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    • 3. 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
    • Fiber laser pressure sensor
    • 光纤激光压力传感器
    • US06630658B1
    • 2003-10-07
    • US09623048
    • 2000-11-20
    • Klaus BohnertHubert Brandle
    • Klaus BohnertHubert Brandle
    • G01J104
    • G02B6/022G01D5/35316G01D5/3538G01L11/025G02B6/02085G02B6/105
    • The invention relates to a frequency-coded fiber laser pressure sensor (1) which is especially suitable for measuring isotropic pressures in oil wells. The sensor principle provided for in the invention is based on the fact that in a fiber laser (2) doped with Er3+ a monomode or bimodal sensor fiber (5, 5a, 5b) is positioned whose pressure-related birefraction results in a frequency shift and beat frequencies between the orthogonal linear polarisation modes x, y or the spatial modes LP01 and LP11straight line. The beat frequencies are easily measured using a frequency counter (19). Temperature-related variations in birefraction are compensated in a differential arrangement of two sensor fiber segments (5a, 5b). Fiber-integrated Bragg gratings (4a, 4b) with low bandwidths (0.2 nm) are especially suitable as laser end reflectors. The pressure sensor (1) is characterized by a large measurement range (100 Mpa) and a high triggering capacity , (kPa), is readily multiplexed and can be housed in a very compact, light-weight and robust pressure-resistant housing (25).
    • 本发明涉及一种频率编码的光纤激光压力传感器(1),其特别适合于测量油井中的各向同性压力。 在本发明中提供的传感器原理基于以下事实:在掺杂有Er 3+的单模或双峰传感器光纤(5,5a,5b)的光纤激光器(2)中定位其压力相关双折射结果 正交线性偏振模x,y或空间模式LP01和LP11 <直线之间的频移和拍频。 使用频率计数器(19)容易地测量拍频。 温度相关的双折射变化在两个传感器光纤段(5a,5b)的差分布置中被补偿。 具有低带宽(0.2nm)的光纤集成布拉格光栅(4a,4b)特别适用于激光端反射器。 压力传感器(1)的特征在于测量范围大(100Mpa)和高触发能力(kPa)容易复用,并且可以容纳在非常紧凑,重量轻且耐用的耐压外壳(25 )。
    • 6. 发明授权
    • Magneto-optic current sensor having a mechanically stress-free
.lambda./4 element
    • 具有机械无应力的λ/ 4元件的磁光电流传感器
    • US5953121A
    • 1999-09-14
    • US986191
    • 1997-12-05
    • Klaus BohnertHubert BrandleTone Schanke
    • Klaus BohnertHubert BrandleTone Schanke
    • G01R15/24G01B9/02
    • G01R15/246
    • Without special measures, a fiber-optic current sensor coil (11) and fiber-optic .lambda./4 time delay elements (9, 9'), which are connected in series with the current sensor coil (11), are temperature-dependent with respect to a relative phase lag of light passing through. In order to avoid a temperature correction or temperature compensation, the current sensor coils (11) and, if appropriate, also the .lambda./4 time delay elements (9, 9') are annealed, so that virtually no mechanical stresses remain in the optical fibers. The current sensor coil (11) is preferably mounted unrestrained in a capillary (20) filled with a protective gas. The capillary (20) is embedded in a gastight fashion in a potting compound (22) made from polyurethane, and is thus also mechanically protected.
    • 没有特殊措施,与电流传感器线圈(11)串联连接的光纤电流传感器线圈(11)和光纤λ/ 4时间延迟元件(9,9')与温度有关 尊重光通过的相对相位滞后。 为了避免温度校正或温度补偿,电流传感器线圈(11)和(如果适用的话)λ/ 4时间延迟元件(9,9')也被退火,使得实际上没有机械应力残留在光学 纤维。 电流传感器线圈(11)优选地安装在填充有保护气体的毛细管(20)中。 毛细管(20)以气密的方式嵌入由聚氨酯制成的灌封化合物(22)中,因此也被机械地保护。