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    • 4. 发明申请
    • High-resolution fiber laser sensor
    • US20060013534A1
    • 2006-01-19
    • US10512574
    • 2003-04-29
    • Klaus BohnertKarim HaroudAndreas FrankHubert Brandle
    • Klaus BohnertKarim HaroudAndreas FrankHubert Brandle
    • G02B6/34
    • H01S3/0675G01D5/344G01L1/246G01L9/0079G01L11/025H01S3/06712H01S3/08031H01S3/1053
    • A high-resolution fiber laser sensor for measuring a quantity to be measured M has a pumping light source (2), a fiber laser (1) and a detection/evaluating unit (3). The fiber laser (1) has: a birefringent first end reflector (11), a second end reflector (12), a laser-amplifying fiber (13), a sensor fiber (14) and a means for mode coupling (15). The laser-amplifying fiber (13), the sensor fiber (14) and the means for mode coupling (15) are arranged between the end reflectors (11, 12). In the fiber laser (1), light is capable of propagating in two optical states (x, y; LP′01, LP′11) which are orthogonal to one another due to their polarization and/or their transversal space structure. The orthogonal optical states (x, y; LP′01, LP′11) can be coupled to one another by the means for mode coupling (15). In the fiber laser (1), a number of longitudinal modes (LMxp, LMxp+1 . . . , LMyq, LMyq+1 . . . ; LM01p, LM01p+1 . . . , LM11q, LM11q+1 . . . ) are capable of oscillating in each of the two optical states (x, y; LP′01, LP′11). In the sensor fiber (14) a change in the birefringence for the two orthogonal optical states (x, y; LP′01, LP′11) can be achieved by interaction of the quantity to be measured (M) with the sensor fiber (14). The change in the birefringence results in a change in the beat frequencies in the laser emission. Due to the fact that the first end reflector (11) is detuned with respect to the second end reflector (12), it is possible to detect individual polarization mode beat signals instead of one beat signal which consists of a number of degenerated PMB signals and is, therefore, broadened. A high sensor resolution is achieved.
    • 5. 发明授权
    • Electro-optical voltage sensor for high voltages
    • 用于高电压的电光电压传感器
    • US06876188B2
    • 2005-04-05
    • US10805517
    • 2004-03-22
    • Klaus BohnertAndreas FrankHubert Brändle
    • Klaus BohnertAndreas FrankHubert Brändle
    • G01R15/24G01R19/00G01R31/00
    • G01R15/242G01R15/247G01R19/0084
    • The voltage sensor for measurement of a voltage V, which is present between two electrodes (3, 4) and generates an electric field E, comprises at least two layers (1a, 2a) made of electro-optically active material and being arranged along a light path (5). Through the layers there passes a light beam, the phase and/or state of polarization of which is influenced on account of the electro-optical effect. The orientation of the electro-optically active layers (1a, 2a) relative to the light path and the electric field E is chosen in such a way, that the influencing of the light (5) in the second layer (2a) counteracts the influencing of the light (5) in the first layer (1a). In this way, it is possible to realize a sensor with a high half wave voltage, so that high voltages V can be measured unambiguously. A plurality of first and second electro-optically active layers are advantageously arranged between the electrodes (3, 4).
    • 用于测量存在于两个电极(3,4)之间并产生电场E的电压V的电压传感器包括至少两层由电光活性材料制成的层(1a,2a),沿着 光路(5)。 通过这些层,通过光束,由于电光效应影响其相位和/或其极化状态。 以这样的方式选择电光活性层(1a,2a)相对于光路和电场E的取向,使得第二层(2a)中的光(5)的影响抵消影响 的第一层(1a)中的光(5)。 以这种方式,可以实现具有高半波电压的传感器,从而可以明确地测量高电压V. 多个第一和第二电光活性层有利地布置在电极(3,4)之间。
    • 7. 发明授权
    • Temperature-compensated electro-optical voltage sensor
    • 温度补偿电光电压传感器
    • US06885182B2
    • 2005-04-26
    • US10804160
    • 2004-03-19
    • Klaus BohnertAndreas FrankHubert Brändle
    • Klaus BohnertAndreas FrankHubert Brändle
    • G01R15/24G01R19/00
    • G01R15/242
    • The electra-optical voltage sensor has an electra-optically active medium and a distance medium between two electrodes, between which the voltage V to be measured is present. The media and the thicknesses d1, d2 of the media are chosen in such a way that the measured voltage signal has no temperature dependence. By way of example, the thicknesses d1, d2 are chosen in such a way that the influence of the temperature dependences of critical electra-optical coefficients and dielectric constants of the media on the voltage signal cancel one another out. The two media are advantageously arranged in the form of a rod, comprising an alternating arrangement of cylindrical elements of the two media, between the electrodes. BGO and fused silica may advantageously be used as media. The sensor is preferably cast in silicone. It is possible to realize a mechanically stable, temperature-stabilized voltage sensor with low reflection losses, a large half wave voltage and a small sensitivity toward disturbances of the electric field.
    • 电光学电压传感器具有电光活性介质和两个电极之间的距离介质,在两个电极之间存在要测量的电压V. 介质和介质的厚度d 1,D 2,N 2被选择为使得所测量的电压信号没有温度依赖性。 作为示例,选择厚度d 1,d 2 2,使得对临界电光学系数和介电常数的温度依赖性的影响 介质上的电压信号相互抵消。 两个介质有利地以杆的形式布置,包括两个介质的圆柱形元件在电极之间的交替布置。 BGO和熔融石英可有利地用作介质。 该传感器优选用硅树脂铸造。 可以实现具有低反射损耗,大的半波电压和对电场干扰的小灵敏度的机械稳定的温度稳定的电压传感器。