1,532 research outputs found

    Stability of Landau-Ginzburg branes

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    We evaluate the ideas of Pi-stability at the Landau-Ginzburg point in moduli space of compact Calabi-Yau manifolds, using matrix factorizations to B-model the topological D-brane category. The standard requirement of unitarity at the IR fixed point is argued to lead to a notion of "R-stability" for matrix factorizations of quasi-homogeneous LG potentials. The D0-brane on the quintic at the Landau-Ginzburg point is not obviously unstable. Aiming to relate R-stability to a moduli space problem, we then study the action of the gauge group of similarity transformations on matrix factorizations. We define a naive moment map-like flow on the gauge orbits and use it to study boundary flows in several examples. Gauge transformations of non-zero degree play an interesting role for brane-antibrane annihilation. We also give a careful exposition of the grading of the Landau-Ginzburg category of B-branes, and prove an index theorem for matrix factorizations.Comment: 46 pages, LaTeX, summary adde

    Single-electron latch with granular film charge leakage suppressor

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    A single-electron latch is a device that can be used as a building block for Quantum-dot Cellular Automata (QCA) circuits. It consists of three nanoscale metal "dots" connected in series by tunnel junctions; charging of the dots is controlled by three electrostatic gates. One very important feature of a single-electron latch is its ability to store ("latch") information represented by the location of a single electron within the three dots. To obtain latching, the undesired leakage of charge during the retention time must be suppressed. Previously, to achieve this goal, multiple tunnel junctions were used to connect the three dots. However, this method of charge leakage suppression requires an additional compensation of the background charges affecting each parasitic dot in the array of junctions. We report a single-electron latch where a granular metal film is used to fabricate the middle dot in the latch which concurrently acts as a charge leakage suppressor. This latch has no parasitic dots, therefore the background charge compensation procedure is greatly simplified. We discuss the origins of charge leakage suppression and possible applications of granular metal dots for various single-electron circuits.Comment: 21 pages, 4 figure

    Semiorthogonal decompositions of derived categories of equivariant coherent sheaves

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    Let X be an algebraic variety with an action of an algebraic group G. Suppose X has a full exceptional collection of sheaves, and these sheaves are invariant under the action of the group. We construct a semiorthogonal decomposition of bounded derived category of G-equivariant coherent sheaves on X into components, equivalent to derived categories of twisted representations of the group. If the group is finite or reductive over the algebraically closed field of zero characteristic, this gives a full exceptional collection in the derived equivariant category. We apply our results to particular varieties such as projective spaces, quadrics, Grassmanians and Del Pezzo surfaces.Comment: 28 pages, uses XY-pi

    Structure of 2-Methyl-5,6,7-triphenyl-6,7-dihydropyrazolo[2,3-\u3cem\u3ea\u3c/em\u3e]pyrimidine

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    C25H21N3, Mr = 363.46, monoclinic, P21/n, a = 9.245 (2), b = 23.502 (5), c = 9.340 (2) Γ…, Ξ²= 103.50(3)Β°, V=1973.3(2) Γ…3, Z=4, Dx= 1.220 (2) g cm-3, Ξ» (Mo KΞ± )= 0.71069 Γ…, ΞΌ = 0.068 cm-1, F(000) = 768, T= 292 K, R = 0.091 for 1442 unique observed reflections. The dihydropyrimidine ring adopts a distorted sofa conformation. The aryl substituents on the saturated C atoms have an axial orientation

    Bound, virtual and resonance SS-matrix poles from the Schr\"odinger equation

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    A general method, which we call the potential SS-matrix pole method, is developed for obtaining the SS-matrix pole parameters for bound, virtual and resonant states based on numerical solutions of the Schr\"odinger equation. This method is well-known for bound states. In this work we generalize it for resonant and virtual states, although the corresponding solutions increase exponentially when rβ†’βˆžr\to\infty. Concrete calculations are performed for the 1+1^+ ground and the 0+0^+ first excited states of 14N^{14}\rm{N}, the resonance 15F^{15}\rm{F} states (1/2+1/2^+, 5/2+5/2^+), low-lying states of 11Be^{11}\rm{Be} and 11N^{11}\rm{N}, and the subthreshold resonances in the proton-proton system. We also demonstrate that in the case the broad resonances their energy and width can be found from the fitting of the experimental phase shifts using the analytical expression for the elastic scattering SS-matrix. We compare the SS-matrix pole and the RR-matrix for broad s1/2s_{1/2} resonance in 15F{}^{15}{\rm F}Comment: 14 pages, 5 figures (figures 3 and 4 consist of two figures each) and 4 table

    Π‘ΠΈΠ½Ρ‚Π΅Π· Ρ‚Π° N-алкілування Π΄Ρ–Π΅Ρ‚ΠΈΠ» 4,7-Π΄ΠΈΠ³Ρ–Π΄Ρ€ΠΎΠ°Π·ΠΎΠ»ΠΎ[1,5-a]ΠΏΡ–Ρ€ΠΈΠΌΡ–Π΄ΠΈΠ½-5,6-дикарбоксилатів

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    It has been shown that the ternary condensation of oxaloacetic ester (diethyl 2-oxosuccinate), aromatic aldehydesΒ and 3-amino-1,2,4-triazole or 5-aminotetrazole in dimethylformamide results in formation of the corresponding diethyl 7-aryl-4,7-dihydroazolo[1,5-a]pyrimidin-5,6-dicarboxylates. By 1H NMR spectroscopy (according to the data of the chemical shifts of C(2)H-protons for the corresponding N(4)H- and N(4)-methylderivatives ofΒ 7-phenyl-4,7-dihydro[1,2,4]triazolo[1,5-a]pyrimidin-5,6-dicarboxylate) it has been found that alkylation of 4,7-dihydro[1,2,4]azolo[1,5-a]pyrimidin-5,6-dicarboxylates in the acetonitrile–saturated water alkali system leads selectively to formation of N(4)-alkyl derivatives. Both the starting compounds obtained and their N(4)-methylsubstitutedΒ analogues together with relative diethyl 4-aryl-3,4-dihydropyrimidin-2(1H)-on-5,6-dicarboxylates, 6-unsubstitutedΒ 4-aryl-3,4-dihydropyrimidin-2(1H)-on-5-dicarboxylates and the derivatives of 6-COR-7-aryl-4,7-dihydro[1,2,4] triazolo[1,5-a]pyrimidines are the promising objects for studying benzyl C(7)-functionalization of 4,7-dihydroazoloΒ 1,5-a]pyrimidines, as well as of reactions associated with the presence of double C=C-bonds activated by twoΒ electron withdrawing groups. Obtaining of the key N(4)H- and N(4)Me-derivatives of 7-phenyl-4,7-dihydro[1,2,4]Β triazolo- and tetrazolo[1,5-a]pyrimidin-5,6-dicarboxylates also opens the way to the research of biological propertiesΒ of the compounds of this class. It is noteworthy that being a three-component one the reaction studied, without any doubts, are appropriate for the synthesis of the derivatives of 7-aryl-4,7-dihydro[1,2,4]triazolo- andΒ tetrazolo[1,5-a]pyrimidines containing two electron withdrawing substituents in positions 5 and 6.Показано, Ρ‡Ρ‚ΠΎ трСхкомпонСнтная кондСнсация щавСлСвоуксусного эфира (диэтил 2-оксосукцината), ароматичСских альдСгидов ΠΈ 3-Π°ΠΌΠΈΠ½ΠΎ-1,2,4-Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»Π° ΠΈΠ»ΠΈ 5-Π°ΠΌΠΈΠ½ΠΎΡ‚Π΅Ρ‚Ρ€Π°Π·ΠΎΠ»Π° Π² Π΄ΠΈΠΌΠ΅Ρ‚ΠΈΠ»Ρ„ΠΎΡ€ΠΌΠ°ΠΌΠΈΠ΄Π΅ ΠΏΡ€ΠΈΠ²ΠΎΠ΄ΠΈΡ‚ ΠΊ ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½ΠΈΡŽ ΡΠΎΠΎΡ‚Π²Π΅Ρ‚ΡΡ‚Π²ΡƒΡŽΡ‰ΠΈΡ… диэтил 7-Π°Ρ€ΠΈΠ»-4,7-Π΄ΠΈΠ³ΠΈΠ΄Ρ€ΠΎΠ°Π·ΠΎΠ»ΠΎ[1,5-a]ΠΏΠΈΡ€ΠΈΠΌΠΈΠ΄ΠΈΠ½-5,6-дикарбоксилатов. Π‘ ΠΏΠΎΠΌΠΎΡ‰ΡŒΡŽ 1Н ЯМР-спСктроскопии (ΠΏΠΎ Π΄Π°Π½Π½Ρ‹ΠΌ химичСских сдвигов сигналов ΠΏΡ€ΠΎΡ‚ΠΎΠ½ΠΎΠ² Π‘(2)H для ΡΠΎΠΎΡ‚Π²Π΅Ρ‚ΡΡ‚Π²ΡƒΡŽΡ‰ΠΈΡ… N(4)H- ΠΈ N(4)МС-ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄Π½Ρ‹Ρ… диэтил 7-Ρ„Π΅Π½ΠΈΠ»-4,7-Π΄ΠΈΠ³ΠΈΠ΄Ρ€ΠΎ[1,2,4]Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎ[1,5-a]Β ΠΏΠΈΡ€ΠΈΠΌΠΈΠ΄ΠΈΠ½-5,6-дикарбоксилата) установлСно, Ρ‡Ρ‚ΠΎ Π°Π»ΠΊΠΈΠ»ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ 7-Π°Ρ€ΠΈΠ»-4,7-Π΄ΠΈΠ³ΠΈΠ΄Ρ€ΠΎΠ°Π·ΠΎΠ»ΠΎ[1,5-a]ΠΏΠΈΡ€ΠΈΠΌΠΈΠ΄ΠΈΠ½-5,6-дикарбоксилатов Π² систСмС Π°Ρ†Π΅Ρ‚ΠΎΠ½ΠΈΡ‚Ρ€ΠΈΠ»-насыщСнная водная Ρ‰Π΅Π»ΠΎΡ‡ΡŒ сСлСктивно ΠΏΡ€ΠΈΠ²ΠΎΠ΄ΠΈΡ‚ ΠΊ ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½ΠΈΡŽ N(4)-Π°Π»ΠΊΠΈΠ»ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄Π½Ρ‹Ρ…. Как ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Π΅ исходныС соСдинСния, Ρ‚Π°ΠΊ ΠΈ ΠΈΡ… N(4)-ΠΌΠ΅Ρ‚ΠΈΠ»Π·Π°ΠΌΠ΅Ρ‰Π΅Π½Π½Ρ‹Π΅ Π°Π½Π°Π»ΠΎΠ³ΠΈ наряду с родствСнными диэтил 4-Π°Ρ€ΠΈΠ»-3,4-Π΄ΠΈΠ³ΠΈΠ΄Ρ€ΠΎΠΏΠΈΡ€ΠΈΠΌΠΈΠ΄ΠΈΠ½-2(1Н)-ΠΎΠ½-5,6-дикарбоксилатами, 6-Π½Π΅Π·Π°ΠΌΠ΅Ρ‰Π΅Π½Π½Ρ‹ΠΌΠΈ этил 4-Π°Ρ€ΠΈΠ»-3,4-Π΄ΠΈΠ³ΠΈΠ΄Ρ€ΠΎΠΏΠΈΡ€ΠΈΠΌΠΈΠ΄ΠΈΠ½-2(1Н)-ΠΎΠ½-5-карбоксилатами ΠΈΒ ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄Π½Ρ‹ΠΌΠΈ 6-COR-7-Π°Ρ€ΠΈΠ»-4,7-Π΄ΠΈΠ³ΠΈΠ΄Ρ€ΠΎ[1,2,4]Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎ[1,5-a]ΠΏΠΈΡ€ΠΈΠΌΠΈΠ΄ΠΈΠ½ΠΎΠ² ΡΠ²Π»ΡΡŽΡ‚ΡΡ пСрспСктивными ΠΎΠ±ΡŠΠ΅ΠΊΡ‚Π°ΠΌΠΈ для изучСния бСнзильной Π‘(7)-Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΎΠ½Π°Π»ΠΈΠ·Π°Ρ†ΠΈΠΈ 4,7-Π΄ΠΈΠ³ΠΈΠ΄Ρ€ΠΎΠ°Π·ΠΎΠ»ΠΎ[1,5-a]ΠΏΠΈΡ€ΠΈΠΌΠΈΠ΄ΠΈΠ½ΠΎΠ², Π° Ρ‚Π°ΠΊΠΆΠ΅ Ρ€Π΅Π°ΠΊΡ†ΠΈΠΉ, связанных с Π½Π°Π»ΠΈΡ‡ΠΈΠ΅ΠΌ Π΄Π²ΠΎΠΉΠ½ΠΎΠΉ C=C-связи, Π°ΠΊΡ‚ΠΈΠ²ΠΈΡ€ΠΎΠ²Π°Π½Π½ΠΎΠΉ двумя Π°ΠΊΡ†Π΅ΠΏΡ‚ΠΎΡ€Π½Ρ‹ΠΌΠΈ Π³Ρ€ΡƒΠΏΠΏΠ°ΠΌΠΈ. ΠŸΠΎΠ»ΡƒΡ‡Π΅Π½ΠΈΠ΅ ΠΊΠ»ΡŽΡ‡Π΅Π²Ρ‹Ρ… N(4)H- ΠΈ N(4)МС-ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄Π½Ρ‹Ρ… 7-Ρ„Π΅Π½ΠΈΠ»-4,7-Π΄ΠΈΠ³ΠΈΠ΄Ρ€ΠΎ[1,2,4]Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎ- ΠΈ Ρ‚Π΅Ρ‚Ρ€Π°Π·ΠΎΠ»ΠΎ[1,5-a]ΠΏΠΈΡ€ΠΈΠΌΠΈΠ΄ΠΈΠ½-5,6-дикарбоксилатов Ρ‚Π°ΠΊΠΆΠ΅ ΠΎΡ‚ΠΊΡ€Ρ‹Π²Π°Π΅Ρ‚ ΠΏΡƒΡ‚ΡŒ ΠΊ биологичСским исслСдованиям соСдинСний этого класса. Π—Π°ΠΌΠ΅Ρ‚ΠΈΠΌ, Ρ‡Ρ‚ΠΎ исслСдованная рСакция, являясь Ρ‚Ρ€Π΅Ρ…ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚Π½ΠΎΠΉ, бСзусловно ΠΏΠΎΠ΄Ρ…ΠΎΠ΄ΠΈΡ‚ для синтСза ΠΈ исслСдования ΠΊΠΎΠΌΠ±ΠΈΠ½Π°Ρ‚ΠΎΡ€Π½Ρ‹Ρ… Π±ΠΈΠ±Π»ΠΈΠΎΡ‚Π΅ΠΊ ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄Π½Ρ‹Ρ… 7-Π°Ρ€ΠΈΠ»-4,7-Π΄ΠΈΠ³ΠΈΠ΄Ρ€ΠΎ[1,2,4]Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎ- ΠΈ Ρ‚Π΅Ρ‚Ρ€Π°Π·ΠΎΠ»ΠΎ[1,5-a]ΠΏΠΈΡ€ΠΈΠΌΠΈΠ΄ΠΈΠ½ΠΎΠ², содСрТащих Π΄Π²Π° элСктроноакцСпторных замСститСля Π² полоТСниях 5 ΠΈ 6.Показано, Ρ‰ΠΎ Ρ‚Ρ€ΠΈΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚Π½Π° кондСнсація Ρ‰Π°Π²Π»Π΅Π²ΠΎΠΎΡ†Ρ‚ΠΎΠ²ΠΎΠ³ΠΎ СстСру (Π΄Ρ–Π΅Ρ‚ΠΈΠ» 2-оксосукцинату), Π°Ρ€ΠΎΠΌΠ°Ρ‚ΠΈΡ‡Π½ΠΈΡ… Π°Π»ΡŒΠ΄Π΅Π³Ρ–Π΄Ρ–Π² Ρ‚Π° 3-Π°ΠΌΡ–Π½ΠΎ-1,2,4-Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»Ρƒ Π°Π±ΠΎ 5-Π°ΠΌΡ–Π½ΠΎΡ‚Π΅Ρ‚Ρ€Π°Π·ΠΎΠ»Ρƒ Π² Π΄ΠΈΠΌΠ΅Ρ‚ΠΈΠ»Ρ„ΠΎΡ€ΠΌΠ°ΠΌΡ–Π΄Ρ– ΠΏΡ€ΠΈΠ·Π²ΠΎΠ΄ΠΈΡ‚ΡŒΒ Π΄ΠΎ утворСння Π²Ρ–Π΄ΠΏΠΎΠ²Ρ–Π΄Π½ΠΈΡ… Π΄Ρ–Π΅Ρ‚ΠΈΠ» 4,7-Π΄ΠΈΠ³Ρ–Π΄Ρ€ΠΎΠ°Π·ΠΎΠ»ΠΎ[1,5-a]ΠΏΡ–Ρ€ΠΈΠΌΡ–Π΄ΠΈΠ½-5,6-дикарбоксилатів. Π—Π° допомогою 1Н ЯМР-спСктроскопії (Π·Π° Π΄Π°Π½ΠΈΠΌΠΈ ΠΏΡ€ΠΎ Ρ…Ρ–ΠΌΡ–Ρ‡Π½Ρ– зсуви сигналів ΠΏΡ€ΠΎΡ‚ΠΎΠ½Ρ–Π² Π‘(2)Н для Π²Ρ–Π΄ΠΏΠΎΠ²Ρ–Π΄Π½ΠΈΡ… N(4)H- Ρ‚Π°Β N(4)Me-ΠΏΠΎΡ…Ρ–Π΄Π½ΠΈΡ… Π΄Ρ–Π΅Ρ‚ΠΈΠ» 7-Ρ„Π΅Π½Ρ–Π»-4,7-Π΄ΠΈΠ³Ρ–Π΄Ρ€ΠΎ[1,2,4]Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎ[1,5-a]ΠΏΡ–Ρ€ΠΈΠΌΡ–Π΄ΠΈΠ½-5,6-дикарбоксилатів) вста-Π½ΠΎΠ²Π»Π΅Π½ΠΎ, Ρ‰ΠΎ алкілування 4,7-Π΄ΠΈΠ³Ρ–Π΄Ρ€ΠΎΠ°Π·ΠΎΠ»ΠΎ[1,5-a]ΠΏΡ–Ρ€ΠΈΠΌΡ–Π΄ΠΈΠ½-5,6-дикарбоксилатів Ρƒ систСмі ацСтонітрилнасичСний Π²ΠΎΠ΄Π½ΠΈΠΉ Π»ΡƒΠ³ сСлСктивно ΠΏΡ€ΠΈΠ·Π²ΠΎΠ΄ΠΈΡ‚ΡŒ Π΄ΠΎ утворСння N(4)-Π°Π»ΠΊΡ–Π»ΠΏΠΎΡ…Ρ–Π΄Π½ΠΈΡ…. Π―ΠΊ ΠΎΡ‚Ρ€ΠΈΠΌΠ°Π½Ρ– вихідні сполуки, Ρ‚Π°ΠΊ Ρ– Ρ—Ρ…Π½Ρ– N(4)-ΠΌΠ΅Ρ‚ΠΈΠ»Π·Π°ΠΌΡ–Ρ‰Π΅Π½Ρ– Π°Π½Π°Π»ΠΎΠ³ΠΈ поряд Π·Ρ– споріднСними Π΄Ρ–Π΅Ρ‚ΠΈΠ» 4-Π°Ρ€ΠΈΠ»-3,4-Π΄ΠΈΠ³Ρ–Π΄Ρ€ΠΎΠΏΡ–Ρ€ΠΈΠΌΡ–Π΄ΠΈΠ½-2(1Н)-ΠΎΠ½-5,6-дикарбоксилатами, 6-Π½Π΅Π·Π°ΠΌΡ–Ρ‰Π΅Π½ΠΈΠΌΠΈ Π΅Ρ‚ΠΈΠ» 4-Π°Ρ€ΠΈΠ»-3,4-Π΄ΠΈΠ³Ρ–Π΄Ρ€ΠΎΠΏΡ–Ρ€ΠΈΠΌΡ–Π΄ΠΈΠ½-2(1Н)-ΠΎΠ½-5-карбоксилатами Ρ‚Π° ΠΏΠΎΡ…Ρ–Π΄Π½ΠΈΠΌΠΈ 6-COR-7-Π°Ρ€ΠΈΠ»-4,7-Π΄ΠΈΠ³Ρ–Π΄Ρ€ΠΎ[1,2,4]Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎ[1,5-a]ΠΏΡ–Ρ€ΠΈΠΌΡ–Π΄ΠΈΠ½Ρ–Π² Ρ” пСрспСктивними об’єктами для вивчСння Π±Π΅Π½Π·ΠΈΠ»ΡŒΠ½ΠΎΡ— Π‘(7)-Ρ„ΡƒΠ½ΠΊΡ†Ρ–ΠΎΠ½Π°Π»Ρ–Π·Π°Ρ†Ρ–Ρ— 4,7-Π΄ΠΈΠ³Ρ–Π΄Ρ€ΠΎΠ°Π·ΠΎΠ»ΠΎ[1,5-a]ΠΏΡ–Ρ€ΠΈΠΌΡ–Π΄ΠΈΠ½Ρ–Π², Π° Ρ‚Π°ΠΊΠΎΠΆ Ρ€Π΅Π°ΠΊΡ†Ρ–ΠΉ, пов’язаних Π· Π½Π°ΡΠ²Π½Ρ–ΡΡ‚ΡŽ ΠΏΠΎΠ΄Π²Ρ–ΠΉΠ½ΠΎΠ³ΠΎ C=C-зв’язку, Π°ΠΊΡ‚ΠΈΠ²ΠΎΠ²Π°Π½ΠΎΠ³ΠΎ Π΄Π²ΠΎΠΌΠ° Π°ΠΊΡ†Π΅ΠΏΡ‚ΠΎΡ€Π½ΠΈΠΌΠΈ Π³Ρ€ΡƒΠΏΠ°ΠΌΠΈ. ΠžΡ‚Ρ€ΠΈΠΌΠ°Π½Π½ΡΒ ΠΊΠ»ΡŽΡ‡ΠΎΠ²ΠΈΡ… N(4)H- Ρ– N(4)МС-ΠΏΠΎΡ…Ρ–Π΄Π½ΠΈΡ… 7-Ρ„Π΅Π½Ρ–Π»-4,7-Π΄ΠΈΠ³Ρ–Π΄Ρ€ΠΎ[1,2,4]Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎ- Ρ‚Π° Ρ‚Π΅Ρ‚Ρ€Π°Π·ΠΎΠ»ΠΎ[1,5-a]ΠΏΡ–Ρ€ΠΈΠΌΡ–Π΄ΠΈΠ½-5,6-дикарбоксилатів Ρ‚Π°ΠΊΠΎΠΆ Π²Ρ–Π΄ΠΊΡ€ΠΈΠ²Π°Ρ” ΡˆΠ»ΡΡ… Π΄ΠΎ Π±Ρ–ΠΎΠ»ΠΎΠ³Ρ–Ρ‡Π½ΠΈΡ… Π΄ΠΎΡΠ»Ρ–Π΄ΠΆΠ΅Π½ΡŒ сполук Ρ†ΡŒΠΎΠ³ΠΎ класу. Π’Ρ–Π΄Π·Π½Π°Ρ‡ΠΈΠΌΠΎ,Β Ρ‰ΠΎ дослідТСна рСакція, Π±ΡƒΠ΄ΡƒΡ‡ΠΈ Ρ‚Ρ€ΠΈΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚Π½ΠΎΡŽ, Π±Π΅Π·ΡƒΠΌΠΎΠ²Π½ΠΎ ΠΏΡ–Π΄Ρ…ΠΎΠ΄ΠΈΡ‚ΡŒ для синтСзу Ρ‚Π° дослідТСння комбінаторних Π±Ρ–Π±Π»Ρ–ΠΎΡ‚Π΅ΠΊ ΠΏΠΎΡ…Ρ–Π΄Π½ΠΈΡ… 7-Π°Ρ€ΠΈΠ»-4,7-Π΄ΠΈΠ³Ρ–Π΄Ρ€ΠΎ[1,2,4]Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎ- Ρ‚Π° Ρ‚Π΅Ρ‚Ρ€Π°Π·ΠΎΠ»ΠΎ[1,5-a]ΠΏΡ–Ρ€ΠΈΠΌΡ–Π΄ΠΈΠ½Ρ–Π²,Β Ρ‰ΠΎ ΠΌΡ–ΡΡ‚ΡΡ‚ΡŒ Π΄Π²Π° Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½ΠΎΠ°ΠΊΡ†Π΅ΠΏΡ‚ΠΎΡ€Π½Ρ– замісники Ρƒ полоТСннях 5 Ρ‚Π° 6

    Anisotropic fragmentation in low-energy dissociative recombination

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    On a dense energy grid reaching up to 75 meV electron collision energy the fragmentation angle and the kinetic energy release of neutral dissociative recombination fragments have been studied in a twin merged beam experiment. The anisotropy described by Legendre polynomials and the extracted rotational state contributions were found to vary on a likewise narrow energy scale as the rotationally averaged rate coefficient. For the first time angular dependences higher than 2nd^{nd} order could be deduced. Moreover, a slight anisotropy at zero collision energy was observed which is caused by the flattened velocity distribution of the electron beam.Comment: 8 pages, 4 figures; The Article will be published in the proceedings of DR 2007, a symposium on Dissociative Recombination held in Ameland, The Netherlands (18.-23. July 2008); Reference 19 has been published meanwhile in S. Novotny, PRL 100, 193201 (2008

    Energy-sensitive imaging detector applied to the dissociative recombination of D2H+

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    We report on an energy-sensitive imaging detector for studying the fragmentation of polyatomic molecules in the dissociative recombination of fast molecular ions with electrons. The system is based on a large area (10 cm x 10 cm) position-sensitive, double-sided Si-strip detector with 128 horizontal and 128 vertical strips, whose pulse height information is read out individually. The setup allows to uniquely identify fragment masses and is thus capable of measuring branching ratios between different fragmentation channels, kinetic energy releases, as well as breakup geometries, as a function of the relative ion-electron energy. The properties of the detection system, which has been installed at the TSR storage ring facility of the Max-Planck Institute for Nuclear Physics in Heidelberg, is illustrated by an investigation of the dissociative recombination of the deuterated triatomic hydrogen cation D2H+. A huge isotope effect is observed when comparing the relative branching ratio between the D2+H and the HD+D channel; the ratio 2B(D2+H)/B(HD+D), which is measured to be 1.27 +/- 0.05 at relative electron-ion energies around 0 eV, is found to increase to 3.7 +/- 0.5 at ~5 eV.Comment: 11 pages, 12 figures, submitted to Physical Review

    Equivalences between GIT quotients of Landau-Ginzburg B-models

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    We define the category of B-branes in a (not necessarily affine) Landau-Ginzburg B-model, incorporating the notion of R-charge. Our definition is a direct generalization of the category of perfect complexes. We then consider pairs of Landau-Ginzburg B-models that arise as different GIT quotients of a vector space by a one-dimensional torus, and show that for each such pair the two categories of B-branes are quasi-equivalent. In fact we produce a whole set of quasi-equivalences indexed by the integers, and show that the resulting auto-equivalences are all spherical twists.Comment: v3: Added two references. Final version, to appear in Comm. Math. Phy

    The first data on the infestation of the parti-coloured bat, Vespertilio murinus (Chiroptera, Vespertilionidae), with gamasid mites, Steatonyssus spinosus (Mesostigmata, Gamasina, Macronyssidae)

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    This article presents one of the very few records of a macronyssid mite (Mesostigmata, Gamasina, Macronyssidae) infestation of vesper bats (Chiroptera, Vespertilionidae). It is the first report of the influence of host parameters on the infestation of the parti-coloured bat, Vespertilio murinus, by the mite Steatonyssus spinosus. It has been shown that the infestation varies considerably throughout the host's occupation of summer roosts and the highest infestation was observed in the post-lactation period. Female bats are infested significantly more intensively than male bats due to changes in their immune status during pregnancy and lactation. The infestation decreases in the period when the breeding colony disbands due to both roost switching and the intensification of grooming during this period. Β© Russian Journal Of Theriology, 2017
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