Titlebook: Intracranial Pressure VI; Proceedings of the S J. D. Miller,G. M. Teasdale,A. D. Mendelow Conference proceedings 1986 Springer-Verlag Berli

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叙述

A. Marmarou,A. L. Maset,J. D. Ward,R. J. Moulton,H. A. Lutz,G. L. Clifton,D. P. BeckerV deposits are introduced and discussed. Based on which, methods for tailoring of mechanical properties of EBWD products similar to Ti–6Al–4V alloy are proposed. Near the end of this chapter, new findings on fracture modes and deformation mechanism in tensile tests of EBWD Ti–6Al–4V are illustrated.

Processes

标准

R. Bullock,G. Blake,M. du Trevou,J. Favierocal spin fluctuations is taken into account by means of the functional-integral method combined with the alloy-analogy approximation [5–8]. We will discuss in this note the finite-temperature properties of ferromagnetic metals (Sec.2), of antiferromagnetic metals (Sec.3) and of concentrated ferroma

去掉

L. Rabow,A. A. F. DeSalles,M. Yang,A. Maset,H. Kontos,H. A. Lutz,J. D. Ward,R. Y. Moulton,G. L. ClifFMS) by a weak external magnetic field (6.2 K0e). This means that the energy difference between the HSDW and the ferromagnetic state (FMS) is much small. The IFMS is supposed to be a typical example of itinerant weak ferromagnetism on the basis of the following experimental facts: (i) The induced fe

murmur

T. Hashimoto,L. H. Pitts,L. Pogliani,H. M. BartkowskiFMS) by a weak external magnetic field (6.2 K0e). This means that the energy difference between the HSDW and the ferromagnetic state (FMS) is much small. The IFMS is supposed to be a typical example of itinerant weak ferromagnetism on the basis of the following experimental facts: (i) The induced fe

难管

D. I. Graham,A. E. Lawrence,J. H. Adams,D. Doyle,D. R. McLellanocal spin fluctuations is taken into account by means of the functional-integral method combined with the alloy-analogy approximation [5–8]. We will discuss in this note the finite-temperature properties of ferromagnetic metals (Sec.2), of antiferromagnetic metals (Sec.3) and of concentrated ferroma

决定性

e Carlo (DMC) method, one is directly concerned with the evolution in imaginary time of the wave function, which corresponds to a diffusion process in configuration space. In the Green Function Monte Carlo (GFMC) technique, on the other hand, a time-integrated form of the Green function or resolvent

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