25 research outputs found
Electron Spin-Lattice Relaxation of doped Yb3+ ions in YBa2Cu3Ox
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
ΠΠ°ΡΠ΄ΠΈΠΎΠ²Π°ΡΠΊΡΠ»ΡΡΠ½ΡΠ΅ ΡΡΡΠ΅ΠΊΡΡ ΠΈΠ½ΠΊΡΠ΅ΡΠΈΠ½ΠΎΠΌΠΈΠΌΠ΅ΡΠΈΠΊΠΎΠ² ΠΈ ΠΈΡ ΡΠ΅ΡΠ°ΠΏΠ΅Π²ΡΠΈΡΠ΅ΡΠΊΠΈΠΉ ΠΏΠΎΡΠ΅Π½ΡΠΈΠ°Π»
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.ΠΠ΅ΠΊΠ°ΡΡΡΠ²Π΅Π½Π½ΡΠ΅ ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΡ Ρ ΠΈΠ½ΠΊΡΠ΅ΡΠΈΠ½ΠΎΠ²ΠΎΠΉ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΡΡ ΠΏΠΎΠΌΠΈΠΌΠΎ Π²ΡΡΠ°ΠΆΠ΅Π½Π½ΠΎΠ³ΠΎ Π³ΠΈΠΏΠΎΠ³Π»ΠΈΠΊΠ΅ΠΌΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π΄Π΅ΠΉΡΡΠ²ΠΈΡ, Π²ΡΠ·ΡΠ²Π°ΡΡ ΡΠΌΠ΅ΡΠ΅Π½Π½ΠΎΠ΅ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΠ΅ Π°ΡΡΠ΅ΡΠΈΠ°Π»ΡΠ½ΠΎΠ³ΠΎ Π΄Π°Π²Π»Π΅Π½ΠΈΡ, ΠΌΠ°ΡΡΡ ΠΆΠΈΡΠΎΠ²ΠΎΠΉ ΡΠΊΠ°Π½ΠΈ ΠΈ ΡΠ»ΡΡΡΠ΅Π½ΠΈΠ΅ Π»ΠΈΠΏΠΈΠ΄Π½ΠΎΠ³ΠΎ ΠΏΡΠΎΡΠΈΠ»Ρ Ρ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Ρ ΡΠ°Ρ
Π°ΡΠ½ΡΠΌ Π΄ΠΈΠ°Π±Π΅ΡΠΎΠΌ (Π‘Π) 2 ΡΠΈΠΏΠ°. Π ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡΡ
Π΄ΠΎΠ±Π°Π²Π»Π΅Π½ΠΈΠ΅ ΠΊ ΡΠ΅ΡΠ°ΠΏΠΈΠΈ Π‘Π 2 ΡΠΈΠΏΠ° Π°Π½Π°Π»ΠΎΠ³ΠΎΠ² Π³Π»ΡΠΊΠ°Π³ΠΎΠ½ΠΎΠΏΠΎΠ΄ΠΎΠ±Π½ΠΎΠ³ΠΎ ΠΏΠ΅ΠΏΡΠΈΠ΄Π°-1 (ΠΠΠ-1) Π·Π½Π°ΡΠΈΠΌΠΎ ΡΠ½ΠΈΠΆΠ°Π»ΠΎ ΡΠΈΡΠΊ ΡΠ°Π·Π²ΠΈΡΠΈΡ ΡΠ°ΡΠ°Π»ΡΠ½ΡΡ
ΠΈ Π½Π΅ΡΠ°ΡΠ°Π»ΡΠ½ΡΡ
ΡΠ΅ΡΠ΄Π΅ΡΠ½ΠΎ-ΡΠΎΡΡΠ΄ΠΈΡΡΡΡ
ΠΎΡΠ»ΠΎΠΆΠ½Π΅Π½ΠΈΠΉ Π‘Π. Π’Π°ΠΊΠΆΠ΅ Π±ΡΠ»ΠΎ ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ Π°Π½Π°Π»ΠΎΠ³ΠΈ ΠΠΠ-1 Π² ΡΡΠ»ΠΎΠ²ΠΈΡΡ
Π‘Π ΠΎΠΊΠ°Π·ΡΠ²Π°ΡΡ ΡΠ½Π΄ΠΎΡΠ΅Π»ΠΈΠΎΠΏΡΠΎΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΠ΅, Π° ΠΏΡΠΈ ΠΈΡΠ΅ΠΌΠΈΡΠ΅ΡΠΊΠΈ-ΡΠ΅ΠΏΠ΅ΡΡΡΠ·ΠΈΠΎΠ½Π½ΠΎΠΌ ΠΏΠΎΡΠ°ΠΆΠ΅Π½ΠΈΠΈ ΠΌΠΈΠΎΠΊΠ°ΡΠ΄Π° ΠΊΠ°ΡΠ΄ΠΈΠΎΠΏΡΠΎΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΠ΅ Π΄Π΅ΠΉΡΡΠ²ΠΈΠ΅. ΠΠ°ΠΊΠΎΠΏΠ»Π΅Π½Π½ΡΠ΅ ΠΊ Π½Π°ΡΡΠΎΡΡΠ΅ΠΌΡ Π²ΡΠ΅ΠΌΠ΅Π½ΠΈ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ (ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈ Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ Π»Π°Π±ΠΎΡΠ°ΡΠΎΡΠ½ΡΡ
ΠΆΠΈΠ²ΠΎΡΠ½ΡΡ
) ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡΡ Π³ΠΎΠ²ΠΎΡΠΈΡΡ ΠΎ ΠΏΠ»Π΅ΠΉΠΎΡΡΠΎΠΏΠ½ΡΡ
ΡΡΡΠ΅ΠΊΡΠ°Ρ
ΠΈΠ½ΠΊΡΠ΅ΡΠΈΠ½ΠΎΠΌΠΈΠΌΠ΅ΡΠΈΠΊΠΎΠ², Π² ΡΠ°ΡΡΠ½ΠΎΡΡΠΈ ΠΊΠ°ΡΠ΄ΠΈΠΎ- ΠΈ ΡΠ½Π΄ΠΎΡΠ΅Π»ΠΈΠΎΠΏΡΠΎΡΠ΅ΠΊΡΠΈΠ²Π½ΡΡ
. ΠΡΠΈ ΡΡΡΠ΅ΠΊΡΡ ΡΠ΅Π°Π»ΠΈΠ·ΡΡΡΡΡ Π±Π»Π°Π³ΠΎΠ΄Π°ΡΡ Π½Π°Π»ΠΈΡΠΈΡ ΡΠ΅ΡΠ΅ΠΏΡΠΎΡΠ° ΠΊ ΠΠΠ-1 Π½Π° ΡΠ½Π΄ΠΎΡΠ΅Π»ΠΈΠΎ- ΠΈ ΠΊΠ°ΡΠ΄ΠΈΠΎΠΌΠΈΠΎΡΠΈΡΠ°Ρ
, Π½Π΅ΠΉΡΠΎΠ½Π°Ρ
, ΠΌΠΎΠ½ΠΎΡΠΈΡΠ°Ρ
ΠΈ ΠΌΠ°ΠΊΡΠΎΡΠ°Π³Π°Ρ
. Π’Π°ΠΊΠΆΠ΅ ΡΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½Π° ΡΠ²ΡΠ·Ρ Π΄Π°Π½Π½ΠΎΠ³ΠΎ ΡΠ΅ΡΠ΅ΠΏΡΠΎΡΠ° Ρ Π²Π°ΠΆΠ½Π΅ΠΉΡΠΈΠΌΠΈ Π²Π½ΡΡΡΠΈΠΊΠ»Π΅ΡΠΎΡΠ½ΡΠΌΠΈ ΡΠΈΠ³Π½Π°Π»ΡΠ½ΡΠΌΠΈ ΠΊΠ°ΡΠΊΠ°Π΄Π°ΠΌΠΈ (ΡΠ΅ΡΠ΅Π· Π°ΠΊΡΠΈΠ²Π°ΡΠΈΡ ΠΏΡΠΎΡΠ΅ΠΈΠ½ΠΊΠΈΠ½Π°Π·Ρ Π ΠΈ B), ΠΏΠΎΡΡΠ΅Π΄ΡΡΠ²ΠΎΠΌ ΡΠ΅Π³ΠΎ ΡΠ΅Π°Π»ΠΈΠ·ΡΠ΅ΡΡΡ Π²Π»ΠΈΡΠ½ΠΈΠ΅ ΠΠΠ-1 Π½Π° ΡΡΠ½ΠΊΡΠΈΠΎΠ½ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅, Π° ΡΠ°ΠΊΠΆΠ΅ ΠΏΡΠΎΡΠ΅ΡΡΡ Π°ΠΏΠΎΠΏΡΠΎΠ·Π° ΠΈ ΡΠ΅Π³Π΅Π½Π΅ΡΠ°ΡΠΈΠΈ ΠΊΠ»Π΅ΡΠΎΠΊ-ΠΌΠΈΡΠ΅Π½Π΅ΠΉ. Π ΠΎΠ±Π·ΠΎΡΠ΅ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Ρ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ ΠΊΠ°ΡΠ΄ΠΈΠΎΠ²Π°ΡΠΊΡΠ»ΡΡΠ½ΡΡ
ΡΡΡΠ΅ΠΊΡΠΎΠ² ΠΈΠ½ΠΊΡΠ΅ΡΠΈΠ½ΠΎΠΌΠΈΠΌΠ΅ΡΠΈΠΊΠΎΠ² Π² ΡΠ΅ΡΠ°ΠΏΠΈΠΈ Π‘Π, Π° ΡΠ°ΠΊΠΆΠ΅ ΠΏΡΠ΅Π΄ΠΏΠΎΠ»Π°Π³Π°Π΅ΠΌΡΠ΅ ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌΡ ΠΈΡ
ΡΠ½Π΄ΠΎΡΠ΅Π»ΠΈΠΎ- ΠΈ ΠΊΠ°ΡΠ΄ΠΈΠΎΠΏΡΠΎΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΠ³ΠΎ Π΄Π΅ΠΉΡΡΠ²ΠΈΡ. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ ΠΈΡ
Π²Π»ΠΈΡΠ½ΠΈΠ΅ Π½Π° ΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΠΎΠ΅ ΡΠΎΡΡΠΎΡΠ½ΠΈΠ΅ ΡΠ½Π΄ΠΎΡΠ΅Π»ΠΈΡ, Π²ΠΎΡΠΏΠ°Π»Π΅Π½ΠΈΠ΅ Π² ΡΠΎΡΡΠ΄ΠΈΡΡΠΎΠΉ ΡΡΠ΅Π½ΠΊΠ΅ (ΡΠΊΡΠΏΡΠ΅ΡΡΠΈΡ ΠΌΠΎΠ»Π΅ΠΊΡΠ» Π°Π΄Π³Π΅Π·ΠΈΠΈ ΠΈ ΠΏΡΠΎΠ²ΠΎΡΠΏΠ°Π»ΠΈΡΠ΅Π»ΡΠ½ΡΡ
ΡΠΈΡΠΎΠΊΠΈΠ½ΠΎΠ²), Π° ΡΠ°ΠΊΠΆΠ΅ Π°ΠΏΠΎΠΏΡΠΎΠ· ΡΠ½Π΄ΠΎΡΠ΅Π»ΠΈΠΎ- ΠΈ ΠΊΠ°ΡΠ΄ΠΈΠΎΠΌΠΈΠΎΡΠΈΡΠΎΠ²
Electron Spin-Lattice Relaxation of Er3+ ions in Er0.01Y0.99Ba2Cu3Ox
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^-)
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 and between 3.12 and 3.72 GeV at the KEDR detector
Using the KEDR detector at the VEPP-4M collider, we have measured
the values of and 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 at most of energy points with a systematic uncertainty of
about . At the moment it is the most accurate measurement of in
this energy range
Search for narrow resonances in e+ e- annihilation between 1.85 and 3.1 GeV with the KEDR Detector
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
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