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Titlebook: Meteorological Fluid Dynamics; Asymptotic Modelling Radyadour K. Zeytounian Book 1991 Springer-Verlag Berlin Heidelberg 1991 Navier-Stokes

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31#
發(fā)表于 2025-3-26 21:29:49 | 只看該作者
32#
發(fā)表于 2025-3-27 03:49:01 | 只看該作者
in a step-by-step manner in two directions under the microscope objective. This configuration allows to obtain important information about the objects in a non-invasive manner and, in the case of samples,on the stratigraphy and the composition of all layers. Three case studies are presented to disc
33#
發(fā)表于 2025-3-27 06:46:14 | 只看該作者
34#
發(fā)表于 2025-3-27 11:54:48 | 只看該作者
w energy elementary excitations in these materials and also for the characterization of their structural, electronic and vibronic properties. The primitive cell of high-.. superconductors is usually centrosymmetric and contains a large number of atoms. While this large number of atoms makes phonon s
35#
發(fā)表于 2025-3-27 14:06:55 | 只看該作者
36#
發(fā)表于 2025-3-27 21:27:22 | 只看該作者
rk doped and undoped La.R.MnO. (R = Ca, Sr) single crystals and thin films deposited on LaAlO. and NdGeO3 substrates are studied in polarized Raman scattering as functions of doping (0 < . < 1) and temperature (5 < . < 423K). Raman spectra of single crystals exhibit a significant dependence on the a
37#
發(fā)表于 2025-3-28 01:17:23 | 只看該作者
eposition and growth of different films, and the fabrication and filling of trenches generate local mechanical stresses. The magnitude of these stresses depends on the geometry of the films, on their chemical properties and thermal expansion coefficient, on the deposition temperature, etc. Because s
38#
發(fā)表于 2025-3-28 05:39:41 | 只看該作者
39#
發(fā)表于 2025-3-28 09:20:33 | 只看該作者
w energy elementary excitations in these materials and also for the characterization of their structural, electronic and vibronic properties. The primitive cell of high-.. superconductors is usually centrosymmetric and contains a large number of atoms. While this large number of atoms makes phonon s
40#
發(fā)表于 2025-3-28 12:05:25 | 只看該作者
eposition and growth of different films, and the fabrication and filling of trenches generate local mechanical stresses. The magnitude of these stresses depends on the geometry of the films, on their chemical properties and thermal expansion coefficient, on the deposition temperature, etc. Because s
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