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唯识学在中国的初期发展
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作者 卢中道 《佛学研究》 1999年第0期315-321,共7页
唯识学在中国的传播、发展,可以分为两个时期。第一个时期为南北朝、隋及唐初,主要是北方的地论学和南方的摄论学;第二个时期为唐贞观十九年以后,玄奘从印度回来,系统地翻译了唯识学的经典以及唯识宗的形成。这两个时期的唯识学,... 唯识学在中国的传播、发展,可以分为两个时期。第一个时期为南北朝、隋及唐初,主要是北方的地论学和南方的摄论学;第二个时期为唐贞观十九年以后,玄奘从印度回来,系统地翻译了唯识学的经典以及唯识宗的形成。这两个时期的唯识学,既有前后的继承性,又存在着诸多的不同之处,要系统地了解唯识学在中国的发展历史,那么对于地论学、摄论学的历史考察,就显得非常必要。 展开更多
关键词 唯识 地论 摄论学
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Perturbation Theory for Open Two-Level Nonlinear Quantum Systems
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作者 张志杰 姜东光 王伟 《Communications in Theoretical Physics》 SCIE CAS CSCD 2011年第7期67-70,共4页
Perturbation theory is an important tool in quantum mechanics. In this paper, we extend the traditional perturbation theory to open nonlinear two-level systems, treating decoherence parameter γ as a perturbation. By ... Perturbation theory is an important tool in quantum mechanics. In this paper, we extend the traditional perturbation theory to open nonlinear two-level systems, treating decoherence parameter γ as a perturbation. By this virtue, we give a perturbative solution to the master equation, which describes a nonlinear open quantum system. The results show that for small decoherence rate γ the ratio of the nonlinear rate C to the tunneling coefficient V (i.e., r = O/V) determines the validity of the perturbation theory. For small ratio r, the perturbation theory is valid, otherwise it yields wrong results. 展开更多
关键词 perturbation theory DECOHERENCE nonlinear system
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Masses and Widths of Light Scalar Mesons in Chiral Perturbation Theory
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作者 CHEN Xiao-Zhao LI Xiao-Ya LU Xiao-Fu 《Communications in Theoretical Physics》 SCIE CAS CSCD 2008年第2期451-455,共5页
Based on the diquark model, we assume that the light scalar mesons are q^2q^-2 states rather than qq^-. The chiral effective Lagrangian for the light scalar meson is constructed, and the mass relations are obtained: ... Based on the diquark model, we assume that the light scalar mesons are q^2q^-2 states rather than qq^-. The chiral effective Lagrangian for the light scalar meson is constructed, and the mass relations are obtained: the isotriplet (a0) and the isosinglet (f0) are the heaviest and are degenerate, the isodoublets (κ) are heavier and the other isosinglet (σ) is the lightest; and 2Mκ^2 = Mα0^2+ Mσ^2. Using experimental value for a0 and σ mass, we obtain Mκ=794 MeV, which is consistent with the experimental value. Then taking Г(a0^0 →ηπ^0) = 90 MeV and Г(f0→π^0π^0) = 20 MeV, we get the width of σ is: Г(σ0→π^+π^-)= 150 MeV. 展开更多
关键词 scalar meson honer diquark model chiral perturbation theory
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Mixed Quark-Gluon Condensate Beyond Chiral Limit
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作者 卢常芳 吕晓夫 《Communications in Theoretical Physics》 SCIE CAS CSCD 2010年第5期893-897,共5页
Using the Dyson-Schwinger equation and perturbation theory, we calculate the mixed quark-gluon condensates in the chiral limit and in the case of nonzero quark current mass for the light quark u/d and strange quark s.... Using the Dyson-Schwinger equation and perturbation theory, we calculate the mixed quark-gluon condensates in the chiral limit and in the case of nonzero quark current mass for the light quark u/d and strange quark s. The results show that the mixed quark-gluon condensate will decrease when the quark mass increases. For the quark with zero mass, we obtain mo2 = g(qσuvGuvq)/(qq) 0.68 GeV2, which is in good agreement with the QCD sum rules estimate mo2=(0.8± 0.2) GeV2. 展开更多
关键词 quark current mass mixed quark-gluon condensates QCD sum rule Schwinger Dyson equation Feynman rules
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