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    • 32. 发明申请
    • METHOD FOR PRODUCING GRAPHENE
    • 生产石墨的方法
    • US20110114499A1
    • 2011-05-19
    • US12736268
    • 2009-03-23
    • Masaru HoriHiroyuki Kano
    • Masaru HoriHiroyuki Kano
    • C01B31/00C25B1/00B82Y40/00
    • B82Y40/00B82Y30/00C01B32/184
    • To provide a simple process for producing graphene.A graphene production apparatus 100 has a vessel 10 and, attached thereto, an immersion electrode 20 and a non-immersion electrode 30. The immersion electrode has an electrode covering 20c and an electrode main body 20e, and the non-immersion electrode has a covering 30c and an electrode main body 30e. An argon-feeding conduit 40 is disposed so as to inject argon into the vessel 10 around the electrode main body 30e. Ethanol is supplied in such an amount that the liquid surface completely covers the electrode main body 20e of the immersion electrode 20 and does not reach the electrode main body 30e of the non-immersion electrode 30. The electrode main body 20e is formed from, for example, iron, nickel, or cobalt. Thus, a 60-Hz AC voltage is applied to the electrode main body 20e immersed in the liquid; i.e., below the ethanol surface, and to the electrode main body 30e located above the liquid, while argon gas is supplied through the argon-feeding conduit 40. As a result, a gas-liquid plasma generates, to thereby induce decomposition of ethanol, etc., whereby graphene is yielded. The graphene disperses in ethanol.
    • 提供生产石墨烯的简单工艺。 石墨烯制造装置100具有容器10,并附接有浸渍电极20和非浸没电极30.浸渍电极具有电极覆盖层20c和电极主体20e,非浸渍电极具有覆盖层 30c和电极主体30e。 氩供给导管40设置成在电极主体30e的周围向容器10内注入氩。 乙醇的供给量使得液面完全覆盖浸没电极20的电极主体20e,并且不会到达非浸没电极30的电极主体30e。电极主体20e由 例如,铁,镍或钴。 因此,向浸没在液体中的电极主体20e施加60Hz的交流电压, 即位于乙醇表面以下的电极主体30e和位于液体上方的电极主体30e,同时通过氩供给导管40供给氩气。结果,产生气液等离子体,从而导致乙醇分解, 等等,由此产生石墨烯。 石墨烯分散在乙醇中。
    • 35. 发明申请
    • CARBON NANOWALL WITH CONTROLLED STRUCTURE AND METHOD FOR CONTROLLING CARBON NANOWALL STRUCTURE
    • 碳纳米管具有控制结构和控制碳纳米结构的方法
    • US20100009242A1
    • 2010-01-14
    • US12374844
    • 2007-07-25
    • Masaru HoriMineo HiramatsuHiroyuki KanoToru SugiyamaYuichiro Hama
    • Masaru HoriMineo HiramatsuHiroyuki KanoToru SugiyamaYuichiro Hama
    • H01M4/86C01B31/02B01J32/00
    • B01J21/185B82Y30/00B82Y40/00C01B32/18H01M4/9083H01M4/926Y10T428/24355
    • Provided is a method for controlling a carbon nanowall (CNW) structure having improved corrosion resistance against high potential by varying the spacing between the carbon nanowall (CNW) walls so that its surface area and crystallinity are controlled. Also provided is a carbon nanowall (CNW) with a high surface arca and a carbon nanowall (CNW) with a high crystallinity, both of which have a controlled structure. According to the present invention, provided are: (1) a carbon nanowall, characterized by having a wall surface area of 50 cm2/cm2-substrate·μm or more; (2) a carbon nanowall, characterized by having a crystallinity such that the D band half value width in the Raman spectrum measured with an irradiation laser wavelength of 514.5 nm is 85 cm−1 or less: and (3) a carbon nanowall, characterized by having not only a wall surface area of 50 cm2/cm2-substrate·μm or more but also a crystallinity such that the D-band half value width in the Raman spectrum measured with an irradiation laser wavelength of 14.5 nm is 85 cm−1 or less.
    • 提供了一种通过改变碳纳米壁(CNW)壁之间的间距来控制其表面积和结晶度来控制具有改善的高电位耐腐蚀性的碳纳米壁(CNW)结构的方法。 还提供具有高表面积的碳纳米壁(CNW)和具有高结晶度的碳纳米壁(CNW),两者都具有受控的结构。 根据本发明,提供:(1)一种碳纳米壁,其特征在于,具有50cm 2 / cm 2以上的基板的壁面积以上; (2)碳纳米壁,其特征在于具有结晶度使得以514.5nm的照射激光波长测量的拉曼光谱中的D带半值宽度为85cm -1以下:(3)碳纳米壁,其特征在于, 通过不仅具有50cm 2 / cm 2以上的壁面积等于或大于50的壁面积,而且结晶度使得以14.5nm的照射激光波长测量的拉曼光谱中的D带半值宽度为85cm -1 或更少。
    • 39. 发明授权
    • Interference measurement device and measurement method
    • 干涉测量装置及测量方法
    • US09041937B2
    • 2015-05-26
    • US13577044
    • 2011-02-02
    • Masaru HoriMasafumi ItoYasuhiro HigashijimaTakayuki Ohta
    • Masaru HoriMasafumi ItoYasuhiro HigashijimaTakayuki Ohta
    • G01B11/02G01B9/02G01K11/00
    • G01B9/02023G01B9/02058G01B9/0209G01K11/00
    • [Problem to be Solved] To improve the measurement accuracy of an interference measurement device which utilizes interference of light.[Means for Solution] An interference measurement device includes a light source 10 for emitting supercontinuum light (SC light), an optical fiber coupler 11 for splitting the SC light into measurement light and reference light, a dispersion compensation element 12, a drive unit 13 for moving the dispersion compensation element 12, and light-receiving means 14 for measuring an interference waveform produced as a result of interference between the measurement 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. Namely, the dispersion compensation element 12 is formed of the same material as that of the measurement object 15 and is 20 μm thinner than the measurement object 15. The interference caused by reflection on the back surface of the measurement object 15 and reflection on the back surface of the dispersion compensation element 12 has a narrow peak width because wavelength dispersion is cancelled almost completely. Thus, the accuracy in measuring the peak position improves. As a result, the accuracy in measuring temperature, etc., improves.
    • [待解决的问题]提高利用干扰的干涉测量装置的测量精度。 解决方案干扰测量装置包括用于发射超连续光(SC灯)的光源10,用于将SC光分解为测量光和参考光的光纤耦合器11,色散补偿元件12,驱动单元13 用于移动色散补偿元件12和用于测量作为测量光和参考光之间的干涉的结果而产生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。 也就是说,色散补偿元件12由与测量对象15相同的材料形成,并且比测量对象15薄20μm。由测量对象15的背面上的反射引起的干涉和背面的反射 由于波长色散几乎完全消除,所以色散补偿元件12的表面具有窄的峰宽。 因此,测量峰值位置的精度提高。 结果,测量温度等的精度提高。
    • 40. 发明授权
    • Plasma generator
    • 等离子发生器
    • US08961888B2
    • 2015-02-24
    • US12733896
    • 2008-09-18
    • Masaru HoriHioryuki Kano
    • Masaru HoriHioryuki Kano
    • B01J19/08H05H1/24H01J37/32
    • H05H1/24H01J37/3244H01J37/32449H01J37/32834H05H1/48
    • To provide a plasma generator having plasma-generating zone of increased volume.A plasma generator 110 has a cylindrical casing 11 made of a sintered ceramic produced from alumina (Al2O3) as a raw material. The casing 11 has a slit-like gas inlet 11i and a plurality of cylindrical gas outlets 11o. From the gas inlet 11i to the top of the plasma-generating zone P, the slit width (the front-to-back direction with respect to the sheet of FIG. 2.A, and the left-to right direction in FIG. 2.B) is adjusted to 1 mm, and gas outlets 11o each having an inner diameter of 1 to 2 mm are formed in straight line along the longitudinal direction of the plasma-generating zone P. The plasma-generating zone P has a square cross-section normal to the longitudinal direction having a side of 2 to 5 mm. Each of the surfaces of the electrodes 2a, 2b facing each other has a plurality of recesses (hollow portions). An elevated voltage of about 9 kV obtained from a commercial AC voltage (60 Hz, 100 V) was applied to the electrodes 2a, 2b, to thereby supply a current of 20 mA. When argon gas was supplied through the gas inlet 11i, even in the case where the electrodes 2a, 2b were separated at a spacing of 4 cm, stable linear electric discharge was observed.
    • 提供具有增加体积的等离子体产生区域的等离子体发生器。 等离子体发生器110具有由作为原料的氧化铝(Al 2 O 3)制成的烧结陶瓷制成的圆筒状壳体11。 壳体11具有狭缝状气体入口11i和多个圆筒形气体出口11o。 从气体入口11i到等离子体产生区域P的顶部,狭缝宽度(相对于图2A的片材的前后方向以及图2中的左右方向) B)被调整为1mm,并且具有内径为1至2mm的气体出口11o沿着等离子体产生区P的纵向方向形成为直线。等离子体产生区P具有正交十字 与纵向方向垂直的截面为2至5mm的一侧。 彼此面对的电极2a,2b的每个表面具有多个凹部(中空部)。 将从市售AC电压(60Hz,100V)获得的约9kV的高电压施加到电极2a,2b,从而提供20mA的电流。 当通过气体入口11i供应氩气时,即使在电极2a,2b以4cm的间隔分离的情况下,也观察到稳定的线性放电。