7,709 research outputs found

    Orbital Properties of Sr3Ru2O7 and Related Ruthenates Probed by 17O-NMR

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    We report a site-separated 17^{17}O-NMR study of the layered perovskite ruthenate Sr3_3Ru2_2O7_7, which exhibits nearly two-dimensional transport properties and itinerant metamagnetism at low temperatures. The local hole occupancies and the spin densities in the oxygen 2p2p orbitals are obtained by means of tight-binding analyses of electric field gradients and anisotropic Knight shifts. These quantities are compared with two other layered perovskite ruthenates: the two-dimensional paramagnet Sr2_2RuO4_4 and the three-dimensional ferromagnet SrRuO3_3. The hole occupancies at the oxygen sites are very large, about one hole per ruthenium atom. This is due to the strong covalent character of the Ru-O bonding in this compound. The magnitude of the hole occupancy might be related to the rotation or tilt of the RuO6_6 octahedra. The spin densities at the oxygen sites are also large, 20-40% of the bulk susceptibilities, but in contrast to the hole occupancies, the spin densities strongly depend on the dimensionality. This result suggests that the density-of-states at the oxygen sites plays an essential role for the understanding of the complex magnetism found in the layered perovskite ruthenates.Comment: 9 pages, 5 figures, to be published in Phys. Rev.

    Quantum System under Periodic Perturbation: Effect of Environment

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    In many physical situations the behavior of a quantum system is affected by interaction with a larger environment. We develop, using the method of influence functional, how to deduce the density matrix of the quantum system incorporating the effect of environment. After introducing characterization of the environment by spectral weight, we first devise schemes to approximate the spectral weight, and then a perturbation method in field theory models, in order to approximately describe the environment. All of these approximate models may be classified as extended Ohmic models of dissipation whose differences are in the high frequency part. The quantum system we deal with in the present work is a general class of harmonic oscillators with arbitrary time dependent frequency. The late time behavior of the system is well described by an approximation that employs a localized friction in the dissipative part of the correlation function appearing in the influence functional. The density matrix of the quantum system is then determined in terms of a single classical solution obtained with the time dependent frequency. With this one can compute the entropy, the energy distribution function, and other physical quantities of the system in a closed form. Specific application is made to the case of periodically varying frequency. This dynamical system has a remarkable property when the environmental interaction is switched off: Effect of the parametric resonance gives rise to an exponential growth of the populated number in higher excitation levels, or particle production in field theory models. The effect of the environment is investigated for this dynamical system and it is demonstrated that there existsComment: 55 pages, LATEX file plus 13 PS figures. A few calculational mistatkes and corresponding figure 1 in field theory model corrected and some changes made for publication in Phys. Rev.D (in press

    The cross-frequency mediation mechanism of intracortical information transactions

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    In a seminal paper by von Stein and Sarnthein (2000), it was hypothesized that "bottom-up" information processing of "content" elicits local, high frequency (beta-gamma) oscillations, whereas "top-down" processing is "contextual", characterized by large scale integration spanning distant cortical regions, and implemented by slower frequency (theta-alpha) oscillations. This corresponds to a mechanism of cortical information transactions, where synchronization of beta-gamma oscillations between distant cortical regions is mediated by widespread theta-alpha oscillations. It is the aim of this paper to express this hypothesis quantitatively, in terms of a model that will allow testing this type of information transaction mechanism. The basic methodology used here corresponds to statistical mediation analysis, originally developed by (Baron and Kenny 1986). We generalize the classical mediator model to the case of multivariate complex-valued data, consisting of the discrete Fourier transform coefficients of signals of electric neuronal activity, at different frequencies, and at different cortical locations. The "mediation effect" is quantified here in a novel way, as the product of "dual frequency RV-coupling coefficients", that were introduced in (Pascual-Marqui et al 2016, http://arxiv.org/abs/1603.05343). Relevant statistical procedures are presented for testing the cross-frequency mediation mechanism in general, and in particular for testing the von Stein & Sarnthein hypothesis.Comment: https://doi.org/10.1101/119362 licensed as CC-BY-NC-ND 4.0 International license: http://creativecommons.org/licenses/by-nc-nd/4.0

    Analytic models for mechanotransduction: gating a mechanosensitive channel

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    Analytic estimates for the forces and free energy generated by bilayer deformation reveal a compelling and intuitive model for MscL channel gating analogous to the nucleation of a second phase. We argue that the competition between hydrophobic mismatch and tension results in a surprisingly rich story which can provide both a quantitative comparison to measurements of opening tension for MscL when reconstituted in bilayers of different thickness and qualitative insights into the function of the MscL channel and other transmembrane proteins

    New Kinetic Equation for Pair-annihilating Particles: Generalization of the Boltzmann Equation

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    A convenient form of kinetic equation is derived for pair annihilation of heavy stable particles relevant to the dark matter problem in cosmology. The kinetic equation thus derived extends the on-shell Boltzmann equation in a most straightforward way, including the off-shell effect. A detailed balance equation for the equilibrium abundance is further analyzed. Perturbative analysis of this equation supports a previous result for the equilibrium abundance using the thermal field theory, and gives the temperature power dependence of equilibrium value at low temperatures. Estimate of the relic abundance is possible using this new equilibrium abundance in the sudden freeze-out approximation.Comment: 19 pages, LATEX file with 2 PS figure

    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
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