3,269 research outputs found

    Nanohyperthermia of malignant tumors. II. In vivo tumor heating with manganese perovskite nanoparticles

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    Objectives: To evaluate the ability of manganese perovskite nanoparticles (lanthanum-strontium manganite) to heat the tumor tissue in vivo under action of external alternating magnetic field. Materials and Methods: The magnetic fluid on the basis of nanoparticles of perovskite manganite was tested in the heating experiments using of alternating magnetic field of frequency 300 kHz and amplitude 7.7 kA/m. Guerin carcinoma was transplanted into the muscle of rat. Magnetic fluid was injected intramuscularly or intratumorally. Temperature was measured by copper-constantan thermocouple. Results: Temperature of magnetic fluid was increased by 56 °C for 10 min of alternating magnetic field action. Administration of magnetic fluid into the muscle followed by alternating magnetic field resulted in the elevation of muscle temperature by 8 °C after 30 min post injection. Temperature of the tumor injected with magnetic fluid and treated by alternating magnetic field was increased by 13.6 °C on the 30 min of combined influence. Conclusion: In vivo study with rat tissue has demonstrated that magnetic fluid of manganite perovskite injected in the tumor increases the tumor temperature under an alternating magnetic field. Obtained results emphasize that magnetic fluid of manganite perovskite can be considered as effective inducer of tumor hyperthermia

    Rapid Depletion of Target Proteins Allows Identification of Coincident Physiological Responses

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    Targeted protein degradation is a powerful tool that can be used to create unique physiologies depleted of important factors. Current strategies involve modifying a gene of interest such that a degradation peptide is added to an expressed target protein and then conditionally activating proteolysis, either by expressing adapters, unmasking cryptic recognition determinants, or regulating protease affinities using small molecules. For each target, substantial optimization may be required to achieve a practical depletion, in that the target remains present at a normal level prior to induction and is then rapidly depleted to levels low enough to manifest a physiological response. Here, we describe a simplified targeted degradation system that rapidly depletes targets and that can be applied to a wide variety of proteins without optimizing target protease affinities. The depletion of the target is rapid enough that a primary physiological response manifests that is related to the function of the target. Using ribosomal protein Si as an example, we show that the rapid depletion of this essential translation factor invokes concomitant changes to the levels of several mRNAs, even before appreciable cell division has occurred

    Evidence for CP Violation in B0 -> D+D- Decays

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    We report measurements of the branching fraction and CP violation parameters in B0 -> D+D- decays. The results are based on a data sample that contains 535 x 10^6 BBbar pairs collected at the Upsilon(4S) resonance, with the Belle detector at the KEKB asymmetric-energy e+e- collider. We obtain [1.97 +- 0.20 (stat) +- 0.20 (syst)] x 10^(-4) for the branching fraction of B0 -> D+D-. The measured values of the CP violation parameters are: S = -1.13 +- 0.37 +- 0.09, A = 0.91 +- 0.23 +- 0.06, where the first error is statistical and the second is systematic. We find evidence of CP violation in B0 -> D+D- at the 4.1 sigma confidence level. While the value of S is consistent with expectations from other measurements, the value of the parameter A favors large direct CP violation at the 3.2 sigma confidence level, in contradiction to Standard Model expectations.Comment: 12 pages, 3 figures, submitted to PR

    Search for the h_c meson in B^+- ->h_c K^+-

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    We report a search for the hch_c meson via the decay chain B±hcK±B^{\pm}\to h_c K^{\pm}, \etac \gamma with ηcKS0K±π\eta_c \to K_S^0 K^{\pm} \pi^{\mp} and ppˉp\bar{p}. No significant signals are observed. We obtain upper limits on the branching fractions for B±ηcγK±B^{\pm} \to \eta_c\gamma K^{\pm} in bins of the ηcγ\eta_c\gamma invariant mass. The results are based on an analysis of 253 fb1^{-1} of data collected by the Belle detector at the KEKB e+ee^+e^- collider.Comment: 12 pages, 6 figures, submitted to Phys. Rev.

    Problem-solving tasks in studying agrarian question of history of Kazakhstan

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    © 2017 Serials Publications.The relevance of the article is to show the problem method of training and a possibility of its application by means of introduction in process of training at lessons of history of Kazakhstan of problem and informative tasks is considered. The purpose, types and stages of work of this technology are defined. Concrete examples of tasks for pupils of 8 classes as the problem of agrarian crisis in the territory of Kazakhstan during his stay as a part of the Russian Empire is subject to consideration (the end of XIX - the beginning of the 20th centuries) are given that corresponds to program material of this age category. The importance of application of the methods aimed at independent search of knowledge and more expanded comprehension of knowledge of pupils reveals. The statå stage of experiment where the initial level of knowledge of pupils reveals is shown in article and the importance of application of problem tasks at further stages of work is proved, questions for questioning at identification of initial knowledge of a subject, and also direct steps in work on drawing up and application of similar tasks are offered. Article Submissions are of practical value for children. having entered life, the child will be more protected from stresses. Problem training forms harmoniously developed creative person capable to think logically, find solutions in various problem situations, capable to systematize and accumulate knowledge, capable to high introspection, self-development itself also corrections. Continuous setting of problem situations leads to the loss of fear by a child to face problems, a child seeks ways to resolve them, and the creative personality, always capable to search is formed

    Влияние ионной бомбардировки на процессы азотирования при комплексной модификации поверхности стали

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    Ионная бомбардировка поверхностей, модифицируемых с использованием вакуумно-дуговых технологий, является основным физическим процессом для таких модификаций. Эксперименты производились на установке типа «Булат». В работе по азотированию поверхностей массивных стальных деталей (ст. 25Х1МФ и 40Х) исследованы особенности использования в качестве бомбардирующих частиц ионов титана и молибдена, обладающих различным энергосодержанием. Этот этап ионной бомбардировки связан с очисткой поверхности и нагревом её до необходимой температуры. На этапе азотирования бомбардировку осуществляли ионами азота, генерированными в двухступенчатом разряде. Для диагностики изменений, происходящих на поверхности образцов и на расстоянии от неё вглубь металла, использовали рентгено-флуоресцентный масс-анализ и производили измерения твёрдости с помощью прибора Nanoindentor G200. Выполнены сравнительные измерения относительных концентраций элементов в составе поверхности стали после бомбардировок различными ионами (Ti или Мо), а также получены профили залегания внедрённого в металл азота и модифицированной твёрдости. Выявлены особенности в результатах азотирования стальной поверхности при использовании разных сортов ионов. Фотографии поперечных шлифов, полученных с помощью оптического металлографического микроскопа ММО 1600, продемонстрировали отличия в структурных характеристиках приповерхностных слоёв при бомбардировках ионами титана и молибдена. Эти отличия связаны с повышенной температурой в слоях при бомбардировке ионами молибдена. Целью настоящей работы является проведение сравнительных экспериментов по обработке стальных поверхностей ускоренными ионами разных металлов с последующим анализом влияния таких воздействий на процессы азотирования этих поверхностей

    Evidence of the Purely Leptonic Decay B- --> tau- nu_tau-bar

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    We present the first evidence of the decay B- --> tau- nu_tau-bar using 414 fb^-1 of data collected at the Upsilon(4S) resonance with the Belle detector at the KEKB asymmetric-energy e+e- collider. Events are tagged by fully reconstructing one of the B mesons in hadronic modes. We detect the signal with a significance of 3.5 standard deviations including systematics, and measure the branching fraction to be Br(B- --> tau- nu_tau-bar) = (1.79 +0.56-0.49(stat) +0.46-0.51(syst))*10^-4. This implies that f_B = 0.229 +0.036-0.031(stat) +0.034-0.037(syst) GeV and is the first direct measurement of this quantity.Comment: 6 pages, 3 figures, to appear in Physical Review Letter

    Study of J/psi to p pbar, Lambda Lambdabar and observation of eta_c to Lambda Lambdabar at Belle

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    We study the baryonic charmonium decays of B mesons, B+ to etac K+ and B+ to J/psi K+, where the etac and J/psi subsequently decay into a p pbar or Lambda Lambdabar pair. We measure the J/psi to p pbar, Lambda Lambdabar anisotropy parameters, alpha_B = -0.60 +- 0.13 +-0.14 (p pbar), -0.44 +- 0.51 +- 0.31 (Lambda Lambdabar) and compare to results from e+e- to J/psi formation experiments. We also report the first observation of etac to Lambda Lambdabar. The measured branching fraction is B(etac to Lambda Lambdabar) = (0.87 +0.24 -0.21(stat) +0.09 -0.14(syst) +- 0.27 (PDG)) x 10^-3. This study is based on a 357 fb^-1 data sample recorded on the Upsilon(4S) resonance with the Belle detector at the KEKB asymmetric-energy e+e- collider.Comment: 8 pages, two figures (4 figure files), an update of hep-ex/0509020 for journal submissio

    Moments of the Hadronic Invariant Mass Spectrum in B --> X_c l nu Decays at Belle

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    We present a measurement of the hadronic invariant mass squared (M^2_X) spectrum in charmed semileptonic B meson decays B --> X_c l nu based on 140 fb^-1 of Belle data collected near the Y(4S) resonance. We determine the first, the second central and the second non-central moments of this spectrum for lepton energy thresholds ranging between 0.7 and 1.9 GeV. Full correlations between these measurements are evaluated.Comment: published version of the paper (one figure added, minor changes in the text); 16 pages, 3 figures, 10 table

    Measurements of CP Violation in B0Dπ+B^0 \to D^{*-}\pi^+ and B0Dπ+B^0 \to D^- \pi^+ Decays

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    We report measurements of time dependent decay rates for B0D()π+B^0 \to D^{(*)-}\pi^+ decays and extraction of CP violation parameters that depend on ϕ3\phi_3. Using fully reconstructed D()πD^{(*)}\pi events and partially reconstructed DπD^{*}\pi events from a data sample that contains 386 million BBˉB\bar{B} pairs that was collected near the Υ(4S)\Upsilon(4S) resonance, with the Belle detector at the KEKB asymmetric energy e+ee^+ e^- collider, we obtain the CP violation parameters S+(D()π)S^+ (D^{(*)}\pi) and S(D()π)S^- (D^{(*)}\pi). We obtain S+(Dπ)=0.049±0.020(stat)±0.011(sys)S^+ (D^* \pi) = 0.049 \pm 0.020(\mathrm{stat}) \pm 0.011(\mathrm{sys}), S(Dπ)=0.031±0.019(stat)±0.011(sys)S^- (D^* \pi) = 0.031 \pm 0.019(\mathrm{stat}) \pm 0.011(\mathrm{sys}), and S+(Dπ)=0.031±0.030(stat)±0.012(sys)S^+ (D \pi) = 0.031 \pm 0.030(\mathrm{stat}) \pm 0.012(\mathrm{sys}), S(Dπ)=0.068±0.029(stat)±0.012(sys)S^- (D \pi) = 0.068 \pm 0.029(\mathrm{stat}) \pm 0.012(\mathrm{sys}). These results are an indication of CP violation in B0Dπ+B^0 \to D^{*-}\pi^+ and B0Dπ+B^0 \to D^- \pi^+ decays at the 2.5σ2.5 \sigma and 2.2σ2.2 \sigma levels, respectively. If we use the values of RD()πR_{D^{(*)}\pi} that are derived using assumptions of factorization and SU(3) symmetry, the branching fraction measurements for the Ds()πD_s^{(*)} \pi modes, and lattice QCD calculations, we can restrict the allowed region of sin(2ϕ1+ϕ3)|\sin (2\phi_1 + \phi_3)| to be above 0.44 and 0.52 at 68% confidence level from the DπD^* \pi and DπD \pi modes, respectively.Comment: 14 pages, 12 figures, submitted to Physical Review
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