150 research outputs found

    Plasma measurements conducted in the vincinity of Venus on the spacecraft VENERA-4

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    Plasma flux measurements in vicinity of Venus by charged particle traps on Venera-4 spacecraf

    Comparison of Certain Results of Simultaneous Measurements of Solar Wind Characteristics on Spacecrafts ''Venera-3'' and ''Pioneer-6''

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    Ion concentration, ion velocity, and other solar wind characteristics measured simultaneously aboard spacecraf

    Regge Behavior of DIS Structure Functions

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    Building on previous works of the mid 1960's, we construct an integral equation for forward elastic scattering (t=0) at arbitrary virtuality Q^2 and large s=W^2. This equation sums the ladder production of massless intermediate bosons to all orders, and the solution exhibits Regge behavior. The equation is used to study scattering in a simple chi^2 phi scalar theory, where it is solved appoximately and applied to the study of DIS at small x. We find that the model can naturally describe the quark distribution in both the large x region and the small x region dominated by Reggeon exchange.Comment: 13 pages with 5 figure

    Off-forward parton distributions and Shuvaev's transformations

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    We review Shuvaev's transformations, that relate off-forward parton distributions (OFPDs) to so-called effective forward parton distributions (EFPDs). The latter evolve like conventional forward partons. We express nonforward amplitudes, depending on OFPDs, directly in terms of EFPDs and construct a model for the EFPDs, which allows to consistently express them in terms of the conventional forward parton distributions and nucleon form factors. Our model is self-consistent for arbitrary x, xi, mu, and t.Comment: 13 pages, 7 eps-figures, LaTeX2e, added references, corrected typo

    Skewed parton distributions and the scale dependence of the transverse size parameter

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    We discuss the scale dependence of a skewed parton distribution of the pion obtained from a generalized light-cone wave function overlap formula. Using a simple ansatz for the transverse momentum dependence of the light-cone wave function and restricting ourselves to the case of a zero skewedness parameter, the skewed parton distribution can be expressed through an ordinary parton distribution multiplied by an exponential function. Matching the generalized and ordinary DGLAP evolution equations of the skewed and ordinary parton distributions, respectively, we derive a constraint for the scale dependence of the transverse size parameter, which describes the width of the pion wave function in transverse momentum space. This constraint has implications for the Fock state probability and valence distribution. We apply our results to the pion form factor.Comment: 10 pages, 4 figures; version to appear in Phys. Rev. D; Refs. added, new discussion of results for pion form factor in view of new dat

    DVCS amplitude at tree level: Transversality, twist-3, and factorization

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    We study the virtual Compton amplitude in the generalized Bjorken region (q^2 -> Infinity, t small) in QCD by means of a light-cone expansion of the product of e.m. currents in string operators in coordinate space. Electromagnetic gauge invariance (transversality) is maintained by including in addition to the twist-2 operators 'kinematical' twist-3 operators which appear as total derivatives of twist-2 operators. The non-forward matrix elements of the elementary twist-2 operators are parametrized in terms of two-variable spectral functions (double distributions), from which twist-2 and 3 skewed distributions are obtained through reduction formulas. Our approach is equivalent to a Wandzura-Wilczek type approximation for the twist-3 skewed distributions. The resulting Compton amplitude is manifestly transverse up to terms of order t/q^2. We find that in this approximation the tensor amplitude for longitudinal polarization of the virtual photon is finite, while the one for transverse polarization contains a divergence already at tree level. However, this divergence has zero projection on the polarization vector of the final photon, so that the physical helicity amplitudes are finite.Comment: 34 pages, revtex, 1 eps figure included using epsf. Misprints corrected, one reference adde

    Π”ΠΎΠΌΡ–Π½ΠΎ-Ρ€Π΅Π°ΠΊΡ†Ρ–Ρ— Ρ–Π·Π°Ρ‚ΠΈΠ½Ρ–Π² Π· 5-Π°ΠΌΡ–Π½ΠΎΠΏΡ–Ρ€Π°Π·ΠΎΠ»Π°ΠΌΠΈ Ρ‚Π° 2,2-Π΄ΠΈΠΌΠ΅Ρ‚ΠΈΠ»-1,3-діоксан-4,6-Π΄Ρ–ΠΎΠ½ΠΎΠΌ

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    Aim. To determine the direction of the interaction of isatins with 5-amino-pyrazoles and 2,2-dimethyl-1,3-dioxane-4,6-dione under different conditions.Results and discussion. The domino-reactions of isatins, 5-aminopyrazoles and 2,2-dimethyl-1,3-dioxane-4,6-dione (Meldrum’s acid) in the alcoholic medium are completed by formation of a mixture of pyrazolo[3,4-b]pyridine-4-spiroindolinones and 3-(5-aminopyrazol-3-yl)-3-hydroxy-2-oxindolines with the predominant content of spiro compounds. 3-(5-Aminopyrazol-4-yl)-3-hydroxy-2-oxindolines may turn into pyrazolo[3,4-b]pyridine-4-spiroindolinones very slowly only as a result of retrograde fragmentation to isatin and aminopyrazole in the presence of Meldrum’s acid.Experimental part. The mixtures of pyrazolo[3,4-b]pyridine-4-spiroindolinones and 3-(5-aminopyrazol-3-yl)-3-hydroxy-2-oxindolines separated by crystallization were obtained by boiling in methanol of the equimolar quantity of isatins, 5-aminopyrazoles and Meldrum’s acids. The yield for spiro compounds is 26-82 %, and for 3-(5-aminopyrazole-3-yl)-3-hydroxy-2-oxindolines it is 5-23 %. The transformation of the latter into the spiro compound in the presence of Meldrum’s acid occurs with prolonged boiling in the alcoholic medium and is accompanied with extremely low yields. The structure of all compounds synthesized has been proven by 1H NMR, mass spectra and elemental analysis.Conclusions. It has been found that in the three-component reactions of isatins, 5-aminopyrazoles and 2,2-dimethyl-1,3-dioxane-4,6-dione there are two competing directions of the interaction of isatin with nucleophiles. One of them is the nucleophilic addition of the C4 reaction center of aminopyrazole to the carbonyl group of isatin, which results in 3-(5-aminopyrazol-4-yl)-3-hydroxy-2-oxidolines. Another one is the Knoevenagel condensation of isatin with dioxane-4,6-dione – a domino process that starts formation of the predominant reaction products – pyrazolo[3,4-b]pyridine-4-spiroindolinones.ЦСль Ρ€Π°Π±ΠΎΡ‚Ρ‹ – ΡƒΡΡ‚Π°Π½ΠΎΠ²ΠΈΡ‚ΡŒ Π½Π°ΠΏΡ€Π°Π²Π»Π΅Π½Π½ΠΎΡΡ‚ΡŒ взаимодСйствия ΠΈΠ·Π°Ρ‚ΠΈΠ½ΠΎΠ² с 5-Π°ΠΌΠΈΠ½ΠΎΠΏΠΈΡ€Π°Π·ΠΎΠ»Π°ΠΌΠΈ ΠΈ 2,2-Π΄ΠΈΠΌΠ΅Ρ‚ΠΈΠ»-1,3-диоксан-4,6-Π΄ΠΈΠΎΠ½ΠΎΠΌ Π² Ρ€Π°Π·Π½Ρ‹Ρ… условиях.Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ ΠΈ ΠΈΡ… обсуТдСниС. Π”ΠΎΠΌΠΈΠ½ΠΎ-Ρ€Π΅Π°ΠΊΡ†ΠΈΠΈ ΠΈΠ·Π°Ρ‚ΠΈΠ½ΠΎΠ², 5-Π°ΠΌΠΈΠ½ΠΎΠΏΠΈΡ€Π°Π·ΠΎΠ»ΠΎΠ² ΠΈ 2,2-Π΄ΠΈΠΌΠ΅Ρ‚ΠΈΠ»-1,3-диоксан-4,6-Π΄ΠΈΠΎΠ½Π° (кислоты ΠœΠ΅Π»ΡŒΠ΄Ρ€ΡƒΠΌΠ°) Π² спиртовой срСдС Π·Π°Π²Π΅Ρ€ΡˆΠ°ΡŽΡ‚ΡΡ ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ смСсСй ΠΏΠΈΡ€Π°Π·ΠΎΠ»ΠΎ[3,4-b]ΠΏΠΈΡ€ΠΈΠ΄ΠΈΠ½-4-спироиндолинонов ΠΈ 3-(5-Π°ΠΌΠΈΠ½ΠΎΠΏΠΈΡ€Π°Π·ΠΎΠ»-3-ΠΈΠ»)-3-гидрокси-2-оксиндолинов с ΠΏΡ€Π΅ΠΎΠ±Π»Π°Π΄Π°ΡŽΡ‰ΠΈΠΌ содСрТаниСм спиро-соСдинСний. 3-(5-Аминопиразол-4-ΠΈΠ»)-3-гидрокси-2-оксиндолины лишь Π² Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π΅ рСтрораспада Π½Π° исходныС ΠΈΠ·Π°Ρ‚ΠΈΠ½ ΠΈ Π°ΠΌΠΈΠ½ΠΎΠΏΠΈΡ€Π°Π·ΠΎΠ» Π² присутствии кислоты ΠœΠ΅Π»ΡŒΠ΄Ρ€ΡƒΠΌΠ° ΠΌΠΎΠ³ΡƒΡ‚ ΠΎΡ‡Π΅Π½ΡŒ ΠΌΠ΅Π΄Π»Π΅Π½Π½ΠΎ с Π½ΠΈΠ·ΠΊΠΈΠΌΠΈ Π²Ρ‹Ρ…ΠΎΠ΄Π°ΠΌΠΈ ΠΏΡ€Π΅Π²Ρ€Π°Ρ‰Π°Ρ‚ΡŒΡΡ Π² ΠΏΠΈΡ€Π°Π·ΠΎΠ»ΠΎ[3,4-b]ΠΏΠΈΡ€ΠΈΠ΄ΠΈΠ½-4-спироиндолиноны.Π­ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Π°Ρ Ρ‡Π°ΡΡ‚ΡŒ. ΠšΠΈΠΏΡΡ‡Π΅Π½ΠΈΠ΅ΠΌ Π² ΠΌΠ΅Ρ‚Π°Π½ΠΎΠ»Π΅ ΡΠΊΠ²ΠΈΠΌΠΎΠ»ΡŒΠ½Ρ‹Ρ… количСств ΠΈΠ·Π°Ρ‚ΠΈΠ½ΠΎΠ², 5-Π°ΠΌΠΈΠ½ΠΎΠΏΠΈΡ€Π°Π·ΠΎΠ»ΠΎΠ² ΠΈ кислоты ΠœΠ΅Π»ΡŒΠ΄Ρ€ΡƒΠΌΠ° ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Ρ‹ смСси ΠΏΠΈΡ€Π°Π·ΠΎΠ»ΠΎ[3,4-b]ΠΏΠΈΡ€ΠΈΠ΄ΠΈΠ½-4-спироиндолинонов ΠΈ 3-(5-Π°ΠΌΠΈΠ½ΠΎΠΏΠΈΡ€Π°Π·ΠΎΠ»-3-ΠΈΠ»)-3-гидрокси-2-оксиндолинов, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ Ρ€Π°Π·Π΄Π΅Π»Π΅Π½Ρ‹ кристаллизациСй. Π’Ρ‹Ρ…ΠΎΠ΄ спиро-соСдинСний составляСт 26-82 %, Π° 3-(5-Π°ΠΌΠΈΠ½ΠΎΠΏΠΈΡ€Π°Π·ΠΎΠ»-3-ΠΈΠ»)-3-гидрокси-2-оксиндолинов – 5-23 %. ΠŸΡ€Π΅Π²Ρ€Π°Ρ‰Π΅Π½ΠΈΠ΅ послСдних Π² присутствии кислоты ΠœΠ΅Π»ΡŒΠ΄Ρ€ΡƒΠΌΠ° Π² спиро-соСдинСния происходит ΠΏΡ€ΠΈ Π΄Π»ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠΌ кипячСнии Π² спиртовой срСдС ΠΈ сопровоТдаСтся ΠΊΡ€Π°ΠΉΠ½Π΅ Π½ΠΈΠ·ΠΊΠΈΠΌΠΈ Π²Ρ‹Ρ…ΠΎΠ΄Π°ΠΌΠΈ. Π‘Ρ‚Ρ€ΠΎΠ΅Π½ΠΈΠ΅ ΠΈ состав всСх синтСзированных соСдинСний Π΄ΠΎΠΊΠ°Π·Π°Π½Ρ‹ Π΄Π°Π½Π½Ρ‹ΠΌΠΈ ЯМР 1Н, масс-спСктров ΠΈ элСмСнтным Π°Π½Π°Π»ΠΈΠ·ΠΎΠΌ.Π’Ρ‹Π²ΠΎΠ΄Ρ‹. УстановлСно, Ρ‡Ρ‚ΠΎ Π² Ρ‚Ρ€Π΅Ρ…ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚Π½Ρ‹Ρ… рСакциях ΠΈΠ·Π°Ρ‚ΠΈΠ½ΠΎΠ², 5-Π°ΠΌΠΈΠ½ΠΎΠΏΠΈΡ€Π°Π·ΠΎΠ»ΠΎΠ² ΠΈ 2,2-Π΄ΠΈΠΌΠ΅Ρ‚ΠΈΠ»-1,3-диоксан-4,6-Π΄ΠΈΠΎΠ½Π° Ρ€Π΅Π°Π»ΠΈΠ·ΡƒΡŽΡ‚ΡΡ Π΄Π²Π° ΠΊΠΎΠ½ΠΊΡƒΡ€ΠΈΡ€ΡƒΡŽΡ‰ΠΈΡ… направлСния взаимодСйствия ΠΈΠ·Π°Ρ‚ΠΈΠ½Π° с Π½ΡƒΠΊΠ»Π΅ΠΎΡ„ΠΈΠ»Π°ΠΌΠΈ. Одно ΠΈΠ· Π½ΠΈΡ… – Π½ΡƒΠΊΠ»Π΅ΠΎΡ„ΠΈΠ»ΡŒΠ½ΠΎΠ΅ присоСдинСниС Π‘4 Ρ€Π΅Π°ΠΊΡ†ΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ Ρ†Π΅Π½Ρ‚Ρ€Π° Π°ΠΌΠΈΠ½ΠΎΠΏΠΈΡ€Π°Π·ΠΎΠ»Π° ΠΊ ΠΊΠ°Ρ€Π±ΠΎΠ½ΠΈΠ»ΡŒΠ½ΠΎΠΉ Π³Ρ€ΡƒΠΏΠΏΠ΅ ΠΈΠ·Π°Ρ‚ΠΈΠ½Π° ΠΏΡ€ΠΈΠ²ΠΎΠ΄ΠΈΡ‚ ΠΊ 3-(5-Π°ΠΌΠΈΠ½ΠΎΠΏΠΈΡ€Π°Π·ΠΎΠ»-4-ΠΈΠ»)-3-гидрокси-2-оксиндолинам. А Π²Ρ‚ΠΎΡ€ΠΎΠ΅ – кондСнсация ΠΈΠ·Π°Ρ‚ΠΈΠ½Π° с диоксан-4,6-Π΄ΠΈΠΎΠ½ΠΎΠΌ ΠΏΠΎ КнСвСнагСлю ΠΈΠ½ΠΈΡ†ΠΈΠΈΡ€ΡƒΠ΅Ρ‚ Π΄ΠΎΠΌΠΈΠ½ΠΎ-процСсс, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹ΠΉ Π·Π°Π²Π΅Ρ€ΡˆΠ°Π΅Ρ‚ΡΡ ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ основных ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚ΠΎΠ² Ρ€Π΅Π°ΠΊΡ†ΠΈΠΈ – ΠΏΠΈΡ€Π°Π·ΠΎΠ»ΠΎ[3,4-b]ΠΏΠΈΡ€ΠΈΠ΄ΠΈΠ½-4-спироиндолинонов.ΠœΠ΅Ρ‚Π° Ρ€ΠΎΠ±ΠΎΡ‚ΠΈ – встановити Π½Π°ΠΏΡ€Π°Π²Π»Π΅Π½Ρ–ΡΡ‚ΡŒ Π²Π·Π°Ρ”ΠΌΠΎΠ΄Ρ–Ρ— Ρ–Π·Π°Ρ‚ΠΈΠ½Ρ–Π² Π· 5-Π°ΠΌΡ–Π½ΠΎΠΏΡ–Ρ€Π°Π·ΠΎΠ»Π°ΠΌΠΈ Ρ‚Π° 2,2-Π΄ΠΈΠΌΠ΅Ρ‚ΠΈΠ»-1,3-діоксан-4,6-Π΄Ρ–ΠΎΠ½ΠΎΠΌ Ρƒ Ρ€Ρ–Π·Π½ΠΈΡ… ΡƒΠΌΠΎΠ²Π°Ρ….Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΈ Ρ‚Π° Ρ—Ρ… обговорСння. Π”ΠΎΠΌΡ–Π½ΠΎ-Ρ€Π΅Π°ΠΊΡ†Ρ–Ρ— Ρ–Π·Π°Ρ‚ΠΈΠ½Ρ–Π², 5-Π°ΠΌΡ–Π½ΠΎΠΏΡ–Ρ€Π°Π·ΠΎΠ»Ρ–Π² Ρ‚Π° 2,2-Π΄ΠΈΠΌΠ΅Ρ‚ΠΈΠ»-1,3-діоксан-4,6-Π΄Ρ–ΠΎΠ½Ρƒ (кислоти ΠœΠ΅Π»ΡŒΠ΄Ρ€ΡƒΠΌΠ°) Ρƒ спиртовому сСрСдовищі Π·Π°Π²Π΅Ρ€ΡˆΡƒΡŽΡ‚ΡŒΡΡ утворСнням ΡΡƒΠΌΡ–ΡˆΡ– ΠΏΡ–Ρ€Π°Π·ΠΎΠ»ΠΎ[3,4-b]ΠΏΡ–Ρ€ΠΈΠ΄ΠΈΠ½-4-спіроіндолінонів Ρ‚Π° 3-(5-Π°ΠΌΡ–Π½ΠΎΠΏΡ–Ρ€Π°Π·ΠΎΠ»-3-Ρ–Π»)-3-гідрокси-2-оксіндолінів Π· ΠΏΠ΅Ρ€Π΅Π²Π°ΠΆΠ½ΠΈΠΌ вмістом спіро-сполук. 3-(5-Амінопіразол-4-Ρ–Π»)-3-гідрокси-2-оксіндоліни лишС Π² Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ– Ρ€Π΅Ρ‚Ρ€ΠΎΡ€ΠΎΠ·ΠΏΠ°Π΄Ρƒ Π½Π° Π²ΠΈΡ…Ρ–Π΄Π½Ρ– Ρ–Π·Π°Ρ‚ΠΈΠ½ Ρ‚Π° Π°ΠΌΡ–Π½ΠΎΠΏΡ–Ρ€Π°Π·ΠΎΠ» Ρƒ присутності кислоти ΠœΠ΅Π»ΡŒΠ΄Ρ€ΡƒΠΌΠ° ΠΌΠΎΠΆΡƒΡ‚ΡŒ Π΄ΡƒΠΆΠ΅ ΠΏΠΎΠ²Ρ–Π»ΡŒΠ½ΠΎ Π· низькими Π²ΠΈΡ…ΠΎΠ΄Π°ΠΌΠΈ ΠΏΠ΅Ρ€Π΅Ρ‚Π²ΠΎΡ€ΡŽΠ²Π°Ρ‚ΠΈΡΡ Π½Π° ΠΏΡ–Ρ€Π°Π·ΠΎΠ»ΠΎ[3,4-b]ΠΏΡ–Ρ€ΠΈΠ΄ΠΈΠ½-4-спіроіндолінони.Π•ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Π° частина. ΠšΠΈΠΏβ€™ΡΡ‚Ρ–Π½Π½ΡΠΌ Ρƒ ΠΌΠ΅Ρ‚Π°Π½ΠΎΠ»Ρ– Π΅ΠΊΠ²Ρ–ΠΌΠΎΠ»ΡŒΠ½ΠΈΡ… ΠΊΡ–Π»ΡŒΠΊΠΎΡΡ‚Π΅ΠΉ Ρ–Π·Π°Ρ‚ΠΈΠ½Ρ–Π², 5-Π°ΠΌΡ–Π½ΠΎΠΏΡ–Ρ€Π°Π·ΠΎΠ»Ρ–Π² Ρ‚Π° кислоти ΠœΠ΅Π»ΡŒΠ΄Ρ€ΡƒΠΌΠ° ΠΎΠ΄Π΅Ρ€ΠΆΠ°Π½ΠΎ ΡΡƒΠΌΡ–ΡˆΡ– ΠΏΡ–Ρ€Π°Π·ΠΎΠ»ΠΎ[3,4-b]ΠΏΡ–Ρ€ΠΈΠ΄ΠΈΠ½-4-спіроіндолінонів Ρ‚Π° 3-(5-Π°ΠΌΡ–Π½ΠΎΠΏΡ–Ρ€Π°Π·ΠΎΠ»-3-Ρ–Π»)-3-гідрокси-2-оксіндолінів, які Ρ€ΠΎΠ·Π΄Ρ–Π»Π΅Π½Ρ– ΠΊΡ€ΠΈΡΡ‚Π°Π»Ρ–Π·Π°Ρ†Ρ–Ρ”ΡŽ. Π’ΠΈΡ…Ρ–Π΄ спіро-сполук складає 26-82 %, Π° 3-(5-Π°ΠΌΡ–Π½ΠΎΠΏΡ–Ρ€Π°Π·ΠΎΠ»-3-Ρ–Π»)-3-гідрокси-2-оксіндолінів – 5-23 %. ΠŸΠ΅Ρ€Π΅Ρ‚Π²ΠΎΡ€Π΅Π½Π½Ρ останніх Ρƒ присутності кислоти ΠœΠ΅Π»ΡŒΠ΄Ρ€ΡƒΠΌΠ° Π½Π° спіро-сполуки Π²Ρ–Π΄Π±ΡƒΠ²Π°Ρ”Ρ‚ΡŒΡΡ ΠΏΡ€ΠΈ Ρ‚Ρ€ΠΈΠ²Π°Π»ΠΎΠΌΡƒ кип’ятінні Ρƒ спиртовому сСрСдовищі Ρ– ΡΡƒΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΆΡƒΡ”Ρ‚ΡŒΡΡ Π²ΠΊΡ€Π°ΠΉ низькими Π²ΠΈΡ…ΠΎΠ΄Π°ΠΌΠΈ. Π‘Ρ‚Ρ€ΡƒΠΊΡ‚ΡƒΡ€Ρƒ Ρ– склад усіх синтСзованих сполук Π΄ΠΎΠ²Π΅Π΄Π΅Π½ΠΎ Π΄Π°Π½ΠΈΠΌΠΈ ЯМР 1Н, мас-спСктрів Ρ– Π΅Π»Π΅ΠΌΠ΅Π½Ρ‚Π½ΠΈΠΌ Π°Π½Π°Π»Ρ–Π·ΠΎΠΌ.Висновки. ВстановлСно, Ρ‰ΠΎ Ρƒ Ρ‚Ρ€ΠΈΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚Π½ΠΈΡ… рСакціях Ρ–Π·Π°Ρ‚ΠΈΠ½Ρ–Π², 5-Π°ΠΌΡ–Π½ΠΎΠΏΡ–Ρ€Π°Π·ΠΎΠ»Ρ–Π² Ρ– 2,2-Π΄ΠΈΠΌΠ΅Ρ‚ΠΈΠ»-1,3-діоксан-4,6-Π΄Ρ–ΠΎΠ½Ρƒ Ρ€Π΅Π°Π»Ρ–Π·ΡƒΡŽΡ‚ΡŒΡΡ Π΄Π²Π° ΠΊΠΎΠ½ΠΊΡƒΡ€ΡƒΡŽΡ‡ΠΈΡ… напрямки Π²Π·Π°Ρ”ΠΌΠΎΠ΄Ρ–Ρ— Ρ–Π·Π°Ρ‚ΠΈΠ½Ρƒ Π· Π½ΡƒΠΊΠ»Π΅ΠΎΡ„Ρ–Π»Π°ΠΌΠΈ. Один Π· Π½ΠΈΡ… – Π½ΡƒΠΊΠ»Π΅ΠΎΡ„Ρ–Π»ΡŒΠ½Π΅ приєднання Π‘4 Ρ€Π΅Π°ΠΊΡ†Ρ–ΠΉΠ½ΠΎΠ³ΠΎ Ρ†Π΅Π½Ρ‚Ρ€Π° Π°ΠΌΡ–Π½ΠΎΠΏΡ–Ρ€Π°Π·ΠΎΠ»Ρƒ Π΄ΠΎ ΠΊΠ°Ρ€Π±ΠΎΠ½Ρ–Π»ΡŒΠ½ΠΎΡ— Π³Ρ€ΡƒΠΏΠΈ Ρ–Π·Π°Ρ‚ΠΈΠ½Ρƒ ΠΏΡ€ΠΈΠ²ΠΎΠ΄ΠΈΡ‚ΡŒ Π΄ΠΎ 3-(5-Π°ΠΌΡ–Π½ΠΎΠΏΡ–Ρ€Π°Π·ΠΎΠ»-4-Ρ–Π»)-3-гідрокси-2-оксіндолінів. А Ρ–Π½ΡˆΠΈΠΉ – кондСнсація Ρ–Π·Π°Ρ‚ΠΈΠ½Ρƒ Π· діоксан-4,6-Π΄Ρ–ΠΎΠ½ΠΎΠΌ Π·Π° КньовСнагСлСм Π·Π°ΠΏΠΎΡ‡Π°Ρ‚ΠΊΠΎΠ²ΡƒΡ” Π΄ΠΎΠΌΡ–Π½ΠΎ-процСс, який Π·Π°Π²Π΅Ρ€ΡˆΡƒΡ”Ρ‚ΡŒΡΡ утворСнням ΠΏΠ΅Ρ€Π΅Π²Π°ΠΆΠ½ΠΈΡ… ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚Ρ–Π² Ρ€Π΅Π°ΠΊΡ†Ρ–Ρ— – ΠΏΡ–Ρ€Π°Π·ΠΎΠ»ΠΎ[3,4-b]ΠΏΡ–Ρ€ΠΈΠ΄ΠΈΠ½-4-спіроіндолінонів
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