We report on the absolute calibration of a CCD camera by exploiting quantum correlation. This novel method exploits a certain number of spatial pairwise quantum correlated modes produced by spontaneous parametric-down-conversion. We develop a measurement model accounting for all the uncertainty contributions, and we reach the relative uncertainty of 0.3% in low photon flux regime. This represents a significant step forward for the characterizaion of (scientific) CCDs used in mesoscopic light regime.
PACS numbers: Valid PACS appear hereIntroduction. The development of quantum metrology, imaging and sensing [1-6] based on quantum optical states aim to reach sensitivity beyond classical limits. For this reason it requires new detection strategies in the low light intensity regime (down to few photons), that are far from the ones where traditional radiometry operates [7]. Development of dedicated methods for absolute calibration of detectors in this context is therefore necessary, as it is widely recognised inside the radiometric community [8]. Some specific activities in this context are already on-going [9, 10], in particular related to the calibration of single-photon detectors exploiting the Klyshko's twinphoton technique [11][12][13][14][15][16][17][18] and its developments [19][20][21][22][23][24][25].In particular, demand for precise calibration of detectors both in mesoscopic light regime it is relevant not only from the point of view of the development of quantum technologies, but also for establishing a connection between the light intensity level typical of classical radiometric measurements and the quantum radiometry operating at single-photon level [8, 9]. Quantum correlations in twin beams offer an opportunity for reaching this goal, as discussed in [26][27][28][29].In [30] we realized the first absolute calibration of a standard CCD camera by exploiting bright squeezed vacuum. Standard CCD cameras, i.e. without any avalanche electro-multiplication, are able to count the number of generated photo-electron in each pixels for a given exposure time with a read-out noise ∆ RN of few photoelectron (for top-level devices), independent of the exposure time. However, a single photon can not be distinguished from the noise and the time resolution does not allow time tagging and coincidence of photon arrivals, instead the signal is proportional to the intensity (analog regime). If a light signal generate N photo-electron, under the condition ∆ RN << N 1/2 , sub-shot-noise sensitivity can be achieved [31][32][33], a properties that has been used also for quantum enhanced sensing and imaging protocols [2,33].The method in [30] is based on the sub-shot-noise measurement of photon number correlation between a pair