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61.
The first object of this paper is to introduce a new evolution equation for the characteristic function of the boundary Γ
of a Lipschitzian domain Ω in the N-dimensional Euclidean space under the influence of a smooth time-dependent velocity field. The originality of this equation is that the evolution takes place in an Lp-space with respect to the (N − 1)-Hausdorff measure. A second more speculative objective is to discuss how that equation can be relaxed to rougher velocity
fields via some weak formulation. A candidate is presented and some of the technical difficulties and open issues are discussed.
Continuity results in several metric topologies are also presented. The paper also specializes the results on the evolution
of the oriented distance function to initial sets with zero N-dimensional Lebesgue measure. 相似文献
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63.
Philippe Boyer Gilles Renversez Evgeny Popov Michel Nevière 《Optical and Quantum Electronics》2006,38(1-3):217-230
The present work adapts a recent grating theory called “Fast Fourier factorization” to cylindrical coordinates in order to study microstructured optical fibers (MOFs). Compared with the classical differential method, this new differential method takes into account the truncation of Fourier series and the discontinuities of the fields across the diffracting surface with the help of new factorization rules. The main advantage of this method is that the directrix of the diffracting cylindrical surface is arbitrary and permits anisotropic and inhomogeneous media although its numerical application needs longer computation time, compared with other well-known numerical methods. The S-propagation algorithm is used to avoid numerical contaminations. The numerical results are validated and compared with the well-established Multipole method in the case of a MOF with six circular cylinders. Further, a new cross-sectional profile (with sectorial inclusions) that the Multipole method cannot consider is studied. 相似文献
64.
Michel Talagrand 《Probability Theory and Related Fields》2006,134(3):339-382
We compute at any temperature the free energy of the multi p-spin spherical model when only terms for p even are considered.
Work partially supported by an NSF grant 相似文献
65.
S. Mathias M. Wessendorf S. Passlack M. Aeschlimann M. Bauer 《Applied Physics A: Materials Science & Processing》2006,82(3):439-445
Epitaxial ultra-thin Ag films grown on Cu(111) have been investigated by angle-resolved photoemission spectroscopy. The thickness
dependence of the binding energy for the Shockley surface state at 300 K could be determined accurately in films up to 5 ML
thick. Furthermore, we observe drastic changes in the film morphology after annealing to 450 K. Spectral modifications in
the shape of the quantum-well states (QWS), characteristic for these ultra-thin silver films, prove that the surface morphology
is homogeneous. The photoemission spectra also indicate that the silver film bifurcates to form a film exhibiting two distinct
film thicknesses. For all levels of silver coverage, we identify surface regions that are 2 ML thick, while the thickness
of the remaining surface depends on the amount of deposited silver. The almost purely Lorentzian line-shape of the spectral
features corresponding to the two different surface regions show that both surface areas are atomically flat.
PACS 68.55.Jk; 73.20.At; 73.21.Fg; 79.60.Dp 相似文献
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69.
D. Bisello G. Busetto A. Castro M. Nigro M. Penzo L. Pescara M. Posocco P. Sartori L. Stanco Z. Ajaltouni A. Falvard J. Jousset B. Michel J. C. Montret A. Antonelli R. Baldini A. Calcaterra G. Capon M. Schioppa J. -E. Augustin G. Cosme F. Couchot B. Dudelzak F. Fulda G. Grosdidier B. Jean-Marie S. Jullian D. Lalanne V. Lepeltier F. Manè C. Paulot R. Riskalla Ph. Roy G. Szklarz DM Collaboration 《Zeitschrift fur Physik C Particles and Fields》1988,39(1):13-19
Thee + e ?→K + K ? cross section has been measured from about 750 events in the energy interval \(1350 \leqq \sqrt s \leqq 2400 MeV\) with the DM2 detector at DCI. TheK ± form factor |F F ±| cannot be explained by the ρ, ω, ? and ρ′(1600). An additional resonant amplitude at 1650 MeV has to be added as suggested by a previous experiment. 相似文献
70.