25 research outputs found

    Electron Spin-Lattice Relaxation of doped Yb3+ ions in YBa2Cu3Ox

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    The electron spin-lattice relaxation (SLR) times T1 of Yb3+‡ ions were measured from the temperature dependence of electron spin resonance linewidth in Y0.99Yb0.01Ba2Cu3Ox with different oxygen contents. Raman relaxation processes dominate the electron SLR. Derived from the temperature dependence of the SLR rate, the Debye temperature (Td) increases with the critical temperature Tc and oxygen content x. Keywords: EPR; ESR; Electron spin-lattice relaxation; Debye temperature; Critical temperatureComment: 5 Pages 4 Figure

    ΠšΠ°Ρ€Π΄ΠΈΠΎΠ²Π°ΡΠΊΡƒΠ»ΡΡ€Π½Ρ‹Π΅ эффСкты ΠΈΠ½ΠΊΡ€Π΅Ρ‚ΠΈΠ½ΠΎΠΌΠΈΠΌΠ΅Ρ‚ΠΈΠΊΠΎΠ² ΠΈ ΠΈΡ… тСрапСвтичСский ΠΏΠΎΡ‚Π΅Π½Ρ†ΠΈΠ°Π»

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    Antidiabetic drugs with incretin activity in addition to pronounced hypoglycemic activity cause moderate reduction in blood pressure and fat mass as well as improve the lipid profile in patients with type 2 diabetes mellitus (T2DM). In clinical trials the addition of glucagon-like peptide-1 (GLP-1) analogues to standart T2DM therapy leads to significantly reduce the risk of fatal and nonfatal cardiovascular complications. According to the results of many experimental and clinical studies it was shown that GLP-1 analogs protect endothelium in diabetic patients and protect cardiomyocytes after ischemia-reperfusion lesion. Pleiotropic effects of GLP-1-based therapies are realized due to the presence of GLP-1-receptor in endothelial cells, cardiomyocytes, neurons, monocytes and macrophages, as well as due to the connection of the receptor with the most important intracellular signaling cascades (through activation of protein kinase A and B). Whereby GLP-1-based therapies affect the functional condition as well as processes of regeneration and apoptosis of target cells. This review presents the results of studies the cardiovascular effects of GLP-1-based therapies of diabetes. Described proposed nowadays mechanisms of endothelium protective and cardioprotective action of GLP-1 analogs that associated with the action on endothelial function, vascular wall inflammation (the expression of adhesion molecules and inflammatory cytokines), and apoptosis of endothelial cells and cardiomyocytes.ЛСкарствСнныС ΠΏΡ€Π΅ΠΏΠ°Ρ€Π°Ρ‚Ρ‹ с ΠΈΠ½ΠΊΡ€Π΅Ρ‚ΠΈΠ½ΠΎΠ²ΠΎΠΉ Π°ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒΡŽ ΠΏΠΎΠΌΠΈΠΌΠΎ Π²Ρ‹Ρ€Π°ΠΆΠ΅Π½Π½ΠΎΠ³ΠΎ гипогликСмичСского дСйствия, Π²Ρ‹Π·Ρ‹Π²Π°ΡŽΡ‚ ΡƒΠΌΠ΅Ρ€Π΅Π½Π½ΠΎΠ΅ сниТСниС Π°Ρ€Ρ‚Π΅Ρ€ΠΈΠ°Π»ΡŒΠ½ΠΎΠ³ΠΎ давлСния, массы ΠΆΠΈΡ€ΠΎΠ²ΠΎΠΉ Ρ‚ΠΊΠ°Π½ΠΈ ΠΈ ΡƒΠ»ΡƒΡ‡ΡˆΠ΅Π½ΠΈΠ΅ Π»ΠΈΠΏΠΈΠ΄Π½ΠΎΠ³ΠΎ профиля Ρƒ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ² с сахарным Π΄ΠΈΠ°Π±Π΅Ρ‚ΠΎΠΌ (Π‘Π”) 2 Ρ‚ΠΈΠΏΠ°. Π’ клиничСских исслСдованиях Π΄ΠΎΠ±Π°Π²Π»Π΅Π½ΠΈΠ΅ ΠΊ Ρ‚Π΅Ρ€Π°ΠΏΠΈΠΈ Π‘Π” 2 Ρ‚ΠΈΠΏΠ° Π°Π½Π°Π»ΠΎΠ³ΠΎΠ² глюкагоноподобного ΠΏΠ΅ΠΏΡ‚ΠΈΠ΄Π°-1 (Π“ΠŸΠŸ-1) Π·Π½Π°Ρ‡ΠΈΠΌΠΎ сниТало риск развития Ρ„Π°Ρ‚Π°Π»ΡŒΠ½Ρ‹Ρ… ΠΈ Π½Π΅Ρ„Π°Ρ‚Π°Π»ΡŒΠ½Ρ‹Ρ… сСрдСчно-сосудистых ослоТнСний Π‘Π”. Π’Π°ΠΊΠΆΠ΅ Π±Ρ‹Π»ΠΎ ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΎ, Ρ‡Ρ‚ΠΎ Π°Π½Π°Π»ΠΎΠ³ΠΈ Π“ΠŸΠŸ-1 Π² условиях Π‘Π” ΠΎΠΊΠ°Π·Ρ‹Π²Π°ΡŽΡ‚ эндотСлиопротСктивноС, Π° ΠΏΡ€ΠΈ ΠΈΡˆΠ΅ΠΌΠΈΡ‡Π΅ΡΠΊΠΈ-Ρ€Π΅ΠΏΠ΅Ρ€Ρ„ΡƒΠ·ΠΈΠΎΠ½Π½ΠΎΠΌ ΠΏΠΎΡ€Π°ΠΆΠ΅Π½ΠΈΠΈ ΠΌΠΈΠΎΠΊΠ°Ρ€Π΄Π° ΠΊΠ°Ρ€Π΄ΠΈΠΎΠΏΡ€ΠΎΡ‚Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΠ΅ дСйствиС. НакоплСнныС ΠΊ настоящСму Π²Ρ€Π΅ΠΌΠ΅Π½ΠΈ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ исслСдований (клиничСских ΠΈ с использованиСм Π»Π°Π±ΠΎΡ€Π°Ρ‚ΠΎΡ€Π½Ρ‹Ρ… ΠΆΠΈΠ²ΠΎΡ‚Π½Ρ‹Ρ…) ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡŽΡ‚ Π³ΠΎΠ²ΠΎΡ€ΠΈΡ‚ΡŒ ΠΎ ΠΏΠ»Π΅ΠΉΠΎΡ‚Ρ€ΠΎΠΏΠ½Ρ‹Ρ… эффСктах ΠΈΠ½ΠΊΡ€Π΅Ρ‚ΠΈΠ½ΠΎΠΌΠΈΠΌΠ΅Ρ‚ΠΈΠΊΠΎΠ², Π² частности ΠΊΠ°Ρ€Π΄ΠΈΠΎ- ΠΈ эндотСлиопротСктивных. Π­Ρ‚ΠΈ эффСкты Ρ€Π΅Π°Π»ΠΈΠ·ΡƒΡŽΡ‚ΡΡ благодаря Π½Π°Π»ΠΈΡ‡ΠΈΡŽ Ρ€Π΅Ρ†Π΅ΠΏΡ‚ΠΎΡ€Π° ΠΊ Π“ΠŸΠŸ-1 Π½Π° эндотСлио- ΠΈ ΠΊΠ°Ρ€Π΄ΠΈΠΎΠΌΠΈΠΎΡ†ΠΈΡ‚Π°Ρ…, Π½Π΅ΠΉΡ€ΠΎΠ½Π°Ρ…, ΠΌΠΎΠ½ΠΎΡ†ΠΈΡ‚Π°Ρ… ΠΈ ΠΌΠ°ΠΊΡ€ΠΎΡ„Π°Π³Π°Ρ…. Π’Π°ΠΊΠΆΠ΅ установлСна связь Π΄Π°Π½Π½ΠΎΠ³ΠΎ Ρ€Π΅Ρ†Π΅ΠΏΡ‚ΠΎΡ€Π° с ваТнСйшими Π²Π½ΡƒΡ‚Ρ€ΠΈΠΊΠ»Π΅Ρ‚ΠΎΡ‡Π½Ρ‹ΠΌΠΈ ΡΠΈΠ³Π½Π°Π»ΡŒΠ½Ρ‹ΠΌΠΈ каскадами (Ρ‡Π΅Ρ€Π΅Π· Π°ΠΊΡ‚ΠΈΠ²Π°Ρ†ΠΈΡŽ ΠΏΡ€ΠΎΡ‚Π΅ΠΈΠ½ΠΊΠΈΠ½Π°Π·Ρ‹ А ΠΈ B), посрСдством Ρ‡Π΅Π³ΠΎ рСализуСтся влияниС Π“ΠŸΠŸ-1 Π½Π° Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΎΠ½ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅, Π° Ρ‚Π°ΠΊΠΆΠ΅ процСссы Π°ΠΏΠΎΠΏΡ‚ΠΎΠ·Π° ΠΈ Ρ€Π΅Π³Π΅Π½Π΅Ρ€Π°Ρ†ΠΈΠΈ ΠΊΠ»Π΅Ρ‚ΠΎΠΊ-мишСнСй. Π’ ΠΎΠ±Π·ΠΎΡ€Π΅ прСдставлСны Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ исслСдований кардиоваскулярных эффСктов ΠΈΠ½ΠΊΡ€Π΅Ρ‚ΠΈΠ½ΠΎΠΌΠΈΠΌΠ΅Ρ‚ΠΈΠΊΠΎΠ² Π² Ρ‚Π΅Ρ€Π°ΠΏΠΈΠΈ Π‘Π”, Π° Ρ‚Π°ΠΊΠΆΠ΅ ΠΏΡ€Π΅Π΄ΠΏΠΎΠ»Π°Π³Π°Π΅ΠΌΡ‹Π΅ ΠΌΠ΅Ρ…Π°Π½ΠΈΠ·ΠΌΡ‹ ΠΈΡ… эндотСлио- ΠΈ ΠΊΠ°Ρ€Π΄ΠΈΠΎΠΏΡ€ΠΎΡ‚Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΠ³ΠΎ дСйствия. Показано ΠΈΡ… влияниС Π½Π° Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΎΠ½Π°Π»ΡŒΠ½ΠΎΠ΅ состояниС эндотСлия, воспалСниС Π² сосудистой стСнкС (ΡΠΊΡΠΏΡ€Π΅ΡΡΠΈΡŽ ΠΌΠΎΠ»Π΅ΠΊΡƒΠ» Π°Π΄Π³Π΅Π·ΠΈΠΈ ΠΈ ΠΏΡ€ΠΎΠ²ΠΎΡΠΏΠ°Π»ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… Ρ†ΠΈΡ‚ΠΎΠΊΠΈΠ½ΠΎΠ²), Π° Ρ‚Π°ΠΊΠΆΠ΅ Π°ΠΏΠΎΠΏΡ‚ΠΎΠ· эндотСлио- ΠΈ ΠΊΠ°Ρ€Π΄ΠΈΠΎΠΌΠΈΠΎΡ†ΠΈΡ‚ΠΎΠ²

    Electron Spin-Lattice Relaxation of Er3+ ions in Er0.01Y0.99Ba2Cu3Ox

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    The temperature dependence of the electron spin-lattice relaxation SLR was studied in Er0.01Y0.99Ba2Cu3Ox compounds. The data derived from the electron spin resonance ESR and SLR measurements were compared to those from inelastic neutron scattering studies. SLR of Er3+ ions in the temperature range from 20 K to 65 K can be explained by the resonant phonon relaxation process with the involvement of the lowest excited crystalline-electric-field electronic states of Er3+. These results are consistent with a local phase separation effects. Possible mechanisms of the ESR line broadening at lower temperatures are discussed. Keywords: YBCO; EPR; ESR; Electron spin-lattice relaxation time, T ; Crystalline-electric-fieldComment: 6 pages, 4 figure

    Measurement of \Gamma_{ee}(J/\psi)*Br(J/\psi->e^+e^-) and \Gamma_{ee}(J/\psi)*Br(J/\psi->\mu^+\mu^-)

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    The products of the electron width of the J/\psi meson and the branching fraction of its decays to the lepton pairs were measured using data from the KEDR experiment at the VEPP-4M electron-positron collider. The results are \Gamma_{ee}(J/\psi)*Br(J/\psi->e^+e^-)=(0.3323\pm0.0064\pm0.0048) keV, \Gamma_{ee}(J/\psi)*Br(J/\psi->\mu^+\mu^-)=(0.3318\pm0.0052\pm0.0063) keV. Their combinations \Gamma_{ee}\times(\Gamma_{ee}+\Gamma_{\mu\mu})/\Gamma=(0.6641\pm0.0082\pm0.0100) keV, \Gamma_{ee}/\Gamma_{\mu\mu}=1.002\pm0.021\pm0.013 can be used to improve theaccuracy of the leptonic and full widths and test leptonic universality. Assuming e\mu universality and using the world average value of the lepton branching fraction, we also determine the leptonic \Gamma_{ll}=5.59\pm0.12 keV and total \Gamma=94.1\pm2.7 keV widths of the J/\psi meson.Comment: 7 pages, 6 figure

    Measurement of RudsR_{\text{uds}} and RR between 3.12 and 3.72 GeV at the KEDR detector

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    Using the KEDR detector at the VEPP-4M e+eβˆ’e^+e^- collider, we have measured the values of RudsR_{\text{uds}} and RR at seven points of the center-of-mass energy between 3.12 and 3.72 GeV. The total achieved accuracy is about or better than 3.3%3.3\% at most of energy points with a systematic uncertainty of about 2.1%2.1\%. At the moment it is the most accurate measurement of R(s)R(s) in this energy range

    Search for narrow resonances in e+ e- annihilation between 1.85 and 3.1 GeV with the KEDR Detector

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    We report results of a search for narrow resonances in e+ e- annihilation at center-of-mass energies between 1.85 and 3.1 GeV performed with the KEDR detector at the VEPP-4M e+ e- collider. The upper limit on the leptonic width of a narrow resonance Gamma(R -> ee) Br(R -> hadr) < 120 eV has been obtained (at 90 % C.L.)

    Measurement of main parameters of the \psi(2S) resonance

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    A high-precision determination of the main parameters of the \psi(2S) resonance has been performed with the KEDR detector at the VEPP-4M e^{+}e^{-} collider in three scans of the \psi(2S) -- \psi(3770) energy range. Fitting the energy dependence of the multihadron cross section in the vicinity of the \psi(2S) we obtained the mass value M = 3686.114 +- 0.007 +- 0.011 ^{+0.002}_{-0.012} MeV and the product of the electron partial width by the branching fraction into hadrons \Gamma_{ee}*B_{h} = 2.233 +- 0.015 +- 0.037 +- 0.020 keV. The third error quoted is an estimate of the model dependence of the result due to assumptions on the interference effects in the cross section of the single-photon e^{+}e^{-} annihilation to hadrons explicitly considered in this work. Implicitly, the same assumptions were employed to obtain the charmonium leptonic width and the absolute branching fractions in many experiments. Using the result presented and the world average values of the electron and hadron branching fractions, one obtains the electron partial width and the total width of the \psi(2S): \Gamma_{ee} =2.282 +- 0.015 +- 0.038 +- 0.021 keV, \Gamma = 296 +- 2 +- 8 +- 3 keV. These results are consistent with and more than two times more precise than any of the previous experiments
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