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    • 2. 发明申请
    • ULTRAFAST MICROSCOPY OF SURFACE ELECTROMAGNETIC FIELDS
    • 表面电磁场超声显微镜
    • US20090066963A1
    • 2009-03-12
    • US12199427
    • 2008-08-27
    • Hrvoje PetekAtsushi KuboNikolaus Johannes Pontius
    • Hrvoje PetekAtsushi KuboNikolaus Johannes Pontius
    • G01N21/63
    • G01B9/04G01B15/00G01N21/636
    • System(s) and method(s) to probe electromagnetic fields at the surface of a solid-state material are provided. The technique combines ultrafast (e.g., less than 10 fs) optical excitation and electron microscopy to generate electronic excitations and image the ensuing electromagnetic fields with nanometer-scale spatial resolution and femtosecond time-scale resolution. In addition, time-of-flight energy analysis facilitates imaging of relaxation a generated electronic excitation. The dynamics of the electromagnetic fields can be probed interferometrically through generation of multi-frame imaging, with inter-frame frequency of the order of a few hundreds of attoseconds, of interference patterns among an electric field associated with an excitation in a sample or device and the electromagnetic field of a probe pulse coherent with an excitation pulse. Quality assurance of nanoscopic devices based on plasmonic, photonic, electronic, spintronic operation can be analyzed with spectroscopy provided in the subject innovation.
    • 提供了在固体材料表面探测电磁场的系统和方法。 该技术结合了超快速(例如小于10fs)的光学激发和电子显微镜来产生电子激发,并以纳米尺度的空间分辨率和飞秒时间刻度分辨率对随后的电磁场进行成像。 此外,飞行时间能量分析有助于放大产生的电子激发的成像。 电磁场的动力学可以通过产生多帧成像而进行干涉测量,其中帧间频率为数百个起始点,在与样品或装置中的激发相关的电场中的干扰图案;以及 探头脉冲的电磁场与激发脉冲相干。 基于等离子体激元,光子,电子,自旋电子操作的纳米级器件的质量保证可以通过本科创新中提供的光谱进行分析。
    • 3. 发明授权
    • Optical interferometer and signal synthesizer using the interferometer
    • 光干涉仪和信号合成器采用干涉仪
    • US06587278B1
    • 2003-07-01
    • US09524549
    • 2000-03-13
    • Susumu OgawaHrvoje PetekHisashi NaganoAlbert HeberleTatsuya Tomaru
    • Susumu OgawaHrvoje PetekHisashi NaganoAlbert HeberleTatsuya Tomaru
    • G02B2714
    • H04B10/50G01J9/02
    • An optical signal synthesizer having an optical slab waveguide constructed from three layers in which optical pulses are introduced. A first cut-away portion of the optical slab waveguide has a plano-concave shape serving as a plano-convex lens which collimates the introduced optical pulses, a second cut-away portion of the optical slab waveguide serving as a diffraction grating for parallel light beams in which the optical pulses are separated into every frequency, and a third cut-away portion of the optical slab waveguide has a plano-concave shape serving as a plano-convex lens by which the separated optical pulses are focused on a different spatial position associated with each frequency. A spatial light modulator is fabricated at the focusing position in the optical slab waveguide which allows the optical pulses subjected to optical modulation every frequency to pass therethrough according to an applied electrical signal. A fourth cut-away portion of the optical slab waveguide has a plano-concave shape serving as a plano-convex lens which collimates each modulated optical frequency component individually, and a fifth cut-away portion of the optical slab waveguide serving as a diffraction grating for the modulated optical pulses restores the modulated optical pulses to the parallel light beams.
    • 一种光信号合成器,具有由三层构成的光学平板波导,其中引入了光脉冲。 光学平板波导的第一切除部分具有用作平行引入的光脉冲的平凸透镜的平凹形状,用作平行光的衍射光栅的光学平板波导的第二切除部分 其中光脉冲被分离成每个频率的光束,光学平板波导的第三切除部分具有用作平凸透镜的平凹形状,通过该平面凹形形状,分离的光脉冲聚焦在不同的空间位置 与每个频率相关联。 在光学平板波导中的聚焦位置处制造空间光调制器,其允许每个频率经受光调制的光脉冲根据所施加的电信号通过。 光学平板波导的第四切除部分具有平面凹形形状,用作将每个调制的光频率分量单独准直的平凸透镜,以及用作衍射光栅的光学平板波导的第五切除部分 对于调制的光脉冲,将调制的光脉冲恢复到平行光束。
    • 5. 发明授权
    • Solid-state laser compensated for pumping-light astigmatism
    • 固体激光补偿泵浦散光
    • US06778579B2
    • 2004-08-17
    • US10084382
    • 2002-02-28
    • Tatsuya TomaruHrvoje Petek
    • Tatsuya TomaruHrvoje Petek
    • H01S391
    • H01S3/09415
    • In a solid-state laser in which a gain crystal is polished to have the Brewster angle or a solid-state laser comprising a dichroic concave mirror to which light enters at an incidence angle which is not zero, astigmatism generally occurs in pumping light. By tilting a focusing lens for pumping light with respect to the optical axis of the pumping light, the astigmatism is compensated. The tilting angle is determined in such a manner that synthetic focusing points in the sagittal and tangential planes, of a series optical system of a focusing lens, a dichroic concave lens, and a gain crystal are calculated and the focusing points almost coincide with focusing points in a cavity mode.
    • 在其中将增益晶体抛光以具有布鲁斯特角的固态激光器或包括以不为零的入射角入射的二色性凹面镜的固态激光器,通常在泵浦光中发生像散。 通过倾斜相对于泵浦光的光轴来泵浦光的聚焦透镜,散光被补偿。 以如下方式确定倾斜角度:计算聚焦透镜的串联光学系统,二向色凹透镜和增益晶体的矢状面和切向平面中的合成聚焦点,并且聚焦点几乎与聚焦点一致 在腔模式。
    • 6. 发明授权
    • Solid-state laser and optical transmitter
    • 固态激光和光发射机
    • US06754248B2
    • 2004-06-22
    • US10420902
    • 2003-04-23
    • Tatsuya TomaruHrvoje Petek
    • Tatsuya TomaruHrvoje Petek
    • H01S308
    • H01S3/0602H01S3/08H01S3/08059H01S3/09415H01S3/1112H01S3/1623H01S3/1643
    • A solid-state laser having an excitation light source, a lens system for focusing an excitation light produced from the light source, and a laser resonator which is laser-oscillated in response to the focused excitation light. The resonator includes only a gain medium and a solid-state medium having dispersion of a wavelength dependence opposite to that of the gain medium, and surfaces of the gain medium and the solid-state medium, which are respectively at opposite sides of opposing surfaces of the gain medium and the solid-state medium, are reflectively coated and act as mirror surfaces. At least one of the other surfaces of the gain medium and the solid-state medium, which ate positioned inside the resonator and are opposite to each other, is polished to a curved surface. The gain medium is excited by the focused excitation light so that the laser oscillation is made in the resonator.
    • 具有激发光源的固态激光器,用于聚焦由光源产生的激发光的透镜系统以及响应于聚焦激发光激光振荡的激光谐振器。 谐振器仅包括增益介质和具有与增益介质的波长依赖相反的色散的固态介质,以及增益介质和固态介质的分别位于相对表面的相对侧的表面 增益介质和固态介质被反射涂覆并用作镜面。 增益介质和固体介质的其他表面中的至少一个,其被放置在谐振器内部并且彼此相对的位置被抛光到弯曲表面。 增益介质被聚焦的激发光激发,使得在谐振器中进行激光振荡。
    • 8. 发明授权
    • Ultrafast microscopy of surface electromagnetic fields
    • 表面电磁场的超快速显微镜
    • US08085406B2
    • 2011-12-27
    • US12199427
    • 2008-08-27
    • Hrvoje PetekAtsushi KuboNikolaus Johannes Pontius
    • Hrvoje PetekAtsushi KuboNikolaus Johannes Pontius
    • G01B9/02
    • G01B9/04G01B15/00G01N21/636
    • System(s) and method(s) to probe electromagnetic fields at the surface of a solid-state material are provided. The technique combines ultrafast (e.g., less than 10 fs) optical excitation and electron microscopy to generate electronic excitations and image the ensuing electromagnetic fields with nanometer-scale spatial resolution and femtosecond time-scale resolution. In addition, time-of-flight energy analysis facilitates imaging of relaxation a generated electronic excitation. The dynamics of the electromagnetic fields can be probed interferometrically through generation of multi-frame imaging, with inter-frame frequency of the order of a few hundreds of attoseconds, of interference patterns among an electric field associated with an excitation in a sample or device and the electromagnetic field of a probe pulse coherent with an excitation pulse. Quality assurance of nanoscopic devices based on plasmonic, photonic, electronic, spintronic operation can be analyzed with spectroscopy provided in the subject innovation.
    • 提供了在固体材料表面探测电磁场的系统和方法。 该技术结合了超快速(例如小于10fs)的光学激发和电子显微镜来产生电子激发,并以纳米尺度的空间分辨率和飞秒时间刻度分辨率对随后的电磁场进行成像。 此外,飞行时间能量分析有助于放大产生的电子激发的成像。 电磁场的动力学可以通过产生多帧成像而进行干涉测量,其中帧间频率为数百个起始点,在与样品或装置中的激发相关的电场中的干扰图案;以及 探头脉冲的电磁场与激发脉冲相干。 基于等离子体激元,光子,电子,自旋电子操作的纳米级器件的质量保证可以通过本科创新中提供的光谱进行分析。
    • 9. 发明授权
    • Solid-state laser and optical transmitter
    • 固态激光和光发射机
    • US06560267B1
    • 2003-05-06
    • US09665619
    • 2000-09-19
    • Tatsuya TomaruHrvoje Petek
    • Tatsuya TomaruHrvoje Petek
    • H01S308
    • H01S3/0602H01S3/08H01S3/08059H01S3/09415H01S3/1112H01S3/1623H01S3/1643
    • In the wavelength-division-multiplexed optical transmission, laser diodes of the number of multiplicity are disposed as a light source to configure a transmitter. However, since this method requires a large number of light sources and highly precise wavelength control, a cost and an apparatus are increased. An ultrashort pulse solid-state laser is used as the light source of the transmitter and its wide spectrum is taken out by a splitter to be assigned to each channel, so that the number of light sources can be reduced greatly. The transmitter requires high repetition rate such as 2.4 GHz, 10 HGz and the like as the repetition rate of the ultrashort pulse solid-state laser, while by configuring the resonator only by two components as shown in FIG. 1, the high repetition rate can be attained. Since each channel is produced passively from the splitter, very precise wavelength management is not required. The light source is made small and the number thereof is reduced. Consequently, the whole apparatus is made small and a cost thereof is also reduced.
    • 在波分复用光传输中,将多个数量的激光二极管设置为光源以配置发射机。 然而,由于该方法需要大量的光源和高精度的波长控制,所以成本和装置都增加。 使用超短脉冲固态激光器作为发射器的光源,并且其分配器将其宽谱线分配给每个通道,从而可以大大减少光源的数量。 发射机需要高重复频率,例如2.4GHz,10Hz等等作为超短脉冲固态激光器的重复频率,而通过仅由两个部件构成谐振器,如图3所示。 如图1所示,可以实现高重复率。 由于每个通道都是从分离器被动产生的,所以不需要非常精确的波长管理。 光源变小,数量减少。 因此,整个装置变小,成本也降低。