1,780 research outputs found

    Magnetic and Structural Studies of the Quasi-Two-Dimensional Spin-Gap System (CuCl)LaNb2O7

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    We report magnetization, nuclear magnetic resonance (NMR), nuclear quadrupole resonance (NQR), and transmission electron microscopy (TEM) studies on the quasi-two-dimensional spin-gap system (CuCl)LaNb2O7, a possible candidate for the J1-J2 model on a square lattice. A sharp single NQR line is observed at the Cu and Cl sites, indicating that both Cu and Cl atoms occupy a unique site. However, the electric field gradient tensors at the Cu, Cl, and La sites do not have axial symmetry. This is incompatible with the reported crystal structure. Thus the J1-J2 model has to be modified. We propose alternative two-dimensional dimer models based on the NMR, NQR, and TEM results. The value of the hyperfine coupling constant at the Cu sites indicates that the spin density is mainly on the d(3z2-r2) orbital (z parallel c). At 1.5 K, Cu- and Nb-NMR signals disappear above the critical field Bc1 = 10.3 T determined from the onset of the magnetization, indicating a field-induced magnetic phase transition at Bc1.Comment: 9 pages, 16 figure

    Collective Singlet Excitations and Evolution of Raman Spectral Weights in the 2D Spin Dimer Compound SrCu2(BO3)2

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    We present a Raman light scattering study of the two-dimensional quantum spin system SrCu2(BO3)2 and show that the magnetic excitation spectrum has a rich structure, including several well-defined bound state modes at low temperature, and a scattering continuum and quasielastic light scattering contributions at high temperature. The key to the understanding of the unique features of SrCu2(BO3)2 is the presence of strong interactions between well-localized triplet excitations in the network of orthogonal spin dimers realized in this compound. Based on our analysis of the Heisenberg model relevant for this material, we argue that the collective excitations involving two and three-particle singlet bound states have large binding energies and are observed as well-defined peaks in the Raman spectrum.Comment: 5 pages, 2 figures. Revised version, to appear in Phys. Rev. Lett. (2000

    Strong damping of phononic heat current by magnetic excitations in SrCu_2(BO_3)_2

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    Measurements of the thermal conductivity as a function of temperature and magnetic field in the 2D dimer spin system SrCu2_2(BO3_3)2_2 are presented. In zero magnetic field the thermal conductivity along and perpendicular to the magnetic planes shows a pronounced double-peak structure as a function of temperature. The low-temperature maximum is drastically suppressed with increasing magnetic field. Our quantitative analysis reveals that the heat current is due to phonons and that the double-peak structure arises from pronounced resonant scattering of phonons by magnetic excitations.Comment: a bit more than 4 pages, 2 figures included; minor changes to improve the clarity of the presentatio

    Geodynamo and mantle convection simulations on the Earth Simulator using the Yin-Yang grid

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    We have developed finite difference codes based on the Yin-Yang grid for the geodynamo simulation and the mantle convection simulation. The Yin-Yang grid is a kind of spherical overset grid that is composed of two identical component grids. The intrinsic simplicity of the mesh configuration of the Yin-Yang grid enables us to develop highly optimized simulation codes on massively parallel supercomputers. The Yin-Yang geodynamo code has achieved 15.2 Tflops with 4096 processors on the Earth Simulator. This represents 46% of the theoretical peak performance. The Yin-Yang mantle code has enabled us to carry out mantle convection simulations in realistic regimes with a Rayleigh number of 10710^7 including strongly temperature-dependent viscosity with spatial contrast up to 10610^6.Comment: Plenary talk at SciDAC 200

    Promotive effects of hyperthermia on the сytostatic activity to ehrlich ascites tumor cells by diverse delta-alkyllactones

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    To evaluate promotive effects of hyperthermia on antitumor activity of new delta-alkyllactones (DALs) of low molecular weight (184–254 Da), chemically synthesized, which are different from natural macrocyclic lactones of high molecular weight (348–439 Da), such as camptothecin and sultriecin. Methods: A suspension of Ehrlich ascites tumor (EAT) cells was mixed with a DAL in a glass tube, heated at 37 or 42 Β°C for 30 min in a water bath, and cultured at 37 Β°C for 20 or 72 h. Cell viability was measured by the mitochondrial dehydrogenase- based WST-1 assay. DALs incorporated into EAT cells was extracted and measured by gas-liquid chromatography. Results: The reduction of cell viability by DALs was markedly enhanced upon the treatment at 42 Β°C compared to that at 37 oC. At 37 oC, delta-hexadecalactone (DH16 : 0) and delta-tetradecalactone (DTe14 : 0) displayed cytostatic activity (at 100 Β΅M survival level: 20.7%, 66.1%; at 50 Β΅M β€” 41.2%, 82.4%, respectively). Their activity was more marked at 42 Β°C (at 100 Β΅M 10.6%, 27.6%; at 50 Β΅M 30.6, 37.5 %, ibid). The other DALs, delta-undecalactone (DU11 : 0), delta-dodecalactone (DD12 : 0), and delta-tridecanolactone (DTr13 : 0) were almost ineffective. Evaluation of survival rate in the cells treated for 30 min by DALs with the next culturing of EAT cells for 72 h resulted in the enhanced carcinostatic activity of DH16:0 and DTe14:0 even at concentrations as low as 25 Β΅M at either 37 Β°C (18.5%, 78.5%, ibid) or 42 Β°C (5.0%, 42.0%, ibid), but the others exhibited slight activity or none. DH16 : 0 was effective at either 37 Β°C (36.0%) or 42 Β°C (23.0%) even at a lower dose of 10 Β΅M. At the same time only the most cytostatic DH16 : 0 was incorporated into EAT cells and the rate of incorporation was more at 42 Β°C than at 37 Β°C. Conclusion: Delta-hexadecanolactone (DH16 : 0) exhibited the most cytostatic effect that was significantly enhanced by hyperthermia. It allows to consider it as a potent antitumor agent, especially in combination with hyperthermia.ЦСль: ΠΎΡ†Π΅Π½ΠΈΡ‚ΡŒ ΠΏΡ€ΠΎΠΌΠΎΡ‚ΠΎΡ€Π½Ρ‹ΠΉ эффСкт Π³ΠΈΠΏΠ΅Ρ€Ρ‚Π΅Ρ€ΠΌΠΈΠΈ Π½Π° ΠΏΡ€ΠΎΡ‚ΠΈΠ²ΠΎΠΎΠΏΡƒΡ…ΠΎΠ»Π΅Π²ΡƒΡŽ Π°ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ Π½ΠΎΠ²Ρ‹Ρ… низкомолСкулярных (184–254 Π”Π°) Π΄Π΅Π»ΡŒΡ‚Π°-Π°Π»ΠΊΠΈΠ»Π»Π°ΠΊΡ‚ΠΎΠ½ΠΎΠ² (DALs), химичСски синтСзированных ΠΈΠ· Ρ€Π°Π·Π½Ρ‹Ρ… макроцикличСских высокомолСкулярных (348–439Π”Π°) Π»Π°ΠΊΡ‚ΠΎΠ½ΠΎΠ² СстСствСнного происхоТдСния, Ρ‚Π°ΠΊΠΈΡ… ΠΊΠ°ΠΊ ΠΊΠ°ΠΌΠΏΡ‚ΠΎΡ‚Π΅Ρ†ΠΈΠ½ ΠΈ салтриСцин. ΠœΠ΅Ρ‚ΠΎΠ΄Ρ‹: ΡΡƒΡΠΏΠ΅Π½Π·ΠΈΡŽ ΠΊΠ»Π΅Ρ‚ΠΎΠΊ асцитной ΠΎΠΏΡƒΡ…ΠΎΠ»ΠΈ Π­Ρ€Π»ΠΈΡ…Π° (EAT) смСшивали с DAL Π² стСклянной ΠΏΡ€ΠΎΠ±ΠΈΡ€ΠΊΠ΅, Π½Π°Π³Ρ€Π΅Π²Π°Π»ΠΈ Π΄ΠΎ 37 Β°C ΠΈΠ»ΠΈ 42 Β°C Π² Ρ‚Π΅Ρ‡Π΅Π½ΠΈΠ΅ 30 ΠΌΠΈΠ½ Π½Π° водяной Π±Π°Π½Π΅ ΠΈ Π΄Π°Π»Π΅Π΅ ΠΊΡƒΠ»ΡŒΡ‚ΠΈΠ²ΠΈΡ€ΠΎΠ²Π°Π»ΠΈ ΠΏΡ€ΠΈ 37 Β°C Π² Ρ‚Π΅Ρ‡Π΅Π½ΠΈΠ΅ 20 ΠΈΠ»ΠΈ 72 Ρ‡. ΠžΡ†Π΅Π½ΠΊΡƒ ТизнСспособности ΠΊΠ»Π΅Ρ‚ΠΎΠΊ ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ с ΠΏΠΎΠΌΠΎΡ‰ΡŒΡŽ WST-1 Π°Π½Π°Π»ΠΈΠ·Π°, основанного Π½Π° ΠΎΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½ΠΈΠΈ ΠΌΠΈΡ‚ΠΎΡ…ΠΎΠ½Π΄Ρ€ΠΈΠ°Π»ΡŒΠ½ΠΎΠΉ Π΄Π΅Π³ΠΈΠ΄Ρ€ΠΎΠ³Π΅Π½Π°Π·Ρ‹. Π˜Π½ΠΊΠΎΡ€ΠΏΠΎΡ€ΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹Π΅ Π² EAT-ΠΊΠ»Π΅Ρ‚ΠΊΠΈ DALs экстрагировали, ΠΈΡ… ΡƒΡ€ΠΎΠ²Π΅Π½ΡŒ измСряли с ΠΏΠΎΠΌΠΎΡ‰ΡŒΡŽ Π³Π°Π·ΠΎ-Тидкостной Ρ…Ρ€ΠΎΠΌΠ°Ρ‚ΠΎΠ³Ρ€Π°Ρ„ΠΈΠΈ. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹: DALs Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ сниТали ΠΆΠΈΠ·Π½Π΅ΡΠΏΠΎΡΠΎΠ±Π½ΠΎΡΡ‚ΡŒ ΠΊΠ»Π΅Ρ‚ΠΎΠΊ послС ΠΏΡ€Π΅Π΄Π²Π°Ρ€ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠΉ ΠΎΠ±Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ ΠΏΡ€ΠΈ 42 Β°C ΠΏΠΎ ΡΡ€Π°Π²Π½Π΅Π½ΠΈΡŽ с 37 Β°C. ΠŸΡ€ΠΈ 37 Β°C Π±Ρ‹Π»ΠΈ эффСктивными Π΄Π΅Π»ΡŒΡ‚Π°-гСксадСкалактон (DH16 : 0) ΠΈ Π΄Π΅Π»ΡŒΡ‚Π°-Ρ‚Π΅Ρ‚Ρ€Π°Π΄Π΅ΠΊΠ°Π»Π°ΠΊΡ‚ΠΎΠ½ (DTe14 : 0) (ΠΏΡ€ΠΈ 100 ΞΌM ΡƒΡ€ΠΎΠ²Π΅Π½ΡŒ выТиваСмости: 20,7; 66,1%; ΠΏΡ€ΠΈ 50 ΞΌM β€” 41,2; 82,4% соотвСтствСнно). Π­Ρ‚ΠΎΡ‚ эффСкт Π±Ρ‹Π» Π±ΠΎΠ»Π΅Π΅ Π²Ρ‹Ρ€Π°ΠΆΠ΅Π½Π½Ρ‹ΠΌ ΠΏΡ€ΠΈ 42 Β°C (ΠΏΡ€ΠΈ 100 ΞΌM 10,6; 27,6%; ΠΏΡ€ΠΈ 50ΞΌM 30,6; 37,5% соотвСтствСнно). Π”Ρ€ΡƒΠ³ΠΈΠ΅ DALs, Π° ΠΈΠΌΠ΅Π½Π½ΠΎ Π΄Π΅Π»ΡŒΡ‚Π°-ΡƒΠ½Π΄Π΅ΠΊΠ°Π»Π°ΠΊΡ‚ΠΎΠ½ (DU11 : 0), Π΄Π΅Π»ΡŒΡ‚Π°-Π΄ΠΎΠ΄Π΅ΠΊΠ°Π»Π°ΠΊΡ‚ΠΎΠ½ (DD12 : 0) ΠΈ Π΄Π΅Π»ΡŒΡ‚Π°-Ρ‚Ρ€ΠΈΠ΄Π΅ΠΊΠ°Π»Π°ΠΊΡ‚ΠΎΠ½ (DTr13 : 0) Π±Ρ‹Π»ΠΈ практичСски Π½Π΅ эффСктивны. ΠžΡ†Π΅Π½ΠΊΠ° уровня выТиваСмости EAT-ΠΊΠ»Π΅Ρ‚ΠΎΠΊ, 30 ΠΌΠΈΠ½ ΠΎΠ±Ρ€Π°Π±ΠΎΡ‚Π°Π½Π½Ρ‹Ρ… DALs с ΠΏΠΎΡΠ»Π΅Π΄ΡƒΡŽΡ‰ΠΈΠΌ ΠΊΡƒΠ»ΡŒΡ‚ΠΈΠ²ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ Π² Ρ‚Π΅Ρ‡Π΅Π½ΠΈΠ΅ 72 Ρ‡, ΠΏΠΎΠΊΠ°Π·Π°Π»Π° ΠΏΠΎΠ²Ρ‹ΡˆΠ΅Π½Π½ΡƒΡŽ ΠΊΠ°Π½Ρ†Π΅Ρ€ΠΎΡΡ‚Π°Ρ‚ΠΈΡ‡ΡΠ΅ΠΊΡƒΡŽ Π°ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ DH16 : 0 ΠΈ DTe14 :0 Π΄Π°ΠΆΠ΅ ΠΏΡ€ΠΈ 25 ΞΌM ΠΊΠΎΠ½Ρ†Π΅Π½Ρ‚Ρ€Π°Ρ†ΠΈΠΈ, ΠΊΠ°ΠΊ ΠΏΡ€ΠΈ 37 Β°C (18,5; 78,5% соотвСтсвСнно), Ρ‚Π°ΠΊ ΠΈ ΠΏΡ€ΠΈ 42 Β°C (5,0; 42,0% соотвСтствСнно). Для Π΄Ρ€ΡƒΠ³ΠΈΡ… DALs Π΄Π°Π½Π½Ρ‹ΠΉ эффСкт Π±Ρ‹Π» Π½Π΅Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹ΠΉ Π»ΠΈΠ±ΠΎ отсутствовал. DH16 : 0 оставался эффСктивным ΠΊΠ°ΠΊ ΠΏΡ€ΠΈ 37 Β°C (36,0%), Ρ‚Π°ΠΊ ΠΈ ΠΏΡ€ΠΈ 42 Β°C (23,0%) Π² 10 ΞΌM ΠΊΠΎΠ½Ρ†Π΅Π½Ρ‚Ρ€Π°Ρ†ΠΈΠΈ. Π’ Ρ‚ΠΎ ΠΆΠ΅ врСмя Ρ‚ΠΎΠ»ΡŒΠΊΠΎ Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ эффСктивный DAL β€” DH16 : 0 инкорпорировался Π² ΠΊΠ»Π΅Ρ‚ΠΊΠΈ EAT, ΠΈ ΡƒΡ€ΠΎΠ²Π΅Π½ΡŒ инкорпорирования Π±Ρ‹Π» Π²Ρ‹ΡˆΠ΅ ΠΏΡ€ΠΈ 42 Β°C, Ρ‡Π΅ΠΌ ΠΏΡ€ΠΈ 37 Β°C. Π’Ρ‹Π²ΠΎΠ΄Ρ‹: Π΄Π΅Π»ΡŒΡ‚Π°-гСксадСканолактон (DH16 : 0) ΠΏΠΎΠΊΠ°Π·Π°Π» Π½Π°ΠΈΠ±ΠΎΠ»ΡŒΡˆΡƒΡŽ Ρ†ΠΈΡ‚ΠΎΡΡ‚Π°Ρ‚ΠΈΡ‡Π΅ΡΠΊΡƒΡŽ Π°ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ, которая Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ ΡƒΡΠΈΠ»ΠΈΠ²Π°Π»Π°ΡΡŒ Π² ΠΊΠΎΠΌΠ±ΠΈΠ½Π°Ρ†ΠΈΠΈ с Π³ΠΈΠΏΠ΅Ρ€Ρ‚Π΅Ρ€ΠΌΠΈΠ΅ΠΉ. Π­Ρ‚ΠΎΡ‚ DAL ΠΌΠΎΠΆΠ½ΠΎ Ρ€Π°ΡΡΠΌΠ°Ρ‚Ρ€ΠΈΠ²Π°Ρ‚ΡŒ ΠΊΠ°ΠΊ ΠΏΠΎΡ‚Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½Ρ‹ΠΉ цитостатик, дСйствиС ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠ³ΠΎ усиливаСтся ΠΏΡ€ΠΈ Π³ΠΈΠΏΠ΅Ρ€Ρ‚Π΅Ρ€ΠΌΠΈΠΈ

    BiCu2_2VO6_6: a new narrow-band spin-gap material

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    A new spin-ladder family material BiCu2_2VO6_6 is studied by means of the magnetic susceptibility, heat capacity and neutron inelastic scattering measurements on powder sample. Singlet ground state and a finite spin gap are confirmed by thermal-activated type susceptibility and by distinct peak at 16 meV in spin excitation. Triple narrow band structure in spin excitation spectrum, probably due to complex crystal structure, is observed and the possibility of weakly-interacting spin-cluster system is discussed
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