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Titlebook: Electronic States and Optical Transitions in Semiconductor Heterostructures; Fedor T. Vasko,Alex V. Kuznetsov Textbook 1999 Springer Scien

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發(fā)表于 2025-3-21 17:03:09 | 只看該作者 |倒序瀏覽 |閱讀模式
書目名稱Electronic States and Optical Transitions in Semiconductor Heterostructures
編輯Fedor T. Vasko,Alex V. Kuznetsov
視頻videohttp://file.papertrans.cn/307/306403/306403.mp4
概述Provides the theoretical basis and experimental knowledge underlying the electronic and optical properties of heterostructuresan area crucial to modern semiconductor design * Describes the electronic
叢書名稱Graduate Texts in Contemporary Physics
圖書封面Titlebook: Electronic States and Optical Transitions in Semiconductor Heterostructures;  Fedor T. Vasko,Alex V. Kuznetsov Textbook 1999 Springer Scien
描述The study of semiconductor heterostructures started more than forty years ago. In the 1980s this area of research moved to the forefront of semiconduc- tor physics, largely due to progress in growth technologies which are now capable of producing ultrathin layers (up to a few monolayers) of different semiconductor materials. The availability of structures with nearly ideal, well-controlled properties has made semiconductor heterostructures a test- ing ground for solid-state physics. These structures have had a profound impact on basic research in semiconductor physics by opening new possibil- ities for studying low-dimensional electrons, as well as the atomic and elec- tronic properties of interfaces. Semiconductor heterostructures have also a variety of important practical applications: they provide a material basis for a number of novel devices, and also open the way for improving the operating characteristics of traditional micro- and optoelectronic compo- nents. As a result of the growing importance of heterostructure physics, more and more people are entering this dynamic field, either from graduate school or from other areas of research. For the new entrants, the task of fami
出版日期Textbook 1999
關鍵詞Exciton; electromagnetic wave; electronic structure; optical properties; optics; quantum wells; semiconduc
版次1
doihttps://doi.org/10.1007/978-1-4612-0535-7
isbn_softcover978-1-4612-6807-9
isbn_ebook978-1-4612-0535-7Series ISSN 0938-037X
issn_series 0938-037X
copyrightSpringer Science+Business Media New York 1999
The information of publication is updating

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V.V. Panasyuk,V.I. Marukha,V.P. Sylovanyukation, which in the second step transforms into a real excitation with energy ?(ω. - ω.) and emits a scattered photon with energy ?ω.. In contrast to that, interband absorption and luminescence considered in previous chapters probe only real electronic excitations, and energy is conserved in all individual acts of absorption or emission.
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Ultrafast Processes in Heterostructures,-time dynamics of condensed matter systems, the interest in these time-resolved studies is driven by the rapidly increasing speed of the operation of micro- and optoelectronic devices, which makes the understanding of the ultrafast dynamics of heterostructures a matter of considerable practical importance.
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Heterostructure-Based Optoelectronic Devices, components, such as consumer electronics, display technology, lighting, and optical data storage. The understanding of the physics of optical transitions in heterostructures is the basis for selecting the appropriate material system and the geometry of the structure that leads to desired operating parameters for a specific application.
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Interband Optical Transitions in Heterostructures,ency of interband transitions can in fact lie in the mid-infrared. The transitions between quantum confined states originating from the same band (intraband transitions) usually correspond to lower photon energies and will be treated separately in Chapter 8.
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Scattering of Light on Low-Dimensional Electrons,ation, which in the second step transforms into a real excitation with energy ?(ω. - ω.) and emits a scattered photon with energy ?ω.. In contrast to that, interband absorption and luminescence considered in previous chapters probe only real electronic excitations, and energy is conserved in all individual acts of absorption or emission.
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