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Einführung in die Halbleitertheorie最新文献

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§ 7. Die Näherung stark gebundener Elektronen §7 .绑得很紧的电子的距离
Einführung in die Halbleitertheorie Pub Date : 1964-12-31 DOI: 10.1515/9783112525388-025
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引用次数: 0
§ 5. Der Begriff des positiven Defektelektrons des fast gefällten Valenzbandes §5 .关于几乎被破译的valenzi上的正缺陷电子
Einführung in die Halbleitertheorie Pub Date : 1964-12-31 DOI: 10.1515/9783112525388-023
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引用次数: 0
§ 2. Beispiele konkreter Kristallstrukturen
Einführung in die Halbleitertheorie Pub Date : 1964-12-31 DOI: 10.1515/9783112525388-004
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引用次数: 0
§ 1. Einführung § 1 导言
Einführung in die Halbleitertheorie Pub Date : 1964-12-31 DOI: 10.1515/9783112525388-046
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引用次数: 0
§ 2. Die Bestimmung der Nichtgleichgewichtsverteilungsfunktion der Leitfähigkeitselektronen im Falle sphärischer Form der Flächen konstanter Energie. Elektrische Leitfähigkeit atomarer nichtentarteter Halbleiter §2 .用于确定某些地区的球形能量的非均衡分配功能。原子无序半导体
Einführung in die Halbleitertheorie Pub Date : 1964-12-31 DOI: 10.1515/9783112525388-047
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引用次数: 0
§ 4. Magnetische Eigenschaften der Stoffe. Der Paramagnetismus der Gase und der Leitungselektronen in Metallen und Halbleitern §4 .各种物质的磁性而且，气体，自制电子，而且半导体
Einführung in die Halbleitertheorie Pub Date : 1964-12-31 DOI: 10.1515/9783112525388-034
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引用次数: 0
§ 8. Die Struktur der Energiebänder für eine Reihe konkreter Halbleiter §8 .为一组特定的半导体输送带的结构
Einführung in die Halbleitertheorie Pub Date : 1964-12-31 DOI: 10.1515/9783112525388-026
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引用次数: 0
§ 1. Transporterscheinungen und BOLTZMANN-Gleichung §1 .传送图和波兹曼公式
Einführung in die Halbleitertheorie Pub Date : 1964-12-31 DOI: 10.1515/9783112525388-039
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引用次数: 0
§ 6. Transporterscheinungen in nichtentarteten Halbleitern mit einfacher Bänderstruktur bei verschiedenen Streumechanismen §6 .而且，如果你半导体做了一套廉价半导体
Einführung in die Halbleitertheorie Pub Date : 1964-12-31 DOI: 10.1515/9783112525388-051
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引用次数: 0
§ 4. Relaxationszeit der Leitungselektronen im atomaren Halbleiter und im Metall §4 .原子中间导体和金属的电路休息时间
Einführung in die Halbleitertheorie Pub Date : 1964-12-31 DOI: 10.1515/9783112525388-042
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引用次数: 0
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