共查询到20条相似文献,搜索用时 109 毫秒
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在不改变荧光分光光度计的结构和影响仪器原有功能的条件下,对荧光仪的光路进行简单的设置,利用白纸导光,即可使原有的荧光分光光度计同时具有与紫外-可见分光光度计相同的功能.利用该简便方法,在荧光分光光度计上分别对滤光片和叶片进行透射光谱和反射光谱的测绘,并与紫外-可见分光光度计上的测绘结果进行比较,两者基本一致,证明该法是可行的. 相似文献
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介绍一种可工作于MC和CRT双操作模式的荧光分光光度计,给出了其工作原理和MC模式下的软硬件实现方案。该仪器可方便的在两种操作模式之间切换。 相似文献
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美国瓦里安技术中国有限公司 《现代科学仪器》2001,(1):66-67
50多年来 ,Cary品牌在分光光度计产品中一直代表着性能优异、质量上乘。最新推出的CaryEclipse荧光分光光度计继承了这一Cary传统。Eclipse的闪烁式氙灯技术、插入即可自动识别的各种附件、出色的技术指标及直观、功能明确的操作软件充分体现了Cary品牌的高品质。1 出色的仪器设计CaryEclipse荧光分光光度计的设计是基于最新的光学与电子学的技术发展 ,将光谱校正功能 ,发射与激发滤光片 ,以及扩展量程的光电倍增管检测器等都做为仪器标准配置 ,从而可保证同一台仪器满足多种应用。另外 ,Ecl… 相似文献
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为了解决高通量数字聚合酶链式反应(dPCR)基因芯片荧光激发问题,设计了一套荧光激发测控系统。系统根据荧光染料的激发光谱特性,选择大功率窄带LED作为荧光激发光源,并通过STM32微处理器系统进行控制。该荧光激发系统有FAM、HEX和ROX三个荧光激发通道,各通道LED激发功率能够分别调节。系统最大输出电流为8 A,单通道最大输出功率为3 W,调节精确度1.0%,系统一次可完成dPCR基因芯片9 600个微液滴的荧光激发和采集。测试实验结果表明,系统达到了设计指标和应用需求。 相似文献
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LED作为新兴光源,与传统的白炽灯光源相比,具有很大的优势。衡量其荧光材料发光性能的一个重要参数就是量子效率。为了准确地测量荧光材料的量子效率,提出了一种基于半积分球装置的量子效率测量系统。该系统采用了中心波长为465nm的蓝光LED芯片作为激发光源,与直径为150mm的半积分球和直径为150mm、中心孔直径为8mm的平面反射镜搭配使用,运用光纤和线阵CCD光谱仪采集光谱数据,并进一步计算出量子效率。为了验证系统的有效性,分别采用两种不同的荧光材料对测量系统进行测试,测量结果与厂商所给的数值基本一致。实验结果表明,该测量系统能有效地评估LED中荧光材料的发光性能。 相似文献
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Simultaneous measurement of quantum yield ratio and absorption ratio between acceptor and donor by linearly unmixing excitation–emission spectra 下载免费PDF全文
Quantum yield ratio (QA/QD) and absorption ratio (KA/KD) in all excitation wavelengths used between acceptor and donor are indispensable to quantitative fluorescence resonance energy transfer (FRET) measurement based on linearly unmixing excitation–emission spectra (ExEm‐spFRET). We here describe an approach to simultaneously measure QA/QD and KA/KD values by linearly unmixing the excitation–emission spectra of at least two different donor–acceptor tandem constructs with unknown FRET efficiency. To measure the QA/QD and KA/KD values of Venus (V) to Cerulean (C), we used a wide‐field fluorescence microscope to image living HepG2 cells separately expressing each of four different C–V tandem constructs at different emission wavelengths with 435 nm and 470 nm excitation respectively to obtain the corresponding excitation–emission spectrum (SDA). Every SDA was linearly unmixed into the contributions (weights) of three excitation–emission spectra of donor (WD) and acceptor (WA) as well as donor–acceptor sensitisation (WS). Plot of WS/WD versus WA/WD for the four C–V plasmids from at least 40 cells indicated a linear relationship with 1.865 of absolute intercept (QA/QD) and 0.273 of the reciprocal of slope (KA/KD), which was validated by quantitative FRET measurements adopting 1.865 of QA/QD and 0.273 of KA/KD for C32V, C5V, CVC and VCV constructs respectively in living HepG2 cells. 相似文献
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为了避免用光学干涉法测量自由落体绝对重力过程中落体旋转对测量结果准确度的影响,提出了基于双干涉仪的绝对重力测量方法。介绍了落体旋转影响绝对重力测量结果的机理,提出了对同时测量的两组干涉仪数据进行融合处理的方法。根据预先设定的重力值,双干涉仪中落体上、下反射棱镜光心与质心垂直方向的初始高度差,以及随机生成的每次测量对应的角速度序列和振动引起的上、下干涉仪重力测量偏差序列,进行了仿真计算。结果表明:光心-质心的距离为2.5mm的双干涉仪通过数据融合处理得到的重力测量结果的偏差约为0.5μGal,标准偏差约为0.3μGal,与现有调校落体光心-质心的方法得到的结果相当。选择合适的上、下棱镜光心-质心距离可以更好地消减落体旋转对测量结果的影响,将其分别设计为±3mm时,用双干涉法数据融合得到的重力值偏差小于1μGal,满足相关领域对精密重力测量的需求。 相似文献
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基于双光学频率梳外差原理测距将长模糊距离、高精度和高更新率3个关键测距特性完美结合,使测量性能能够满足航空航天、科学研究和工业生产等众多领域的需求。然而所使用的双光学频率梳的脉冲时域宽度、重复频率及相对差值、脉冲的固有时间抖动等特性都将会影响测距的性能。对基于双光学频率梳外差原理测距进行了全面的理论分析,并数值模拟了数据脉冲宽度、双光学频率梳重复频率差、啁啾参量、定时噪声、脉冲类型等各因素对测距性能的影响。模拟结果在数值上验证了奈奎斯特采样定律对测距精度的显著影响,表明实验中数据脉冲宽度和重频差的选择应严格满足奈奎斯特采样定律;当飞秒脉冲序列存在一定的时间抖动时,重频差越小,测距性能越差;而脉冲的啁啾特性可转化为脉冲宽度的影响,随着啁啾的增大脉冲宽度被压窄,奈奎斯特采样频率对应的重频差临界值也会变小。通过上述数值分析,为研究人员在特定实验条件下优化测距性能提供了重要指导。 相似文献
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Borlinghaus RT 《Microscopy research and technique》2006,69(9):689-692
True confocal microscopy requires point-shaped illumination and detection. To generate an image, a diffraction limited spot is moved over the sample. Single spot scanning has suffered in the past from low image rates; a solution is the employment of very fast scanning devices (resonant scanners) for x-movement. In the process of introducing resonant scanning devices, it was found that both signal yield is improved and bleaching is decreased-in contrary to the assumed performance. This article will show by a simple and well understood model a straightforward explanation for the potential increase of signal yield and decrease in photobleaching. The time that is ruling the dose-rate effects is the effective time; a fluorochrome is illuminated. This time depends on the diameter of the spot that is moved over the sample and the speed at which the spot moves. In essence, the scan process causes a pulsed illumination of the fluorochromes. Various schemes of pulsed illumination are simulated with a fluorescence model. The model includes a dark state, where fluorochromes will exit the fluorescence process and slowly decay back into the ground state. Upon splitting a single dose into two pulses separated by a dark time-reflecting an increased scan speed-the amount of fluorescence emission is increased and bleaching is reduced. These results show a potential increase of fluorescence and a lower photobleaching upon higher scan speed. As illumination during the bleach-phase in a FRAP-experiment is similar to a light pulse, the findings also suggest to critically consider the very beginning of fluorescence recovery in terms of triplet relaxation process that potentially could falsify the measurements. 相似文献