΠ½-2-ΠΎΠ½ΠΎΠ² являСтся ΠΏΡ€ΠΈΡΡƒΡ‚ΡΡ‚Π²ΡƒΡŽΡ‰Π°Ρ Π² Ρ€Π΅Π°Π³Π΅Π½Ρ‚Π°Ρ… Π²ΠΎΠ΄Π°. Π ΡƒΠΊΠΎΠ²ΠΎΠ΄ΡΡ‚Π²ΡƒΡΡΡŒ ΠΏΡ€ΠΈΠ½Ρ†ΠΈΠΏΠ°ΠΌΠΈ Β«Π·Π΅Π»Ρ‘Π½ΠΎΠΉ Ρ…ΠΈΠΌΠΈΠΈΒ», ΠΌΡ‹ ΠΏΡ€Π΅Π΄Π»ΠΎΠΆΠΈΠ»ΠΈ Π°Π΄Π°ΠΏΡ‚ΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹ΠΉ ΠΏΠΎΠ΄ ΠΏΡ€ΠΎΠΌΡ‹ΡˆΠ»Π΅Π½Π½ΠΎΠ΅ производство Π²Π°Ρ€ΠΈΠ°Π½Ρ‚ провСдСния синтСзов этиловых эфиров 4-гидрокси-2-оксо-1,2-Π΄ΠΈΠ³ΠΈΠ΄Ρ€ΠΎΡ…ΠΈΠ½ΠΎΠ»ΠΈΠ½-3-ΠΊΠ°Ρ€Π±ΠΎΠ½ΠΎΠ²Ρ‹Ρ… кислот Π½Π° основС N-Π·Π°ΠΌΠ΅Ρ‰Ρ‘Π½Π½Ρ‹Ρ… Π°Π½ΠΈΠ»ΠΈΠ½ΠΎΠ² ΠΈ триэтилмСтантрикарбоксилата.Одним Π· Π½Π°ΠΉΠ±Ρ–Π»ΡŒΡˆ Π·Ρ€ΡƒΡ‡Π½ΠΈΡ… способів одСрТання Π΅Ρ‚ΠΈΠ»ΠΎΠ²ΠΈΡ… СстСрів N-Π·Π°ΠΌΡ–Ρ‰Π΅Π½ΠΈΡ… 4-гідрокси-2-оксо-1,2-Π΄ΠΈΠ³Ρ–Π΄Ρ€ΠΎΡ…Ρ–Π½ΠΎΠ»Ρ–Π½-3-ΠΊΠ°Ρ€Π±ΠΎΠ½ΠΎΠ²ΠΈΡ… кислот Ρ‚Π° Ρ—Ρ… Ρ‚Ρ€ΠΈΡ†ΠΈΠΊΠ»Ρ–Ρ‡Π½ΠΈΡ… Π°Π½Π°Π»ΠΎΠ³Ρ–Π² Π½Π° Ρ‚Π΅ΠΏΠ΅Ρ€Ρ–ΡˆΠ½Ρ–ΠΉ час Π·Π°Π»ΠΈΡˆΠ°Ρ”Ρ‚ΡŒΡΡ кондСнсація Π²Ρ–Π΄ΠΏΠΎΠ²Ρ–Π΄Π½ΠΈΡ… Π°Π½Ρ–Π»Ρ–Π½Ρ–Π² Π· триСтилмСтантрикарбоксилатом. ΠΠ΅Π·Π²Π°ΠΆΠ°ΡŽΡ‡ΠΈ Π½Π° Ρ‚Π΅, Ρ‰ΠΎ ΠΌΠ΅Ρ‚ΠΎΠ΄Ρ–Π² ΡƒΡΠΏΡ–ΡˆΠ½ΠΎΠ³ΠΎ провСдСння Ρ†Ρ–Ρ”Ρ— Ρ€Π΅Π°ΠΊΡ†Ρ–Ρ— Π² Π»Π°Π±ΠΎΡ€Π°Ρ‚ΠΎΡ€Π½ΠΈΡ… ΡƒΠΌΠΎΠ²Π°Ρ… описано Π΄ΠΎΡΠΈΡ‚ΡŒ Π±Π°Π³Π°Ρ‚ΠΎ, всі Π²ΠΎΠ½ΠΈ, Π½Π° Таль, Π· Ρ€Ρ–Π·Π½ΠΈΡ… ΠΏΡ€ΠΈΡ‡ΠΈΠ½ виявились зовсім Π½Π΅ΠΏΡ€ΠΈΠ΄Π°Ρ‚Π½ΠΈΠΌΠΈ для ΠΌΠ°ΡΡˆΡ‚Π°Π±Π½ΠΎΠ³ΠΎ Π²ΠΈΡ€ΠΎΠ±Π½ΠΈΡ†Ρ‚Π²Π°. ВивчСння якості ΠΎΠ΄Π΅Ρ€ΠΆΡƒΠ²Π°Π½ΠΈΡ… СстСрів 4-гідрокси-2- оксо-1,2-Π΄ΠΈΠ³Ρ–Π΄Ρ€ΠΎΡ…Ρ–Π½ΠΎΠ»Ρ–Π½-3-ΠΊΠ°Ρ€Π±ΠΎΠ½ΠΎΠ²ΠΈΡ… кислот ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ Π’Π•Π Π₯ ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΎ, Ρ‰ΠΎ всі Π²ΠΎΠ½ΠΈ ΠΌΡ–ΡΡ‚ΡΡ‚ΡŒ Π²Ρ–Π΄ 2,4 Π΄ΠΎ 5,6% спСцифічних Π΄ΠΎΠΌΡ–ΡˆΠΎΠΊ 4-гідрокси-1,2-Π΄ΠΈΠ³Ρ–Π΄Ρ€ΠΎΡ…Ρ–Π½ΠΎΠ»Ρ–Π½-2-ΠΎΠ½Ρ–Π². Π£ Π»Π°Π±ΠΎΡ€Π°Ρ‚ΠΎΡ€Π½Ρ–ΠΉ ΠΏΡ€Π°ΠΊΡ‚ΠΈΡ†Ρ– Ρ‚Π°ΠΊΠΈΠΌΠΈ ΠΊΡ–Π»ΡŒΠΊΠΎΡΡ‚ΡΠΌΠΈ ΠΌΠΎΠΆΠ½Π° Π·Π½Π΅Ρ…Ρ‚ΡƒΠ²Π°Ρ‚ΠΈ, Π°Π»Π΅ для промислового Π²ΠΈΡ€ΠΎΠ±Π½ΠΈΡ†Ρ‚Π²Π° Π²ΠΎΠ½ΠΈ ΠΌΠΎΠΆΡƒΡ‚ΡŒ обСрнутися Π·Π½Π°Ρ‡Π½ΠΈΠΌΠΈ Π²Ρ‚Ρ€Π°Ρ‚Π°ΠΌΠΈ. Π”ΠΆΠ΅Ρ€Π΅Π»ΠΎΠΌ появи Π² Π½Π΅ΠΎΡ‡ΠΈΡ‰Π΅Π½ΠΈΡ… СстСрах Π΄ΠΎΠΌΡ–ΡˆΠΎΠΊ 4-гідрокси-1,2-Π΄ΠΈΠ³Ρ–Π΄Ρ€ΠΎΡ…Ρ–Π½ΠΎΠ»Ρ–Π½-2-ΠΎΠ½Ρ–Π² ΠΌΠΎΠΆΡƒΡ‚ΡŒ Π±ΡƒΡ‚ΠΈ Ρ‚Ρ–Π»ΡŒΠΊΠΈ самі Ρ†Ρ– СстСри. ΠžΡ‡Π΅Π²ΠΈΠ΄Π½ΠΎ СстСрнС угрупування частково Ρ€ΠΎΠ·ΠΊΠ»Π°Π΄Π°Ρ”Ρ‚ΡŒΡΡ Π½Π΅ ΠΏΡ€ΠΈ Π²ΠΈΠ΄Ρ–Π»Π΅Π½Π½Ρ– ΠΊΡ–Π½Ρ†Π΅Π²ΠΈΡ… ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚Ρ–Π², Π° Ρ‰Π΅ Π² процСсі провСдСння основної Ρ€Π΅Π°ΠΊΡ†Ρ–Ρ—. Π•ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½ΠΎ Π΄ΠΎΠ²Π΅Π΄Π΅Π½ΠΎ, Ρ‰ΠΎ ΠΏΡ€ΠΈΡ‡ΠΈΠ½ΠΎΡŽ забруднСння Ρ†Ρ–Π»ΡŒΠΎΠ²ΠΈΡ… ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚Ρ–Π² спСцифічними Π΄ΠΎΠΌΡ–ΡˆΠΊΠ°ΠΌΠΈ Π²Ρ–Π΄ΠΏΠΎΠ²Ρ–Π΄Π½ΠΈΡ… 4-гідрокси-1,2-Π΄ΠΈΠ³Ρ–Π΄Ρ€ΠΎΡ…Ρ–Π½ΠΎΠ»Ρ–Π½-2-ΠΎΠ½Ρ–Π² Ρ” присутня Π² Ρ€Π΅Π°Π³Π΅Π½Ρ‚Π°Ρ… Π²ΠΎΠ΄Π°. ΠšΠ΅Ρ€ΡƒΡŽΡ‡ΠΈΡΡŒ ΠΏΡ€ΠΈΠ½Ρ†ΠΈΠΏΠ°ΠΌΠΈ Β«Π·Π΅Π»Π΅Π½ΠΎΡ— Ρ…Ρ–ΠΌΡ–Ρ—Β», ΠΌΠΈ Π·Π°ΠΏΡ€ΠΎΠΏΠΎΠ½ΡƒΠ²Π°Π»ΠΈ Π°Π΄Π°ΠΏΡ‚ΠΎΠ²Π°Π½ΠΈΠΉ ΠΏΡ–Π΄ промисловС Π²ΠΈΡ€ΠΎΠ±Π½ΠΈΡ†Ρ‚Π²ΠΎ Π²Π°Ρ€Ρ–Π°Π½Ρ‚ провСдСння синтСзів Π΅Ρ‚ΠΈΠ»ΠΎΠ²ΠΈΡ… СстСрів 4-гідрокси-2-оксо-1,2-Π΄ΠΈΠ³Ρ–Π΄Ρ€ΠΎΡ…Ρ–Π½ΠΎΠ»Ρ–Π½-3-ΠΊΠ°Ρ€Π±ΠΎΠ½ΠΎΠ²ΠΈΡ… кислот Π½Π° основі N-Π·Π°ΠΌΡ–Ρ‰Π΅Π½ΠΈΡ… Π°Π½Ρ–Π»Ρ–Π½Ρ–Π² Ρ‚Π° триСтилмСтантрикарбоксилату

    Clustering in light nuclei in fragmentation above 1 A GeV

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    The relativistic invariant approach is applied to analyzing the 3.3 A GeV 22^{22}Ne fragmentation in a nuclear track emulsion. New results on few-body dissociations have been obtained from the emulsion exposures to 2.1 A GeV 14^{14}N and 1.2 A GeV 9^{9}Be nuclei. It can be asserted that the use of the invariant approach is an effective means of obtaining conclusions about the behavior of systems involving a few He nuclei at a relative energy close to 1 MeV per nucleon. The first observations of fragmentation of 1.2 A GeV 8^{8}B and 9^{9}C nuclei in emulsion are described. The presented results allow one to justify the development of few-body aspects of nuclear astrophysics.Comment: 7 pages, 8 figures, 3 tables, Nuclear Physics in Astrophysics-2, 16-20 May, 2005 (ATOMKI), Debrecen, Hungar

    Double-spiral magnetic structure of the Fe/Cr multilayer revealed by nuclear resonance scattering

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    We have studied the magnetization depth profiles in a [57Fe(dFe)/Cr(dCr)]x30 multilayer with ultrathin Fe layers and nominal thickness of the chromium spacers dCr 2.0 nm using nuclear resonance scattering of synchrotron radiation. The presence of a broad pure-magnetic half-order (1/2) Bragg reflection has been detected at zero external field. The joint fit of the reflectivity curves and Mossbauer spectra of reflectivity measured near the critical angle and at the "magnetic" peak reveals that the magnetic structure of the multilayer is formed by two spirals, one in the odd and another one in the even iron layers, with the opposite signs of rotation. The double-spiral structure starts from the surface with the almost antiferromagnetic alignment of the adjacent Fe layers. The rotation of the two spirals leads to nearly ferromagnetic alignment of the two magnetic subsystems at some depth, where the sudden turn of the magnetic vectors by ~180 deg (spin-flop) appears, and both spirals start to rotate in opposite directions. The observation of this unusual double-spiral magnetic structure suggests that the unique properties of giant magneto-resistance devices can be further tailored using ultrathin magnetic layers.Comment: 9 pages, 3 figure

    Topology of "white" stars in relativistic fragmentation of light nuclei

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    In the present paper, experimental observations of the multifragmentation processes of light relativistic nuclei carried out by means of emulsions are reviewed. Events of the type of "white" stars in which the dissociation of relativistic nuclei is not accompanied by the production of mesons and the target-nucleus fragments are considered. A distinctive feature of the charge topology in the dissociation of the Ne, Mg, Si, and S nuclei is an almost total suppression of the binary splitting of nuclei to fragments with charges higher than 2. The growth of the nuclear fragmentation degree is revealed in an increase in the multiplicity of singly and doubly charged fragments with decreasing charge of the non-excited part of the fragmenting nucleus. The processes of dissociation of stable Li, Be, B, C, N, and O isotopes to charged fragments were used to study special features of the formation of systems consisting of the lightest Ξ±\alpha, d, and t nuclei. Clustering in form of the 3^3He nucleus can be detected in "white" stars via the dissociation of neutron-deficient Be, B, C, and N isotopes.Comment: 20 pages, 3 figures, 9 tables, conference: Conference on Physics of Fundamental Interactions, Moscow, Russia, 1-5 Mar 2004.(Author's translation

    Representative elementary volume via averaged scalar Minkowski functionals

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    Representative Elementary Volume (REV) at which the material properties do not vary with change in volume is an important quantity for making measurements or simulations which represent the whole. We discuss the geometrical method to evaluation of REV based on the quantities coming in the Steiner formula from convex geometry. For bodies in the three-space this formula gives us four scalar functionals known as scalar Minkowski functionals. We demonstrate on certain samples that the values of such averaged functionals almost stabilize for cells for which the length of edges are greater than certain threshold value R. Therefore, from this point of view, it is reasonable to consider cubes of volume R^3 as representative elementary volumes.Comment: 7 page

    Fragmentation of relativistic nuclei in peripheral interactions in nuclear track emulsion

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    The technique of nuclear track emulsions is used to explore the fragmentation of light relativistic nuclei down to the most peripheral interactions - nuclear "white" stars. A complete pattern of therelativistic dissociation of a 8^8B nucleus with target fragment accompaniment is presented. Relativistic dissociation 9^{9}Be→2α\to2\alpha is explored using significant statistics and a relative contribution of 8^{8}Be decays from 0+^+ and 2+^+ states is established. Target fragment accompaniments are shown for relativistic fragmentation 14^{14}N→\to3He+H and 22^{22}Ne→\to5He. The leading role of the electromagnetic dissociation on heavy nuclei with respect to break-ups on target protons is demonstrated in all these cases. It is possible to conclude that the peripheral dissociation of relativistic nuclei in nuclear track emulsion is a unique tool to study many-body systems composed of lightest nuclei and nucleons in the energy scale relevant for nuclear astrophysics.Comment: 15 pages, 4 figures, 4 tables, conference: Relativistic nuclear physics: from Nuclotron to LHC energies, Kiev, June 18-22, 200

    Search for a signal on intermediate baryon systems formation in hadron-nuclear and nuclear-nuclear interactions at high energies

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    We have analyzed the behavior of different characteristics of hadron-nuclear and nuclear-nuclear interactions as a function of centrality to get a signal on the formation of intermediate baryon systems. We observed that the data demonstrate the regime change and saturation. The angular distributions of slow particles exhibit some structure in the above mentioned reactions at low energy. We believe that the structure could be connected with the formation and decay of the percolation cluster. With increasing the mass of colliding nuclei, the structure starts to become weak and almost disappears ultimately. This shows that the number of secondary internuclear interactions increases with increasing the mass of the colliding nuclei. The latter could be a reason of the disintegration of any intermediate formations as well as clusters, which decrease their influence on the angular distribution of the emitted particles.Comment: 2 pages and one figur

    Project approach to the development of rural tourism

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    The authors of the article provide an overview of scientific approaches to the definition of the essence and role of event and gastronomic tourism against the backdrop of the rural tourism promotion currently carried out. The interrelation between all the aforementioned types of tourism and the expediency of their joint development are substantiated. The necessity of holding events in order to smooth out the seasonality of rural tourism and attract tourists interested not only in standard services of rural guest houses but also in entertainment events is proved. Special emphasis is placed on the application of the project approach to the process of creating events. A description of the festivals held in the Vologda region is provided. The main problems of the implementation of project management at the municipal level are identified. The possibility of holding gastronomic festivals within the clusters operating in the region is considered. The example of the Β«SyrFestΒ» gastronomic festival is used to demonstrate a possible project structure designed for such event

    Electromagnetic dissociation of relativistic 8^8B nuclei in nuclear track emulsion

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    Experimental data on fragmentation channels in peripheral interactions of 8^8B nuclei in nuclear track emulsions are presented. A detailed analysis made it possible to justify selections of events of the electromagnetic-dissociation process 8^8B β†’7\to^7Be + \emph{p} and to estimate its cross section. Events of 10^{10}C peripheral dissociation that were observed in the same exposure are described.Comment: 12 pages, 10 figures, 4 tables, Published in Phys.Atom.Nucl.72:690-701,200
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