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    • 1. 发明授权
    • Ellipsoidal raman signal amplifier
    • 椭圆形拉曼信号放大器
    • US08824042B2
    • 2014-09-02
    • US13564461
    • 2012-08-01
    • James M. TedescoJoseph B. Slater
    • James M. TedescoJoseph B. Slater
    • H01S3/30G02B5/10
    • G01N21/65G01J3/021G01J3/44H01S3/08H01S3/08095H01S3/305H01S3/307
    • Raman signal amplification apparatus comprises an ellipsoidal reflector providing a first real focus f1, and second real or virtual focus f2, both foci being situated within a sample volume. When an input laser excitation beam having an initial numerical aperture (NA) is focused onto one of the foci, the beam is reflected by the reflector and refocused onto alternating foci, such that the NA of the reflected optical path progressively increases for higher efficiency collection of Raman emissions from the multiple foci. The ellipsoidal reflector may be a half section providing a single real focus f1, with a flat reflector producing a mirror image of the ellipsoidal reflector, such that f2 is a virtual focus occupying the same point as f1. Alternatively, the ellipsoidal reflector may have a first half section with a first real focus f1 and a second half section with a second real focus f2.
    • 拉曼信号放大装置包括提供第一实际焦点f1的椭球反射器和第二实际或虚拟焦点f2,两个焦点位于样本体积内。 当具有初始数值孔径(NA)的输入激光激发光束聚焦到焦点之一时,光束被反射器反射并重新聚焦到交替的焦点上,使得反射光路的NA逐渐增加以获得更高的效率 的多焦点的拉曼散射。 椭圆反射器可以是提供单个实际焦点f1的半部分,平面反射器产生椭圆反射体的镜像,使得f2是与f1相同的点。 或者,椭球反射器可以具有带有第一实际焦点f1的第一半部分和具有第二实心f2的第二半部分。
    • 3. 发明申请
    • RAMAN PROBE CONFIGURED FOR LOW-CONCENTRATION MEASUREMENTS
    • 拉曼探头配置低浓度测量
    • US20080180663A1
    • 2008-07-31
    • US11873718
    • 2007-10-17
    • James M. TedescoJoseph B. Slater
    • James M. TedescoJoseph B. Slater
    • G01J3/44
    • G01J3/44G01J3/02G01J3/0208G01J3/021G01J3/0218G01J3/0227G01J3/0262
    • Raman measurement apparatus optimized for gaseous and other low-concentration samples includes a focusing objective that uses only first-surface mirrors instead of lenses, thereby dramatically reducing background noise. In the preferred embodiment, the focusing and collimation functions performed by the objective section are performed by an off-axis parabolic mirror. A spherical first-surface mirror opposing the parabolic mirror re-images the counter-propagating beam back through the same focus for re-collimation by the parabolic mirror. A probe-head section operative to generate the counter-propagating beam has substrates and surfaces arranged such that the excitation beam does not pass through any substrates after it is filtered by the bandpass coating, thereby further decreasing background signals. Additionally, when the objective section includes the opposing spherical mirror, the excitation beam is collected substantially in its entirety and neutralized out of the collection path by the probe-head section.
    • 针对气态和其他低浓度样品优化的拉曼测量装置包括仅使用第一表面镜而不是透镜的聚焦目标,从而显着降低背景噪声。 在优选实施例中,由目标部分执行的聚焦和准直功能由离轴抛物面镜执行。 与抛物面镜相对的球形第一表面镜将通过相同的焦点重新对反向传播的光束进行反像,以通过抛物面反射镜进行再准直。 可操作以产生反向传播光束的探针头部分具有布置成使得激发光束在被带通涂层过滤之后不通过任何基底的基板和表面,从而进一步减小背景信号。 此外,当目标部分包括相对的球面镜时,基本上整体地收集激发光束,并且通过探头部被中心到收集路径之外。
    • 5. 发明授权
    • Optical probe focusing apparatus and method
    • 光探头聚焦装置及方法
    • US06757060B2
    • 2004-06-29
    • US10350499
    • 2003-01-24
    • Kevin DavisJoseph B. Slater
    • Kevin DavisJoseph B. Slater
    • G01J344
    • G01N21/65G01N21/645
    • Disclosed is a method of positioning a focused image within a sampled medium in an optical measurement probe of the type wherein a focused sampling image is transmitted through a window having a surface facing a sampled medium. A test medium is measured, preferably through the window, and the magnitude of an optical signal associated with the test medium is then compared to the magnitude of an optical signal associated with the window, and the result of the comparison is used to position the focused image. Typically, the magnitudes of optical signals are representative or Raman scattering or another wavelength-selective radiative sampling process such as fluorescence detection. The method is not limited in terms of window composition, and is compatible with sapphire windows commonly used in industry. Nor is the invention limited in terms of test medium though, in the preferred embodiment a fluid hydrocarbon such as isopropyl alcohol is used.
    • 公开了一种将聚焦图像定位在采样介质中的光学测量探针中的方法,其中聚焦采样图像通过具有面向采样介质的表面的窗口传输。 最好通过窗口测量测试介质,然后将与测试介质相关联的光学信号的大小与与窗口相关联的光学信号的幅度进行比较,并且比较结果用于定位聚焦 图片。 通常,光信号的大小是代表性的或拉曼散射或另一种波长选择性辐射采样过程,例如荧光检测。 该方法不限于窗口组成,并且与工业中通常使用的蓝宝石窗口兼容。 本发明也不限于测试介质,尽管在优选实施方案中使用流化烃如异丙醇。
    • 6. 发明授权
    • Optical measurement probe with leak minimization features suited to process control applications
    • 具有适用于过程控制应用的泄漏最小化特性的光学测量探头
    • US06603545B2
    • 2003-08-05
    • US09871045
    • 2001-05-31
    • Joseph B. Slater
    • Joseph B. Slater
    • G01J344
    • G01N21/8507
    • Various optical probe configurations are particularly suited to the monitoring of a process flow through the wall of a containment vessel. A probe body extends through, and is sealed to, the wall of the containment vessel. The probe body has an inner wall terminating in a distal end with a window, enabling light from the process flow to pass therethrough and into the probe body. In one embodiment, one or more lenses are disposed within the probe body to focus the light into a focal point, and a restriction of the inner wall of the probe body is used to create a narrow aperture at the focal point. In an alternative embodiment, a plug transparent to the light of interest is sealed to the inner wall of the probe body. As a further alternative, the elements include a second window creating a cavity with the distal window, and a port into the cavity accessible from outside the window for sampling purposes. Although these embodiments are referred to as ‘alternative,’ they may be used in combination as well as separately. Indeed, all three embodiments may be used simultaneously for increased integrity. In addition, although the probe body is presumed to carry light in both directions for excitation and collection, invention is not limited in this regard or the way in which light is carried to, or from, the body itself. That is, a probe according to the invention may be used only for excitation or collection, and optical fibers may, or may not, be used between the body and a source or radiation and/or analysis means.
    • 各种光学探针配置特别适用于监控通过安全壳的壁的工艺流程。 探针主体延伸穿过并密封到安全壳的壁上。 探针主体具有终止于具有窗口的远端的内壁,使得来自过程流的光能够通过其并进入探针体。 在一个实施例中,一个或多个透镜设置在探针体内以将光聚焦到焦点中,并且使用探针体的内壁的限制在焦点处产生窄孔。 在替代实施例中,对感兴趣的光线透明的塞子被密封到探针主体的内壁。 作为另一替代方案,元件包括产生具有远端窗口的空腔的第二窗口和从外部窗口可进入取样目的的入口。 虽然这些实施例被称为“替代”,但是它们可以组合使用,也可以单独使用,实际上,所有三个实施例可以同时使用以提高完整性。另外,虽然探针体被推定为在两个方向上携带光 对于激发和收集,本发明不限于此,也不限于将光传送到身体或从身体本身的方式。也就是说,根据本发明的探针可以仅用于激发或收集,并且光纤 可以或可以不在身体和源或辐射和/或分析手段之间使用。
    • 7. 发明授权
    • Wavelength calibration and tracking methods and apparatus
    • 波长校准和跟踪方法和装置
    • US6067156A
    • 2000-05-23
    • US79772
    • 1998-05-15
    • Joseph B. SlaterJames M. Tedesco
    • Joseph B. SlaterJames M. Tedesco
    • G01J3/28G01J3/44G01D18/00G01J3/30
    • G01J3/44G01J3/28G01J2003/2866
    • Calibration wavelengths are injected into an optical detection system preferably at a point after laser rejection filtration, enabling the known spectral content of the calibration radiation to pass through and into a spectrograph. In a preferred embodiment, at least some of the wavelengths used for calibration are derived through the excitation of a noble gas such as neon, thereby conveniently and economically providing a full-spectrum calibration line set. The feed from the laser source used to illuminate the sample is also preferably introduced into the collection path, enabling both the calibration wavelengths and laser line to be detected and used in calibration. The invention is applicable to spectral analysis systems in general, including non-Raman systems and systems which do not require a laser notch pre-filter stage.
    • 校准波长优选地在激光去除过滤之后的点被注入到光学检测系统中,使得校准辐射的已知光谱含量能够通过并进入光谱仪。 在优选实施例中,用于校准的至少一些波长是通过激发诸如氖的惰性气体得到的,从而方便和经济地提供了全谱校准线组。 来自用于照亮样品的激光源的进料也优选地被引入到收集路径中,使得能够检测校准波长和激光线,并在校准中使用。 本发明一般适用于光谱分析系统,包括不需要激光陷波预滤波器级的非拉曼系统和系统。
    • 10. 发明申请
    • ELLIPSOIDAL RAMAN SIGNAL AMPLIFIER
    • ELLIPSOIDAL拉曼信号放大器
    • US20140036347A1
    • 2014-02-06
    • US13564461
    • 2012-08-01
    • James M. TedescoJoseph B. Slater
    • James M. TedescoJoseph B. Slater
    • H01S3/30
    • G01N21/65G01J3/021G01J3/44H01S3/08H01S3/08095H01S3/305H01S3/307
    • Raman signal amplification apparatus comprises an ellipsoidal reflector providing a first real focus f1, and second real or virtual focus f2, both foci being situated within a sample volume. When an input laser excitation beam having an initial numerical aperture (NA) is focused onto one of the foci, the beam is reflected by the reflector and refocused onto alternating foci, such that the NA of the reflected optical path progressively increases for higher efficiency collection of Raman emissions from the multiple foci. The ellipsoidal reflector may be a half section providing a single real focus f1, with a flat reflector producing a mirror image of the ellipsoidal reflector, such that f2 is a virtual focus occupying the same point as f1. Alternatively, the ellipsoidal reflector may have a first half section with a first real focus f1 and a second half section with a second real focus f2.
    • 拉曼信号放大装置包括提供第一实际焦点f1的椭球反射器和第二实际或虚拟焦点f2,两个焦点位于样本体积内。 当具有初始数值孔径(NA)的输入激光激发光束聚焦到焦点之一时,光束被反射器反射并重新聚焦到交替的焦点上,使得反射光路的NA逐渐增加以获得更高的效率 的多焦点的拉曼散射。 椭圆反射器可以是提供单个实际焦点f1的半部分,平面反射器产生椭圆反射体的镜像,使得f2是与f1相同的点。 或者,椭球反射器可以具有带有第一实际焦点f1的第一半部分和具有第二实心f2的第二半部分。