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    • 1. 发明授权
    • Photocathode plate and electron tube
    • 光电阴极板和电子管
    • US07176625B2
    • 2007-02-13
    • US10969319
    • 2004-10-21
    • Tomoko MochizukiMinoru NiigakiToru HirohataKuniyoshi Mori
    • Tomoko MochizukiMinoru NiigakiToru HirohataKuniyoshi Mori
    • H01J40/06
    • H01J1/34H01J1/78H01J43/08H01J2231/50
    • Provided are a photocathode plate capable of stably achieving a high sensitive property, and an electron tube using such a photocathode plate.In a photomultiplier tube 1, an insulating layer 63 is formed between a semiconductor electron emission layer 51 in a photocathode plate 23A, and a first electrode 65 electrically connected to an electron releasing portion 59. This insulating layer 63 permits the photocathode plate 23A to be cleaned by heat cleaning at a high temperature, in a stage before formation of an active layer 61 on an exposed region of the semiconductor electron emission layer 51 in the electron releasing portion 59. This makes it feasible to effectively clean the exposed region of the semiconductor electron emission layer 51 in the electron releasing portion 59 and to stabilize the physical properties of the exposed region. In consequence, a higher sensitive property can be stably achieved in the photocathode plate 23A and in the photomultiplier tube 1 using the photocathode plate 23A.
    • 提供能够稳定地实现高灵敏度的光电阴极板和使用这种光电阴极板的电子管。 在光电倍增管1中,在光电阴极板23A中的半导体电子发射层51和与电子释放部分59电连接的第一电极65之间形成绝缘层63。 该绝缘层63允许在电子释放部分59中的半导体电子发射层51的暴露区域上形成有源层61之前的阶段,通过在高温下的热清洗来清洁光电阴极板23A。 这使得有效地清洁电子释放部分59中的半导体电子发射层51的暴露区域并且稳定暴露区域的物理性能是可行的。 因此,在光电阴极板23A和使用光电阴极板23A的光电倍增管1中可以稳定地实现更高的敏感性。
    • 2. 发明申请
    • Photocathode plate and electron tube
    • 光电阴极板和电子管
    • US20060038473A1
    • 2006-02-23
    • US10969319
    • 2004-10-21
    • Tomoko MochizukiMinoru NiigakiToru HirohataKuniyoshi Mori
    • Tomoko MochizukiMinoru NiigakiToru HirohataKuniyoshi Mori
    • H01J31/00H01J31/26H01J40/06
    • H01J1/34H01J1/78H01J43/08H01J2231/50
    • Provided are a photocathode plate capable of stably achieving a high sensitive property, and an electron tube using such a photocathode plate. In a photomultiplier tube 1, an insulating layer 63 is formed between a semiconductor electron emission layer 51 in a photocathode plate 23A, and a first electrode 65 electrically connected to an electron releasing portion 59. This insulating layer 63 permits the photocathode plate 23A to be cleaned by heat cleaning at a high temperature, in a stage before formation of an active layer 61 on an exposed region of the semiconductor electron emission layer 51 in the electron releasing portion 59. This makes it feasible to effectively clean the exposed region of the semiconductor electron emission layer 51 in the electron releasing portion 59 and to stabilize the physical properties of the exposed region. In consequence, a higher sensitive property can be stably achieved in the photocathode plate 23A and in the photomultiplier tube 1 using the photocathode plate 23A.
    • 提供能够稳定地实现高灵敏度的光电阴极板和使用这种光电阴极板的电子管。 在光电倍增管1中,在光电阴极板23A中的半导体电子发射层51和与电子释放部分59电连接的第一电极65之间形成绝缘层63。 该绝缘层63允许在电子释放部分59中的半导体电子发射层51的暴露区域上形成有源层61之前的阶段,通过在高温下的热清洗来清洁光电阴极板23A。 这使得有效地清洁电子释放部分59中的半导体电子发射层51的暴露区域并且稳定暴露区域的物理性能是可行的。 因此,在光电阴极板23A和使用光电阴极板23A的光电倍增管1中可以稳定地实现更高的敏感性。
    • 3. 发明授权
    • Semiconductor photocathode
    • 半导体光电阴极
    • US06917058B2
    • 2005-07-12
    • US10433060
    • 2001-12-18
    • Minoru NiigakiToru HirohataHirofumi KanKuniyoshi Mori
    • Minoru NiigakiToru HirohataHirofumi KanKuniyoshi Mori
    • H01J1/34H01J29/38H01J31/50H01J40/06H01L29/24
    • H01J1/34H01J2201/3423
    • In the case of a thick light-absorbing layer 2, a phenomenon of a decrease in the time resolution occurs. However, when the thickness of the light-absorbing layer 2 is limited, a portion of low electron concentration in one electron group is cut out, and hence overlap regions of adjacent electron concentration distributions decrease. Therefore, by shortening the transit time necessary for the passage of electrons, regions of overlapping electron distributions due to diffusion can also be suppressed. Furthermore, the strength of an electric field within a light-absorbing layer can be increased by thinning the light-absorbing layer. Therefore, the time resolution of infrared rays can be remarkably improved by a synergistic action of these effects. If it is assumed that the time resolution is 40 ps (picoseconds), for example, when the thickness of a light-absorbing layer is 1.3 μm which is nearly equal to the wavelength of infrared, then a possible time resolution is 7.5 ps when this thickness is 0.19 μm.
    • 在厚光吸收层2的情况下,会发生时间分辨率降低的现象。 然而,当光吸收层2的厚度受限时,一个电子组中的低电子浓度部分被切掉,因此相邻电子浓度分布的重叠区域减小。 因此,通过缩短电子通过所需的通行时间,也可以抑制由扩散引起的重叠电子分布的区域。 此外,可以通过使光吸收层变薄来增加光吸收层内的电场强度。 因此,通过这些效果的协同作用,可以显着提高红外线的时间分辨率。 如果假设时间分辨率为40ps(皮秒),例如,当光吸收层的厚度为1.3μm,几乎等于红外线的波长时,则当这样的时间分辨率为7.5ps时 厚度为0.19毫米。
    • 4. 发明授权
    • Photocathode comprising a plurality of openings on an electron emission layer
    • 光电阴极包括在电子发射层上的多个开口
    • US07816866B2
    • 2010-10-19
    • US11585936
    • 2006-10-25
    • Kazutoshi NakajimaMinoru NiigakiTomoko MochizukiToru Hirohata
    • Kazutoshi NakajimaMinoru NiigakiTomoko MochizukiToru Hirohata
    • H01J40/06H01J37/08G21K5/10H01L29/12
    • H01J1/34H01J2201/3423
    • A semiconductor photocathode 1 includes: a transparent substrate 11; a first electrode 13, formed on the transparent substrate 11 and enabling passage of light that has been transmitted through the transparent substrate 11; a window layer 14, formed on the first electrode 13 and formed of a semiconductor material with a thickness of no less than 10 nm and no more than 200 nm; a light absorbing layer 15, formed on the window layer 14, formed of a semiconductor material that is lattice matched to the window layer 14, is narrower in energy band gap than the window layer 14, and in which photoelectrons are excited in response to the incidence of light; an electron emission layer 16, formed on the light absorbing layer 15, formed of a semiconductor material that is lattice matched to the light absorbing layer 15, and emitting the photoelectrons excited in the light absorbing layer 15 to the exterior from a surface; and a second electrode 18, formed on the electron emission layer.
    • 半导体光电阴极1包括:透明基板11; 第一电极13,其形成在透明基板11上,并能透过透明基板11的光通过; 窗口层14,其形成在第一电极13上并且由不小于10nm且不大于200nm的厚度的半导体材料形成; 形成在与窗口层14格子匹配的半导体材料的窗口层14上的光吸收层15的能带隙比窗口层14更窄,并且其中光电子响应于 光的发生; 由与光吸收层15晶格匹配的半导体材料形成的光吸收层15上形成的电子发射层16,并且将从光吸收层15激发的光电子从表面发射到外部; 以及形成在电子发射层上的第二电极18。
    • 5. 发明申请
    • Photocathode
    • 光电阴极
    • US20070096648A1
    • 2007-05-03
    • US11585936
    • 2006-10-25
    • Kazutoshi NakajimaMinoru NiigakiTomoko MochizukiToru Hirohata
    • Kazutoshi NakajimaMinoru NiigakiTomoko MochizukiToru Hirohata
    • H01J40/06
    • H01J1/34H01J2201/3423
    • A semiconductor photocathode 1 includes: a transparent substrate 11; a first electrode 13, formed on the transparent substrate 11 and enabling passage of light that has been transmitted through the transparent substrate 11; a window layer 14, formed on the first electrode 13 and formed of a semiconductor material with a thickness of no less than 10 nm and no more than 200 nm; a light absorbing layer 15, formed on the window layer 14, formed of a semiconductor material that is lattice matched to the window layer 14, is narrower in energy band gap than the window layer 14, and in which photoelectrons are excited in response to the incidence of light; an electron emission layer 16, formed on the light absorbing layer 15, formed of a semiconductor material that is lattice matched to the light absorbing layer 15, and emitting the photoelectrons excited in the light absorbing layer 15 to the exterior from a surface; and a second electrode 18, formed on the electron emission layer.
    • 半导体光电阴极1包括:透明基板11; 第一电极13,其形成在透明基板11上,并能透过透明基板11的光通过; 窗口层14,其形成在第一电极13上并且由不小于10nm且不大于200nm的厚度的半导体材料形成; 形成在与窗口层14格子匹配的半导体材料的窗口层14上的光吸收层15的能带隙比窗口层14更窄,并且其中光电子响应于 光的发生; 由与光吸收层15晶格匹配的半导体材料形成的光吸收层15上形成的电子发射层16,并且将从光吸收层15激发的光电子从表面发射到外部; 以及形成在电子发射层上的第二电极18。
    • 10. 发明授权
    • Photodetector having first and second antenna areas with patterns having different cycle intervals
    • 光检测器具有第一和第二天线区域,其图案具有不同的周期间隔
    • US07557336B2
    • 2009-07-07
    • US11798040
    • 2007-05-09
    • Minoru NiigakiToru HirohataHiroyasu FujiwaraAkira Higuchi
    • Minoru NiigakiToru HirohataHiroyasu FujiwaraAkira Higuchi
    • H01L31/00
    • H01L31/02162
    • When light is made incident into antenna layers 11a, 11b, and 11c of a photodetector 1, specific wavelength components of light contained in the incident light combine with surface plasmons of the antenna layers 11a, 11b, and 11c, and surface plasmon resonance occurs. Thereby, near-field lights are outputted from through-holes 13 of the antenna layers 11a, 11b, and 11c. The near-field light outputted from each through-hole 13 reaches a light absorbing layer 4 via light receiving surfaces 4a, 4b, and 4c. The light absorbing layer 4 generates a charge of an amount according to the amount of received light. Since cycle intervals Λa, Λb, and Λc of convex portions 12 in the antenna layers 11a, 11b, and 11c are different from each other, the wavelength component of light that combines with a surface plasmon differs in each of the antenna layers 11a, 11b, and 11c. Consequently, a plurality of wavelength components of light can be detected.
    • 当光入射到光电检测器1的天线层11a,11b和11c中时,入射光中包含的光的特定波长分量与天线层11a,11b和11c的表面等离子体相结合,并发生表面等离子体共振。 由此,从天线层11a,11b,11c的通孔13输出近场光。 从每个通孔13输出的近场光通过光接收表面4a,4b和4c到达光吸收层4。 光吸收层4产生与接收光量相关的量的电荷。 由于天线层11a,11b和11c中的凸部12的周期间隔Lambda,Lambdab和Lambdac彼此不同,所以在每个天线层11a,11b中与表面等离子体的组合的光的波长成分不同 ,和11c。 因此,可以检测多个波长分量的光。