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单光子探测器日益广泛地应用于科学研究的各个领域,精确地标定其量子效率成为应用的先决条件。我们首次实现了单光子探测器量子效率自绝对标定的原理性实验,即只利用待测探测器本身就可以对其量子效率进行绝对标定,而不需要第二个探测器或任何参考标准。该方法基于自发参量下转换产生的纠缠光子对的时间关联性,在信号光子和闲散光子之间引入延时,由单光子计数率和符合计数率测得探测器的量子效率。  相似文献   
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We report an experimental demonstration of two-dimensional(2D) lensless ghost imaging with true thermal light. An electrodeless discharge lamp with a higher light intensity than the hollow cathode lamp used before is employed as a light source. The main problem encountered by the 2D lensless ghost imaging with true thermal light is that its coherence time is much shorter than the resolution time of the detection system. To overcome this difficulty we derive a method based on the relationship between the true and measured values of the second-order optical intensity correlation, by which means the visibility of the ghost image can be dramatically enhanced. This method would also be suitable for ghost imaging with natural sunlight.  相似文献   
3.
Third-order Hanbrury Brown–Twiss and double-slit interference experiments with a pseudo-thermal light are performed by recording intensities in single, double and triple optical paths, respectively. The experimental results verifies the theoretical prediction that the indispensable condition for achieving a interference pattern or ghost image in Nth-order intensity correlation measurements is the synchronous detection of the same light field by each reference detector, no matter the intensities recorded in one, or two, or N optical paths. It is shown that, when the reference detectors are scanned in the opposite directions, the visibility and resolution of the third-order spatial correlation function of thermal light is much better than that scanned in the same direction, but it is no use for obtaining the Nth-order interference pattern or ghost image in the thermal Nth-order interference or ghost imaging.  相似文献   
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