118 research outputs found

    Anomaly analysis of Hawking radiation from Kaluza-Klein black hole with squashed horizon

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    Considering gravitational and gauge anomalies at the horizon, a new method that to derive Hawking radiations from black holes has been developed by Wilczek et al. In this paper, we apply this method to non-rotating and rotating Kaluza-Klein black holes with squashed horizon, respectively. For the rotating case, we found that, after the dimensional reduction, an effective U(1) gauge field is generated by an angular isometry. The results show that the gauge current and energy-momentum tensor fluxes are exactly equivalent to Hawking radiation from the event horizon.Comment: 15 pages, no figures, the improved version, accepted by Eur. Phys. J.

    Structural Strength and Service Life of the Extrusion Forming Die for Agricultural Engine Piston Heads

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    Three-tier high-strength prestressed combination concave dies are designed to manifacture highpower corn combine harvester engine piston heads. This design integrates the advantages of traditional casting or hot die forging and warm extrusion. The following key parameters, viz radial dimensions of each mating layer, axial bonding and radial contact interaction, are obtained by theoretical calculation. Nonlinear analysis of the contact interaction was carried out, and the die contact condition was studied at no-load and full-load. Based on the Archard wear theory, thermomechanical bonding was studied in operation of the die. Through numerical simulation of the die wear in each operation cycle, the univariate linear regression equation of the die service life was derived, and the reliability of this equation was verified. The results show that the die contact is both stable and reliable if the radial contact interaction of the inner and outer layers is ή₂= 1.9716 mm and ή₃= 1.3870 mm, respectively. With the nitriding layer thickness of 0.24 mm, the extrusion die service life in the production of piston heads corresponds to 6357 pieces.Đ Đ°Đ·Ń€Đ°Đ±ĐŸŃ‚Đ°ĐœŃ‹ Ń‚Ń€Đ”Ń…ŃŠŃŃ€ŃƒŃĐœŃ‹Đ” ĐČŃ‹ŃĐŸĐșĐŸĐżŃ€ĐŸŃ‡ĐœŃ‹Đ” прДЎĐČĐ°Ń€ĐžŃ‚Đ”Đ»ŃŒĐœĐŸ-ĐœĐ°ĐżŃ€ŃĐ¶Đ”ĐœĐœŃ‹Đ” ĐŒĐœĐŸĐłĐŸĐŒĐ”ŃŃ‚ĐœŃ‹Đ” ĐČĐŸĐłĐœŃƒŃ‚Ń‹Đ” ĐłĐŸĐ»ĐŸĐČĐșĐž ĐŽĐ»Ń ĐžĐ·ĐłĐŸŃ‚ĐŸĐČĐ»Đ”ĐœĐžŃ ĐŽĐœĐžŃ‰ ĐżĐŸŃ€ŃˆĐœŃ ĐŽĐČĐžĐłĐ°Ń‚Đ”Đ»Ń ĐŒĐŸŃ‰ĐœĐŸĐłĐŸ ĐșуĐșŃƒŃ€ŃƒĐ·ĐŸŃƒĐ±ĐŸŃ€ĐŸŃ‡ĐœĐŸĐłĐŸ ĐșĐŸĐŒĐ±Đ°ĐčĐœĐ°. ĐšĐŸĐœŃŃ‚Ń€ŃƒĐșцоя ŃĐŸĐ”ĐŽĐžĐœŃĐ”Ń‚ ĐČ ŃĐ”Đ±Đ” ĐżŃ€Đ”ĐžĐŒŃƒŃ‰Đ”ŃŃ‚ĐČĐ° Đ»ĐžŃ‚ŃŒŃ ОлО ĐłĐŸŃ€ŃŃ‡Đ”Đč ĐșĐŸĐČĐșĐž Đž ĐłĐŸŃ€ŃŃ‡Đ”Đč эĐșŃŃ‚Ń€ŃƒĐ·ĐžĐž. Đ Đ°ĐŽĐžĐ°Đ»ŃŒĐœŃ‹Đ” Ń€Đ°Đ·ĐŒĐ”Ń€Ń‹ ĐșĐ°Đ¶ĐŽĐŸĐłĐŸ ŃĐŸĐ”ĐŽĐžĐœŃĐ”ĐŒĐŸĐłĐŸ ŃĐ»ĐŸŃ, ĐŸŃĐ”ĐČĐŸĐ” ŃŃ†Đ”ĐżĐ»Đ”ĐœĐžĐ” Đž Ń€Đ°ĐŽĐžĐ°Đ»ŃŒĐœĐŸĐ” ĐșĐŸĐœŃ‚Đ°ĐșŃ‚ĐœĐŸĐ” ĐČĐ·Đ°ĐžĐŒĐŸĐŽĐ”ĐčстĐČОД Ń€Đ°ŃŃŃ‡ĐžŃ‚Đ°ĐœŃ‹ Ń‚Đ”ĐŸŃ€Đ”Ń‚ĐžŃ‡Đ”ŃĐșĐž. Đ’Ń‹ĐżĐŸĐ»ĐœĐ”Đœ ĐœĐ”Đ»ĐžĐœĐ”ĐčĐœŃ‹Đč Đ°ĐœĐ°Đ»ĐžĐ· ĐșĐŸĐœŃ‚Đ°ĐșŃ‚ĐœĐŸĐłĐŸ ĐČĐ·Đ°ĐžĐŒĐŸĐŽĐ”ĐčстĐČоя, ĐžĐ·ŃƒŃ‡Đ”ĐœŃ‹ ŃƒŃĐ»ĐŸĐČоя ĐșĐŸĐœŃ‚Đ°ĐșŃ‚ĐžŃ€ĐŸĐČĐ°ĐœĐžŃ ĐČ ĐłĐŸĐ»ĐŸĐČĐșĐ” про ĐœŃƒĐ»Đ”ĐČĐŸĐč Đž ĐżĐŸĐ»ĐœĐŸĐč ĐœĐ°ĐłŃ€ŃƒĐ·ĐșĐ”. На ĐŸŃĐœĐŸĐČĐ°ĐœĐžĐž Ń‚Đ”ĐŸŃ€ĐžĐž ĐžĐ·ĐœĐŸŃĐ° АрчарЮа ĐČŃ‹ĐżĐŸĐ»ĐœĐ”ĐœĐ° ĐŸŃ†Đ”ĐœĐșĐ° Ń‚Đ”Ń€ĐŒĐŸĐŒĐ”Ń…Đ°ĐœĐžŃ‡Đ”ŃĐșĐŸĐłĐŸ ŃŃ†Đ”ĐżĐ»Đ”ĐœĐžŃ ĐČ ĐżŃ€ĐŸŃ†Đ”ŃŃĐ” эĐșŃĐżĐ»ŃƒĐ°Ń‚Đ°Ń†ĐžĐž ĐłĐŸĐ»ĐŸĐČĐșĐž. ĐŸŃƒŃ‚Đ”ĐŒ Ń‡ĐžŃĐ»Đ”ĐœĐœĐŸĐłĐŸ ĐŒĐŸĐŽĐ”Đ»ĐžŃ€ĐŸĐČĐ°ĐœĐžŃ ĐžĐ·ĐœĐŸŃĐ° ĐłĐŸĐ»ĐŸĐČĐșĐž ĐČ ĐșĐ°Đ¶ĐŽĐŸĐŒ Ń€Đ°Đ±ĐŸŃ‡Đ”ĐŒ цоĐșлД ĐżĐŸĐ»ŃƒŃ‡Đ”ĐœĐŸ ĐŸĐŽĐœĐŸĐżĐ°Ń€Đ°ĐŒĐ”Ń‚Ń€ĐžŃ‡Đ”ŃĐșĐŸĐ” ураĐČĐœĐ”ĐœĐžĐ” Đ»ĐžĐœĐ”ĐčĐœĐŸĐč рДгрДссОО ĐŽĐ»Ń ŃŃ€ĐŸĐșĐ° ДД ŃĐ»ŃƒĐ¶Đ±Ń‹; ĐżŃ€ĐŸĐČĐ”Ń€Đ”ĐœĐ° ĐŽĐŸŃŃ‚ĐŸĐČĐ”Ń€ĐœĐŸŃŃ‚ŃŒ ĐŽĐ°ĐœĐœĐŸĐłĐŸ ураĐČĐœĐ”ĐœĐžŃ. ĐŸĐŸĐșĐ°Đ·Đ°ĐœĐŸ, Ń‡Ń‚ĐŸ ĐșĐŸĐœŃ‚Đ°Đșт ĐČ ĐłĐŸĐ»ĐŸĐČĐșĐ” ŃƒŃŃ‚ĐŸĐčчоĐČ Đž ĐœĐ°ĐŽĐ”Đ¶Đ”Đœ, про Ń€Đ°ĐŽĐžĐ°Đ»ŃŒĐœĐŸĐŒ ĐșĐŸĐœŃ‚Đ°ĐșŃ‚ĐœĐŸĐŒ ĐČĐ·Đ°ĐžĐŒĐŸĐŽĐ”ĐčстĐČОО ĐČĐœŃƒŃ‚Ń€Đ”ĐœĐœĐ”ĐłĐŸ Đž ĐœĐ°Ń€ŃƒĐ¶ĐœĐŸĐłĐŸ ŃĐ»ĐŸĐ”ĐČ ÎŽâ‚‚= 1.9716 ĐŒĐŒ Đž ή₃= 1.3870 ĐŒĐŒ ŃĐŸĐŸŃ‚ĐČДтстĐČĐ”ĐœĐœĐŸ. Про Ń‚ĐŸĐ»Ń‰ĐžĐœĐ” ĐœĐžŃ‚Ń€ĐžĐŽĐœĐŸĐłĐŸ ŃĐ»ĐŸŃ 0,24 ĐŒĐŒ ŃŃ€ĐŸĐș ŃĐ»ŃƒĐ¶Đ±Ń‹ эĐșŃŃ‚Ń€ŃƒĐ·ĐžĐŸĐœĐœĐŸĐč ĐłĐŸĐ»ĐŸĐČĐșĐž ĐČ ĐżŃ€ĐŸĐžĐ·ĐČĐŸĐŽŃŃ‚ĐČĐ” ĐŽĐœĐžŃ‰ ĐżĐŸŃ€ŃˆĐœŃ ŃĐŸĐŸŃ‚ĐČДтстĐČŃƒĐ”Ń‚ 6357 ĐžĐ·ĐŽĐ”Đ»ĐžŃĐŒ

    Corrections to Hawking-like Radiation for a Friedmann-Robertson-Walker Universe

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    Recently, a Hamilton-Jacobi method beyond semiclassical approximation in black hole physics was developed by \emph{Banerjee} and \emph{Majhi}\cite{beyond0}. In this paper, we generalize their analysis of black holes to the case of Friedmann-Robertson-Walker (FRW) universe. It is shown that all the higher order quantum corrections in the single particle action are proportional to the usual semiclassical contribution. The corrections to the Hawking-like temperature and entropy of apparent horizon for FRW universe are also obtained. In the corrected entropy, the area law involves logarithmic area correction together with the standard inverse power of area term.Comment: 10 pages, no figures, comments are welcome; v2: references added and some typoes corrected, to appear in Euro.Phys.J.C; v3:a defect corrected. We thank Dr.Elias Vagenas for pointing out a defect of our pape

    The ARGO-YBJ Experiment Progresses and Future Extension

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    Gamma ray source detection above 30TeV is an encouraging approach for finding galactic cosmic ray origins. All sky survey for gamma ray sources using wide field of view detector is essential for population accumulation for various types of sources above 100GeV. To target the goals, the ARGO-YBJ experiment has been established. Significant progresses have been made in the experiment. A large air shower detector array in an area of 1km2 is proposed to boost the sensitivity. Hybrid detection with multi-techniques will allow a good discrimination between different types of primary particles, including photons and protons, thus enable an energy spectrum measurement for individual specie. Fluorescence light detector array will extend the spectrum measurement above 100PeV where the second knee is located. An energy scale determined by balloon experiments at 10TeV will be propagated to ultra high energy cosmic ray experiments

    High Altitude test of RPCs for the ARGO-YBJ experiment

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    A 50 m**2 RPC carpet was operated at the YangBaJing Cosmic Ray Laboratory (Tibet) located 4300 m a.s.l. The performance of RPCs in detecting Extensive Air Showers was studied. Efficiency and time resolution measurements at the pressure and temperature conditions typical of high mountain laboratories, are reported.Comment: 16 pages, 10 figures, submitted to Nucl. Instr. Met

    Quantifying atmospheric nitrogen deposition through a nationwide monitoring network across China

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    A Nationwide Nitrogen Deposition Monitoring Network (NNDMN) containing 43 monitoring sites was established in China to measure gaseous NH3, NO2, and HNO3 and particulate NH4+ and NO3− in air and/or precipitation from 2010 to 2014. Wet/bulk deposition fluxes of Nr species were collected by precipitation gauge method and measured by continuous-flow analyzer; dry deposition fluxes were estimated using airborne concentration measurements and inferential models. Our observations reveal large spatial variations of atmospheric Nr concentrations and dry and wet/bulk Nr deposition. On a national basis, the annual average concentrations (1.3–47.0 ÎŒg N m−3) and dry plus wet/bulk deposition fluxes (2.9–83.3 kg N ha−1 yr−1) of inorganic Nr species are ranked by land use as urban > rural > background sites and by regions as north China > southeast China > southwest China > northeast China > northwest China > Tibetan Plateau, reflecting the impact of anthropogenic Nr emission. Average dry and wet/bulk N deposition fluxes were 20.6 ± 11.2 (mean ± standard deviation) and 19.3 ± 9.2 kg N ha−1 yr−1 across China, with reduced N deposition dominating both dry and wet/bulk deposition. Our results suggest atmospheric dry N deposition is equally important to wet/bulk N deposition at the national scale. Therefore, both deposition forms should be included when considering the impacts of N deposition on environment and ecosystem health

    Measurement of the Atmospheric Muon Spectrum from 20 to 3000 GeV

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    The absolute muon flux between 20 GeV and 3000 GeV is measured with the L3 magnetic muon spectrometer for zenith angles ranging from 0 degree to 58 degree. Due to the large exposure of about 150 m2 sr d, and the excellent momentum resolution of the L3 muon chambers, a precision of 2.3 % at 150 GeV in the vertical direction is achieved. The ratio of positive to negative muons is studied between 20 GeV and 500 GeV, and the average vertical muon charge ratio is found to be 1.285 +- 0.003 (stat.) +- 0.019 (syst.).Comment: Total 32 pages, 9Figure

    ARGO-YBJ constraints on very high energy emission from GRBs

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    The ARGO-YBJ (Astrophysical Radiation Ground-based Observatory at YangBaJing) experiment is designed for very high energy Îł\gamma-astronomy and cosmic ray researches. Due to the full coverage of a large area (5600m25600 m^2) with resistive plate chambers at a very high altitude (4300 m a.s.l.), the ARGO-YBJ detector is used to search for transient phenomena, such as Gamma-ray bursts (GRBs). Because the ARGO-YBJ detector has a large field of view (∌\sim2 sr) and is operated with a high duty cycle (>>90%), it is well suited for GRB surveying and can be operated in searches for high energy GRBs following alarms set by satellite-borne observations at lower energies. In this paper, the sensitivity of the ARGO-YBJ detector for GRB detection is estimated. Upper limits to fluence with 99% confidence level for 26 GRBs inside the field of view from June 2006 to January 2009 are set in the two energy ranges 10−-100 GeV and 10 GeV−-1 TeV.Comment: accepted for publication in Astroparticle Physic
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