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1)  taste profundity
审美深度
1.
The article puts forward opinions of Dufrenne concerning profundity from the development and switch of taste profundity in painting field,he opened out an issue of taste profundity mainly from indivisible connections of taste principal part and taste object,discussed taste profundity in reappearance art and representation art,and the function of taste principal part in it as wel
从绘画领域中审美深度的发展转换提出杜夫海纳关于审美深度的见解 ,他集中从审美主体与审美对象不可分割的关系中来揭示审美深度问题 ,探讨了再现性艺术和表现性艺术中的审美深度以及审美主体在其中的作
2)  Deep Aesthetics
深度审美
3)  the depth of review
审查深度
4)  aesthetic attitude
审美态度
1.
From the systematic theory point of view, we discuss the quality, the structure and the flow of the aesthetic attitude.
审美态度是一种既不同于实用态度又不同于科学态度的专为审美服务的特殊的心理态度,它是一种立体、动态和多层面的复合心理结构,由外及里分别是注意层、时空层和人格层。
2.
As a result of the highly development of science and technology, the democratization of politics, the decentralization of thoughts and culture, and the booming of market economy and cultural industry, people s aesthetic attitude changes in contemporary popular arts.
在当代社会,由于科技的高度发展、政治的民主化、思想文化的宽容和多元化及市场经济和文化工业的影响,导致了审美态度在当代大众艺术中发生了蜕变,这在艺术形式方面表现得尤其突出。
3.
The theory of the aesthetic attitude can be traced back to Plato, but Shaftesbury was the person who first used the word "Attitude".
在经典艺术中 ,艺术家和审美主体在从事审美活动时大都能保持一种不同于日常态度的审美态度。
5)  Latitude of aesthetics
审美纬度
6)  aesthetic measure
审美尺度
1.
The Study on aesthetic measure in the past years mainly focused on the aesthetic and artistic actions and drew conclusions far from the real aesthetic context.
既往的审美尺度研究,较多地将其局限于审美与艺术活动本身做架空推论,而与现实审美情境相去甚远。
2.
Therefore, while the ritual activities come to be the tradition with the propagating of ethnic group, aesthetic activities mingled with them also gradually develop into some kind of “convention” that could be regarded as objective aesthetic measure.
正因如此,当仪式活动随族群延续而作为一种传统固定下来之后,交融在仪式中的审美活动也因此获得某种“惯例”意味,而这似乎可以看成某种客观存在的审美尺度。
补充资料:BCS穿透深度(BCSpenetrationdepth)
BCS穿透深度(BCSpenetrationdepth)

对纯超导体,由BCS电流方程,在伦敦极限下(`\xi_0\lt\lt\lambda`或$l\lt\lt\xi_0$)的穿透深度与伦敦穿透深度λL(T)相符。对非纯超导体(含杂质),在伦敦极限下为

$\lambda(T)=\lambda_L(T)(1 \xi_0//l)^{1/2}$

一般地,λL(T)由经验公式表示其与温度T的关系(见“伦敦穿透深度”)。在皮帕德极限下($\xi_0\gt\gt\lambda$或$\xi_0\lt\ltl$),ξp=ξ0,则给出为

$\lambda(T)=\frac{8}{9}\lambda_L(T)[\frac{sqrt3\xi_0}{2\pi\lambda_L(T)}]^{1/3}$

说明:补充资料仅用于学习参考,请勿用于其它任何用途。
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