基于单模光纤的分布式温度传感器研制

在对光纤背向喇曼散射温度效应理论分析的基础上,研制了基于单模光纤的5km分布式温度传感器。实验比较了温度传感解调方法,选择反斯托克斯(Anti-Stokes)和斯托克斯(Stokes)背向喇曼散射光强度比值进行解调。介绍了系统的硬件组成和软件实现。实验表明,系统能精确地进行分布式测温,温度分辨率为1℃,空间分辨率为2m。     

一种提高分布式光纤测温系统空间分辨率的线性修正算法

由于分布式光纤喇曼测温系统带宽不足,导致系统的空间分辨率低;当光纤的感温区域长度接近空间分辨率的时候,系统温度响应幅值不够,导致测温不准.为解决此问题,本文提出了一种线性修正算法;在分析温度与喇曼比值关系及系统的频率响应特性的基础上,建立了该算法的数学模型,搭建了基于单模光纤的10km分布式测温系统,并利用该算法进行了相关测温实验.实验结果与理论分析一致,该算法能有效修正3～6m光纤的温度响应幅值,使系统测温准确度达1℃,测量时间为40s.本算法在不增加效系统成本的同时,克服了系统带宽不足,优化了空间分辨率、温度分辨率及测量时间.     

一种提高分布式光纤测温系统空间分辨率的线性修正算法

由于分布式光纤喇曼测温系统带宽不足,导致系统的空间分辨率低;当光纤的感温区域长度接近空间分辨率的时候,系统温度响应幅值不够,导致测温不准.为解决此问题,本文提出了一种线性修正算法;在分析温度与喇曼比值关系及系统的频率响应特性的基础上,建立了该算法的数学模型,搭建了基于单模光纤的10 km分布式测温系统,并利用该算法进行了相关测温实验.实验结果与理论分析一致,该算法能有效修正3~6 m光纤的温度响应幅值,使系统测温准确度达1℃,测量时间为40 s.本算法在不增加效系统成本的同时,克服了系统带宽不足,优化了空间分辨率、温度分辨率及测量时间.     

基于误差补偿的分布式喇曼温度传感器(英文)

基于分布式喇曼传感器,对斯托克斯光和反斯托克斯光两路信号的同步问题进行了合理假设,并给出相应的补偿方法.为了进一步提高解调温度的准确度,采用温度解调系统及温度解调软件对实验系统收集到的数据进行分析.给出了实际开发分布式喇曼传感系统中补偿后离散式的温度解调算法,对该算法解调出来的温度进行实验测试.结果表明:解调温度的误差和监测点到光纤光注射端的距离及相应监测点待解调的温度值均有线性关系.该温度传感器空间分辨率达1m,对于整个2km的探测光纤,即使考虑到温控箱拥有0.5℃左右温度误差,整个实验系统的温度解调误差也在1℃左右.     

光纤分布式测温系统中基于迭代法的高准确度温度解调算法

提出了一种利用喇曼散射原理的光纤分布式测温系统中基于迭代的高准确度温度解调算法.针对于常规的反斯托克斯-斯托克斯双光路比值的温度解调算法,该迭代算法进一步校正了光纤中双光路衰减系数差对温度敏感带来的温度测量误差,尤其适用于中距离且温度场复杂的测温环境,实现了高准确度的温度测量.通过理论分析确定了该迭代法的迭代格式,测量了相应的光纤参量,并在传感样机上编写相应的代码通过实验予以验证,在0～90℃温度范围,5km测量长度输出的测温曲线符合预期的测温效果.     

光纤分布式测温系统中基于迭代法的高准确度温度解调算法

提出了一种利用喇曼散射原理的光纤分布式测温系统中基于迭代的高准确度温度解调算法.针对于常规的反斯托克斯-斯托克斯双光路比值的温度解调算法,该迭代算法进一步校正了光纤中双光路衰减系数差对温度敏感带来的温度测量误差,尤其适用于中距离且温度场复杂的测温环境,实现了高准确度的温度测量.通过理论分析确定了该迭代法的迭代格式,测量了相应的光纤参量,并在传感样机上编写相应的代码通过实验予以验证,在0~90℃温度范围,5 km测量长度输出的测温曲线符合预期的测温效果.     

分布式光纤温度传感器系统分辨率确定的理论分析

本文对基于反斯托克斯/斯托克斯比值的分布式光纤温度传感器系统的分辨率,即温度分辨率、空间分辨率和时间分辨率的确定进行了全面而深入的研究,首次用一个数学表达式揭示了三个分辨率的关系。     

光纤背向激光自发喇曼散射的温度效应研究

从理论和实验上研究了光纤背向激光自发喇曼散射的温度效应.光纤背向激光自发反斯托克斯喇曼散射、斯托克斯喇曼散射光的相对强度正比于光纤分子上、下能级粒子数的布居,依赖于温度.由于实际系统中,作为分光用的干涉滤光片不可能完全隔离背向瑞利散射光,因此,实际系统温度曲线比理论曲线低,本文给出了理论修正公式,提出了附加修正项,它与隔离度和波长有关.     

LDS751染料的受激喇曼散射

报道了用532nm激光抽运LDS751染料产生720—780nm可调谐染料激光输出的同时,观察到喇曼频移为102和45cm-1的反斯托克斯线,前者谱线较强,后者较弱.与这两条强线对应的斯托克斯线未能观察到.另外,还观察到喇曼频移为34cm-1的一级和二级斯托克斯线与反斯托克斯线 关键词： LDS751染料 受激喇曼散射 喇曼位移 斯托克斯线 反斯托克斯线     

高效率599 nm Ba(NO3)2外腔喇曼激光器

橘黄色波段固体激光器在基于荧光探测的生物医学诊断和显示等众多方面有着广泛的实际应用. 报道了利用532 nm的Nd∶YAG倍频激光抽运外置喇曼腔内的硝酸钡晶体,获得高效率的599 nm橘黄色喇曼激光的实验结果.对外置喇曼腔实验装置和运转参量进行了优化,喇曼振荡腔由对二阶斯托克斯光有最优化反射率的腔镜构成,对实验中所得到的二阶斯托克斯喇曼激光脉宽压缩及出现双尖峰的现象进行了分析.当抽运光功率达到4.1 W时,获得二阶斯托克斯喇曼激光功率为710 mW,输出光中心波长为599.38 nm,半峰全宽（FWHM）为1.1 nm,激光器最大光光转换效率为17.5%,斜率效率为24.8%.     

新颖透射式分辨率板

回顾国内目前常的ＷＴ１００５－６２透射式分辨率板的情况，指出该分辨率板所存在的缺陷。在此基础上，引入一种国外普遍使用的新颖的透射式分辨率板，并简单介绍的性能和应用情况。     

Performance testing of a long-strip two-end readout multi-gap resistive plate chamber

Multi-gap Resistive Plate Chamber (MRPC) is a new generation of gas detector with good tim-ing and spacial resolution, whose technique is widely applied in some recent high energy (nuclear) physics experiments. In this letter, we report a long-strip two-end readout MRPC and its test beam performance. The measurements show that the long-strip performs a transmission line characteristic and the impedance is independent of the length of strip. The MRPC module we developed is presented to gain a timing resolution of～80 ps and a spacial resolution of ～6.4 mm. The possible application of the MRPC is also discussed.     

Performance testing of a long-strip two-end readout multi-gap resistive plate chamber

Multi-gap Resistive Plate Chamber （MRPC） is a new generation of gas detector with good timing and spacial resolution, whose technique is widely applied in some recent high energy （nuclear） physics experiments. In this letter, we report a long-strip two-end readout MRPC and its test beam performance. The measurements show that the long-strip performs a transmission line characteristic and the impedance is independent of the length of strip. The MRPC module we developed is presented to gain a timing resolution of -80 ps and a spacial resolution of -6.4 mm. The possible application of the MRPC is also discussed.     

铅-闪烁光纤夹层电磁量能器的角分辨研究

深入讨论了如何提高铅--闪烁光纤夹层电磁量能器角分辨的分析方法. 用MC方法模拟量能器对不同能量光子事例的响应, 得到了量能器电磁簇射位置测量误差函数; 通过量能器束流测试数据分析, 证明用每层所有测量单元计算该层重心、所有18层做方向重建、并运用误差函数来拟合入射方向, 能够从分析角度显著地改善量能器的角分辨.     

A digital image analysis method for diagnostic ultrasound calibration

Acoustic test objects are commonly used for quality assurance testing of diagnostic ultrasound machines. However, the accompanying calibration protocols rely heavily on the judgment of the sonographer, are dependent on machine settings and are semi-quantitative. In the current study, two unique test objects and protocols were designed to quantitatively determine diagnostic ultrasound parameters, namely axial resolution and geometric uniformity, and lateral resolution and geometric uniformity of the ultrasound field. The effect of focal zone, signal gain, and distance from the ultrasound probe on these parameters was assessed. The investigation was performed using a typical low-frequency diagnostic unit equipped with a 7.5 MHz linear pulse–echo probe. Results underline the need to ensure that sensitivity of routine testing regimes is adequate for the measurements to be made. This study is a preliminary part of a larger project developing an ultrasound technique to be used as an engineering design tool in a non-clinical industrial setting for quality assurance testing of total knee replacements immersed in water.     

Timing characteristics of the scintillation response of Gd3Al2Ga3O12:Ce and Gd3Al2.6Ga2.4O12:Ce single crystal scintillators

The timing characteristics of scintillation response of Czochralski-grown Gd₃Al₂Ga₃O₁₂:Ce and Gd₃Al_2.6Ga_2.4O₁₂:Ce single crystals were compared. The photoelectron yield, scintillation decay times, and coincidence time resolution were measured. At 662 keV γ-rays, the photoelectron yield of 6200 phe MeV⁻¹ obtained for Gd₃Al₂Ga₃O₁₂:Ce is higher than that of 4970 phe MeV⁻¹ obtained for Gd₃Al_2.6Ga_2.4O₁₂:Ce, while an inferior energy resolution of the former (7.2% vs. 5.6%) is observed. Scintillation decays are approximated by sum of exponentials with the dominant fast component decay time and its relative intensity of 89 ns (73%) for Gd₃Al₂Ga₃O₁₂:Ce and 136 ns (69%) for Gd₃Al_2.6Ga_2.4O₁₂:Ce. The coincidence time resolution obtained for Gd₃Al₂Ga₃O₁₂:Ce is superior than that of Gd₃Al_2.6Ga_2.4O₁₂:Ce. The normalized time resolution was also discussed in terms of a number of photoelectrons and decay characteristics of the light pulse.     

X射线皮秒变象管扫描相机时空分辨率测量

X射线皮秒变象管扫描相机是一种应用变象管技术测量X射线波段脉冲辐射而能达到皮秒级时间分辨率和微米级空间分辨率的时空测试系统,是高功率激光打靶产生等离子体诊断的有力工具。时间分辨率和空间分辨率是X射线皮秒变象管扫描相机最基本的性能参数。这些参数的测量有其不同于可见光扫描相机的特殊性。     

Scintillation timing characteristics of (La,Gd)2Si2O7:Ce and Gd2SiO5:Ce single crystal scintillators: A comparative study

The scintillation timing characteristics of (La,Gd)₂Si₂O₇:Ce (GPSLa23.5%:Ce) single crystal were studied and compared with Gd₂SiO₅:Ce (GSO:Ce) single crystal. The photoelectron yield, scintillation decay times and coincidence time resolution were measured. At 511 keV γ-rays, the photoelectron yield of 10,770 ± 500 phe MeV⁻¹ and energy resolution of 5.4 ± 0.2% obtained for GPSLa23.5%:Ce are much better than those of 3350 ± 160 phe MeV⁻¹ and 7.8 ± 0.3% obtained for GSO:Ce. The scintillation decay time profile was measured by the time-correlated single photon counting technique using a fast-slow coincidence setup. In both materials the comparable rise times of several nanoseconds are present. The fast component decay time of 56 ns with relative intensity of 49% obtained for GPSLa23.5%:Ce is inferior to that of 32 ns(88%) obtained for GSO:Ce. Consequently, the coincidence time resolution of GPSLa23.5%:Ce is slightly worse than that of GSO:Ce. The normalized time resolution was also discussed in terms of a number of photoelectrons and decay time of the scintillation pulse.     

超快电子衍射系统的时间空间分辨能力研究及其优化

超快电子衍射技术是研究物质瞬态结构变化及超快结构动力学的有效手段.研制了国内第一套同时具有超快时间分辨及超高空间分辨能力的超快电子衍射系统,并研究了在该超快电子衍射系统上实现超快时间分辨及超高空间分辨能力的技术手段及其优化方法.实验结果表明：经过优化后该系统可以具有优于500 fs的时间分辨能力,其空间分辨能力达到0.04%的衍射峰位置变化,对应的晶面变化为0.0005?.该系统可以为实时测量超快光脉冲激发的物质瞬态结构变化,特别是为研究晶体材料的超快动力学行为提供了强有力的实验工具. 关键词： 超快电子衍射 空间分辨 时间分辨     

BES实验数据离线刻度

概述了北京谱仪(BES)各子探测器的实验离线数据刻度,包括主漂移室、飞行时间计数器、簇射计数器和μ子鉴别器.给出了BES1994年D_s运行期间的探测器运行性能,以及数据质量情况.