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High-speed fluorescence lifetime imaging

机译:高速荧光寿命成像

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In Fluorescence Lifetime Imaging (FLIM) the ns fluorescence decay is used for imaging. It yields information about the local environment of the fluorescent molecule and is very well suited for quantitative imaging. FLIM was introduced more than one decade ago now. Most of the implementations of FLIM require comparatively long acquisition times on the order of ten seconds or more. This hampers the use of FLIM for the study of dynamic processes. In FLIM at least one order of magnitude more signal is required than in conventional intensity imaging. Therefore, fast FLIM acquisition rates require efficient detection schemes and detectors. We evaluated the count rate limitation in time gated and TCSPC FLIM of a number of single photon counting detectors. In particular we looked at the performance of a conventional fast head-on PMT (R1894), a GaAs photocathode PMT (H7422P-40) and a single photon counting avalanche photo diode (SPCM-AQR14). The high quantum efficiency GaAs photocathode PMT and avalanche photo diode detectors show lifetime shifts in both time gated detection and in TCSPC starting at a detection count rate of 1 - 2 MHz. The conventional PMT shows lifetime shifts starting at a detection count rate of about 2.5 MHz in TCSPC and at about 6 MHz for the time gated detection system. The detection efficiency of the TCSPC based system goes down rapidly above about 1 MHz due to the dead time of the detection electronics. The time gated detection system shows little or no reduction of the detection efficiency up to detection count rates of 10 MHz with the conventional fast PMT. The time gated-detection system was coupled to a multi-photon excitation microscope. Calcium transients were recorded in cardiac rat myocytes at a 1 Hz frame rate. The system operated at the full repetition rate of the Ti:Sa laser. Here, the frame rate was limited by the maximum count rate of the PMT.
机译:在荧光寿命成像(FLIM)中,ns荧光衰减用于成像。它产生有关荧光分子局部环境的信息,非常适合定量成像。 FLIM是在十多年前推出的。 FLIM的大多数实现都需要相对较长的获取时间,大约十秒或更多。这阻碍了将FLIM用于动态过程的研究。与常规强度成像相比,在FLIM中至少需要多一个数量级的信号。因此,快速的FLIM采集速率需要有效的检测方案和检测器。我们评估了许多单光子计数检测器在时间门控和TCSPC FLIM中的计数率限制。特别是,我们研究了常规快速正面PMT(R1894),GaAs光电阴极PMT(H7422P-40)和单光子计数雪崩光电二极管(SPCM-AQR14)的性能。高量子效率GaAs光电阴极PMT和雪崩光电二极管检测器在时间门控检测和TCSPC中都显示出从1-2 MHz的检测计数率开始的寿命变化。传统的PMT在TCSPC中的检测计数率大约为2.5 MHz,而对于时间门控检测系统则大约为6 MHz,显示出寿命变化。基于TCSPC的系统的检测效率由于检测电子设备的停滞时间而迅速下降到大约1 MHz以上。对于传统的快速PMT,时间门控检测系统在10 MHz的检测计数速率下,检测效率几乎没有降低或没有降低。时间选通检测系统耦合到多光子激发显微镜。在心脏大鼠心肌细胞中以1 Hz帧频记录钙瞬变。该系统以Ti:Sa激光器的完全重复率运行。此处,帧速率受PMT的最大计数速率限制。

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