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    • 1. 发明专利
    • Method and apparatus for evaluating semiconductor device
    • 用于评估半导体器件的方法和装置
    • JP2006100780A
    • 2006-04-13
    • JP2005161639
    • 2005-06-01
    • Matsushita Electric Ind Co Ltd松下電器産業株式会社
    • OKADA KENJI
    • H01L21/66H01L21/822H01L27/04
    • PROBLEM TO BE SOLVED: To provide a method and apparatus which enable the evaluation of the thickness of the lower insulating film easily and preciously in semiconductor devices using a laminated insulating film formed by a laminate of two or more insulating films as a gate insulating film. SOLUTION: Gate voltage sweep takes place on a semiconductor device with a laminated insulating film for which the thickness of the lower insulating film is to be measured (step S11). A low voltage peak current mode is found from the current-voltage characteristic obtained by this sweep to determine the peak voltage and peak current (step S12). Then, the thickness of the lower insulating film is obtained from the correlation between the determined and predetermined peak voltages and the lower insulating film thickness (step S13). COPYRIGHT: (C)2006,JPO&NCIPI
    • 要解决的问题:提供一种方法和装置,其能够使用由两个或更多个绝缘膜的叠层形成的层叠绝缘膜作为栅极,在半导体器件中容易且珍贵地评估下绝缘膜的厚度 绝缘膜。 解决方案:在具有要测量下绝缘膜的厚度的层压绝缘膜的半导体器件上进行栅极电压扫描(步骤S11)。 从通过该扫描获得的电流 - 电压特性可以发现低电压峰值电流模式,以确定峰值电压和峰值电流(步骤S12)。 然后,根据确定的和预定的峰值电压之间的相关性和较低的绝缘膜厚度获得下部绝缘膜的厚度(步骤S13)。 版权所有(C)2006,JPO&NCIPI
    • 3. 发明专利
    • RESONANCE TUNNEL CONSTRUCTION AND MANUFACTURE OF IT
    • JPH07153934A
    • 1995-06-16
    • JP29928093
    • 1993-11-30
    • MATSUSHITA ELECTRIC IND CO LTD
    • OKADA KENJI
    • H01L29/68H01L21/338H01L29/812
    • PURPOSE:To improve the ununiformity of a second tunnel oxide film by making a resonance tunnel layer of conductive islandlike single crystal grains between two tunnel barriers, and insulating each the single crystal grain with insulator. CONSTITUTION:A first polycrystalline silicon 4 is composed of a first single crystal grain 11, a second single crystal grain 12, and a crystal grain boundary 13. Since the crystal grain boundary 13 is quicker in diffusion of oxidation seeds compared to the part of single crystal powder, the upper parts of the single crystal grains are oxidized and the part of the crystal grain boundary 13 is oxidized too, and a wedgelike thermal oxide film 7 is formed. If the thermal oxidation is continued further. The oxide film in the grain boundary reaches to a first tunnel oxide film 3, and the first and second single crystal grain parts 11 and 12 are completely separated by the oxide film in the grain boundary. After the removal of the thermal oxide film 7, a second tunnel oxide film (tunnel barrier) 5 is formed by thermal oxidation. Accordingly, it becomes possible to improve the ununiformity of the second tunnel oxide film 5 caused by the difference of the oxidation speed of the single crystal grains having different crystal orientation.