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Titlebook: Electron Holography; Akira Tonomura Book 1999Latest edition Springer-Verlag Berlin Heidelberg 1999 Aharanov-Bohm effect.Experiment.Hologra

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發(fā)表于 2025-3-25 03:46:25 | 只看該作者
22#
發(fā)表于 2025-3-25 08:13:41 | 只看該作者
High-Resolution Microscopy,e combination of concave and convex lenses in the electron case because of the lack of a concave electron lens, the resolution is determined by the aberrations of the objective lens and not by a fundamental limit of the electron wavelength. In fact, it was theoretically verified by . [8.1] that an a
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發(fā)表于 2025-3-25 14:32:08 | 只看該作者
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發(fā)表于 2025-3-25 18:37:38 | 只看該作者
Book 1999Latest editionible em- ploying other techniques. Full use is made of the extremely short wave- length of electrons, enabling electron holography to have a great impact on fields ranging from basic science to industrial applications. This book will provide an overview of the present state of electron holography fo
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發(fā)表于 2025-3-25 21:08:42 | 只看該作者
0342-4111 electrons, enabling electron holography to have a great impact on fields ranging from basic science to industrial applications. This book will provide an overview of the present state of electron holography fo978-3-642-08421-8978-3-540-37204-2Series ISSN 0342-4111 Series E-ISSN 1556-1534
26#
發(fā)表于 2025-3-26 00:21:16 | 只看該作者
https://doi.org/10.1007/978-3-540-37204-2Aharanov-Bohm effect; Experiment; Holography; electron holography; electron microscopy; electron optics; f
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發(fā)表于 2025-3-26 08:13:09 | 只看該作者
Der Funktionswandel der Wahrnehmung,tical image by illuminating the hologram with a laser beam. In this process, electron wave fronts are transformed into optical wave fronts. Images of microscopic objects and fields that are so small that they can be observed only by using an electron beam with an extremely short wavelength are enlar
28#
發(fā)表于 2025-3-26 12:02:56 | 只看該作者
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發(fā)表于 2025-3-26 16:37:06 | 只看該作者
https://doi.org/10.1007/978-981-13-3606-5vergent spherical wave from a point focus close to the object (Fig.4.1). This kind of hologram is a highly magnified projected interference pattern between the object and the transmitted waves. No lenses are necessary, but this method requires a very small electron point focus. The diameter of the f
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發(fā)表于 2025-3-26 20:38:04 | 只看該作者
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