会员体验
专利管家(专利管理)
工作空间(专利管理)
风险监控(情报监控)
数据分析(专利分析)
侵权分析(诉讼无效)
联系我们
交流群
官方交流:
QQ群: 891211   
微信请扫码    >>>
现在联系顾问~
热词
    • 5. 发明授权
    • Microscope with wavelength compensation
    • 具有波长补偿的显微镜
    • US07095556B2
    • 2006-08-22
    • US10771729
    • 2004-02-04
    • Yoshinori IketakiTakeshi WatanabeMasaaki FujiiYasunori IgasakiToshio Suzuki
    • Yoshinori IketakiTakeshi WatanabeMasaaki FujiiYasunori IgasakiToshio Suzuki
    • G02B21/06G01J3/30
    • G02B26/08
    • A microscope capable of being shaped into a beam with complete hollow shape by removing the disorder of the wavefront to the erase light, particularly, and capable of improving the spatial resolution by inducing a super-resolution near the limit, is provided. In the microscope, wherein a first light to excite a molecule from a ground-state to first electron excited state or a second light to excite the molecule from the first electron excited state to the second electron excited state with higher energy level, for a sample 56 including the molecule with three electronic states including at least a ground-state, are spatial phase-modulated into the prescribed beam shape, and parts of these first light and the second light are overlapped and focused to detect luminescence from the sample 56, a wavefront compensation means 61 is provided in the optical path of the first light and/or in the optical path of the second light, and the wavefront aberration caused in the first light and/or in the second light, is removed by the wavefront compensation means 61.
    • 提供了能够通过将擦除光的波阵面除去特别是并且能够通过在接近极限附近引起超分辨率来改善空间分辨率而将具有完全中空形状的光束成形为显微镜的显微镜。 在显微镜中,其中将分子从基态激发到第一电子激发态的第一光或第二光以将分子从第一电子激发态激发至具有较高能级的第二电子激发态,对于样品 包括具有至少包括基态的三种电子状态的分子被空间相位调制成规定的波束形状,并且这些第一光和第二光的一部分被重叠和聚焦以检测来自样品56的发光, 波前补偿装置61设置在第一光的光路和/或第二光的光路中,并且在第一光和/或第二光中引起的波前像差被波前补偿装置除去 61。
    • 7. 发明申请
    • Super-Resolution Microscope
    • 超分辨率显微镜
    • US20070291353A1
    • 2007-12-20
    • US11659525
    • 2005-07-25
    • Yoshinori IketakiTakeshi WatanabeMasaaki Fujii
    • Yoshinori IketakiTakeshi WatanabeMasaaki Fujii
    • G02B21/06H01S3/00
    • G01N21/6458G01N2021/6419G01N2021/6439G02B21/002G02B21/16G02B27/58
    • [Task] To provide a super-resolution microscope whereby the light source of pump light and erase light can be selected easily and a super-resolution can be reliably achieved through a simple and inexpensive arrangement. [Solution of the Task] A super-resolution microscope includes an optical system (3, 4, 9) for combining a part of a first coherent light from a first light source (2) and a part of a second coherent light from a second light source (1) and focusing the coherent lights onto a sample (10), scanning means (6, 7) for scanning the coherent lights, and detecting means (16) for detecting an optical response signal from the sample (10). The microscope is configured so as to satisfy the following conditions: σ01Ipτ≦1, and 0.65(λe/λp)≦τσdipIe where λp is the wavelength of the first coherent light, λe is the wavelength of the second coherent light, τ is the excited lifetime in which the molecule is excited by the first coherent light from the ground state to the first electron-excited state, Ip is the maximum photon flux on the sample surface of the first coherent light, Ie is the maximum photon flux on the sample surface of the second coherent light, σ01, is the absorption cross-sectional area when the molecule is exited from the ground state to the first electron-excited state, and σdip is the fluorescence suppression cross-sectional area.
    • [任务]提供一种能够容易地选择泵浦光和擦除光的光源的超分辨率显微镜,并且通过简单且廉价的布置可以可靠地实现超分辨率。 [任务的解决方案]超分辨率显微镜包括用于组合来自第一光源(2)的第一相干光的一部分和来自第二光源的第二相干光的一部分的光学系统(3,4,9) 光源(1),并将相干光聚焦到样品(10)上,用于扫描相干光的扫描装置(6,7)以及用于检测来自样品(10)的光响应信号的检测装置(16)。 显微镜被配置为满足以下条件:<?in-line-formula description =“In-line Formulas”end =“lead”?> sigma Iptau <= 1, ?in-line-formula description =“In-line Formulas”end =“tail”?> <?in-line-formula description =“In-line formula”end =“lead”?> 0.65(lambdae / lambdap) = tausigma Ie <?in-line-formula description =“In-line Formulas”end =“tail”?>其中lambdap是第一个相干光的波长,lambdae是 第二相干光,tau是分子被从基态到第一电子激发态的第一相干光激发的激发寿命,Ip是第一相干光的样品表面上的最大光子通量,Ie是 第二相干光的样品表面上的最大光子通量σσ是当分子从基态退出到第一电子激发态时的吸收横截面积,而西格玛 浸渍 是荧光抑制截面积。
    • 10. 发明授权
    • Radio transmission apparatus and method, radio reception apparatus and method, transmitting and receiving method, and recording medium
    • 无线发送装置和方法,无线电接收装置和方法,发送和接收方法以及记录介质
    • US07936740B2
    • 2011-05-03
    • US11356149
    • 2006-02-17
    • Masaaki Fujii
    • Masaaki Fujii
    • H04B7/00H04B7/208H04B7/216H04B1/60H04B17/02
    • H04L1/0631H04B7/0678H04L1/0625H04L5/026
    • Provided are a radio transmission apparatus and method, a radio receiving apparatus and method, a transmitting and receiving method, and a recording medium for use in a mobile communication system according to an Orthogonal Frequency Division Multiplexing-Code Division Multiplexing (OFDM-CDM)-based transmission diversity method. The radio transmitter codes transmission data into a plurality of time-space codes, generates spread signals by respectively mapping a plurality of spread codes and the time-space codes, and transmits the spread signals via a plurality of transmission antennae, each of the spread codes containing a combination of codes whose signs are alternately equal and opposite in units of specific spreading lengths. Accordingly, it is possible to transmit data without a feedback of control information from a radio receiver.
    • 提供了根据正交频分复用码分多址(OFDM-CDM)的移动通信系统中使用的无线发送装置和方法,无线接收装置和方法,发送和接收方法以及记录介质, 基于传输的分集方法。 无线电发射机将传输数据编码成多个时空码,通过分别映射多个扩展码和时间空间码产生扩展信号,并经由多个发射天线发射扩展信号,每个扩展码 包含符号交替相等并且以特定扩展长度为单位的代码的组合。 因此,可以从无线电接收机发送没有控制信息的反馈的数据。