过程系统管理与技术的综合集成

在激烈的市场竞争中，过程企业不仅要重视技术、更要加强管理，实现全局优化运行。提高过程企业的市场竞争能力必须全面综合集成人、组织、战略管理、经营管理、过程管理及信息自动化技术等因素。本文以石化企业为背景，对过程企业面临的问题及发展趋势进行了分析，并且对过程企业管理模式、过程企业的体系结构以及过程集成与优化技术进行了探讨。

我国制造业面临的内外形势及对策研究──抓住机遇,参加全球化敏捷生产体系

：本文从信息时代对人们认识上的影响，讨论了信息时代对生产、对统一的世界市场、对社会的影响。列举了世界经济进入新的繁荣期的特征。讨论了世界生产的形成和发展，市场竞争的三准则，市场竞争的各个历史阶段及全球化敏捷制造体系迅速发展的原因。分析了二十一世纪制造业面临的形势。详细地讨论了我国国有大中型企业的主要问题：1．产品问题；2．企业结构不合理；3．管理问题；4．质量问题；5．工艺手段和装备落后；6．历史包袱沉重等。提出了利用世界全球化生产体系发展的大好形势的三条对策：1．利用敏捷制造原理对企业进行重组；2．加速产品设计队伍的重建，增强新产品的设计能力；3．利用现代化手段实现现代化管理。

21世纪企业的主要模式──敏捷制造企业

２０世纪９０年代以后，由于科学技术的迅猛发展，知识─技术─产品的周期日益缩短，如何加速开发质优价廉的新产品就成为企业竞争的核心内容。２１世纪即将到来，世界无疑将沿着２０世纪的道路继续向前发展，它的趋势是：新产品开发速度日益加快、产品生命周期不断缩短、生产批量越来越小、市场竞争日趋激烈；加上环太平洋地区的兴起，有能力参与这场竞争的企业不断增多。这一切虽给企业带来了机遇，但也给企业造成了严酷的生存环境。为了适应这种环境，１９９１年美国在总结日本、德国和本国经验的基础上，提出把现有企业改造成敏捷制造企业（ＡｇｉｌｅＭａｎｕｆａｃｔｕｒｉｎｇＥｎｔｅｒｐｒｉｓｅ）的模式，并认为这是奠定美国２１世纪经济霸主地位的战略举措。敏捷制造企业是从客观经济发展的实践中总结出来的。我国如何改造企业并和世界经济接轨，敏捷制造企业给我们提出了值得高度重视的发展方向，本文对此作了较为详尽的论述。

Energy Dissipation In Fracture Of Bulk Metallic Glasses Via Inherent Competition Between Local Softening And Quasi-Cleavage

Compression, tension and high-velocity plate impact experiments were performed on a typical tough Zr41.2Ti13.8Cu10Ni12.5Be22.5 (Vit 1) bulk metallic glass (BMG) over a wide range of strain rates from similar to 10(-4) to 10(6) s(-1). Surprisingly, fine dimples and periodic corrugations on a nanoscale were also observed on dynamic mode I fracture surfaces of this tough Vit 1. Taking a broad overview of the fracture patterning of specimens, we proposed a criterion to assess whether the fracture of BMGs is essentially brittle or plastic. If the curvature radius of the crack tip is greater than the critical wavelength of meniscus instability [F. Spaepen, Acta Metall. 23 615 (1975); A.S. Argon and M. Salama, Mater. Sci. Eng. 23 219 (1976)], microscale vein patterns and nanoscale dimples appear on crack surfaces. However, in the opposite case, the local quasi-cleavage/separation through local atomic clusters with local softening in the background ahead of the crack tip dominates, producing nanoscale periodic corrugations. At the atomic cluster level, energy dissipation in fracture of BMGs is, therefore, determined by two competing elementary processes, viz. conventional shear transformation zones (STZs) and envisioned tension transformation zones (TTZs) ahead of the crack tip. Finally, the mechanism for the formation of nanoscale periodic corrugation is quantitatively discussed by applying the present energy dissipation mechanism.

Study of oscillatory behavior of recording process arising from electron-hole competition in strongly oxidized LiNbO3 : Ce : Cu

We have investigated ultraviolet (UV) photorefractive effect of lithium niobate doubly doped with Ce and Cu. It is found the diffraction efficiency shows oscillating behavior Under UV-1ight-recording. A model in which electrons and holes can be excited from impurity centers in the UV region is proposed to study the oscillatory behavior of the diffraction efficiency. Oil the basis of the material equations and the coupled-wave equations, we found that the oscillatory behavior is due to the oscillation of the relative spatial phase shift Phi. And the electron-hole competition may cause the oscillation of the relative spatial phase shift. A switch point from electron grating to hole grating is chosen to realize nonvolatile readout by a red light with high sensitivity (0.4 cm/J). (c) 2005 Elsevier GmbH. All rights reserved.

Mode competition in acousto-optically Q-switched planar waveguide lasers

Multi-mode rate equations have been developed to investigate mode competition in high-power acousto-optically Q-switched planar waveguide lasers. The mode competition arises from coupling effects and temporal losses in the transform between guided modes and free-space propagation. Pulse-to-pulse instability and temporal beam distortions are enlarged by mode competition when the laser works in the multi-mode regime. The influence of parasitic oscillation is also discussed. A Nd:YAG planar waveguide laser has been established with a folded hybrid/unstable resonator. A maximum average power of 83 W with a beam propagation factor M-x(2) x M-y(2) = 1.2 x 1.4 is obtained. The theoretical simulation agrees well with the experimental observation. (c) 2006 Elsevier Ltd. All rights reserved.