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     The results of the other papers[3], [4]are generalized to the transitive closure of a fuzzy max-product composition.
     把[3],[4]的结果推广到模糊最大—积传递闭包上来。
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     Transitive Closure of a Fuzzy Max-Product Composition
     模糊最大—积传递闭包
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     Influences of perturbations of training pattern pairs on max-product fuzzy associative memory
     训练模式的摄动对最大——乘积型模糊联想记忆网络的影响
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     In ATM networks, the traffic control of ABR service was only partly solved in ATM forum recommandation TM4.0. The rate based close loop control for ABR under max min fairness has improved the ABR traffic control in some cases.
     ATM网络中 ABR业务的流量控制是 ATM论坛的流量管理规范 (TM4.0 )中没有完全解决的问题 ,ABR基于速率的闭环控制方案在最大——最小准则下获得了一定进展。
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     Based on the drawbacks of the software quality evaluation methods at home and abroad, this paper proposes a new method called Fuzzy Logic theory, i.e. selecting software quality evaluation factors through engineering method, and determining the fuzzy sets of evaluation factors and scales, hence setting up Fuzzy relationships among them and a weight set of quality factors, computing the evaluation vector which represents the quality of the software by minimizing-maximizing compound calculating.
     在国内外对软件质量定量评价方法研究的不足之处的基础上,提出了运用模糊逻辑理论对软件质量进行定量评价的技术方法,即首先通过工程化方法筛选软件质量评价要素,并确定软件质量评价要素和质量评价等级模糊集,然后建立它们之间的模糊关系和质量要素权重集,经过最大——最小复合运算,计算出反映软件质量的评价向量值;
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     The Maximum Alternative-Flow
     并流
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     the maximum fight altitude;
     飞行高度 ;
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     The Maximum Size of F-graphs
     F图的边数
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     Control is the Most Serious Misunderstanding of Management
     管理的误区“管”
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  max-
The minimization of nonconvex, nondifferentiable functions that are compositions of max-type functions formed by nondifferentiable convex functions is discussed in this paper.
      
A successive quadratic programming algorithm for SDP relaxation of Max-Bisection
      
A successive quadratic programming algorithm for solving SDP relaxation of Max-Bisection is provided and its convergence result is given.
      
Solution of Fuzzy Equations with Max-Product Composition in Inverse Control and Decision Making Problems
      
A system of "max-product" type of equations, to which many inverse problems of fuzzy sets and relations, is solved.
      
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The effect of pressure on photographic sensitivity is discussed on the experimental basis that the quantity E/EC, where E is the illumination actually used when the photographic emulsion is under pressure, and Ee the illumination which would be required to produce the same optical density when the emulsion is under no pressure, is a function of pressure only and that for pressures greater than a certain value, E/Ee becomes a linear function of the pressure.

当照相时,照相片子——映像纸,软片,或玻璃板——被压,则其感光性减弱,是为照相的压力效应。设E为照相片子在压力P下得光密度d所需之光照度,若片子不受压力则用光照度E_e即可得此同一之光密度d,故E_e可称在压力P下E之有效照度。吾人实验证明E/E_e为压力P之函数,当p>200kg/cm~2时,E/E_e与P成正比例。 此照相的压力效应,与照相时所用光之颜色,极有关系。黄色光较绿色光为显,绿色光较蓝色光紫色光为显至紫外光则几无此效应。 又此效应之大小,随各种照相片子而不同。就我们所研究的蔡爱斯伊康正色软片,伊司门人像软片,和矮克发等色软片而论,以第一种为最大第二种次之第三种为最小。 这个效应,在实际上,或可有些应用。

The beta-ray spectrum of RaE was investigated by the cloud chamber experiments. About 600 tracks with H σ above 2000 were obtained. The spectrum was found to have an end point at 7500 Hσ. The average energy per disintegration was estimated to be 4.01×105 electron-volts.

戊种镭原质(Ra E)所放出之β线穿过威尔圣成云箱之径迹(tracks),用照相机照下。因成云箱在磁场中,而磁力之方向又与β线所取之途径垂直,故由照片上所量出径迹之半径,ρ,可定β线之能力,盖磁场之强度,H,亦已知也。通常以Hρ代表能力大小之相当值。用戊种镭原质所摄之照片上量出10Oβ线径迹,其Hρ值皆在2000高斯-厘米(Gauss-cm.)以上。以各种Hρ值及在该值范围内所有径迹之数目作一曲线。将该曲线延长至与Hρ轴相交,其交点7500高斯——厘米,即为β线具有最大能力者之Hρ值。由β线能力大小之分配,用绘图方法得计算该线之平均能力,其值为4.01×10~5电子——伏特(electron—volts)。

An attempt to observe the spectrum of doubly excited helium by excitation by electron impact, with energies between 500-600 electron volts, is made without success. This and other failures are discussed by considering of the life times of the doubly excited states. An approximate calculation gives for 2s3s3S a life time of the order 10-15 sec, corresponding to a natural width of the level of the order 1000 cm-1. While this accounts for the absence of a line spectrum of doubly excited helium, it renders the former...

An attempt to observe the spectrum of doubly excited helium by excitation by electron impact, with energies between 500-600 electron volts, is made without success. This and other failures are discussed by considering of the life times of the doubly excited states. An approximate calculation gives for 2s3s3S a life time of the order 10-15 sec, corresponding to a natural width of the level of the order 1000 cm-1. While this accounts for the absence of a line spectrum of doubly excited helium, it renders the former suggestion that the corona lines may be due to it untenable.

(1)日晕光谱线之来源,至今为未决定之问题。Goudsmit与吴大猷曾假设诸谱线乃由氦气双激起原子所生。过去有人企图用实验方法得到双激起氦原子之光谱,未能成功。但有数种实验室内现象,均有人用此假设以解释之。故作者希望在适当情形下得到双激起氦原子之光谱。 (2)由理论上知用电子撞击法造成双激起之可能性甚小,但此可能性之最大值在电子能为300至600electron volts时故作者企图在人为的此种情形下观察双激起氦原子光谱,但结果未能发现。 (3)此种实验结果可从理论方面予以解释。作者由双激起2s3s~3S状态之计算,知其谱线之宽约为1000cm~(-1),故实验时不能观察因此以前关於日晕光谱之解释,亦成疑问。

 
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