排序方式: 共有63条查询结果,搜索用时 46 毫秒
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Savajols H Korichi A Ward D Appelbe D Ball GC Beausang C Beck FA Byrski T Curien D Dagnall P de France G Disdier D Duchêne G Erturk S Finck C Flibotte S Gall B Galindo-Uribarri A Haas B Hackman G Janzen VP Kharraja B Lisle JC Merdinger JC Mullins SM Pilotte S Prévost D Radford DC Rauch V Rigollet C Smalley D Smith MB Stezowski O Styczen J Theisen C Twin PJ Vivien JP Waddington JC Zuber K Ragnarsson I 《Physical review letters》1996,76(24):4480-4483
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Becker-Szendy R Bratton CB Cady DR Casper D Claus R Crouch M Dye ST Gajewski W Goldhaber M Haines TJ Halverson PG Jones TW Kielczewska D Kropp WR Learned JG LoSecco JM McGrew C Matsuno S Mudan MS Price L Reines F Schultz J Sinclair D Sobel HW Stone JL Sulak LR Svoboda R Thornton G van der Velde JC 《Physical review D: Particles and fields》1990,42(9):2974-2976
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α-Haloketones and -dibromides are converted to the corresponding ketones and alkenes respectively with nickel boride generated from sodium borohydride and nickel chloride. 相似文献
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In this paper the exact solution of the non-symmetric matrixRiccati equation with analytic coefficients is approximatedby a rational matrix function with a prefixed accuracy. Thisrational matrix function is locally defined as the exact solutionof a Riccati problem with matrix polynomial coefficients obtainedby truncation of the Taylor expansions of the matrix coefficientsof the original problem. 相似文献
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Casper D Becker-Szendy R Bratton CB Cady DR Claus R Dye ST Gajewski W Goldhaber M Haines TJ Halverson PG Jones TW Kielczewska D Kropp WR Learned JG LoSecco JM McGrew C Matsuno S Matthews J Mudan MS Price L Reines F Schultz J Sinclair D Sobel HW Stone JL Sulak LR Svoboda R Thornton G van der Velde JC 《Physical review letters》1991,66(20):2561-2564
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This paper presents a numerical method for solving the two‐dimensional unsteady incompressible Navier–Stokes equations in a vorticity–velocity formulation. The method is applicable for simulating the nonlinear wave interaction in a two‐dimensional boundary layer flow. It is based on combined compact difference schemes of up to 12th order for discretization of the spatial derivatives on equidistant grids and a fourth‐order five‐ to six‐alternating‐stage Runge–Kutta method for temporal integration. The spatial and temporal schemes are optimized together for the first derivative in a downstream direction to achieve a better spectral resolution. In this method, the dispersion and dissipation errors have been minimized to simulate physical waves accurately. At the same time, the schemes can efficiently suppress numerical grid‐mesh oscillations. The results of test calculations on coarse grids are in good agreement with the linear stability theory and comparable with other works. The accuracy and the efficiency of the current code indicate its potential to be extended to three‐dimensional cases in which full boundary layer transition happens. Copyright © 2011 John Wiley & Sons, Ltd. 相似文献
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J.C. Bacelar R. Chapman J.R. Leslie J.C. Lisle J.N. Mo E. Paul A. Simcock J.C. Willmott J.D. Garrett G.B. Hagemann B. Herskind A. Holm P.M. Walker 《Nuclear Physics A》1985,442(3):547-577
High-spin data are presented for 170Ta and 171Ta for the first time, and the known level scheme of 173Ta is extended to higher spins. Anomalies found in the crossing frequencies for the alignment of a pair of neutrons are considered. At high spin a large and constant value of J(2), with J(2) > J(1), is found for two 171Ta bands and the implications of this are discussed. The πi13/2 [660]1/2+, α = + 1/2 orbital is identified as it crosses the rotational band built on the [402]5/2+, α = + 1/2 orbital in 171Ta. Magnetic transition probabilities obtained from measured branching ratios show the effects of the aligning pair of neutrons and the spectator orbital. The data are interpreted using cranked shell-model calculations and a semiclassical vector-coupling scheme developed by Donau and Frauendorf. 相似文献