395 research outputs found

    Π‘Ρ€Π°Π²Π½ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹ΠΉ Π°Π½Π°Π»ΠΈΠ· биомСханичСских ΠΏΠΎΠΊΠ°Π·Π°Ρ‚Π΅Π»Π΅ΠΉ Π² систСмах ΠΌΠ°Ρ€ΠΊΠ΅Ρ€Π½ΠΎΠ³ΠΎ ΠΈ Π±Π΅Π·ΠΌΠ°Ρ€ΠΊΠ΅Ρ€Π½ΠΎΠ³ΠΎ Π²ΠΈΠ΄Π΅ΠΎΠ·Π°Ρ…Π²Π°Ρ‚Π° Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠΉ

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    Motion capture systems are a key tool for performing quantitative analysis and evaluation of complex in movements sports. The prospect of the development and practical application of markerless motion capture tecnology in applied biomechanics increases research interest regarding the features of using such systems, as well as evaluat ing their accuracy and reliability in comparison with marker-based motion capture systems, which are the gold standard nowadays. Markerless motion capture systems have incomparable advantages over marker-based ones.In particular, significantly reduced time costs for the registration and data processing procedures, since registration is represented by filming a video from different angles, and processing is accompanied by the use of software algorithms for tracking the silhouette of an athlete using a presetted computer avatar. However, there is still no clear answer regarding the accuracy and reliability of the data recorded using markerless motion capture systems in relation to specific sports movements. Thus, the purpose of the presented work is to assess the statistical relationship of the data based on the correlation analysis of biomechanical variables on the example of a golf swing recorded using the Qualisys motion capture system and Simi Reality Motion markerless motion capture system.БистСмы Π·Π°Ρ…Π²Π°Ρ‚Π° Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠΉ ΡΠ²Π»ΡΡŽΡ‚ΡΡ ΠΊΠ»ΡŽΡ‡Π΅Π²Ρ‹ΠΌ инструмСнтом Π°Π½Π°Π»ΠΈΠ·Π° ΠΈ ΠΎΡ†Π΅Π½ΠΊΠΈ Ρ‚Π΅Ρ…Π½ΠΈΠΊΠΈ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠΉ Π² слоТнокоординационных Π²ΠΈΠ΄Π°Ρ… спорта. ΠŸΠ΅Ρ€ΡΠΏΠ΅ΠΊΡ‚ΠΈΠ²Π° развития ΠΈ внСдрСния Π² ΠΏΡ€Π°ΠΊΡ‚ΠΈΠΊΡƒ ΠΏΡ€ΠΈΠΊΠ»Π°Π΄Π½ΠΎΠΉ Π±ΠΈΠΎΠΌΠ΅Ρ…Π°Π½ΠΈΠΊΠΈ Ρ‚Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ Π±Π΅Π·ΠΌΠ°Ρ€ΠΊΠ΅Ρ€Π½ΠΎΠ³ΠΎ Π·Π°Ρ…Π²Π°Ρ‚Π° Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠΉ ΠΏΠΎΠ²Ρ‹ΡˆΠ°Π΅Ρ‚ Π½Π°ΡƒΡ‡Π½ΠΎ-ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Ρ‚Π΅Π»ΡŒΡΠΊΠΈΠΉ интСрСс ΠΊ особСнностям использования ΠΏΠΎΠ΄ΠΎΠ±Π½Ρ‹Ρ… систСм, Π° Ρ‚Π°ΠΊΠΆΠ΅ ΠΊ ΠΎΡ†Π΅Π½ΠΊΠ΅ ΠΈΡ… точности ΠΈ достовСрности Π² сравнСнии с ΠΌΠ°Ρ€ΠΊΠ΅Ρ€Π½Ρ‹ΠΌΠΈ систСмами Π·Π°Ρ…Π²Π°Ρ‚Π° Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠΉ, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ сСгодня ΡΠ²Π»ΡΡŽΡ‚ΡΡ Π·ΠΎΠ»ΠΎΡ‚Ρ‹ΠΌ стандартом. БистСмы Π±Π΅Π·ΠΌΠ°Ρ€ΠΊΠ΅Ρ€Π½ΠΎΠ³ΠΎ Π·Π°Ρ…Π²Π°Ρ‚Π° Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠΉ ΠΎΠ±Π»Π°Π΄Π°ΡŽΡ‚ нСсравнСнными прСимущСствами ΠΏΠ΅Ρ€Π΅Π΄ ΠΌΠ°Ρ€ΠΊΠ΅Ρ€Π½Ρ‹ΠΌΠΈ. Π’ частности, сущСствСнно ΡƒΠΌΠ΅Π½ΡŒΡˆΠ΅Π½Ρ‹ Π²Ρ€Π΅ΠΌΠ΅Π½Π½Ρ‹Π΅ Π·Π°Ρ‚Ρ€Π°Ρ‚Ρ‹ Π½Π° Ρ€Π΅Π³ΠΈΡΡ‚Ρ€Π°Ρ†ΠΈΡŽ ΠΈ ΠΎΠ±Ρ€Π°Π±ΠΎΡ‚ΠΊΡƒ Π΄Π°Π½Π½Ρ‹Ρ…, ΠΏΠΎΡΠΊΠΎΠ»ΡŒΠΊΡƒ рСгистрация прСдставляСт собой ΡΡŠΠ΅ΠΌΠΊΡƒ Π²ΠΈΠ΄Π΅ΠΎ с Ρ€Π°Π·Π½Ρ‹Ρ… ракурсов, Π° ΠΎΠ±Ρ€Π°Π±ΠΎΡ‚ΠΊΠ° сопровоТдаСтся ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ ΠΏΡ€ΠΎΠ³Ρ€Π°ΠΌΠΌΠ½Ρ‹Ρ… Π°Π»Π³ΠΎΡ€ΠΈΡ‚ΠΌΠΎΠ² отслСТивания силуэта спортсмСна посрСдством ΠΊΠΎΠΌΠΏΡŒΡŽΡ‚Π΅Ρ€Π½ΠΎΠ³ΠΎ Π°Π²Π°Ρ‚Π°Ρ€Π°. Однако Π΄ΠΎ сих ΠΏΠΎΡ€ Π½Π΅Ρ‚ ΠΎΠ΄Π½ΠΎΠ·Π½Π°Ρ‡Π½ΠΎΠ³ΠΎ ΠΎΡ‚Π²Π΅Ρ‚Π° ΠΎΡ‚Π½ΠΎΡΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ точности ΠΈ достовСрности Π΄Π°Π½Π½Ρ‹Ρ…, рСгистрируСмых с использованиСм систСм Π±Π΅Π·ΠΌΠ°Ρ€ΠΊΠ΅Ρ€Π½ΠΎΠ³ΠΎ Π·Π°Ρ…Π²Π°Ρ‚Π° Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠΉ ΠΏΡ€ΠΈΠΌΠ΅Π½ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ ΠΊ ΠΊΠΎΠ½ΠΊΡ€Π΅Ρ‚Π½Ρ‹ΠΌ Π²ΠΈΠ΄Π°ΠΌ спорта ΠΈ спортивным двиТСниям. Π’ ΡΡ‚Π°Ρ‚ΡŒΠ΅ ΠΏΡ€ΠΈΠ²Π΅Π΄Π΅Π½Π° ΠΎΡ†Π΅Π½ΠΊΠ° статистичСской взаимосвязи Π΄Π°Π½Π½Ρ‹Ρ… Π½Π° основС коррСляционного Π°Π½Π°Π»ΠΈΠ·Π° биомСханичСских ΠΏΠΎΠΊΠ°Π·Π°Ρ‚Π΅Π»Π΅ΠΉ Π½Π° ΠΏΡ€ΠΈΠΌΠ΅Ρ€Π΅ выполнСния ΡƒΠ΄Π°Ρ€Π° Π² Π³ΠΎΠ»ΡŒΡ„Π΅, зарСгистрированных с использованиСм ΠΌΠ°Ρ€ΠΊΠ΅Ρ€Π½ΠΎΠΉ систСмы оптичСского Π·Π°Ρ…Π²Π°Ρ‚Π° Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠΉ Qualisys ΠΈ Π±Π΅Π·ΠΌΠ°Ρ€ΠΊΠ΅Ρ€Π½ΠΎΠΉ систСмы Π·Π°Ρ…Π²Π°Ρ‚Π° Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠΉ Simi Reality Motion

    Excitonic instability and electric-field-induced phase transition towards a two dimensional exciton condensate

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    We present an InAs-GaSb-based system in which the electric-field tunability of its 2D energy gap implies a transition towards a thermodynamically stable excitonic condensed phase. Detailed calculations show a 3 meV BCS-like gap appearing in a second-order phase transition with electric field. We find this transition to be very sharp, solely due to exchange interaction, and so, the exciton binding energy is greatly renormalized even at small condensate densities. This density gradually increases with external field, thus enabling the direct probe of the Bose-Einstein to BCS crossover.Comment: LaTex, 11 pages, 3 ps figures, To appear in PR

    High-pressure x-ray diffraction study on the structure and phase transitions of the defect-stannite ZnGa2Se4 and defect-chalcopyrite CdGa2S4

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    X-ray diffraction measurements on the sphalerite-derivatives ZnGa2Se4 and CdGa2S4 have been performed upon compression up to 23 GPa in a diamond-anvil cell. ZnGa2Se4 exhibits a defect tetragonal stannite-type structure (I-42m) up to 15.5 GPa and in the range from 15.5 GPa to 18.5 GPa the low-pressure phase coexists with a high-pressure phase, which remains stable up to 23 GPa. In CdGa2S4, we find the defect tetragonal chalcopyrite-type structure (I-4) is stable up to 17 GPa. Beyond this pressure a pressure-induced phase transition takes place. In both materials, the high-pressure phase has been characterized as a defect-cubic NaCl-type structure (Fm-3m). The occurrence of the pressure induced phase transitions is apparently related with an increase of the cation disorder on the semiconductors investigated. In addition, the results allow the evaluation of the axial compressibility and the determination of the equation of state for each compound. The obtained results are compared with those previously reported for isomorphic digallium sellenides. Finally, a systematic study of the pressure-induced phase transition in twenty-three different sphalerite-related ABX2 and AB2X4 compounds indicates that the transition pressure increases as the ratio of the cationic radii and anionic radii of the compounds increases.Comment: 34 pages, 3 tables, 6 figure

    Technologies for measuring the dynamic parameters of rowing based on strain gauge systems

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    One of the criteria for the effectiveness of flatwater rowing biomechanics is the interaction of the athlete with the surface of the water by an oar, as well as the effectiveness of transferring the efforts developed by the athlete to the boat for its advancement. The quality of an athlete's move-ments with a paddle in rowing locomotives depends on the level of development of power abilities and can be quantified using strain gauge systems. However, the lack of recommendations describ-ing the specifics of the preparation and use of such systems in training process significantly reduce the degree of their use. The article discusses the technical features and methodological founda-tions of the use of strain gauge systems to measure the efforts of an athlete when interacting with an oar in flatwater kayaking and canoeing. To substantiate the choice of the scheme of loading and securing the paddle when graduating the strain gauge system, as well as the place of its direct attachment to the forearm, the authors carried out mathematical modeling of diagrams of bending moments arising on the paddle in response to external forces, as a result of which three options for the support and orientation of the paddle are presented, depending on the location of key sup-port points. To substantiate the method of attaching the strain gauge system to the forearm, a series of tests with paddle loading was carried out, as a result of which the presence of a linear relationship between the values of the external load and the readings of the strain gauge system was assessed, as well as the repeatability of the recorded data. Based on the results of the as-sessment, recommendations are presented for the practical application of the results of the study in assessing the speed and strength training of rowers on kayaks and canoes.Одним ΠΈΠ· ΠΊΡ€ΠΈΡ‚Π΅Ρ€ΠΈΠ΅Π² эффСктивности Π±ΠΈΠΎΠΌΠ΅Ρ…Π°Π½ΠΈΠΊΠΈ Π³Ρ€Π΅Π±Π»ΠΈ Π½Π° плоской Π²ΠΎΠ΄Π΅ являСтся взаимодСйствиС спортсмСна с ΠΏΠΎΠ²Π΅Ρ€Ρ…Π½ΠΎΡΡ‚ΡŒΡŽ Π²ΠΎΠ΄Ρ‹ ΠΏΡ€ΠΈ ΠΏΠΎΠΌΠΎΡ‰ΠΈ вСсла, Π° Ρ‚Π°ΠΊΠΆΠ΅ ΡΡ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ ΠΏΠ΅Ρ€Π΅Π΄Π°Ρ‡ΠΈ усилий, Ρ€Π°Π·Π²ΠΈΠ²Π°Π΅ΠΌΡ‹Ρ… спортсмСном, Π½Π° Π»ΠΎΠ΄ΠΊΡƒ для Π΅Π΅ продвиТСния. ΠšΠ°Ρ‡Π΅ΡΡ‚Π²ΠΎ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠΉ спортсмСна с вСслом Π² Π³Ρ€Π΅Π±Π½Ρ‹Ρ… Ρ‚Ρ€Π΅Π½Π°ΠΆΠ΅Ρ€Π°Ρ… зависит ΠΎΡ‚ уровня развития силовых способностСй ΠΈ ΠΌΠΎΠΆΠ΅Ρ‚ Π±Ρ‹Ρ‚ΡŒ количСствСнно ΠΎΡ†Π΅Π½Π΅Π½ΠΎ с ΠΏΠΎΠΌΠΎΡ‰ΡŒΡŽ тСнзомСтричСских систСм. Однако отсутствиС Ρ€Π΅ΠΊΠΎΠΌΠ΅Π½Π΄Π°Ρ†ΠΈΠΉ, ΠΎΠΏΠΈΡΡ‹Π²Π°ΡŽΡ‰ΠΈΡ… спСцифику ΠΏΠΎΠ΄Π³ΠΎΡ‚ΠΎΠ²ΠΊΠΈ ΠΈ использования Ρ‚Π°ΠΊΠΈΡ… систСм Π² Ρ‚Ρ€Π΅Π½ΠΈΡ€ΠΎΠ²ΠΎΡ‡Π½ΠΎΠΌ процСссС, сущСствСнно сниТаСт ΡΡ‚Π΅ΠΏΠ΅Π½ΡŒ ΠΈΡ… использования. Π’ ΡΡ‚Π°Ρ‚ΡŒΠ΅ Ρ€Π°ΡΡΠΌΠ°Ρ‚Ρ€ΠΈΠ²Π°ΡŽΡ‚ΡΡ тСхничСскиС особСнности ΠΈ мСтодологичСскиС основы использования тСнзомСтричСских систСм для измСрСния усилий спортсмСна ΠΏΡ€ΠΈ взаимодСйствии с вСслом Π² ΠΏΠ»Π°Π²Π°Π½ΠΈΠΈ Π½Π° плоских Π±Π°ΠΉΠ΄Π°Ρ€ΠΊΠ°Ρ… ΠΈ каноэ. Для обоснования Π²Ρ‹Π±ΠΎΡ€Π° схСмы нагруТСния ΠΈ закрСплСния Π»ΠΎΠΏΠ°Ρ‚ΠΊΠΈ ΠΏΡ€ΠΈ Π³Ρ€Π°Π΄ΡƒΠΈΡ€ΠΎΠ²ΠΊΠ΅ тСнзомСтричСской систСмы, Π° Ρ‚Π°ΠΊΠΆΠ΅ мСста Π΅Π΅ нСпосрСдствСнного крСплСния ΠΊ Ρ†Π΅Π²ΡŒΡŽ, Π°Π²Ρ‚ΠΎΡ€Π°ΠΌΠΈ Π±Ρ‹Π»ΠΎ ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½ΠΎ матСматичСскоС ΠΌΠΎΠ΄Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ Π΄ΠΈΠ°Π³Ρ€Π°ΠΌΠΌ ΠΈΠ·Π³ΠΈΠ±Π°ΡŽΡ‰ΠΈΡ… ΠΌΠΎΠΌΠ΅Π½Ρ‚ΠΎΠ², Π²ΠΎΠ·Π½ΠΈΠΊΠ°ΡŽΡ‰ΠΈΡ… Π½Π° Π»ΠΎΠΏΠ°Ρ‚ΠΊΠ΅ Π² ΠΎΡ‚Π²Π΅Ρ‚ Π½Π° воздСйствиС Π²Π½Π΅ΡˆΠ½ΠΈΡ… сил, Π² Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π΅ ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠ³ΠΎ Π±Ρ‹Π»ΠΈ ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Ρ‹ Ρ‚Ρ€ΠΈ прСдставлСны Π²Π°Ρ€ΠΈΠ°Π½Ρ‚Ρ‹ крСплСния ΠΈ ΠΎΡ€ΠΈΠ΅Π½Ρ‚Π°Ρ†ΠΈΠΈ лопасти Π² зависимости ΠΎΡ‚ располоТСния ΠΊΠ»ΡŽΡ‡Π΅Π²Ρ‹Ρ… Ρ‚ΠΎΡ‡Π΅ΠΊ ΠΎΠΏΠΎΡ€Ρ‹. Для обоснования способа крСплСния тСнзомСтричСской систСмы ΠΊ ΠΏΡ€Π΅Π΄ΠΏΠ»Π΅Ρ‡ΡŒΡŽ Π±Ρ‹Π»Π° ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½Π° сСрия испытаний с лопастной Π½Π°Π³Ρ€ΡƒΠ·ΠΊΠΎΠΉ, Π² Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π΅ ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ… Π±Ρ‹Π»ΠΎ ΠΎΡ†Π΅Π½Π΅Π½ΠΎ Π½Π°Π»ΠΈΡ‡ΠΈΠ΅ Π»ΠΈΠ½Π΅ΠΉΠ½ΠΎΠΉ зависимости ΠΌΠ΅ΠΆΠ΄Ρƒ значСниями внСшнСй Π½Π°Π³Ρ€ΡƒΠ·ΠΊΠΈ ΠΈ показаниями тСнзомСтричСской систСмы, Π° Ρ‚Π°ΠΊΠΆΠ΅ ΠΏΠΎΠ²Ρ‚ΠΎΡ€ΡΠ΅ΠΌΠΎΡΡ‚ΡŒ записанныС Π΄Π°Π½Π½Ρ‹Π΅. По Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π°ΠΌ ΠΎΡ†Π΅Π½ΠΊΠΈ прСдставлСны Ρ€Π΅ΠΊΠΎΠΌΠ΅Π½Π΄Π°Ρ†ΠΈΠΈ ΠΏΠΎ практичСскому ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΡŽ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΎΠ² исслСдования ΠΏΡ€ΠΈ ΠΎΡ†Π΅Π½ΠΊΠ΅ скоростно-силовой ΠΏΠΎΠ΄Π³ΠΎΡ‚ΠΎΠ²ΠΊΠΈ Π³Ρ€Π΅Π±Ρ†ΠΎΠ² Π½Π° Π±Π°ΠΉΠ΄Π°Ρ€ΠΊΠ°Ρ… ΠΈ каноэ

    Charged vortices in superfluid systems with pairing of spatially separated carriers

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    It is shown that in a magnetic field the vortices in superfluid electron-hole systems carry a real electrical charge. The charge value depends on the relation between the magnetic length and the Bohr radiuses of electrons and holes. In double layer systems at equal electron and hole filling factors in the case of the electron and hole Bohr radiuses much larger than the magnetic length the vortex charge is equal to the universal value (electron charge times the filling factor).Comment: 4 page

    Bilateral percutaneous mininephrolithotripsy: simultaneous or staged approach?

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    Introduction. Patients with bilateral nephrolithiasis are a challenge for the treating physician. Therefore, such patients traditionally are subject to phased surgery to reduce the rate of complications. At the same time, the enhancement of endoscopic technologies and anesthesia makes it possible to perform surgical treatment of bilateral nephrolithiasis simultaneously.Objective. To evaluate the effectiveness and safety of performing simultaneous bilateral percutaneous nephrolithotripsy (PCNL).Materials & methods. The main group comprises 19 patients (avg age 45.0 Β± 2.25 years) suffering from bilateral nephrolithiasis (13 men and 6 women). The control group include 20 patients (avg age 45.80 Β± 2.29 years) suffering from bilateral nephrolithiasis. Main group patients underwent simultaneous bilateral mini-PCNL, control group patients β€” staged PCNL within two hospitalisations. The visual analogue scale (VAS) was used to assess the pain severity. Patients noted subjective pain sensations on post-op days 1 and 3. QoL indicators were assessed using the SF-36 general questionnaire, as well as the Russian-language validated version of the WISQoL questionnaire.Results. There were no statistically significant differences between the parameters (the difference between the hemoglobin before and after mini-PCNL was 12 g/l; between the serum creatinine was 18 Β΅mol/l). There was a decrease in total surgery time (121.0 Β± 6.1 min) for main group patients compared to (147.0 Β± 7.3 min) control group patients (total surgery time during the first and second hospitalisations) and a reduction in hospital stay (4.50 Β± 0.23 days) for main group patients compared to control group patients (10.0 Β± 0.5 days). Complications observed by us in the two groups were comparable. The valuesobtained on the SF, RE and MH scales in main group patients were higher both on post-op day 1 (67.9 Β± 3.39; 56.90 Β± 2.85 and 63.80 Β± 3.19, respectively) and post-op day 3 (86.80 Β± 4.34; 83.70 Β± 4.19 and 82.50 Β± 4.13, respectively) compared to control group patients during the first and second hospitalizations. Statistically significant differences were also recorded according to the grades "Social functioning" and "Emotional influence" in main group patients (80.90 Β± 0.26 and 82.6 Β± 0.19, respectively).Conclusion. Simultaneous bilateral mini-PCNL is safe and effective in well-selected patients

    Models of coherent exciton condensation

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    That excitons in solids might condense into a phase-coherent ground state was proposed about 40 years ago, and has been attracting experimental and theoretical attention ever since. Although experimental confirmation has been hard to come by, the concepts released by this phenomenon have been widely influential. This tutorial review discusses general aspects of the theory of exciton and polariton condensates, focussing on the reasons for coherence in the ground state wavefunction, the BCS to Bose crossover(s) for excitons and for polaritons, and the relationship of the coherent condensates to standard lasers.Comment: 27 pages, 6 figures. Submitted for a special issue of J. Phys. Cond. Matt. associated with the EU network "Photon-mediated phenomena in semiconductor nanostructures

    Mimicking diffuse supernova antineutrinos with the Sun as a source

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    Measuring the electron antineutrino component of the cosmic diffuse supernova neutrino background (DSNB) is the next ambitious goal for low-energy neutrino astronomy. The largest flux is expected in the lowest accessible energy bin. However, for E < 15 MeV a possible signal can be mimicked by a solar electron antineutrino flux that originates from the usual 8B neutrinos by spin-flavor oscillations. We show that such an interpretation is possible within the allowed range of neutrino electromagnetic transition moments and solar turbulent field strengths and distributions. Therefore, an unambiguous detection of the DSNB requires a significant number of events at E > 15 MeV.Comment: 4 pages, 1 figur

    The Relation Between the Surface Brightness and the Diameter for Galactic Supernova Remnants

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    In this work, we have constructed a relation between the surface brightness (Ξ£\Sigma) and diameter (D) of Galactic C- and S-type supernova remnants (SNRs). In order to calibrate the Ξ£\Sigma-D dependence, we have carefully examined some intrinsic (e.g. explosion energy) and extrinsic (e.g. density of the ambient medium) properties of the remnants and, taking into account also the distance values given in the literature, we have adopted distances for some of the SNRs which have relatively more reliable distance values. These calibrator SNRs are all C- and S-type SNRs, i.e. F-type SNRs (and S-type SNR Cas A which has an exceptionally high surface brightness) are excluded. The Sigma-D relation has 2 slopes with a turning point at D=36.5 pc: Ξ£\Sigma(at 1 GHz)=8.4βˆ’6.3+19.5^{+19.5}_{-6.3}Γ—10βˆ’12\times10^{-12} Dβˆ’5.99βˆ’0.33+0.38^{{-5.99}^{+0.38}_{-0.33}} Wmβˆ’2^{-2}Hzβˆ’1^{-1}sterβˆ’1^{-1} (for Ξ£\Sigma≀3.7Γ—10βˆ’21\le3.7\times10^{-21} Wmβˆ’2^{-2}Hzβˆ’1^{-1}sterβˆ’1^{-1} and Dβ‰₯\ge36.5 pc) and Ξ£\Sigma(at 1 GHz)=2.7βˆ’1.4+2.1^{+2.1}_{-1.4}Γ—\times 10βˆ’17^{-17} Dβˆ’2.47βˆ’0.16+0.20^{{-2.47}^{+0.20}_{-0.16}} Wmβˆ’2^{-2}Hzβˆ’1^{-1}sterβˆ’1^{-1} (for Ξ£\Sigma>3.7Γ—10βˆ’21>3.7\times10^{-21} Wmβˆ’2^{-2}Hzβˆ’1^{-1}sterβˆ’1^{-1} and D<<36.5 pc). We discussed the theoretical basis for the Ξ£\Sigma-D dependence and particularly the reasons for the change in slope of the relation were stated. Added to this, we have shown the dependence between the radio luminosity and the diameter which seems to have a slope close to zero up to about D=36.5 pc. We have also adopted distance and diameter values for all of the observed Galactic SNRs by examining all the available distance values presented in the literature together with the distances found from our Ξ£\Sigma-D relation.Comment: 45 pages, 2 figures, accepted for publication in Astronomical and Astrophysical Transaction
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