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Titlebook: Electron Correlation and Magnetism in Narrow-Band Systems; Proceedings of the T T?ru Moriya Conference proceedings 1981 Springer-Verlag Ber

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書(shū)目名稱(chēng)Electron Correlation and Magnetism in Narrow-Band Systems
副標(biāo)題Proceedings of the T
編輯T?ru Moriya
視頻videohttp://file.papertrans.cn/307/306086/306086.mp4
叢書(shū)名稱(chēng)Springer Series in Solid-State Sciences
圖書(shū)封面Titlebook: Electron Correlation and Magnetism in Narrow-Band Systems; Proceedings of the T T?ru Moriya Conference proceedings 1981 Springer-Verlag Ber
描述Speech by Toyosaburo Taniguchi Welcome my friends to the Third International Symposium, Division on the Theory of Condensed Matter, of the Taniguchi Foundation. The need is now greater than ever for Japan to consider how to strengthen and foster international understanding between nations, peoples and societies, and how to contribute towards the establishment of peace and prosperity in the world. For more than twenty years, I have been supporting a symposium on mathe- matics in which distinguished scholars from allover the world have engaged in free discussions. In this symposium, all the participants live together in community style. I have heard from members of some of these study groups that this type of setup has helped to strengthen their ties and relationships with their colleagues on a personal basis. What developed in the mathematics group led me to reorganize and strengthen the Taniguchi Foundation only a few years ago through additional funding. In order to effectively translate the objectives of the Foundation into action with the funds available, it becomes necessary to select those fields which are not necessarily in the limelight of popular interest, which means those
出版日期Conference proceedings 1981
關(guān)鍵詞Ferromagnetismus; condensed matter; magnetism; übergangselement; übergangselementverbindung
版次1
doihttps://doi.org/10.1007/978-3-642-81639-0
isbn_softcover978-3-642-81641-3
isbn_ebook978-3-642-81639-0Series ISSN 0171-1873 Series E-ISSN 2197-4179
issn_series 0171-1873
copyrightSpringer-Verlag Berlin Heidelberg 1981
The information of publication is updating

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Effective Spin Fluctuation Energies: How Should They Be Calculated? What Do They Mean?igh, the probability of the configuration appearing thermally is small, so finding the energy is the first step in understanding which are the most important configurations. Some of the questions which arise in the course of this computation are numerical in nature, and some conceptual. The numerica
板凳
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Functional Integral Representations in Spin Fluctuation Theory: Is There a Right One?ust in the present application, would include EVENSON, WANG, and SCHRIEFFER [36]., CYROT [37], MURATA and DONIACH [38], HERTZ and KLENIN [39], MORIYA and coworkers [40], HASEGAWA [23], HUBBARD [22], and KORENMAN and PRANGE [7]. There are, however, important mathematical problems which are encountere
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Spin Fluctuations and a Unified Picture of Magnetisme the modern theoretical research of magnetism has started with the advent of quantum mechanics. As is well known, in the major part of the modern theory of solids the mean-field approximation or the one-electron picture has been extremely successful. While in the problem of magnetism, especially at
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Ferromagnetism in Iron and Nickel1], and based on the concept of . (SRMO). Most of the material in this talk has been published in a series of papers and conference reports [2–13]. Some of the unpublished work will be discussed in shorter talks.
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Functional Integral Approach to the Low-Temperature Properties of Itinerant Ferromagnetseatments employ static or classical approximation. From the sense of this approximation, applicability of these theories ought to be restricted to the high-temperature properties. Therefore in order to give more adequate descriptions, in particular, when we discuss the ordered phase, we must be face
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Calculation of the Magnetic Properties of Iron and Nickel by the Functional Integral Method effort is made to discuss the technical difficulties and developments and to compare alternative approaches. The strength of the method is that it provides a mathematical formalism to describe a physical model discussed in section 2. The method is formulated in section 3 and an inherent ambiguity i
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