2,341 research outputs found

    The Geant4 Hadronic Verification Suite for the Cascade Energy Range

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    A Geant4 hadronic process verification suite has been designed to test and optimize Geant4 hadronic models in the cascade energy range. It focuses on quantities relevant to the LHC radiation environment and spallation source targets. The general structure of the suite is presented, including the user interface, stages of verification, management of experimental data, event generation, and comparison of results to data. Verification results for the newly released Binary cascade and Bertini cascade models are presented.Comment: Talk from the 2003 Computing in High Energy and Nuclear Physics (CHEP03), La Jolla, Ca, USA, March 2003, 5 pages, LaTeX, 3 eps figures. PSN MOMT00

    Phase diffusion and charging effects in Josephson junctions

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    The supercurrent of a Josephson junction is reduced by phase diffusion. For ultrasmall capacitance junctions the current may be further decreased by Coulomb blockade effects. We calculate the Cooper pair current by means of time-dependent perturbation theory to all orders in the Josephson coupling energy and obtain the current-voltage characteristic in closed form in a range of parameters of experimental interest. The results comprehend phase diffusion of the coherent Josephson current in the classical regime as well as the supercurrent peak due to incoherent Cooper pair tunneling in the strong Coulomb blockade regime.Comment: 4 pages, 3 figures, RevTe

    Towards the observation of phase locked Bloch oscillations in arrays of small Josephson junctions

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    We have designed an experiment and performed extensive simulations and preliminary measurements to identify a set of realistic circuit parameters that should allow the observation of constant-current steps at I=2ef in short arrays of small Josephson junctions under external AC drive of frequency f. Observation of these steps demonstrating phase lock of the Bloch oscillations with the external drive requires a high-impedance environment for the array, which is provided by on-chip resistors close to the junctions. We show that the width and shape of the steps crucially depend on the shape of the drive and the electron temperature in the resistors

    Current and universal scaling in anomalous transport

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    Anomalous transport in tilted periodic potentials is investigated within the framework of the fractional Fokker-Planck dynamics and the underlying continuous time random walk. The analytical solution for the stationary, anomalous current is obtained in closed form. We derive a universal scaling law for anomalous diffusion occurring in tilted periodic potentials. This scaling relation is corroborated with precise numerical studies covering wide parameter regimes and different shapes for the periodic potential, being either symmetric or ratchet-like ones

    Determination of the Weak Axial Vector Coupling from a Measurement of the Beta-Asymmetry Parameter A in Neutron Beta Decay

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    We report on a new measurement of the neutron beta-asymmetry parameter AA with the instrument \perkeo. Main advancements are the high neutron polarization of P=99.7(1)P = 99.7(1)% from a novel arrangement of super mirror polarizers and reduced background from improvements in beam line and shielding. Leading corrections were thus reduced by a factor of 4, pushing them below the level of statistical error and resulting in a significant reduction of systematic uncertainty compared to our previous experiments. From the result A0=βˆ’0.11996(58)A_0 = -0.11996(58), we derive the ratio of the axial-vector to the vector coupling constant Ξ»=gA/gV=βˆ’1.2767(16)\lambda = g_\mathrm{A}/g_\mathrm{V} = -1.2767(16)Comment: 5 pages, 4 figure

    Quantum Brownian Motion With Large Friction

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    Quantum Brownian motion in the strong friction limit is studied based on the exact path integral formulation of dissipative systems. In this limit the time-nonlocal reduced dynamics can be cast into an effective equation of motion, the quantum Smoluchowski equation. For strongly condensed phase environments it plays a similar role as master equations in the weak coupling range. Applications for chemical, mesoscopic, and soft matter systems are discussed and reveal the substantial role of quantum fluctuations.Comment: 11 pages, 6 figures, to appear in: Chaos: "100 years of Brownian motion

    Quantum charge diffusion in underdamped Josephson junctions and superconducting nanowires

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    The effect of quantum fluctuations on the current-voltage characteristics of Josephson junctions and superconducting nanowires is studied in the underdamped limit. Quantum fluctuations induce transitions between a Coulomb--blockade and a supercurrent branch, and can significantly modify the shape of current-voltage characteristics in the case of a highly resistive environment. Owing to the phase-charge duality, our results can be directly extended to the opposite overdamped limit.Comment: 6 pages, 2 figures, replaced with published versio

    Evidence of Josephson-coupled superconducting regions at the interfaces of Highly Oriented Pyrolytic Graphite

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    Transport properties of a few hundreds of nanometers thick (in the graphene plane direction) lamellae of highly oriented pyrolytic graphite (HOPG) have been investigated. Current-Voltage characteristics as well as the temperature dependence of the voltage at different fixed input currents provide evidence for Josephson-coupled superconducting regions embedded in the internal two-dimensional interfaces, reaching zero resistance at low enough temperatures. The overall behavior indicates the existence of superconducting regions with critical temperatures above 100 K at the internal interfaces of oriented pyrolytic graphite.Comment: 6 Figures, 5 page

    Π‘ΠΈΠ½Ρ‚Π΅Π· Ρ‚Π° Π΄Ρ–ΡƒΡ€Π΅Ρ‚ΠΈΡ‡Π½Π° дія 8-Π°ΠΌΡ–Π½ΠΎΠ·Π°ΠΌΡ–Ρ‰Π΅Π½ΠΈΡ… 7-(2-гідрокси-3-ΠΏ-мСтоксифСноксипропіл-1)-3-мСтилксантину

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    It has been found that natural xanthines, as well as their synthetic analogs, possess the diuretic effect. Analysis of the literature proves that there is a great opportunity of applying synthetic derivatives of N-methylated xanthines as potential diuretics.Aim. To develop preparative methods of the synthesis of 8-aminosubstituted of 7-(2-hydroxy-3-p-metoxyphenoxypropyl-1)-3-methylxanthine and study their physical, chemical and biological properties. Results. The synthesis of a series of 8-aminosubstituted of 7-(2-hydroxy-3-p-metoxyphenoxypropyl-1)-3-methylxanthine was carried out. According to the results of the biological testing the compounds synthesized belong to the toxicity of class IV. 7-(2-Hydroxy-3-p-methoxyphenoxypropyl-1)-8-(furyl-2-methylamino)-3-methylxanthine xanthine shows the highest diuretic activity, and hence, requires a more in-depth study since it is twice more active than hydrochlorothiazide. It should be emphasized that all compounds synthesized exhibit a marked diuretic effect. Experimental part. 8-Bromo-7-(2-hydroxy-3-p-methoxyphenoxypropyl-1)-3-methylxanthine was obtained by heating 8-bromo-3-methylxanthine with p-methoxyphenoxymethyloxirane in butanol-1 and in the presence of N,N-dimethylbenzylamine. 8-Aminosubstitutied of 7-(2-hydroxy-3-p-metoxyphenoxypropyl-1)-3-methylxanthine was obtained by boiling of bromoalcohol with the primary and secondary amines. The structure of the compounds synthesized was unambiguously confirmed by NMR-spectroscopy. The acute toxicity of the compounds obtained was studied by Kerber method. The study of the diuretic activity of the compounds was carried out using Ye. Berkhin method. Hydrochlorothiazide was used as a reference substance. Conclusions. Simple methods for the synthesis of 8-amino-7- (2-hydroxy-3-p-methoxyphenoxypropyl-1)-3-methylxanthines have been developed. The structure of the compounds synthesized has been confirmed by the method of NMR 1H-spectroscopy. The acute toxicity and the diuretic activity of the compounds obtained have been studied.Π˜Π·Π²Π΅ΡΡ‚Π½ΠΎ, Ρ‡Ρ‚ΠΎ ΠΊΠ°ΠΊ ΠΏΡ€ΠΈΡ€ΠΎΠ΄Π½Ρ‹Π΅ ксантины, Ρ‚Π°ΠΊ ΠΈ ΠΈΡ… синтСтичСскиС Π°Π½Π°Π»ΠΎΠ³ΠΈ ΠΎΠ±Π»Π°Π΄Π°ΡŽΡ‚ диурСтичСским дСйствиСм. Анализ Π΄Π°Π½Π½Ρ‹Ρ… Π»ΠΈΡ‚Π΅Ρ€Π°Ρ‚ΡƒΡ€Ρ‹ ΡΠ²ΠΈΠ΄Π΅Ρ‚Π΅Π»ΡŒΡΡ‚Π²ΡƒΠ΅Ρ‚ ΠΎ Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠΉ пСрспСктивС использования синтСтичСских ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄Π½Ρ‹Ρ… N-ΠΌΠ΅Ρ‚ΠΈΠ»ΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹Ρ… ксантинов Π² качСствС ΠΏΠΎΡ‚Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½Ρ‹Ρ… диурСтичСских срСдств. ЦСль Π΄Π°Π½Π½ΠΎΠΉ Ρ€Π°Π±ΠΎΡ‚Ρ‹ – Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚ΠΊΠ° ΠΏΡ€Π΅ΠΏΠ°Ρ€Π°Ρ‚ΠΈΠ²Π½Ρ‹Ρ… ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠ² синтСза 8-Π°ΠΌΠΈΠ½ΠΎΠ·Π°ΠΌΠ΅Ρ‰Π΅Π½Π½Ρ‹Ρ… 7-(2-гидрокси-3-ΠΏ-мСтоксифСноксипропил-1)-3-мСтилксантина ΠΈ ΠΈΠ·ΡƒΡ‡Π΅Π½ΠΈΠ΅ ΠΈΡ… Ρ„ΠΈΠ·ΠΈΠΊΠΎ-химичСских ΠΈ биологичСских свойств. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ ΠΈ ΠΈΡ… обсуТдСниС. Π‘ΠΈΠ½Ρ‚Π΅Π·ΠΈΡ€ΠΎΠ²Π°Π½ ряд 8-Π°ΠΌΠΈΠ½ΠΎΠ·Π°ΠΌΠ΅Ρ‰Π΅Π½Π½Ρ‹Ρ… 7-(2-гидрокси-3-ΠΏ-мСтоксифСноксипропил-1)-3-мСтилксантина. По Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π°ΠΌ биологичСских испытаний синтСзированныС соСдинСния относятся ΠΊ IV классу токсичности. 7-(2-Гидрокси-3-ΠΏ-мСтоксифСноксипропил-1)-8-(Ρ„ΡƒΡ€ΠΈΠ»-2-ΠΌΠ΅Ρ‚ΠΈΠ»Π°ΠΌΠΈΠ½ΠΎ)-3-мСтилксантин ΠΈΠΌΠ΅Π΅Ρ‚ Π½Π°ΠΈΠ±ΠΎΠ»ΡŒΡˆΡƒΡŽ Π΄ΠΈΡƒΡ€Π΅Ρ‚ΠΈΡ‡Π΅ΡΠΊΡƒΡŽ Π°ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ, Π° ΡΠ»Π΅Π΄ΠΎΠ²Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎ Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΠΎ доскональноС ΠΈΠ·ΡƒΡ‡Π΅Π½ΠΈΠ΅, ΠΏΠΎΡΠΊΠΎΠ»ΡŒΠΊΡƒ ΠΎΠ½ Π±ΠΎΠ»Π΅Π΅ Ρ‡Π΅ΠΌ Π² 2 Ρ€Π°Π·Π° Π°ΠΊΡ‚ΠΈΠ²Π½Π΅Π΅Β  Π³ΠΈΠ΄Ρ€ΠΎΡ…Π»ΠΎΡ€Ρ‚ΠΈΠ°Π·ΠΈΠ΄Π°. НСобходимо ΠΏΠΎΠ΄Ρ‡Π΅Ρ€ΠΊΠ½ΡƒΡ‚ΡŒ, Ρ‡Ρ‚ΠΎ всС синтСзированныС соСдинСния ΠΎΠΊΠ°Π·Ρ‹Π²Π°ΡŽΡ‚ Π²Ρ‹Ρ€Π°ΠΆΠ΅Π½Π½ΠΎΠ΅ диурСтичСскоС дСйствиС. Π­ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Π°Ρ Ρ‡Π°ΡΡ‚ΡŒ. 8-Π‘Ρ€ΠΎΠΌ-7-(2-гидрокси-3-ΠΏ-мСтоксифСнокси­пропил-1)-3-мСтилксантин ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½ Π½Π°Π³Ρ€Π΅Π²Π°Π½ΠΈΠ΅ΠΌ 8-Π±Ρ€ΠΎΠΌ-3-мСтилксантина с ΠΏ-мСтоксифСноксимСтилоксираном Π² Π±ΡƒΡ‚Π°Π½ΠΎΠ»Π΅-1 Π² присутствии N,N-Π΄ΠΈΠΌΠ΅Ρ‚ΠΈΠ»Π±Π΅Π½Π·ΠΈΠ»Π°ΠΌΠΈΠ½Π°. 8-АминозамСщСнныС 7-(2-гидрокси-3-ΠΏ-мСтокси­фСноксипропил-1)-3-мСтилксантина синтСзированы ΠΏΡƒΡ‚Π΅ΠΌ кипячСния бромоспирта с ΠΏΠ΅Ρ€Π²ΠΈΡ‡Π½Ρ‹ΠΌΠΈ ΠΈ Π²Ρ‚ΠΎΡ€ΠΈΡ‡Π½Ρ‹ΠΌΠΈ Π°ΠΌΠΈΠ½Π°ΠΌΠΈ. Π‘Ρ‚Ρ€ΡƒΠΊΡ‚ΡƒΡ€Π° синтСзированных соСдинСний ΠΎΠ΄Π½ΠΎΠ·Π½Π°Ρ‡Π½ΠΎ Π΄ΠΎΠΊΠ°Π·Π°Π½Π° ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ ПМР-спСктроскопии. ΠžΡΡ‚Ρ€Π°Ρ Ρ‚ΠΎΠΊΡΠΈΡ‡Π½ΠΎΡΡ‚ΡŒ синтСзированных соСдинСний ΠΈΠ·ΡƒΡ‡Π°Π»Π°ΡΡŒ ΠΏΠΎ ΠΌΠ΅Ρ‚ΠΎΠ΄Ρƒ ΠšΠ΅Ρ€Π±Π΅Ρ€Π°. Π˜Π·ΡƒΡ‡Π΅Π½ΠΈΠ΅ диурСтичСской активности ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Ρ… соСдинСний ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ ΠΏΠΎ ΠΌΠ΅Ρ‚ΠΎΠ΄Ρƒ Π‘Π΅Ρ€Ρ…ΠΈΠ½Π° Π•. Π‘. Π’ качСствС эталона сравнСния использовали Π³ΠΈΠ΄Ρ€ΠΎΡ…Π»ΠΎΡ€Ρ‚ΠΈΠ°Π·ΠΈΠ΄. Π’Ρ‹Π²ΠΎΠ΄Ρ‹. Π Π°Π·Ρ€Π°Π±ΠΎΡ‚Π°Π½Ρ‹ простыС Π² Π²Ρ‹ΠΏΠΎΠ»Π½Π΅Π½ΠΈΠΈ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΠΊΠΈ синтСза 8-Π°ΠΌΠΈΠ½ΠΎΠ·Π°ΠΌΠ΅Ρ‰Π΅Π½Π½Ρ‹Ρ… 7-(2-гидрокси-3-ΠΏ-мСтоксифСноксипропил-1)-3-мСтилксантина. Π‘Ρ‚Ρ€ΡƒΠΊΡ‚ΡƒΡ€Π° синтСзированных соСдинСний Π΄ΠΎΠΊΠ°Π·Π°Π½Π° ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ ПМР-спСктроскопии. Π˜Π·ΡƒΡ‡Π΅Π½Π° острая Ρ‚ΠΎΠΊΡΠΈΡ‡Π½ΠΎΡΡ‚ΡŒ ΠΈ диурСтичСская Π°ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Ρ… вСщСств.Π’Ρ–Π΄ΠΎΠΌΠΎ, Ρ‰ΠΎ як ΠΏΡ€ΠΈΡ€ΠΎΠ΄Π½Ρ– ксантини, Ρ‚Π°ΠΊ Ρ– Ρ—Ρ… синтСтичні Π°Π½Π°Π»ΠΎΠ³ΠΈ Π²ΠΈΡΠ²Π»ΡΡŽΡ‚ΡŒ Π΄Ρ–ΡƒΡ€Π΅Ρ‚ΠΈΡ‡Π½Ρƒ Π΄Ρ–ΡŽ. Аналіз Π΄Π°Π½ΠΈΡ… Π»Ρ–Ρ‚Π΅Ρ€Π°Ρ‚ΡƒΡ€ΠΈ ΡΠ²Ρ–Π΄Ρ‡ΠΈΡ‚ΡŒ ΠΏΡ€ΠΎ Π·Π½Π°Ρ‡Π½Ρƒ пСрспСктиву використання синтСтичних ΠΏΠΎΡ…Ρ–Π΄Π½ΠΈΡ… N-ΠΌΠ΅Ρ‚ΠΈΠ»ΡŒΠΎΠ²Π°Π½ΠΈΡ… ксантинів Π² якості ΠΏΠΎΡ‚Π΅Π½Ρ†Ρ–ΠΉΠ½ΠΈΡ… Π΄Ρ–ΡƒΡ€Π΅Ρ‚ΠΈΡ‡Π½ΠΈΡ… засобів. ΠœΠ΅Ρ‚ΠΎΡŽ Π΄Π°Π½ΠΎΡ— Ρ€ΠΎΠ±ΠΎΡ‚ΠΈ Ρ” Ρ€ΠΎΠ·Ρ€ΠΎΠ±ΠΊΠ° ΠΏΡ€Π΅ΠΏΠ°Ρ€Π°Ρ‚ΠΈΠ²Π½ΠΈΡ… ΠΌΠ΅Ρ‚ΠΎΠ΄Ρ–Π² синтСзу 8-Π°ΠΌΡ–Π½ΠΎΠ·Π°ΠΌΡ–Ρ‰Π΅Π½ΠΈΡ… 7-(2-гідрокси-3-ΠΏ-мСтоксифСноксипропіл-1)-3-мСтилксантину Ρ‚Π° вивчСння Ρ—Ρ… Ρ„Ρ–Π·ΠΈΠΊΠΎ-Ρ…Ρ–ΠΌΡ–Ρ‡Π½ΠΈΡ… Ρ‚Π° Π±Ρ–ΠΎΠ»ΠΎΠ³Ρ–Ρ‡Π½ΠΈΡ… властивостСй. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΈ Ρ‚Π° Ρ—Ρ… обговорСння. Π‘ΡƒΠ² синтСзований ряд 8-Π°ΠΌΡ–Π½ΠΎΠ·Π°ΠΌΡ–Ρ‰Π΅Π½ΠΈΡ… 7-(2-гідрокси-3-ΠΏ-мСтоксифСноксипропіл-1)-3-мСтилксантину. Π—Π° Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π°ΠΌΠΈ Π±Ρ–ΠΎΠ»ΠΎΠ³Ρ–Ρ‡Π½ΠΈΡ… Π²ΠΈΠΏΡ€ΠΎΠ±ΡƒΠ²Π°Π½ΡŒ синтСзовані сполуки Π²Ρ–Π΄Π½ΠΎΡΡΡ‚ΡŒΡΡ Π΄ΠΎ IV класу токсичності. 7-(2-Гідрокси-3-ΠΏ-мСтоксифСноксипропіл-1)-8-(Ρ„ΡƒΡ€ΠΈΠ»-2-ΠΌΠ΅Ρ‚ΠΈΠ»Π°ΠΌΡ–Π½ΠΎ)-3-мСтилксантин виявляє Π½Π°ΠΉΠ²ΠΈΡ‰Ρƒ Π΄Ρ–ΡƒΡ€Π΅Ρ‚ΠΈΡ‡Π½Ρƒ Π°ΠΊΡ‚ΠΈΠ²Π½Ρ–ΡΡ‚ΡŒ, Π° ΠΎΡ‚ΠΆΠ΅ ΠΏΠΎΡ‚Ρ€Π΅Π±ΡƒΡ” Π±Ρ–Π»ΡŒΡˆ досконалого вивчСння, ΠΎΡΠΊΡ–Π»ΡŒΠΊΠΈ Π²Ρ–Π½ Π±Ρ–Π»ΡŒΡˆ Π½Ρ–ΠΆ Ρƒ 2 Ρ€Π°Π·ΠΈ Π°ΠΊΡ‚ΠΈΠ²Π½Ρ–ΡˆΠΈΠΉ Π·Π° Π³Ρ–Π΄Ρ€ΠΎΡ…Π»ΠΎΡ€Ρ‚Ρ–Π°Π·ΠΈΠ΄. НСобхідно підкрСслити, Ρ‰ΠΎ всі синтСзовані сполуки Π²ΠΈΡΠ²Π»ΡΡŽΡ‚ΡŒ Π²ΠΈΡ€Π°Π·Π½Ρƒ Π΄Ρ–ΡƒΡ€Π΅Ρ‚ΠΈΡ‡Π½Ρƒ Π΄Ρ–ΡŽ.Π•ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Π° частина. 8-Π‘Ρ€ΠΎΠΌΠΎ-7-(2-гідрокси-3-ΠΏ-мСтоксифСноксипропіл-1)-3-мСтилксантин ΠΎΡ‚Ρ€ΠΈΠΌΠ°Π»ΠΈ нагріванням 8-Π±Ρ€ΠΎΠΌΠΎ-3-мСтилксантину Π· ΠΏ-мСтоксифСноксимСтилоксираном Ρƒ Π±ΡƒΡ‚Π°Π½ΠΎΠ»Ρ–-1 Π² присутності N,N-Π΄ΠΈΠΌΠ΅Ρ‚ΠΈΠ»Π±Π΅Π½Π·ΠΈΠ»Π°ΠΌΡ–Π½Ρƒ. 8-АмінозаміщСні 7-(2-гідрокси-3-ΠΏ-мСтоксифСноксипропіл-1)-3-мСтилксантину синтСзовані ΡˆΠ»ΡΡ…ΠΎΠΌ кип’ятіння бромоспирту Π· ΠΏΠ΅Ρ€Π²ΠΈΠ½Π½ΠΈΠΌΠΈ Ρ‚Π° Π²Ρ‚ΠΎΡ€ΠΈΠ½Π½ΠΈΠΌΠΈ Π°ΠΌΡ–Π½Π°ΠΌΠΈ. Π‘Ρ‚Ρ€ΡƒΠΊΡ‚ΡƒΡ€Π° синтСзованих сполук Π±ΡƒΠ»Π° ΠΎΠ΄Π½ΠΎΠ·Π½Π°Ρ‡Π½ΠΎ Π΄ΠΎΠ²Π΅Π΄Π΅Π½Π° ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ ПМР-спСктроскопії. Гостра Ρ‚ΠΎΠΊΡΠΈΡ‡Π½Ρ–ΡΡ‚ΡŒ синтСзованих сполук Π±ΡƒΠ»Π° Π²ΠΈΠ²Ρ‡Π΅Π½Π° Π·Π° ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ ΠšΠ΅Ρ€Π±Π΅Ρ€Π°. ВивчСння Π΄Ρ–ΡƒΡ€Π΅Ρ‚ΠΈΡ‡Π½ΠΎΡ— Π΄Ρ–Ρ— ΠΎΡ‚Ρ€ΠΈΠΌΠ°Π½ΠΈΡ… сполук ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ Π·Π° ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ Π‘Π΅Ρ€Ρ…Ρ–Π½Π° Π„. Π‘. Π’ якості Π΅Ρ‚Π°Π»ΠΎΠ½Ρƒ порівняння використовували Π³Ρ–Π΄Ρ€ΠΎΡ…Π»ΠΎΡ€Ρ‚Ρ–Π°Π·ΠΈΠ΄. Висновки. Π‘ΡƒΠ»ΠΈ Ρ€ΠΎΠ·Ρ€ΠΎΠ±Π»Π΅Π½Ρ– прості Ρƒ Π²ΠΈΠΊΠΎΠ½Π°Π½Π½Ρ– ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΠΊΠΈ синтСзу 8-Π°ΠΌΡ–Π½ΠΎΠ·Π°ΠΌΡ–Ρ‰Π΅Π½ΠΈΡ… 7-(2-гідрокси-3-ΠΏ-мСтоксифСноксипропіл-1)-3-мСтилксантину. Π‘Ρ‚Ρ€ΡƒΠΊΡ‚ΡƒΡ€Π° синтСзованих сполук Π±ΡƒΠ»Π° Π΄ΠΎΠ²Π΅Π΄Π΅Π½Π° ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ ПМР-спСктроскопії. Π’ΠΈΠ²Ρ‡Π΅Π½Π° гостра Ρ‚ΠΎΠΊΡΠΈΡ‡Π½Ρ–ΡΡ‚ΡŒ Ρ‚Π° Π΄Ρ–ΡƒΡ€Π΅Ρ‚ΠΈΡ‡Π½Π° Π°ΠΊΡ‚ΠΈΠ²Π½Ρ–ΡΡ‚ΡŒ ΠΎΡ‚Ρ€ΠΈΠΌΠ°Π½ΠΈΡ… Ρ€Π΅Ρ‡ΠΎΠ²ΠΈΠ½

    Resistively-shunted superconducting quantum point contacts

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    We have studied the Josephson dynamics of resistively-shunted ballistic superconducting quantum point contacts at finite temperatures and arbitrary number of conducting modes. Compared to the classical Josephson dynamics of tunnel junctions, dynamics of quantum point contacts exhibits several new features associated with temporal fluctuations of the Josephson potential caused by fluctuations in the occupation of the current-carrying Andreev levels.Comment: 5 pages, RevTex, 3 postscript figures include
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