3 research outputs found

    The Content and Direction of the Artificial Hypoxic Exercising Methods in Training Elite Ski-Racers

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    На соврСмСнном этапС ΠΏΠΎΠ΄Π³ΠΎΡ‚ΠΎΠ²ΠΊΠ° Π»Ρ‹ΠΆΠ½ΠΈΠΊΠΎΠ²-Π³ΠΎΠ½Ρ‰ΠΈΠΊΠΎΠ² высокой ΠΊΠ²Π°Π»ΠΈΡ„ΠΈΠΊΠ°Ρ†ΠΈΠΈ характСризуСтся Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹ΠΌ ростом физичСских Π½Π°Π³Ρ€ΡƒΠ·ΠΎΠΊ, объСм ΠΈ ΠΈΠ½Ρ‚Π΅Π½ΡΠΈΠ²Π½ΠΎΡΡ‚ΡŒ Ρ‚Ρ€Π΅Π½ΠΈΡ€ΠΎΠ²ΠΎΡ‡Π½ΠΎΠΉ Ρ€Π°Π±ΠΎΡ‚Ρ‹ достигаСт ΠΏΡ€Π΅Π΄Π΅Π»ΡŒΠ½Ρ‹Ρ… Π²Π΅Π»ΠΈΡ‡ΠΈΠ½, дальнСйший рост ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ… лимитируСтся Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΎΠ½Π°Π»ΡŒΠ½Ρ‹ΠΌΠΈ возмоТностями ΠΎΡ€Π³Π°Π½ΠΈΠ·ΠΌΠ° спортсмСнов. Π’ связи с этим Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚ΠΊΠ° эффСктивных, соврСмСнных, Π½Π°ΡƒΡ‡Π½ΠΎ обоснованных Ρ‚Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ ΠΌΠΎΠΆΠ΅Ρ‚ ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΡ‚ΡŒ сущСствСнно Ρ€Π°ΡΡˆΠΈΡ€ΠΈΡ‚ΡŒ Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΎΠ½Π°Π»ΡŒΠ½Ρ‹ΠΉ Ρ€Π΅Π·Π΅Ρ€Π² ΠΎΡ€Π³Π°Π½ΠΈΠ·ΠΌΠ° ΠΏΡ€ΠΈ достигнутом объСмС ΠΈ интСнсивности Ρ‚Ρ€Π΅Π½ΠΈΡ€ΠΎΠ²ΠΎΡ‡Π½Ρ‹Ρ… Π½Π°Π³Ρ€ΡƒΠ·ΠΎΠΊ, Π° Ρ‚Π°ΠΊΠΆΠ΅ ΠΏΠΎΠ²Ρ‹ΡΠΈΡ‚ΡŒ ΡƒΡ€ΠΎΠ²Π΅Π½ΡŒ спортивных . At present, the preparation of highly skilled skiers is characterized by a significant increase in physical activity, training volume and the intensity of work reaches a limit value, the further growth of which is limited by the functionality of an athlete’s body. In this context, the development of effective modern, science-based technology may allow to significantly expand the functional reserve of the organism with the existing volume and the intensity of training loads, and improve athletic performance

    Implementation of Imitation Hypoxic Workout when Training Highly Qualified Downhill Skiers Based on Physical Exercise Individualization

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    Π’ Ρ€Π°Π±ΠΎΡ‚Π΅ приводятся ΠΈΡ‚ΠΎΠ³ΠΈ ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ исслСдования, Π½Π°ΠΏΡ€Π°Π²Π»Π΅Π½Π½ΠΎΠ³ΠΎ Π½Π° выяснСниС вопроса ΠΎ возмоТности примСнСния Π² ΠΏΠΎΠ΄Π³ΠΎΡ‚ΠΎΠ²ΠΊΠ΅ Π»Ρ‹ΠΆΠ½ΠΈΠΊΠΎΠ²-Π³ΠΎΠ½Ρ‰ΠΈΠΊΠΎΠ² высокой ΠΊΠ²Π°Π»ΠΈΡ„ΠΈΠΊΠ°Ρ†ΠΈΠΈ искусствСнной гипоксичСской Ρ‚Ρ€Π΅Π½ΠΈΡ€ΠΎΠ²ΠΊΠΈ (Π˜Π“Π’), которая Π² сочСтании с общСпринятыми срСдствами спортивной Ρ‚Ρ€Π΅Π½ΠΈΡ€ΠΎΠ²ΠΊΠΈ обСспСчиваСт высокий ΡƒΡ€ΠΎΠ²Π΅Π½ΡŒ достиТСний Π² ΠΎΡ‚Π΄Π΅Π»ΡŒΠ½Ρ‹Ρ… Π²ΠΈΠ΄Π°Ρ… спорта. Π’ ΠΏΡƒΠ±Π»ΠΈΠΊΠ°Ρ†ΠΈΠΈ прСдставлСны ΠΏΠΎΠΊΠ°Π·Π°Ρ‚Π΅Π»ΠΈ физичСской Π½Π°Π³Ρ€ΡƒΠ·ΠΊΠΈ Π² ΠΌΠΈΠΊΡ€ΠΎ- ΠΈ ΠΌΠ΅Π·ΠΎΡ†ΠΈΠΊΠ»Π°Ρ… ΠΏΠΎΠ΄Π³ΠΎΡ‚ΠΎΠ²ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠ³ΠΎ ΠΏΠ΅Ρ€ΠΈΠΎΠ΄Π°, Π° Ρ‚Π°ΠΊΠΆΠ΅ Π½Π°ΠΏΡ€Π°Π²Π»Π΅Π½Π½ΠΎΡΡ‚ΡŒ ΠΈ содСрТаниС Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚Π°Π½Π½ΠΎΠΉ Π°Π²Ρ‚ΠΎΡ€Π°ΠΌΠΈ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΠΊΠΈ развития ΡΠΏΠ΅Ρ†ΠΈΠ°Π»ΡŒΠ½ΠΎΠΉ физичСской подготовлСнности высококвалифицированных Π»Ρ‹ΠΆΠ½ΠΈΠΊΠΎΠ²-Π³ΠΎΠ½Ρ‰ΠΈΠΊΠΎΠ² ΠΏΡ€ΠΈ использовании Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Ρ… срСдств ΠΈ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠ² искусствСнной гипоксичСской Ρ‚Ρ€Π΅Π½ΠΈΡ€ΠΎΠ²ΠΊΠΈ. Π”ΠΎΠΊΠ°Π·Π°Π½Π° ΡΡ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½ΠΎΠΉ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΠΊΠΈ Π² ΠΏΠΎΠ²Ρ‹ΡˆΠ΅Π½ΠΈΠΈ уровня физичСской подготовлСнности, Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΎΠ½Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ Ρ€Π΅Π·Π΅Ρ€Π²Π° ΠΎΡ€Π³Π°Π½ΠΈΠ·ΠΌΠ° спортсмСнов ΠΈ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΈΠ²Π½ΠΎΡΡ‚ΠΈ ΠΈΡ… ΡΠΎΡ€Π΅Π²Π½ΠΎΠ²Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠΉ . This article presents the results of research on the expediency of imitation hypoxic workout when training highly qualified downhill skiers. This method, along with some other sports training methods, provides for impressive results in certain kinds of sport. This paper shows the indicators of physical exercise in micro and mesocycle of pre-season, as well as the material on the expediency of imitation hypoxic workout when training highly qualified downhill skiers. The effectiveness of experimental methods in increasing physical fitness as well as β€œthe functional reservoir” of sportsmen’s bodies and their competitiveness has been proved

    Measurements of the Total and Differential Higgs Boson Production Cross Sections Combining the H??????? and H???ZZ*???4??? Decay Channels at s\sqrt{s}=8??????TeV with the ATLAS Detector

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    Measurements of the total and differential cross sections of Higgs boson production are performed using 20.3~fbβˆ’1^{-1} of pppp collisions produced by the Large Hadron Collider at a center-of-mass energy of s=8\sqrt{s} = 8 TeV and recorded by the ATLAS detector. Cross sections are obtained from measured Hβ†’Ξ³Ξ³H \rightarrow \gamma \gamma and Hβ†’ZZβˆ—β†’4β„“H \rightarrow ZZ ^{*}\rightarrow 4\ell event yields, which are combined accounting for detector efficiencies, fiducial acceptances and branching fractions. Differential cross sections are reported as a function of Higgs boson transverse momentum, Higgs boson rapidity, number of jets in the event, and transverse momentum of the leading jet. The total production cross section is determined to be Οƒppβ†’H=33.0Β±5.3 (stat)Β±1.6 (sys)pb\sigma_{pp \to H} = 33.0 \pm 5.3 \, ({\rm stat}) \pm 1.6 \, ({\rm sys}) \mathrm{pb}. The measurements are compared to state-of-the-art predictions.Measurements of the total and differential cross sections of Higgs boson production are performed using 20.3  fb-1 of pp collisions produced by the Large Hadron Collider at a center-of-mass energy of s=8  TeV and recorded by the ATLAS detector. Cross sections are obtained from measured Hβ†’Ξ³Ξ³ and Hβ†’ZZ*β†’4β„“ event yields, which are combined accounting for detector efficiencies, fiducial acceptances, and branching fractions. Differential cross sections are reported as a function of Higgs boson transverse momentum, Higgs boson rapidity, number of jets in the event, and transverse momentum of the leading jet. The total production cross section is determined to be Οƒppβ†’H=33.0Β±5.3 (stat)Β±1.6 (syst)  pb. The measurements are compared to state-of-the-art predictions.Measurements of the total and differential cross sections of Higgs boson production are performed using 20.3 fbβˆ’1^{-1} of pppp collisions produced by the Large Hadron Collider at a center-of-mass energy of s=8\sqrt{s} = 8 TeV and recorded by the ATLAS detector. Cross sections are obtained from measured Hβ†’Ξ³Ξ³H \rightarrow \gamma \gamma and Hβ†’ZZβˆ—β†’4β„“H \rightarrow ZZ ^{*}\rightarrow 4\ell event yields, which are combined accounting for detector efficiencies, fiducial acceptances and branching fractions. Differential cross sections are reported as a function of Higgs boson transverse momentum, Higgs boson rapidity, number of jets in the event, and transverse momentum of the leading jet. The total production cross section is determined to be Οƒppβ†’H=33.0Β±5.3 (stat)Β±1.6 (sys)pb\sigma_{pp \to H} = 33.0 \pm 5.3 \, ({\rm stat}) \pm 1.6 \, ({\rm sys}) \mathrm{pb}. The measurements are compared to state-of-the-art predictions
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