TN242 2001020917采用调幅光波测量无源谐振腔的损耗=Determiningthe total loss of a passive resonant cavity byamplitude-modulated light[刊,中]/梁永辉(国防科技大学应用物理系.湖南,长沙(410073))//中国激光.—2000,27(5).-423-...TN242 2001020917采用调幅光波测量无源谐振腔的损耗=Determiningthe total loss of a passive resonant cavity byamplitude-modulated light[刊,中]/梁永辉(国防科技大学应用物理系.湖南,长沙(410073))//中国激光.—2000,27(5).-423-426讨论了一种在"小抖动"稳频条件下采用调幅光波测量无源谐振腔损耗的方法,并进行了深入的理论分析。图2参8(赵桂云)展开更多
In order to facilitate solution, a complex problem is normally decomposed into many small sub-problems during product development process. Teams are formed to resolve each sub-problem. The original problem is resolved...In order to facilitate solution, a complex problem is normally decomposed into many small sub-problems during product development process. Teams are formed to resolve each sub-problem. The original problem is resolved from solutions of sub-problems. Ideally, sub-problems are not only mutually independent but also inherent parameters of original problem. Solution of original problem can be directly derived from the collection of solutions from simplified sub-problems. In practice, the degree of interdependency is indeed reduced, sub-problems are neither totally independent nor all inherent parameters of original problem. This paper discusses team coordination under this condition and design solution from each team, which not only satisfies total requirements but also is an optimal one. The suggested optimized constraint decomposition method will insure workable Pareto solution.展开更多
Let M be a connected orientable compact irreducible 3-manifold. Suppose that αM consists of two homeomorphic surfaces F1 and F2, and both F1 and F2 are compressible in M. Suppose furthermore that g(M, F1) = g(M) + g(...Let M be a connected orientable compact irreducible 3-manifold. Suppose that αM consists of two homeomorphic surfaces F1 and F2, and both F1 and F2 are compressible in M. Suppose furthermore that g(M, F1) = g(M) + g(F1), where g(M, F1)is the Heegaard genus of M relative to F1. Let Mfbe the closed orientable 3-manifold obtained by identifying F1 and F2 using a homeomorphism f : F1 → F2. The authors show that if f is sufficiently complicated, then g(Mf) = g(M, αM) + 1.展开更多
文摘TN242 2001020917采用调幅光波测量无源谐振腔的损耗=Determiningthe total loss of a passive resonant cavity byamplitude-modulated light[刊,中]/梁永辉(国防科技大学应用物理系.湖南,长沙(410073))//中国激光.—2000,27(5).-423-426讨论了一种在"小抖动"稳频条件下采用调幅光波测量无源谐振腔损耗的方法,并进行了深入的理论分析。图2参8(赵桂云)
基金Supportedby 86 3/CIMS (No .2 0 0 1AA4 1114 0 )andtheNationalNaturalScienceFoundationofChina (No .6 0 10 4 0 0 8)
文摘In order to facilitate solution, a complex problem is normally decomposed into many small sub-problems during product development process. Teams are formed to resolve each sub-problem. The original problem is resolved from solutions of sub-problems. Ideally, sub-problems are not only mutually independent but also inherent parameters of original problem. Solution of original problem can be directly derived from the collection of solutions from simplified sub-problems. In practice, the degree of interdependency is indeed reduced, sub-problems are neither totally independent nor all inherent parameters of original problem. This paper discusses team coordination under this condition and design solution from each team, which not only satisfies total requirements but also is an optimal one. The suggested optimized constraint decomposition method will insure workable Pareto solution.
基金supported by the National Natural Science Foundation of China(No.11271058)The second author is supported by the National Natural Science Foundation of China(No.11171108)
文摘Let M be a connected orientable compact irreducible 3-manifold. Suppose that αM consists of two homeomorphic surfaces F1 and F2, and both F1 and F2 are compressible in M. Suppose furthermore that g(M, F1) = g(M) + g(F1), where g(M, F1)is the Heegaard genus of M relative to F1. Let Mfbe the closed orientable 3-manifold obtained by identifying F1 and F2 using a homeomorphism f : F1 → F2. The authors show that if f is sufficiently complicated, then g(Mf) = g(M, αM) + 1.
