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Titlebook: Many-Particle Physics; Gerald D. Mahan Book 2000Latest edition Springer Science+Business Media New York 2000 Boson.Particle Physics.Potent

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发表于 2025-3-21 16:54:34 | 显示全部楼层 |阅读模式
书目名称Many-Particle Physics
编辑Gerald D. Mahan
视频videohttp://file.papertrans.cn/624/623695/623695.mp4
概述Includes supplementary material:
丛书名称Physics of Solids and Liquids
图书封面Titlebook: Many-Particle Physics;  Gerald D. Mahan Book 2000Latest edition Springer Science+Business Media New York 2000 Boson.Particle Physics.Potent
描述The first, second, and third editions of this book seem to occur at ten year intervals. The intent is to keep the book up-to-date. Many-body theory is a field which continually evolves in time. Journals only publish new results, conferences only invite speakers to report new phenomena, and agencies only fund scientists to do new physics. Today‘s physics is old hat by tomorrow. Students want to learn new material, and textbooks must be modified to keep up with the times. The early chapters in this book teach the techniques of many-body theory. They are largely unchanged in format. The later chapters apply the techniques to specific problems. The third edition increases the number of applications. New sections have been added, while old sections have been modified to include recent applications. The previous editions were set in type using pre-computer technology. No computer file existed of the prior editions. The publisher scanned the second edition and gave me a disk with the contents. This scan recorded the words accurately and scrambled the equations into unintelligible form. So I retyped the equations using LaTeX. Although tedious, it allowed me to correct the infinite numbers
出版日期Book 2000Latest edition
关键词Boson; Particle Physics; Potential; Theoretical physics; quantum dot
版次3
doihttps://doi.org/10.1007/978-1-4757-5714-9
isbn_softcover978-1-4419-3339-3
isbn_ebook978-1-4757-5714-9
copyrightSpringer Science+Business Media New York 2000
The information of publication is updating

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发表于 2025-3-21 20:29:50 | 显示全部楼层
,Green’s Functions at Zero Temperature,ugh they are often at low temperature. Many quantities are not very sensitive to temperature, particularly at low temperature. Zero temperature calculations are useful even for describing real systems. Furthermore, the zero temperature property of a system is an important conceptual quantity—the gro
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Nonzero Temperatures,should be done at nonzero temperatures too. It is often unnecessary if the temperature is small compared to other energies in the problem. But often temperature is important, and here it will be incorporated into Green’s functions. The nonzero temperature formalism was originated by Matsubara (1955)
发表于 2025-3-22 08:17:15 | 显示全部楼层
Homogeneous Electron Gas,ds were applied to a variety of problems, some areas of work were more successful than others. The two areas which enjoyed early success were the homogeneous electron gas and the polaron problem. Later there were other successes such as the theories of superconductivity and superfluidity. However, t
发表于 2025-3-22 11:44:48 | 显示全部楼层
Strong Correlations,d be calculated simply and accurately. The present chapter discusses other metallic systems in which correlation plays a much larger role in the dynamics of the electron. These topics come under the title of .. Strong correlation causes itinerant magnetism.
发表于 2025-3-22 14:37:49 | 显示全部楼层
,Electron—Phonon Interaction,derived in Chapter 1, with the form of the interaction given in Sec. 1.3.5. The LO phonons are usually represented by an Einstein model, i.e., the phonon frequency ω. = ω. is taken to be a constant. Since there is a single electron, the Hamiltonian may also be written as .where . and . are the conju
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Optical Properties of Solids,ron system does not absorb light at all, so that its optical properties are uninteresting. The ability of the nearly free-particle system to absorb light is due to its imperfections or deviations from homogeneity. If these effects are small, then so is the light absorption. This situation is describ
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Superfluids,e. Each has unusual properties and displays collective behavior of a unique character. The boson liquid .He shows a phase transition at .. = 2.172 K to a superfluid state which is similar to Bose—Einstein condensation, although vastly modified by the strong interparticle interactions Similarly, the
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