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    ΠžΡ†Π΅Π½ΠΊΠ° свойств ΠΊΠΎΡΡ‚Π½ΠΎΠ·Π°ΠΌΠ΅Ρ‰Π°ΡŽΡ‰ΠΈΡ… ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ² Π½Π° основС ΠΏΠΎΠ»ΠΈΡΡ‚ΠΈΠ»Π΅Π½Π³Π»ΠΈΠΊΠΎΠ»ΡŒ Π΄ΠΈΠ°ΠΊΡ€ΠΈΠ»Π°Ρ‚Π° ΠΈ ΠΎΠΊΡ‚Π°ΠΊΠ°Π»ΡŒΡ†ΠΈΠ΅Π²ΠΎΠ³ΠΎ фосфата Π½Π° ΠΌΠΎΠ΄Π΅Π»ΠΈ ΠΌΠΎΠ½ΠΎΠΊΠΎΡ€Ρ‚ΠΈΠΊΠ°Π»ΡŒΠ½ΠΎΠ³ΠΎ Π΄ΠΈΠ°Ρ„ΠΈΠ·Π°Ρ€Π½ΠΎΠ³ΠΎ Π΄Π΅Ρ„Π΅ΠΊΡ‚Π° Π±Π΅Π΄Ρ€Π΅Π½Π½ΠΎΠΉ кости крысы: ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½ΠΎΠ΅ исслСдованиС

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    Background. The problem of bone defects replacement is relevant nowadays, that is why many scientists create new synthetic bone substitutes, but the ideal material has not been found so far. The aims of the study: 1) to determine the suitability of the monocortical defect model in the rat femur diaphysis with additional prophylactic reinforcement with a bone plate for assessing the biological properties of implanted materials using the commercially available ChronOS material as an example; 2) to assess of the osteoconductive properties of composite materials based on poly(ethylene glycol)diacrylate and octacalcium phosphate with architecture Kelvin and gyroid types on the developed model. Methods. A prospective study, level of evidence II. A monocortical defect of the rat femoral diaphysis (length 7 mm) was produced under anaesthesia in aseptic conditions and fixed with a polyetheretherketone plate and six titanium screws. In the control group, the defect was left empty. In other groups, blocks of one of three materials were implanted сhronOS and composites of poly(ethylene glycol)diacrylate and octacalcium phosphate with 3D-printed Kelvin and gyroid architectures. After 3 and 6 weeks, the rats were sacrificed, and histological examination of the defect zone was performed. The amount of newly formed bone tissue was histometricly assessed, followed by statistical processing of the results. Results. All rats have reached the planned endpoint, and there were no infectious complications or loss of fixation. Histological examination of the defect zone revealed minimal bone growth in the Control group, rather slow bone formation in the Gyroid group, and statistically significantly more pronounced bone formation in the pores of the materials in the Kelvin and Chronos groups. Conclusions. Bone defect in this model was not spontaneously filled with bone tissue and allowed us to study the biological properties of bone substitutes (the ability to biodegrade and osteoconductive properties). The osteoconductive properties of a composite material based on poly(ethylene glycol)diacrylate and octacalcium phosphate with a Kelvin architecture are higher than with a gyroid architecture and are comparable to that of the сhronOS.ΠΠΊΡ‚ΡƒΠ°Π»ΡŒΠ½ΠΎΡΡ‚ΡŒ. ΠŸΡ€ΠΎΠ±Π»Π΅ΠΌΠ° замСщСния Π΄Π΅Ρ„Π΅ΠΊΡ‚ΠΎΠ² кости Π°ΠΊΡ‚ΡƒΠ°Π»ΡŒΠ½Π° Π² настоящСС врСмя, постоянно вСдутся поиски Π½ΠΎΠ²Ρ‹Ρ… синтСтичСских ΠΊΠΎΡΡ‚Π½ΠΎΠ·Π°ΠΌΠ΅Ρ‰Π°ΡŽΡ‰ΠΈΡ… ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ², ΠΎΠ΄Π½Π°ΠΊΠΎ ΠΈΠ΄Π΅Π°Π»ΡŒΠ½Ρ‹ΠΉ ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π» Π½Π΅ Π½Π°ΠΉΠ΄Π΅Π½ Π΄ΠΎ сих ΠΏΠΎΡ€. Π¦Π΅Π»ΠΈ исслСдования: 1) ΠΎΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ пригодности ΠΌΠΎΠ΄Π΅Π»ΠΈ ΠΌΠΎΠ½ΠΎΠΊΠΎΡ€Ρ‚ΠΈΠΊΠ°Π»ΡŒΠ½ΠΎΠ³ΠΎ Π΄Π΅Ρ„Π΅ΠΊΡ‚Π° Π΄ΠΈΠ°Ρ„ΠΈΠ·Π° Π±Π΅Π΄Ρ€Π΅Π½Π½ΠΎΠΉ кости крысы с Π΄ΠΎΠΏΠΎΠ»Π½ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹ΠΌ профилактичСским Π°Ρ€ΠΌΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΏΡ€ΠΈ ΠΏΠΎΠΌΠΎΡ‰ΠΈ накостной пластины для ΠΎΡ†Π΅Π½ΠΊΠΈ биологичСских свойств ΠΈΠΌΠΏΠ»Π°Π½Ρ‚ΠΈΡ€ΡƒΠ΅ΠΌΡ‹Ρ… ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ² Π½Π° ΠΏΡ€ΠΈΠΌΠ΅Ρ€Π΅ коммСрчСски доступного ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Π° сhronOS; 2) ΠΎΡ†Π΅Π½ΠΊΠ° остСокондуктивных свойств ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡ‚Π½Ρ‹Ρ… ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ² Π½Π° основС ΠΏΠΎΠ»ΠΈΡΡ‚ΠΈΠ»Π΅Π½Π³Π»ΠΈΠΊΠΎΠ»ΡŒ Π΄ΠΈΠ°ΠΊΡ€ΠΈΠ»Π°Ρ‚Π° ΠΈ ΠΎΠΊΡ‚Π°ΠΊΠ°Π»ΡŒΡ†ΠΈΠ΅Π²ΠΎΠ³ΠΎ фосфата с Π°Ρ€Ρ…ΠΈΡ‚Π΅ΠΊΡ‚ΡƒΡ€ΠΎΠΉ КСльвина ΠΈ Ρ‚ΠΈΠΏΠ° Π³ΠΈΡ€ΠΎΠΈΠ΄ Π½Π° Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚Π°Π½Π½ΠΎΠΉ ΠΌΠΎΠ΄Π΅Π»ΠΈ. ΠœΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π» ΠΈ ΠΌΠ΅Ρ‚ΠΎΠ΄Ρ‹. ΠœΠΎΠ½ΠΎΠΊΠΎΡ€Ρ‚ΠΈΠΊΠ°Π»ΡŒΠ½Ρ‹ΠΉ Π΄Π΅Ρ„Π΅ΠΊΡ‚ Π΄ΠΈΠ°Ρ„ΠΈΠ·Π° Π±Π΅Π΄Ρ€Π΅Π½Π½ΠΎΠΉ кости крыс Ρ€Π°Π·ΠΌΠ΅Ρ€ΠΎΠΌ 7 ΠΌΠΌ Π² Π΄Π»ΠΈΠ½Ρƒ ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄ΠΈΠ»ΠΈ ΠΏΠΎΠ΄ Π½Π°Ρ€ΠΊΠΎΠ·ΠΎΠΌ Π² асСптичСских условиях ΠΎΠΏΠ΅Ρ€Π°Ρ†ΠΈΠΎΠ½Π½ΠΎΠΉ ΠΈ фиксировали полиэфирэфиркСтоновой пластиной ΠΈ ΡˆΠ΅ΡΡ‚ΡŒΡŽ Ρ‚ΠΈΡ‚Π°Π½ΠΎΠ²Ρ‹ΠΌΠΈ Π²ΠΈΠ½Ρ‚Π°ΠΌΠΈ. ΠšΡ€Ρ‹Ρ распрСдСляли случайным ΠΎΠ±Ρ€Π°Π·ΠΎΠΌ Π½Π° Ρ‡Π΅Ρ‚Ρ‹Ρ€Π΅ Π³Ρ€ΡƒΠΏΠΏΡ‹ ΠΏΠΎ 12 особСй Π² ΠΊΠ°ΠΆΠ΄ΠΎΠΉ. Π’ Π³Ρ€ΡƒΠΏΠΏΠ΅ ΠšΠΎΠ½Ρ‚Ρ€ΠΎΠ»ΡŒ Ρƒ ΠΆΠΈΠ²ΠΎΡ‚Π½Ρ‹Ρ… костный Π΄Π΅Ρ„Π΅ΠΊΡ‚ Π½Π΅ заполняли. Π£ ΠΆΠΈΠ²ΠΎΡ‚Π½Ρ‹Ρ… Π² Π³Ρ€ΡƒΠΏΠΏΠ΅ Π₯ронос Π΄Π΅Ρ„Π΅ΠΊΡ‚ заполняли ΠΏΠΎΠ΄Π³ΠΎΡ‚ΠΎΠ²Π»Π΅Π½Π½Ρ‹ΠΌ ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠΌ chronOS Π² Π²ΠΈΠ΄Π΅ полуцилиндричСского Π±Π»ΠΎΠΊΠ°, Π² Π³Ρ€ΡƒΠΏΠΏΠ΅ КСльвин исслСдуСмым ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠΌ с Π°Ρ€Ρ…ΠΈΡ‚Π΅ΠΊΡ‚ΡƒΡ€ΠΎΠΉ КСльвина, Π² Π³Ρ€ΡƒΠΏΠΏΠ΅ Π“ΠΈΡ€ΠΎΠΈΠ΄ исслСдуСмым ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠΌ с Π°Ρ€Ρ…ΠΈΡ‚Π΅ΠΊΡ‚ΡƒΡ€ΠΎΠΉ Ρ‚ΠΈΠΏΠ° Π³ΠΈΡ€ΠΎΠΈΠ΄. Π§Π΅Ρ€Π΅Π· 3 ΠΈ 6 Π½Π΅Π΄. крыс Π²Ρ‹Π²ΠΎΠ΄ΠΈΠ»ΠΈ ΠΈΠ· экспСримСнта ΠΈ ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄ΠΈΠ»ΠΈ гистологичСскоС исслСдованиС Π·ΠΎΠ½Ρ‹ Π΄Π΅Ρ„Π΅ΠΊΡ‚Π°. Π—Π°Ρ‚Π΅ΠΌ выполняли Π³ΠΈΡΡ‚ΠΎΠΌΠ΅Ρ‚Ρ€ΠΈΡ‡Π΅ΡΠΊΡƒΡŽ ΠΎΡ†Π΅Π½ΠΊΡƒ количСства Π½ΠΎΠ²ΠΎΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½Π½ΠΎΠΉ костной Ρ‚ΠΊΠ°Π½ΠΈ с ΠΏΠΎΡΠ»Π΅Π΄ΡƒΡŽΡ‰Π΅ΠΉ статистичСской ΠΎΠ±Ρ€Π°Π±ΠΎΡ‚ΠΊΠΎΠΉ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΎΠ². Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹. Π’ Ρ…ΠΎΠ΄Π΅ экспСримСнта всС ΠΆΠΈΠ²ΠΎΡ‚Π½Ρ‹Π΅ достигли ΠΏΠ»Π°Π½ΠΈΡ€ΡƒΠ΅ΠΌΠΎΠΉ ΠΊΠΎΠ½Π΅Ρ‡Π½ΠΎΠΉ Ρ‚ΠΎΡ‡ΠΊΠΈ, ΠΈΠ½Ρ„Π΅ΠΊΡ†ΠΈΠΎΠ½Π½Ρ‹Π΅ ослоТнСния ΠΈ потСря фиксации зафиксированы Π½Π΅ Π±Ρ‹Π»ΠΈ. ΠŸΡ€ΠΈ гистологичСском исслСдовании Π·ΠΎΠ½Ρ‹ Π΄Π΅Ρ„Π΅ΠΊΡ‚Π° выявлСн ΠΌΠΈΠ½ΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹ΠΉ рост кости Π² Π³Ρ€ΡƒΠΏΠΏΠ΅ ΠšΠΎΠ½Ρ‚Ρ€ΠΎΠ»ΡŒ, достаточно ΠΌΠ΅Π΄Π»Π΅Π½Π½ΠΎΠ΅ ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½ΠΈΠ΅ кости Π² ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Π΅ Π³Ρ€ΡƒΠΏΠΏΡ‹ Π“ΠΈΡ€ΠΎΠΈΠ΄ ΠΈ статистичСски Π·Π½Π°Ρ‡ΠΈΠΌΠΎ Π±ΠΎΠ»Π΅Π΅ Π²Ρ‹Ρ€Π°ΠΆΠ΅Π½Π½ΠΎΠ΅ ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½ΠΈΠ΅ костной Ρ‚ΠΊΠ°Π½ΠΈ Π² ΠΏΠΎΡ€Π°Ρ… ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ² Π² Π³Ρ€ΡƒΠΏΠΏΠ°Ρ… КСльвин ΠΈ Π₯ронос. Π—Π°ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΠ΅. Разработанная модСль Π΄Π΅Ρ„Π΅ΠΊΡ‚Π° кости спонтанно Π½Π΅ заполняСтся костной Ρ‚ΠΊΠ°Π½ΡŒΡŽ ΠΈ позволяСт ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΡ‚ΡŒ ΠΈΠ·ΡƒΡ‡Π΅Π½ΠΈΠ΅ биологичСских свойств костнопластичСских ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ² (ΡΠΏΠΎΡΠΎΠ±Π½ΠΎΡΡ‚ΡŒ ΠΊ Π±ΠΈΠΎΠ΄Π΅Π³Ρ€Π°Π΄Π°Ρ†ΠΈΠΈ ΠΈ остСокондуктивныС свойства). ΠžΡΡ‚Π΅ΠΎΠΊΠΎΠ½Π΄ΡƒΠΊΡ‚ΠΈΠ²Π½Ρ‹Π΅ свойства ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡ‚Π½ΠΎΠ³ΠΎ ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Π° Π½Π° основС ΠΏΠΎΠ»ΠΈΡΡ‚ΠΈΠ»Π΅Π½Π³Π»ΠΈΠΊΠΎΠ»ΡŒ Π΄ΠΈΠ°ΠΊΡ€ΠΈΠ»Π°Ρ‚Π° ΠΈ ΠΎΠΊΡ‚Π°ΠΊΠ°Π»ΡŒΡ†ΠΈΠ΅Π²ΠΎΠ³ΠΎ фосфата с Π°Ρ€Ρ…ΠΈΡ‚Π΅ΠΊΡ‚ΡƒΡ€ΠΎΠΉ КСльвина Π²Ρ‹ΡˆΠ΅, Ρ‡Π΅ΠΌ с Π°Ρ€Ρ…ΠΈΡ‚Π΅ΠΊΡ‚ΡƒΡ€ΠΎΠΉ Ρ‚ΠΈΠΏΠ° Π³ΠΈΡ€ΠΎΠΈΠ΄, ΠΈ сопоставимы с Ρ‚Π°ΠΊΠΎΠ²Ρ‹ΠΌΠΈ Ρƒ ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Π° сhronOS

    New precise determination of the \tau lepton mass at KEDR detector

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    The status of the experiment on the precise Ο„\tau lepton mass measurement running at the VEPP-4M collider with the KEDR detector is reported. The mass value is evaluated from the Ο„+Ο„βˆ’\tau^+\tau^- cross section behaviour around the production threshold. The preliminary result based on 6.7 pbβˆ’1^{-1} of data is mΟ„=1776.80βˆ’0.23+0.25Β±0.15m_{\tau}=1776.80^{+0.25}_{-0.23} \pm 0.15 MeV. Using 0.8 pbβˆ’1^{-1} of data collected at the Οˆβ€²\psi' peak the preliminary result is also obtained: Ξ“eeBττ(Οˆβ€²)=7.2Β±2.1\Gamma_{ee}B_{\tau\tau}(\psi') = 7.2 \pm 2.1 eV.Comment: 6 pages, 8 figures; The 9th International Workshop on Tau-Lepton Physics, Tau0

    Liquid krypton electromagnetic calorimeter

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    Abstract A calorimeter using 30 tons of liquid krypton for the KEDR detector is being constructed. The main effects which determine the energy and space resolution have been studied. An energy resolution of 1.7% at 1.2 GeV was obtained with the prototype. A space resolution of 0.4 mm for relativistic particles has been reached with the prototype

    A two-phase argon avalanche detector operated in a single electron counting mode

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    The performance of a two-phase Ar avalanche detector in a single electron counting mode was studied, with regard to potential application in coherent neutrino-nucleus scattering and dark matter search experiments. The detector comprised of a 1 cm thick liquid Ar layer and a triple-GEM multiplier operated in the saturated vapour above the liquid phase. Successful operation of the detector in single electron counting mode, in the gain range from 6000 to 40000, has for the first time been demonstrated.Comment: 9 pages, 9 figures. Submitted to JINS

    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

    Technological coaxial plasma accelerator

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    Plasma sources for accelerators intended for separation processes and surface treatment have been investigated. The conditions for the choice of system parameters, as well as plasma flux, injection system, and power source have been discussed. These parameters have been obtained experimentally. A conclusion about the role of metal erosion products of the electrodes has also been drawn.Π˜ΡΡΠ»Π΅Π΄ΡƒΡŽΡ‚ΡΡ ΠΏΠ»Π°Π·ΠΌΠ΅Π½Π½Ρ‹Π΅ источники-ускоритСли для процСссов сСпарации ΠΈ ΠΎΠ±Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ повСрхностСй. ΠžΠ±ΡΡƒΠΆΠ΄Π°ΡŽΡ‚ΡΡ условия Π²Ρ‹Π±ΠΎΡ€Π° ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠ² систСмы, ΠΏΠ»Π°Π·ΠΌΠ΅Π½Π½ΠΎΠ³ΠΎ ΠΏΠΎΡ‚ΠΎΠΊΠ°, систСмы напуска Π³Π°Π·Π°, источника питания. Π­ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½ΠΎ ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Ρ‹ ΠΈΡ… ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Ρ‹. Π‘Π΄Π΅Π»Π°Π½ Π²Ρ‹Π²ΠΎΠ΄ ΠΎ Ρ€ΠΎΠ»ΠΈ мСталличСских ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚ΠΎΠ² эрозии элСктродов.Π”ΠΎΡΠ»Ρ–Π΄ΠΆΡƒΡŽΡ‚ΡŒΡΡ ΠΏΠ»Π°Π·ΠΌΠΎΠ²Ρ– Π΄ΠΆΠ΅Ρ€Π΅Π»Π° ΠΏΡ€ΠΈΡΠΊΠΎΡ€ΡŽΠ²Π°Ρ‡Ρ–Π² для процСсів сСпарації Ρ‚Π° ΠΎΠ±Ρ€ΠΎΠ±ΠΊΠΈ ΠΏΠΎΠ²Π΅Ρ€Ρ…ΠΎΠ½ΡŒ. ΠžΠ±Π³ΠΎΠ²ΠΎΡ€ΡŽΡŽΡ‚ΡŒΡΡ ΡƒΠΌΠΎΠ²ΠΈ Π²ΠΈΠ±ΠΎΡ€Ρƒ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Ρ–Π² систСми, ΠΏΠ»Π°Π·ΠΌΠΎΠ²ΠΎΠ³ΠΎ ΠΏΠΎΡ‚ΠΎΠΊΡƒ, систСми напуску Π³Π°Π·Π°, Π΄ΠΆΠ΅Ρ€Π΅Π»Π° ТивлСння. Π•ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½ΠΎ ΠΎΠ΄Π΅Ρ€ΠΆΠ°Π½Ρ– Ρ—Ρ… ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΈ. Π—Ρ€ΠΎΠ±Π»Π΅Π½Ρ– висновки Ρ‰ΠΎΠ΄ΠΎ ΠΌΠ΅Ρ‚Π°Π»Π΅Π²ΠΈΡ… ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚Ρ–Π² Π΅Ρ€ΠΎΠ·Ρ–Ρ— Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ΄Ρ–Π²

    Pion Form Factor at SND (new edition)

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    The update of the e^+e^-\to\pi^+\pi^- process cross section, measured in the energy region \sqrt{s}<1 GeV with SND detector at VEPP-2M collider is presented.Comment: Talk given at Int. Workshop e+e- Collisions from phi to psi, February 27 - March 2, 200

    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.)
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