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    • 91. 发明专利
    • Diffraction lens
    • 衍射镜
    • JP2011215271A
    • 2011-10-27
    • JP2010081869
    • 2010-03-31
    • Nagoya Univ国立大学法人名古屋大学
    • EBIZUKA NOBORUISHIKAWA KENJIKONDO HIROMOTOHORI MASARU
    • G02B5/18G02B3/08
    • PROBLEM TO BE SOLVED: To provide a diffraction lens which is bright and whose diffraction efficiency is successfully maintained.SOLUTION: The diffraction lens includes an inner element part and an outer element part. In the inner element part, a plurality of surface ruling type gratings formed concentrically around a concentric axis perpendicular to the surface of a substrate are arranged so that the interval of the gratings is gradually narrower as it is away from the axis. In the outer element part, VP gratings including a plurality of trenches extending from the surface of the substrate in a depth direction, so as to surround the inner element part concentrically and a filler with which the trenches are filled and which has a refractive index different from that of the substrate are formed so that the interval of the gratings is gradually narrower as it is away from the axis.
    • 要解决的问题:提供一种光亮的衍射透镜,其衍射效率被成功地保持。解决方案:衍射透镜包括内部元件部分和外部元件部分。 在内部元件部分中,与垂直于基板的表面的同心轴同心地形成多个表面刻划型光栅,使得光栅的间隔从远离轴线逐渐变窄。 在外部元件部分中,VP光栅包括在深度方向上从基板的表面延伸的多个沟槽,以便同心地包围内部元件部分,并且填充物与沟槽被填充并具有不同的折射率 形成基板的间隔使得光栅的间隔随着离开轴线而逐渐变窄。
    • 93. 发明专利
    • Surface analyzer and surface analysis method
    • 表面分析仪和表面分析方法
    • JP2011163825A
    • 2011-08-25
    • JP2010024492
    • 2010-02-05
    • Meijo UnivNagoya UnivNu System KkNuシステム株式会社国立大学法人名古屋大学学校法人 名城大学
    • HORI MASARUITO AKIFUMITOJIMA YASUHIROOTA TAKAYUKI
    • G01J5/00G01J5/58G01N21/35G01N21/3563G01N21/359
    • PROBLEM TO BE SOLVED: To achieve a surface analyzer measuring a temperature of an object to be measured as well as analyzing condition of a desired surface of the object to be measured. SOLUTION: The surface analyzer is constituted of: a light source 10 emitting supercontinuum light; an optical fiber coupler 11 dividing the SC light into measuring light and reference light; a mirror 12; a driving device 13 moving the mirror 12; a light-receiving means 14 measuring an interference waveform between the measuring light and the reference light; and an interference waveform analysis means 15 analyzing a temperature and surface condition of the object to be measured from the interference waveform. The interference waveform analysis means 15, together with a means of measuring a temperature from temperature change of a interference peak position of the interference waveform, measures film quality, surface condition, etc. of the object to be measured by cutting out an interference peak corresponding to an intended surface of the object to be measured, from the interference waveform, and obtaining a Fourier transformed spectrum of the cut out waveform. COPYRIGHT: (C)2011,JPO&INPIT
    • 要解决的问题:为了实现测量待测物体的温度的表面分析仪以及分析待测物体的期望表面的状态。 解决方案:表面分析仪由发射超连续光的光源10构成; 将SC光分成测量光和参考光的光纤耦合器11; 镜子12; 移动镜子12的驱动装置13; 测量测量光和参考光之间的干涉波形的光接收装置14; 以及干扰波形分析单元15,根据干扰波形分析被测量物体的温度和表面状态。 干扰波形分析装置15与干扰波形的干扰峰值位置的温度变化测量温度的装置一起测量待测物体的膜质量,表面状况等,通过切出相应的干涉峰 从干涉波形到被测量物体的预期表面,并获得切出波形的傅里叶变换光谱。 版权所有(C)2011,JPO&INPIT
    • 94. 发明专利
    • Interference measuring apparatus and measuring method
    • 干扰测量装置和测量方法
    • JP2011163824A
    • 2011-08-25
    • JP2010024491
    • 2010-02-05
    • Meijo UnivNagoya UnivNu System KkNuシステム株式会社国立大学法人名古屋大学学校法人 名城大学
    • HORI MASARUITO AKIFUMITOJIMA YASUHIROOTA TAKAYUKI
    • G01B11/06G01B9/02G01K11/12
    • G01B9/02023G01B9/02058G01B9/0209G01K11/00
    • PROBLEM TO BE SOLVED: To improve measurement accuracy in an interference measuring apparatus using the interference of light. SOLUTION: The interference measuring apparatus is constituted of a light source 10 for radiating supercontinuum light (SC light); an optical fiber coupler 11 for dividing the SC light into measuring light and reference light; a dispersion compensation element 12; a drive unit 13 for moving the dispersion compensation element 12; and a light-receiving means 14 for measuring the interference waveform between the measuring light and the reference light. A measurement object 15 to be measured is an Si substrate having a thickness of 800 μm. The dispersion compensation element 12 is an Si substrate having a thickness of 780 μm. In other words, the dispersion compensation element 12 is made of the same material as that of the measurement object 15 and is thinner by 20 μm than the measurement object 15. Interference by reflection at the back surface of the measurement object 15 and the back surface of the dispersion compensation element 12 has a narrow peak width since wavelength dispersion is mostly negated to improve measurement accuracy of peak positions. As a result, measurement accuracy in temperature and others is improved. COPYRIGHT: (C)2011,JPO&INPIT
    • 要解决的问题:提高使用光的干涉的干涉测量装置的测量精度。 解决方案:干涉测量装置由用于辐射超连续光(SC灯)的光源10构成; 用于将SC光分成测量光和参考光的光纤耦合器11; 色散补偿元件12; 用于移动色散补偿元件12的驱动单元13; 以及用于测量测量光和参考光之间的干涉波形的光接收装置14。 待测量的测量对象15是厚度为800μm的Si衬底。 色散补偿元件12是厚度为780μm的Si衬底。 换句话说,色散补偿元件12由与测量对象15相同的材料制成,并且比测量对象15薄20μm。通过测量对象15的背面的反射和背面 色散补偿元件12具有窄的峰宽,因为波长色散被大部分否定,以提高峰位置的测量精度。 结果,提高了温度等测量精度。 版权所有(C)2011,JPO&INPIT
    • 95. 发明专利
    • Combinatorial type plasma process testing method, and inclined plasma generating device
    • 组合式等离子体工艺测试方法和等离子体生成装置
    • JP2011119030A
    • 2011-06-16
    • JP2008081959
    • 2008-03-26
    • Kyushu UnivNagoya UnivOsaka Univ国立大学法人九州大学国立大学法人名古屋大学国立大学法人大阪大学
    • HORI MASARUSEKINE MAKOTOSETSUHARA YUICHISHIRATANI MASAHARU
    • H05H1/00H01L21/3065H05H1/24H05H1/46
    • H01J37/3299H01J37/32935
    • PROBLEM TO BE SOLVED: To easily optimize external conditions of a plasma process. SOLUTION: There is provided a small-sized plasma generating device capable of establishing a state in which a plasma density is different depending on positions as shown in 4.A, and a radical density is different depending on positions as shown in 4.B. In this small-sized plasma generating device, an object to be processed by the plasma process and a material-forming substrate are arranged, and the plasma process is executed while measuring the plasma density and the radical density on a surface of the processed object. Resultant products of the plasma process are evaluated by positions and the plasma density and the radical density are decided at the positions at the highest evaluations. Moreover, in another large-sized or batch type plasma process, external conditions are adjusted so as to create those optimum plasma density and radical density. These adjustments need no plasma processing and the like for the processed object etc. COPYRIGHT: (C)2011,JPO&INPIT
    • 要解决的问题:容易优化等离子体工艺的外部条件。 解决方案:提供一种能够建立等离子体密度根据4.A所示的位置而不同的状态的小型等离子体产生装置,并且根据4中所示的位置的自由基密度不同 .B。 在这种小型等离子体产生装置中,布置了通过等离子体处理的物体和材料形成基板,并且在测量处理物体的表面上的等离子体密度和自由基浓度的同时执行等离子体处理。 通过位置评估等离子体工艺的产物,并且在最高评价的位置处确定等离子体密度和自由基密度。 此外,在另一种大型或间歇式等离子体工艺中,调节外部条件以产生最佳的等离子体密度和自由基密度。 这些调整不需要处理对象等的等离子体处理等。版权所有:(C)2011,JPO&INPIT
    • 96. 发明专利
    • Microwave waveguide device, plasma processing device, and plasma processing method
    • 微波波长装置,等离子体处理装置和等离子体处理方法
    • JP2014175051A
    • 2014-09-22
    • JP2013043404
    • 2013-03-05
    • Tokyo Electron Ltd東京エレクトロン株式会社Nagoya Univ国立大学法人名古屋大学
    • ITO HITOSHIKUBOTA YUSUKETOYODA HIROTAKAHORI MASARU
    • H05H1/24H05H1/46
    • H01J37/32229H01J37/32211
    • PROBLEM TO BE SOLVED: To provide a microwave waveguide device, a plasma processing device, and a plasma processing method, with which plasma is generated with stability.SOLUTION: A microwave waveguide device includes: a waveguide 21 that propagates a microwave, which is received from an input end 2A, from a first end 21a to a second end 21b; a circulator 22 that includes a first port 22a, a second port 22b coupled with the first end 21a, and a third port 22c coupled with the second end 21b and is constructed to receive the microwave from the input end 2A at the first port 22a, couples the microwave from the second port 22b to the first end 21a, receives the microwave from the second end 21b at the third port 22c, and returns the microwave to an input end 2A side; and an EH tuner 18 that is interposed between the input end 21a and the circulator 22 and reflects a part of the microwave, which is received at the third port 22c of the circulator 22 and is returned to the input end 2A side, to the first port 22a of the circulator 22, wherein a slot hole 28 is formed in the waveguide 21.
    • 要解决的问题:提供一种稳定地产生等离子体的微波波导装置,等离子体处理装置和等离子体处理方法。微波波导装置包括:传播微波的波导21,其被接收 从输入端2A,从第一端21a到第二端21b; 包括第一端口22a,与第一端部21a耦合的第二端口22b和与第二端部21b耦合的第三端口22c的循环器22构造成从第一端口22a处的输入端2A接收微波, 将微波从第二端口22b耦合到第一端21a,在第三端口22c处从第二端21b接收微波,并将微波返回到输入端2A侧; 以及插入在输入端21a和循环器22之间的EH调谐器18,并且将在循环器22的第三端口22c处接收并返回到输入端2A侧的微波的一部分反射到第一 环形器22的端口22a,其中在波导21中形成有槽孔28。
    • 97. 发明专利
    • Method for producing carbon nanotubes
    • 生产碳纳米管的方法
    • JP2014028733A
    • 2014-02-13
    • JP2012275890
    • 2012-12-18
    • Toyota Motor Corpトヨタ自動車株式会社Nagoya Univ国立大学法人名古屋大学
    • KATAYAMA YUKIHISAHORI MASARUKONDO HIROKI
    • C01B31/02B82Y40/00C23C16/26
    • PROBLEM TO BE SOLVED: To provide a method for producing carbon nanotubes (CNT's) capable of controlling spacing between CNT's over a broad range easily and a low cost.SOLUTION: The method for producing carbon nanotubes includes a carbon nanotube growth step of growing carbon nanotubes on a surface of a substrate by decomposing, with a plasma, a source gas including a carbon source gas and by contacting, with the surface of the substrate, the carbon source gas thus decomposed. There is placed a blocking member which is capable of permitting arrival, at the substrate surface, of the carbon source gas decomposed in a plasma generating region and, on the other hand, of blocking the arrival, at the substrate surface, of the carbon source gas decomposed within the plasma generating region. The source gas further includes a nitrogen-containing gas having a molecular structure containing a nitrogen atom, and a content of nitrogen atoms derived from the nitrogen-containing gas in the source gas is 20 mg/L or less.
    • 要解决的问题:提供能够容易地控制CNT在宽范围内控制间隔的碳纳米管(CNT)的制造方法和低成本。解决方案:碳纳米管的制造方法包括生长碳纳米管的碳纳米管生长步骤 通过用等离子体分解包含碳源气体的源气体并通过与基板的表面接触由此分解的碳源气体而在基板的表面上。 放置有阻挡构件,其能够允许在等离子体产生区域中分解的碳源气体在基板表面到达,另一方面阻止碳源的到达基板表面 气体在等离子体产生区域内分解。 源气体还包括具有含氮原子的分子结构的含氮气体,源气体中的含氮气体的氮原子含量为20mg / L以下。
    • 98. 发明专利
    • Diffraction grating and method for manufacturing the same, and optical waveguide
    • 衍射光栅及其制造方法及光波导
    • JP2013210589A
    • 2013-10-10
    • JP2012082527
    • 2012-03-30
    • Nagoya Univ国立大学法人名古屋大学Nu System KkNuシステム株式会社
    • EBIZUKA NOBORUHORI MASARUITO MASAFUMITOJIMA YASUHIRO
    • G02B5/32G02F1/13G11B7/135
    • PROBLEM TO BE SOLVED: To solve the problem that diffraction efficiency to natural polarization or the like is deteriorated since diffraction efficiency characteristics between S polarization and P polarization are deviated in accordance with a fact that a Bragg angle becomes larger in a transmission type VPH (volume Phase Holographic) diffraction grating and a thick transmission type rectangular diffraction grating.SOLUTION: It becomes possible to set diffraction efficiency of S polarization and P polarization to desired spectral characteristics in arbitrary wavelength and an arbitrary Bragg angle by making two values: difference between the maximum refractive index and the minimum refractive index to the S polarization; and difference between the maximum refractive index and the minimum refractive index to the P polarization to different predetermined values, by using an optical anisotropic medium as a material of a transmission type VPH diffraction grating and a thick transmission type rectangular diffraction grating.
    • 要解决的问题为了解决由于S偏振和P偏振之间的衍射效率特性偏离传播类型VPH(布拉格角变大)的事实来解决自然极化等的衍射效率劣化的问题(体积 相位全息)衍射光栅和厚透射型矩形衍射光栅。解决方案:通过制作两个值,可以将S偏振和P偏振的衍射效率设置为任意波长和任意布拉格角的期望光谱特性:最大值 折射率和S极化的最小折射率; 以及通过使用光学各向异性介质作为透射型VPH衍射光栅和厚透射型矩形衍射光栅的材料,使P偏振的最大折射率和最小折射率之间的差异达到不同的预定值。