2,072 research outputs found
Ferromagnetic Polarons in La0.5Ca0.5MnO3 and La0.33Ca0.67MnO3
Unrestricted Hartree-Fock calculations on La0.5Ca0.5MnO3 and La0.33Ca0.67MnO3
in the full magnetic unit cell show that the magnetic ground states of these
compounds consist of 'ferromagnetic molecules' or polarons ordered in
herring-bone patterns. Each polaron consists of either three or five Mn ions
separated by O- ions with a magnetic moment opposed to those of the Mn ions.
Ferromagnetic coupling within the polarons is strong while coupling between
them is relatively weak. Magnetic moments on the Mn ions range between 3.8 and
3.9 Bohr magnetons in La0.5Ca0.5MnO3 and moments on the O- ions are -0.7 Bohr
magnetons. Each polaron has a net magnetic moment of 7.0 Bohr magnetons, in
good agreement with recently reported magnetisation measurements from electron
microscopy. The polaronic nature of the electronic structure reported here is
obviously related to the Zener polaron model recently proposed for
Pr0.6Ca0.4MnO3 on the basis of neutron scattering data.Comment: 4 pages 5 figure
Sinusoidal cells and cytokine response in the tetrachloromethane-induced hepatotoxicity and an approach to its correction
High occurence of liver diseases (toxic, viral hepatitis, liver failure, cirrhosis) requires urgent search of new methods for management of the hepatobiliary diseases. At the present time, the role of immune mechanisms in pathogenesis of diffuse toxic liver damage is not finally clarified. The model of toxic hepatitis induced by carbon tetrachloride (CCl4) is widely known, but this approach allows us to perform complex evaluation and develop the methods for adequate correction of liver disorders in experimental model, which is not always feasible in clinical setting. To design a model of diffuse toxic liver damage, the CCl4 oil solution was used, having been administered intraperitoneally to experimental animals, at a single dose of 50 mg per 100 g body mass. Aiming for correction of toxic liver damage, the injections of aminophthalhydrazide (APH) to experimental animals were carried out intramuscularly at the dose of 2 mg/kg over the terms of experiment. An evaluation of the role of sinusoidal cells (SC) and cytokine production at the local and systemic level were carried out in the model of toxic liver damage caused by CCl4 and its correction by APH treatment. In the course of developing diffuse toxic liver damage induced by CCl4, the production of proinflammatory cytokines TNFΞ±, IL-1Ξ± and IL-18 was enhanced at the local level, whereas an increase in TNFΞ± concentration was observed in blood plasma. Following aminophthalhydrazide (APH) administration, the concentrations of proinflammatory cytokines (TNFΞ± and IL-18) decreased at system level, along with locally decreased levels of IL-6 and IFNΞ³. Changes in the functional state of immunocompetent cells, which include sinusoidal cells (SC), have a significant impact on the development of pathological processes in the liver. The results of our study presume that, over the early periods of toxic impact upon liver tissue, the number of SCs increases both due to influx of blood monocytes and mature macrophages from the peritoneal cavity that enter the injury site directly via mesothelial layer. The SCs provide phagocytosis of damaged hepatocytes and contribute to resolution of the inflammatory process. Modulation of the macrophage activities by APH contributes to increased amounts of SCs at the early stages, and stabilizes their quantities after 2 weeks of APH injections. Change in the numbers of liver SCs during toxic damage affects the production of cytokines. A direct effect of APH upon the SCs may change the production of regulatory factors and compensate the insufficient rate of recovery processes after the toxic damage. Β© 2019, SPb RAACI
ΠΠΏΡΡ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΡ N-Π°ΡΠ΅ΡΠΈΠ»ΡΠΈΡΡΠ΅ΠΈΠ½Π° Π² ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ½ΠΎΠΌ Π»Π΅ΡΠ΅Π½ΠΈΠΈ ΡΡΠ΅Π΄Π½Π΅ΡΡΠΆΠ΅Π»ΠΎΠΉ COVID-Π°ΡΡΠΎΡΠΈΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΉ ΠΏΠ½Π΅Π²ΠΌΠΎΠ½ΠΈΠΈ
The need for safe and effective treatment is becoming increasingly urgent due to the high COVID-19 mortality rates observed worldwide. The choice of drug products for COVID-19 treatment regimens is based on the efficacy and safety data, the mechanism of action, and potential interactions. N-acetylcysteine's (NAC) pharmacological activity and its potential to suppress the progression of COVID-19 make it a promising therapeutic agent for COVID-19. Aim of the study was to evaluate the efficacy of NAC in the complex treatment of moderate COVID-associated pneumonia. Methods. The study included adult patients (n = 46) with moderate COVID-associated (the 2nd degree on CT) pneumonia (age 57 (51; 71) years, body mass index - 30 (27.1; 32.3) kg/m2, duration of the disease before hospitalization - 7 (6; 8) days, body temperature at the admission - 37.5 (37.1; 37.8)Β°Π‘). The patients were randomized into two study groups. The 1st group (n= 22) received standard COVID-19 treatment [1]. The 2nd group (n= 24) additionally received NAC 1,200 - 1,500 mg/day intravenously. Treatment with NAC was started together with the standard therapy. Results. Our study showed that the inclusion of NAC in the complex treatment of moderate COVID-associated pneumonia led to a statistically significant increase in blood oxygen saturation, oxygenation index, the difference in delta increase in oxygenation index, a quicker reduction in the volume of lung damage and the difference between the groups in delta reduction of this index. Also, the rate of reduction of C-reactive protein and reduction of the duration of hospitalization in the group of patients who received NAC was statistically significantly more profound than in the standard treatment group. Conclusion. The study confirmed the effectiveness of NAC as a part of the complex treatment of moderate COVID-associated pneumonia.ΠΠΎΡΡΠ΅Π±Π½ΠΎΡΡΡ Π² Π±Π΅Π·ΠΎΠΏΠ°ΡΠ½ΠΎΠΌ ΠΈ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΠΌ Π»Π΅ΡΠ΅Π½ΠΈΠΈ COVID-19 ΡΡΠ°Π½ΠΎΠ²ΠΈΡΡΡ Π²ΡΠ΅ Π±ΠΎΠ»Π΅Π΅ Π°ΠΊΡΡΠ°Π»ΡΠ½ΠΎΠΉ ΠΈΠ·-Π·Π° Π²ΡΡΠΎΠΊΠΈΡ
ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Π΅ΠΉ ΡΠΌΠ΅ΡΡΠ½ΠΎΡΡΠΈ Π² ΠΌΠΈΡΠ΅. ΠΡΠ±ΠΎΡ Π»Π΅ΠΊΠ°ΡΡΡΠ²Π΅Π½Π½ΡΡ
ΡΡΠ΅Π΄ΡΡΠ² (ΠΠ‘), Π²Ρ
ΠΎΠ΄ΡΡΠΈΡ
Π² ΡΡ
Π΅ΠΌΡ Π»Π΅ΡΠ΅Π½ΠΈΡ COVID-19, ΠΎΡΠ½ΠΎΠ²Π°Π½ Π½Π° Π΄Π°Π½Π½ΡΡ
ΠΎΠ± ΠΈΡ
ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ ΠΈ Π±Π΅Π·ΠΎΠΏΠ°ΡΠ½ΠΎΡΡΠΈ, ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌΠ΅ ΠΈΡ
Π΄Π΅ΠΉΡΡΠ²ΠΈΡ ΠΈ ΠΏΠΎΡΠ΅Π½ΡΠΈΠ°Π»ΡΠ½ΡΡ
Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΠΉ. Π€Π°ΡΠΌΠ°ΠΊΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠ°Ρ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ N-Π°ΡΠ΅ΡΠΈΠ»ΡΠΈΡΡΠ΅ΠΈΠ½Π° (NAC) ΠΈ ΠΏΠΎΡΠ΅Π½ΡΠΈΠ°Π»ΡΠ½ΠΎ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΠ΅ Π΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ Π² ΠΏΠΎΠ΄Π°Π²Π»Π΅Π½ΠΈΠΈ ΠΏΡΠΎΠ³ΡΠ΅ΡΡΠΈΡΠΎΠ²Π°Π½ΠΈΡ COVID-19 Π΄Π΅Π»Π°ΡΡ Π΅Π³ΠΎ ΠΌΠ½ΠΎΠ³ΠΎΠΎΠ±Π΅ΡΠ°ΡΡΠΈΠΌ ΡΠ΅ΡΠ°ΠΏΠ΅Π²ΡΠΈΡΠ΅ΡΠΊΠΈΠΌ ΡΡΠ΅Π΄ΡΡΠ²ΠΎΠΌ ΠΏΡΠΈ COVID-19. Π¦Π΅Π»ΡΡ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΡΠ²ΠΈΠ»Π°ΡΡ ΠΎΡΠ΅Π½ΠΊΠ° ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ NAC Π² ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ½ΠΎΠΌ Π»Π΅ΡΠ΅Π½ΠΈΠΈ ΡΡΠ΅Π΄Π½Π΅ΡΡΠΆΠ΅Π»ΠΎΠΉ COVID-Π°ΡΡΠΎΡΠΈΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΉ ΠΏΠ½Π΅Π²ΠΌΠΎΠ½ΠΈΠΈ. ΠΠ°ΡΠ΅ΡΠΈΠ°Π»Ρ ΠΈ ΠΌΠ΅ΡΠΎΠ΄Ρ. Π ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ Π²ΠΊΠ»ΡΡΠ΅Π½Ρ Π²Π·ΡΠΎΡΠ»ΡΠ΅ ΠΏΠ°ΡΠΈΠ΅Π½ΡΡ (ΠΏ = 46; Π²ΠΎΠ·ΡΠ°ΡΡ β 57 (51; 71) Π»Π΅Ρ, ΠΈΠ½Π΄Π΅ΠΊΡ ΠΌΠ°ΡΡΡ ΡΠ΅Π»Π° - 30 (27,1; 32,3) ΠΊΠ³ / ΠΌ2, ΠΏΡΠΎΠ΄ΠΎΠ»ΠΆΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΡ Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π½ΠΈΡ Π΄ΠΎ Π³ΠΎΡΠΏΠΈΡΠ°Π»ΠΈΠ·Π°ΡΠΈΠΈ - 7 (6; 8) Π΄Π½Π΅ΠΉ, ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ° ΡΠ΅Π»Π° Π½Π° ΠΌΠΎΠΌΠ΅Π½Ρ Π³ΠΎΡΠΏΠΈΡΠ°Π»ΠΈΠ·Π°ΡΠΈΠΈ β 37,5 (37,1; 37,8) Β°Π‘) ΡΠΎ ΡΡΠ΅Π΄Π½Π΅ΡΡΠΆΠ΅Π»ΠΎΠΉ (II ΡΡΠ΅ΠΏΠ΅Π½Ρ ΠΏΠΎ Π΄Π°Π½Π½ΡΠΌ ΠΊΠΎΠΌΠΏΡΡΡΠ΅ΡΠ½ΠΎΠΉ ΡΠΎΠΌΠΎΠ³ΡΠ°ΡΠΈΠΈ) COVID-Π°ΡΡΠΎΡΠΈΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΉ ΠΏΠ½Π΅Π²ΠΌΠΎΠ½ΠΈΠ΅ΠΉ. Π‘Π»ΡΡΠ°ΠΉΠ½ΡΠΌ ΠΎΠ±ΡΠ°Π·ΠΎΠΌ ΡΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½Ρ 2 Π³ΡΡΠΏΠΏΡ: ΠΏΠ°ΡΠΈΠ΅Π½ΡΡ 1-ΠΉ Π³ΡΡΠΏΠΏΡ (n = 22) ΠΏΠΎΠ»ΡΡΠ°Π»ΠΈ ΡΡΠ°Π½Π΄Π°ΡΡΠ½ΠΎΠ΅ Π»Π΅ΡΠ΅Π½ΠΈΠ΅ COVID-19; Π±ΠΎΠ»ΡΠ½ΡΠ΅ 2-ΠΉ (n = 24) Π³ΡΡΠΏΠΏΡ Π΄ΠΎΠΏΠΎΠ»Π½ΠΈΡΠ΅Π»ΡΠ½ΠΎ ΠΏΠΎΠ»ΡΡΠ°Π»ΠΈ NAC 1 200-1 500 ΠΌΠ³ Π² ΡΡΡΠΊΠΈ Π²Π½ΡΡΡΠΈΠ²Π΅Π½Π½ΠΎ ΠΊΠ°ΠΏΠ΅Π»ΡΠ½ΠΎ. NAC Π½Π°Π·Π½Π°ΡΠ°Π»ΡΡ ΠΎΠ΄Π½ΠΎΠ²ΡΠ΅ΠΌΠ΅Π½Π½ΠΎ Ρ Π½Π°ΡΠ°Π»ΠΎΠΌ ΡΡΠ°Π½Π΄Π°ΡΡΠ½ΠΎΠΉ ΡΠ΅ΡΠ°ΠΏΠΈΠΈ. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ. ΠΠΎ Π΄Π°Π½Π½ΡΠΌ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ ΠΏΡΠΈ Π²ΠΊΠ»ΡΡΠ΅Π½ΠΈΠΈ Π² ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ½ΠΎΠ΅ Π»Π΅ΡΠ΅Π½ΠΈΠ΅ ΡΡΠ΅Π΄Π½Π΅ΡΡΠΆΠ΅Π»ΠΎΠΉ COVID-Π°ΡΡΠΎΡΠΈΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΉ ΠΏΠ½Π΅Π²ΠΌΠΎΠ½ΠΈΠΈ NAC ΡΡΠ°ΡΠΈΡΡΠΈΡΠ΅ΡΠΊΠΈ Π·Π½Π°ΡΠΈΠΌΠΎ ΠΏΠΎΠ²ΡΡΠΈΠ»ΠΈΡΡ ΡΡΠΎΠ²Π΅Π½Ρ Π½Π°ΡΡΡΠ΅Π½ΠΈΡ ΠΊΡΠΎΠ²ΠΈ ΠΊΠΈΡΠ»ΠΎΡΠΎΠ΄ΠΎΠΌ, ΠΈΠ½Π΄Π΅ΠΊΡ ΠΎΠΊΡΠΈΠ³Π΅Π½Π°ΡΠΈΠΈ, ΡΠ°Π·Π»ΠΈΡΠΈΡ ΡΠ°Π·Π½ΠΎΡΡΠΈ Π΄Π΅Π»ΡΡΠ° (Ξ), ΠΈΠ½Π΄Π΅ΠΊΡ ΠΎΠΊΡΠΈΠ³Π΅Π½Π°ΡΠΈΠΈ, ΡΠΊΠΎΡΠΎΡΡΡ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΡ ΠΎΠ±ΡΠ΅ΠΌΠ° ΠΏΠΎΡΠ°ΠΆΠ΅Π½ΠΈΡ Π»Π΅Π³ΠΊΠΈΡ
ΠΈ ΠΌΠ΅ΠΆΠ³ΡΡΠΏΠΏΠΎΠ²ΠΎΠ΅ ΡΠ°Π·Π»ΠΈΡΠΈΠ΅ Ξ ΡΠΌΠ΅Π½ΡΡΠ΅Π½ΠΈΡ Π΄Π°Π½Π½ΠΎΠ³ΠΎ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Ρ. ΠΡΠΌΠ΅ΡΠ΅Π½Ρ ΡΡΠ°ΡΠΈΡΡΠΈΡΠ΅ΡΠΊΠΈ Π·Π½Π°ΡΠΈΠΌΠΎ Π±ΠΎΠ»Π΅Π΅ ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½Π°Ρ, ΡΠ΅ΠΌ Π² Π³ΡΡΠΏΠΏΠ΅ ΡΡΠ°Π½Π΄Π°ΡΡΠ½ΠΎΠ³ΠΎ Π»Π΅ΡΠ΅Π½ΠΈΡ, ΡΠΊΠΎΡΠΎΡΡΡ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΡ ΡΡΠΎΠ²Π½Ρ Π‘-ΡΠ΅Π°ΠΊΡΠΈΠ²Π½ΠΎΠ³ΠΎ Π±Π΅Π»ΠΊΠ°, Π° ΡΠ°ΠΊΠΆΠ΅ ΡΠΎΠΊΡΠ°ΡΠ΅Π½ΠΈΠ΅ ΠΏΡΠΎΠ΄ΠΎΠ»ΠΆΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΠΈ Π³ΠΎΡΠΏΠΈΡΠ°Π»ΠΈΠ·Π°ΡΠΈΠΈ Π² Π³ΡΡΠΏΠΏΠ΅ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ², ΠΏΠΎΠ»ΡΡΠ°Π²ΡΠΈΡ
NAC. ΠΠ°ΠΊΠ»ΡΡΠ΅Π½ΠΈΠ΅. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½Π½ΠΎΠ³ΠΎ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΡΠ²ΠΈΠ΄Π΅ΡΠ΅Π»ΡΡΡΠ²ΡΡΡ ΠΎΠ± ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ Π²ΠΊΠ»ΡΡΠ΅Π½ΠΈΡ NAC Π² ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ½ΠΎΠ΅ Π»Π΅ΡΠ΅Π½ΠΈΠ΅ ΡΡΠ΅Π΄Π½Π΅ΡΡΠΆΠ΅Π»ΠΎΠΉ COVID-Π°ΡΡΠΎΡΠΈΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΉ ΠΏΠ½Π΅Π²ΠΌΠΎΠ½ΠΈΠΈ
Improved measurement of time-dependent CP violation in B0 -> J/Psi pi0 decays
We report improved measurements of time-dependent CP violation parameters for
decay. This analysis is based on 535 million
pairs accumulated at the resonance with the Belle
detector at the KEKB asymmetric-energy e^+e^- collider. From the distribution
of proper time intervals between the two B decays, we obtain the following CP
violation parameters and , which are consistent with Standard Model
expectations.Comment: Resubmitted to PRD(RC), including 4 figures, 6pages Revision has been
made according to communication with PRD referee
Study of B -> D** l nu with full reconstruction tagging
We report a study of semileptonic B decays to P-wave D** mesons. Semileptonic
decay to D*_2 meson is observed for the first time and its product branching
ratio is measured to be
Br(B+ -> anti-D*0_2 l+nu) x Br(anti-D*0_2 -> D- pi+) = 0.22 +- 0.03(stat.) +-
0.04(syst.)%. The result is obtained using the fully reconstructed B tags from
a data sample that contains 657 millions BB-bar pairs collected at the
Upsilon(4S) resonance with the Belle detector at the KEKB asymmetric-energy e+
e- collider.Comment: 12 pages, 4 figures, submitted to PRD(RC
Observation of Two Resonant Structures in e+e- to pi+ pi- psi(2S) via Initial State Radiation at Belle
The cross section for e+e- to pi+ pi- psi(2S) between threshold and
\sqrt{s}=5.5 GeV is measured using 673 fb^{-1} of data on and off the
\Upsilon(4S) resonance collected with the Belle detector at KEKB. Two resonant
structures are observed in the pi+ pi- psi(2S) invariant mass distribution, one
at 4361\pm 9\pm 9 MeV/c2 with a width of 74\pm 15\pm 10 MeV/c2, and another at
4664\pm 11\pm 5 MeV/c2 with a width of 48\pm 15\pm 3 MeV/c2, if the mass
spectrum is parameterized with the coherent sum of two Breit-Wigner functions.
These values do not match those of any of the known charmonium states.Comment: 10 pages, 5 figures, 2 tables, version to appear in Phys. Rev. Let
Electronic Structure and Valence Band Spectra of Bi4Ti3O12
The x-ray photoelectron valence band spectrum and x-ray emission valence-band
spectra (Ti K _beta_5, Ti L_alpha, O K_alpha) of Bi4Ti3O12 are presented
(analyzed in the common energy scale) and interpreted on the basis of a
band-structure calculation for an idealized I4/mmm structure of this material.Comment: 6 pages + 7 PostScript figures, RevTex3.0, to be published in
Phys.Rev.B52 (Oct.95). Figures also available via anonymous ftp at
ftp://ftp.physik.uni-osnabrueck.de/pub/apostnik/BiTiO
Study of the suppressed B meson decay B^- -> D K^-, D -> K^+ \pi^-
We report a study of the suppressed B meson decay B^- -> D K^- followed by D
-> K^+ \pi^-, where D indicates a D^0 or \bar{D}^0 state. The two decay paths
interfere and provide information on the CP-violating angle \phi_3. We use a
data sample containing 657 x 10^6 B\bar{B} pairs recorded at the \Upsilon(4S)
resonance with the Belle detector at the KEKB asymmetric-energy e^+e^- storage
ring. We do not find significant evidence for the mode B^- -> D K^-, D -> K^+
\pi^-, and set an upper limit of r_B < 0.19, where r_B is the magnitude of the
ratio of amplitudes |A(B^- -> \bar{D}^0 K^-)/A(B^- -> D^0 K^-)|. The decay B^-
-> D \pi^-, D -> K^+ \pi^- is also analyzed as a reference, for which we
observe a signal with 6.6\sigma significance, and measure the charge asymmetry
A_{D\pi} to be -0.02^{+0.15}_{-0.16}(stat) \pm 0.04(syst). In addition, the
ratio B(B^- -> D^0 K^-)/B(B^- -> D^0 \pi^-) is measured to be [6.77 \pm
0.23(stat) \pm 0.30(syst)] x 10^{-2}.Comment: 6 pages, 3 figures, 2 table
Measurement of e^+e^- to pi^+pi^-J/psi Cross Section via Initial State Radiation at Belle
The cross section for e^+e^- to pi^+pi^-J/psi between 3.8 and 5.5 GeV/c^2 is
measured using a 548 fb^{-1} data sample collected on or near the Upsilon(4S)
resonance with the Belle detector at KEKB. A peak near 4.25 GeV/c^2,
corresponding to the so called Y(4260), is observed. In addition, there is
another cluster of events at around 4.05 GeV/c^2. A fit using two interfering
Breit-Wigner shapes describes the data better than one that uses only the
Y(4260), especially for the lower mass side of the 4.25 GeV enhancement.Comment: 11 pages, 5 figures, 2 tables; version to appear in PR
Improved search for D^0 mixing using semileptonic decays at Belle
A search for mixing in the neutral D meson system has been performed using
semileptonic D0 -> K(*)- e+ \nu and D0 -> K(*)- \mu+ \nu decays. Neutral D
mesons from D*+ -> D0 \pi_s^+ decays are used and the flavor at production is
tagged by the charge of the slow pion. The measurement is performed using 492
fb^-1 of data recorded by the Belle detector. From the yield of right-sign and
wrong-sign decays arising from non-mixed and mixed events, respectively, we
measure the ratio of the time-integrated mixing rate to the unmixed rate to be
R_M = (1.3 +- 2.2 +- 2.0) x 10^-4. This corresponds to an upper limit of R_M <
6.1 x 10^-4 at the 90% C.L.Comment: 20 pages, 16 figures, 8 tables; accepted by PRD; changes from
previous version: minor rewording
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