899 research outputs found
ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ Π»Π΅Π΄Π½ΠΈΠΊΠΎΠ² Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΈΡ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΠΉ
The possibility of glacier ice flow studies using the method of acoustic emission (AE) in frequency range from 15 Hz to 20 kHz has been considered. A portable acoustic line system has been developed and a number of methodological issues (mounting of acoustic sensors into glacial ice, their location, reliability of acoustic coupling, etc.) have been solved. Acoustic studies of glacial ice have been performed; rock fall effect, ice cracking and ice movement on bedrock have been simulated. Correspondences of AE parameters to specific sources have been identified. The results of acoustic studies on Aldegondabreen (Spitsbergen), Central Tuyuksu and Molodezhny glaciers (northern Tien Shan) have been summarized. The dependence of the adhesive strength of ice with smooth substrate (serpentenite) on the shear rate has been considered; the effect of tor-shaped obstacle on shear force has been estimated. It is shown that the acoustic effects at cohesive ice failure on obstacles are similar to the observed natural acoustic vibrations generated in glaciers from distant sources. The results might be applied in development of the mobile ice lab and system for remote acoustic monitoring the processes in the bottom layers of glaciers.Π Π°ΡΡΠΌΠΎΡΡΠ΅Π½Ρ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΠΈ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΡ Π»ΡΠ΄Π° Π² Π»Π΅Π΄Π½ΠΈΠΊΠ΅ ΠΈ Π΅Π³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π° Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΠΌΠ΅ΡΠΎΠ΄Π° Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠΌΠΈΡΡΠΈΠΈ Π² Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π΅ ΡΠ°ΡΡΠΎΡ 15β20Β ΠΊΠΡ. Π‘ΠΎΠ·Π΄Π°Π½Π° ΠΏΠΎΡΡΠ°ΡΠΈΠ²Π½Π°Ρ ΠΈΠ·ΠΌΠ΅ΡΠΈΡΠ΅Π»ΡΠ½Π°Ρ Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠ°Ρ Π»ΠΈΠ½ΠΈΡ ΠΈ ΡΠ΅ΡΡΠ½ ΡΡΠ΄ ΠΌΠ΅ΡΠΎΠ΄ΠΈΡΠ΅ΡΠΊΠΈΡ
Π²ΠΎΠΏΡΠΎΡΠΎΠ². ΠΡΠΏΠΎΠ»Π½Π΅Π½Ρ Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ Π»Π΅Π΄Π½ΠΈΠΊΠΎΠ²ΠΎΠ³ΠΎ Π»ΡΠ΄Π°, ΠΈΠΌΠΈΡΠΈΡΠΎΠ²Π°Π½Ρ ΠΊΠ°ΠΌΠ½Π΅ΠΏΠ°Π΄, ΡΡΠ΅ΡΠΈΠ½ΠΎΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΠ΅ Π² Π»Π΅Π΄Π½ΠΈΠΊΠ΅ ΠΈ Π΅Π³ΠΎ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠ΅ ΠΏΠΎ Π»ΠΎΠΆΡ. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½Ρ ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΠΈΡ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠΌΠΈΡΡΠΈΠΈ ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ½Π½ΠΎΠΌΡ ΠΈΡΡΠΎΡΠ½ΠΈΠΊΡ. ΠΠ±ΠΎΠ±ΡΠ΅Π½Ρ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ Π½Π° Π»Π΅Π΄Π½ΠΈΠΊΠ°Ρ
ΠΠ»ΡΠ΄Π΅Π³ΠΎΠ½Π΄Π° (Π¨ΠΏΠΈΡΠ±Π΅ΡΠ³Π΅Π½), Π¦Π΅Π½ΡΡΠ°Π»ΡΠ½ΡΠΉ Π’ΡΡΠΊΡΡ ΠΈ ΠΠΎΠ»ΠΎΠ΄ΡΠΆΠ½ΡΠΉ (Π‘Π΅Π²Π΅ΡΠ½ΡΠΉ Π’ΡΠ½Ρ-Π¨Π°Π½Ρ). Π Π°ΡΡΠΌΠΎΡΡΠ΅Π½Π° Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΡ Π°Π΄Π³Π΅Π·ΠΈΠΎΠ½Π½ΠΎΠΉ ΠΏΡΠΎΡΠ½ΠΎΡΡΠΈ ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΡ Π»ΡΠ΄Π° Ρ Π³Π»Π°Π΄ΠΊΠΎΠΉ ΠΏΠΎΠ΄Π»ΠΎΠΆΠΊΠΎΠΉ (ΡΠ΅ΡΠΏΠ΅Π½ΡΠΈΠ½ΠΈΡ) ΠΎΡ ΡΠΊΠΎΡΠΎΡΡΠΈ ΡΠ΄Π²ΠΈΠ³Π°, ΠΎΡΠ΅Π½Π΅Π½ΠΎ Π²Π»ΠΈΡΠ½ΠΈΠ΅ ΠΏΡΠ΅ΠΏΡΡΡΡΠ²ΠΈΡ Π² Π²ΠΈΠ΄Π΅ ΡΠΎΡΠ° Π½Π° ΡΠΈΠ»Ρ ΡΠ΄Π²ΠΈΠ³Π°. ΠΒ ΡΠΎΠ±ΡΡΠ²Π΅Π½Π½ΡΡ
Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠΏΠ΅ΠΊΡΡΠ°Ρ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Π½ΡΡ
Π»Π΅Π΄Π½ΠΈΠΊΠΎΠ² ΠΎΠ±Π½Π°ΡΡΠΆΠ΅Π½Ρ Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΡΡΡΠ΅ΠΊΡΡ, Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠ½ΡΠ΅ Π΄Π»Ρ ΡΠ°Π·ΡΡΡΠ΅Π½ΠΈΡ Π»ΡΠ΄Π° Π½Π° ΠΏΡΠ΅ΠΏΡΡΡΡΠ²ΠΈΡΡ
. ΠΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΌΠΎΠΆΠ½ΠΎ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°ΡΡ Π΄Π»Ρ ΡΠΎΠ·Π΄Π°Π½ΠΈΡ ΠΌΠΎΠ±ΠΈΠ»ΡΠ½ΠΎΠΉ Π»Π΅Π΄Π½ΠΈΠΊΠΎΠ²ΠΎΠΉ Π»Π°Π±ΠΎΡΠ°ΡΠΎΡΠΈΠΈ ΠΈ ΡΠΈΡΡΠ΅ΠΌΡ Π΄ΠΈΡΡΠ°Π½ΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΌΠΎΠ½ΠΈΡΠΎΡΠΈΠ½Π³Π° ΠΏΡΠΎΡΠ΅ΡΡΠΎΠ² Π² ΠΏΡΠΈΠ΄ΠΎΠ½Π½ΡΡ
ΡΠ»ΠΎΡΡ
Π»Π΅Π΄Π½ΠΈΠΊΠ°
Measurement of the cross section with the CMD-3 detector at the VEPP-2000 collider
The process has been studied in the
center-of-mass energy range from 1500 to 2000\,MeV using a data sample of 23
pb collected with the CMD-3 detector at the VEPP-2000 collider.
Using about 24000 selected events, the cross
section has been measured with a systematic uncertainty decreasing from 11.7\%
at 1500-1600\,MeV to 6.1\% above 1800\,MeV. A preliminary study of
production dynamics has been performed
Study of the process in the c.m. energy range from threshold to 2 GeV with the CMD-3 detector
Using a data sample of 6.8 pb collected with the CMD-3 detector at the
VEPP-2000 collider we select about 2700 events of the process and measure its cross section at 12 energy ponts with about
6\% systematic uncertainty. From the angular distribution of produced nucleons
we obtain the ratio
Π€ΠΈΠ·ΠΈΡΠ΅ΡΠΊΠΎΠ΅ ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΠΊΠΎΠ½ΡΠ°ΠΊΡΠ° Π»Π΅Π΄Π½ΠΈΠΊΠ° Ρ Π»ΠΎΠΆΠ΅ΠΌ (ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΡ)
Studies of the adhesive strength of glacial ice connection with bedrock has been studied using the analysis of the amplitude-frequency characteristics of acoustic emission (AE) in the frequency range from 15Β Hz to 20,000Β Hz. Identification of signal source on bed is based on physical modeling of adhesive ice fracture at the complex shear and patterns of elastic waves propagation in the ice using data on ice thickness of the ice and its acoustic properties. The experimental dependence of the ice and serpentinite substrate adhesive strength with temperature (from 0Β Β°C to β30Β Β°C) has been obtained at constraint axial shear. It is shown that the destruction of adhesive ice contact with substrate begins long before the maximum shear stress achieved, and AE signals in the coordinates amplitude-frequency-time have been obtained for the for static friction and sliding parts of deformation curves. Influence of shear to normal stresses ratio on the adhesive ice/substrate strength has been shown. Influence of the ratio of longitudinal and transverse shear stresses on the adhesive bond strength of ice to the substrate has been shown. The natural glacier spectra revealed periodic reduction of AE signals frequency in the middle range of frequencies. The similar effect of AE signals shifting along the frequency axis to the low frequency domain was obtained by testing of freshwater ice samples and related with expansion of the destruction scale. Practical application of the strain AE results for remote determination of the local glacial stability and for studies of glacier ice mechanics is discussed.ΠΡΠΎΠ²Π΅Π΄Π΅Π½Ρ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ½ΡΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ Π°Π΄Π³Π΅Π·ΠΈΠΎΠ½Π½ΠΎΠΉ ΠΏΡΠΎΡΠ½ΠΎΡΡΠΈ ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΡ Π»ΡΠ΄Π° Ρ ΠΏΠΎΠ΄Π»ΠΎΠΆΠΊΠΎΠΉ, ΠΏΡΠ΅Π΄ΡΡΠΌΠ°ΡΡΠΈΠ²Π°ΡΡΠΈΠ΅ Π°Π½Π°Π»ΠΈΠ· Π°ΠΌΠΏΠ»ΠΈΡΡΠ΄Π½ΠΎ-ΡΠ°ΡΡΠΎΡΠ½ΡΡ
Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊ ΡΠΈΠ³Π½Π°Π»ΠΎΠ² Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠΌΠΈΡΡΠΈΠΈ (ΠΠ) Π² Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π΅ ΡΠ°ΡΡΠΎΡ ΠΎΡ 15 Π΄ΠΎ 20Β ΡΡΡ.Β ΠΡ. ΠΠ°Π½Π½ΡΠ΅ ΡΠΈΠ·ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΏΡΠΎΡΠ΅ΡΡΠΎΠ² Π°Π΄Π³Π΅Π·ΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΡΠ°Π·ΡΡΡΠ΅Π½ΠΈΡ Π»ΡΠ΄Π° ΠΏΠΎΠ΄ΡΠ²Π΅ΡΠΆΠ΄Π΅Π½Ρ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ°ΠΌΠΈ ΠΏΠΎΠ»Π΅Π²ΡΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ Π»Π΅Π΄Π½ΠΈΠΊΠΎΠ² Π¦Π΅Π½ΡΡΠ°Π»ΡΠ½ΡΠΉ Π’ΡΡΠΊΡΡ ΠΈ ΠΠΎΠ»ΠΎΠ΄Π΅ΠΆΠ½ΡΠΉ Π² ΠΠ°ΠΈΠ»ΠΈΠΉΡΠΊΠΎΠΌ ΠΠ»Π°ΡΠ°Ρ. ΠΠΎΠ»ΡΡΠ΅Π½Π° ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½Π°Ρ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΡ Π°Π΄Π³Π΅Π·ΠΈΠΎΠ½Π½ΠΎΠΉ ΠΏΡΠΎΡΠ½ΠΎΡΡΠΈ ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΡ Π»ΡΠ΄Π° Ρ ΡΠ΅ΡΠΏΠ΅Π½ΡΠΈΠ½ΠΈΡΠΎΠΌ (ΠΏΠΎΠ΄Π»ΠΎΠΆΠΊΠΎΠΉ) ΠΎΡ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ (ΠΎΡ 0 Π΄ΠΎ β25Β Β°Π‘) ΠΏΡΠΈ ΠΎΡΠ΅Π²ΠΎΠΌ ΡΠ΄Π²ΠΈΠ³Π΅ Π² ΡΡΠ»ΠΎΠ²ΠΈΡΡ
ΡΡΠ΅ΡΠ½Π΅Π½ΠΈΡ. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ Π°Π΄Π³Π΅Π·ΠΈΠΎΠ½Π½ΡΠΉ ΠΊΠΎΠ½ΡΠ°ΠΊΡ Π»ΡΠ΄βΠΏΠΎΠ΄Π»ΠΎΠΆΠΊΠ° Π½Π°ΡΠΈΠ½Π°Π΅Ρ ΡΠ°Π·ΡΡΡΠ°ΡΡΡΡ Π½Π°ΠΌΠ½ΠΎΠ³ΠΎ ΡΠ°Π½ΡΡΠ΅ Π΄ΠΎΡΡΠΈΠΆΠ΅Π½ΠΈΡ ΠΌΠ°ΠΊΡΠΈΠΌΠ°Π»ΡΠ½ΡΡ
Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΠΉ ΡΠ΄Π²ΠΈΠ³Π°, ΠΏΡΠΈΡΡΠΌ Π΄Π»Ρ ΡΡΠ°ΡΡΠΊΠΎΠ² Π΄Π΅ΡΠΎΡΠΌΠ°ΡΠΈΠΎΠ½Π½ΡΡ
ΠΊΡΠΈΠ²ΡΡ
(ΡΡΠ΅Π½ΠΈΠ΅ ΠΏΠΎΠΊΠΎΡ ΠΈ ΡΠΊΠΎΠ»ΡΠΆΠ΅Π½ΠΈΡ) ΠΏΠΎΠ»ΡΡΠ΅Π½Ρ Π΄ΠΈΠ°Π³ΡΠ°ΠΌΠΌΡ ΡΠΈΠ³Π½Π°Π»ΠΎΠ² ΠΠ Π² ΠΊΠΎΠΎΡΠ΄ΠΈΠ½Π°ΡΠ°Ρ
Π°ΠΌΠΏΠ»ΠΈΡΡΠ΄Π°βΡΠ°ΡΡΠΎΡΠ°βΠ²ΡΠ΅ΠΌΡ. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ Π²Π»ΠΈΡΠ½ΠΈΠ΅ ΡΠΎΠΎΡΠ½ΠΎΡΠ΅Π½ΠΈΡ ΠΏΡΠΎΠ΄ΠΎΠ»ΡΠ½ΡΡ
ΠΈ ΠΏΠΎΠΏΠ΅ΡΠ΅ΡΠ½ΡΡ
ΡΠ΄Π²ΠΈΠ³ΠΎΠ²ΡΡ
Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΠΉ Π½Π° Π°Π΄Π³Π΅Π·ΠΈΠΎΠ½Π½ΡΡ ΠΏΡΠΎΡΠ½ΠΎΡΡΡ ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΡ Π»ΡΠ΄Π° Ρ ΠΏΠΎΠ΄Π»ΠΎΠΆΠΊΠΎΠΉ. Π ΡΡΠ΅Π΄Π½Π΅ΠΌ Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π΅ ΡΠ°ΡΡΠΎΡ ΡΠΎΠ±ΡΡΠ²Π΅Π½Π½ΡΡ
Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠΏΠ΅ΠΊΡΡΠΎΠ² Π»Π΅Π΄Π½ΠΈΠΊΠΎΠ² ΡΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ ΠΏΠ΅ΡΠΈΠΎΠ΄ΠΈΡΠ΅ΡΠΊΠΎΠ΅ ΡΠΌΠ΅Π½ΡΡΠ΅Π½ΠΈΠ΅ ΡΠ°ΡΡΠΎΡΡ Π·Π°ΠΏΠΎΠ»Π½Π΅Π½ΠΈΡ ΡΠΈΠ³Π½Π°Π»ΠΎΠ² ΠΠ. ΠΠ½Π°Π»ΠΎΠ³ΠΈΡΠ½ΡΠΉ ΡΡΡΠ΅ΠΊΡ ΡΠΌΠ΅ΡΠ΅Π½ΠΈΡ ΡΠΈΠ³Π½Π°Π»ΠΎΠ² ΠΠ ΠΏΠΎ ΠΎΡΠΈ ΡΠ°ΡΡΠΎΡ Π² ΡΡΠΎΡΠΎΠ½Ρ Π½ΠΈΠ·ΠΊΠΎΡΠ°ΡΡΠΎΡΠ½ΠΎΠ³ΠΎ Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π° ΠΏΠΎΠ»ΡΡΠ΅Π½ ΠΏΡΠΈ ΠΈΡΠΏΡΡΠ°Π½ΠΈΠΈ ΠΎΠ±ΡΠ°Π·ΡΠΎΠ² ΠΏΡΠ΅ΡΠ½ΠΎΠ²ΠΎΠ΄Π½ΠΎΠ³ΠΎ Π»ΡΠ΄Π° ΠΈ ΠΎΠ±ΡΡΠ»ΠΎΠ²Π»Π΅Π½ ΡΠ°ΡΡΠΈΡΠ΅Π½ΠΈΠ΅ΠΌ ΠΌΠ°ΡΡΡΠ°Π±Π° ΡΠ°Π·ΡΡΡΠ΅Π½ΠΈΡ. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ ΠΌΠΎΠΆΠ½ΠΎ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°ΡΡ Π΄Π»Ρ Π΄ΠΈΡΡΠ°Π½ΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΈΠ·ΡΡΠ΅Π½ΠΈΡ ΠΊΠΈΠ½Π΅ΡΠΈΠΊΠΈ Π½Π°ΠΊΠΎΠΏΠ»Π΅Π½ΠΈΡ ΡΡΠ΅ΡΠΈΠ½ Π² ΠΏΡΠΈΠ΄ΠΎΠ½Π½ΡΡ
ΡΠ»ΠΎΡΡ
Π»Π΅Π΄Π½ΠΈΠΊΠΎΠ²ΠΎΠ³ΠΎ Π»ΡΠ΄Π°
Measurement of the Pion Form Factor in the Energy Range 1.04-1.38 GeV with the CMD-2 Detector
The cross section for the process is measured in the
c.m. energy range 1.04-1.38 GeV from 995 000 selected collinear events
including 860000 events, 82000 events, and 33000
events. The systematic and statistical errors of measuring the
pion form factor are equal to 1.2-4.2 and 5-13%, respectively.Comment: 5 pages, 2 figure
The Determination of alpha_s from Tau Decays Revisited
We revisit the determination of alpha_s(m_tau) using a fit to inclusive tau
hadronic spectral moments in light of (1) the recent calculation of the
fourth-order perturbative coefficient K_4 in the expansion of the Adler
function, (2) new precision measurements from BABAR of e+e- annihilation cross
sections, which decrease the uncertainty in the separation of vector and
axial-vector spectral functions, and (3) improved results from BABAR and Belle
on tau branching fractions involving kaons. We estimate that the fourth-order
perturbative prediction reduces the theoretical uncertainty, introduced by the
truncation of the series, by 20% with respect to earlier determinations. We
discuss to some detail the perturbative prediction and show that the effect of
the incomplete knowledge of the series is reduced by using the so-called
contour-improved calculation, as opposed to fixed-order perturbation theory
which manifests convergence problems. The corresponding theoretical
uncertainties are studied at the tau and Z mass scales. Nonperturbative
contributions extracted from the most inclusive fit are small, in agreement
with earlier determinations. Systematic effects from quark-hadron duality
violation are estimated with simple models and found to be within the quoted
systematic errors. The fit gives alpha_s(m_tau) = 0.344 +- 0.005 +- 0.007,
where the first error is experimental and the second theoretical. After
evolution to M_Z we obtain alpha_s(M_Z) = 0.1212 +- 0.0005 +- 0.0008 +- 0.0005,
where the errors are respectively experimental, theoretical and due to the
evolution. The result is in agreement with the corresponding NNNLO value
derived from essentially the Z width in the global electroweak fit. The
alpha_s(M_Z) determination from tau decays is the most precise one to date.Comment: 22 pages, 7 figure
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