Abstract
Scalable technologies to characterize the performance of quantum devices are crucial to creating large quantum networks and quantum processing units. Chief among the resources of quantum information processing is entanglement. Here we describe the full temporal and spatial characterization of polarizationentangled photons produced by Spontaneous Parametric Down Conversions using an intensified highspeed optical camera, Tpx3Cam. This novel technique allows for precise determination of Bell inequality parameters with minimal technical overhead, and for new characterization methods for the spatial distribution of entangled quantum information. The fastoptical camera could lead to multiple applications in Quantum Information Science, opening new perspectives for the scalability of quantum experiments.
Introduction
Ever since the original experiments with entangled photons^{1}, photonic entanglement has become a remarkable resource in the development of quantum technologies, including entanglement over longdistance for quantum communication^{2}, entanglement swapping^{3}, teleportation between a photon and an atomic ensemble^{4}, violation of the CHSH (ClauserHorneShimonyHolt) inequality measured over long distances^{5,6} and entanglement of spin waves among four quantum memories^{7}.
The creation of quantum networks of many such quantum devices in which entanglement is shared among multiple network nodes is the next technological frontier for the successful development of these applications. Easytouse, scalable, and compact characterization devices, providing all the information regarding entanglement in nearrealtime are fundamental for further largescale network developments.
Recent developments have shown that spatial characterization of entangled states with singlephoton sensitive cameras provides access to a myriad of new possibilities, such as imaging highdimensional entanglement^{8}, generalized Bell inequalities^{9} and the study of EinsteinPodolskyRosen nonlocalities^{10,11}. However, most of these measurements used resourceintensive methods, such as sequential scanning or multiple standalone detectors. More recent experiments used low noise CCD^{12,13} and electronmultiplying CCD (EMCCD)^{14} cameras to study spatial quantum correlations between twin beams of pulsed parametric downconversion photon sources. In those cases, the temporal resolution was determined by the pulsed nature of the source, albeit the cameras were not operated in the singlephoton regime, as the results required integrating millions of photons per laser pulse. EMCCDs were also used in the singlephoton mode to study spatial correlations using an SPDC source^{15}. However, the exposure time was 33 ms, so albeit the individual single photons were indeed spatially resolved, multiple photon pairs were registered in a single shot. The main motivation in the above studies was a demonstration of subshot noise that can be achieved by exploiting quantum correlations. These experiments did not perform entanglement characterization, as it would require to analyze the pair coincidences.
Early studies of entanglement with modern imagers used an EMCCD camera with an active area of 201 × 201 pixels and frame readoutrate of 5 Hz^{8}. Although the EMCCD quantum efficiency was up to 90%, a long exposure time of about 1 ms was necessary to operate this device at minimum photon rates to avoid multiple photons in the same frame. Furthermore, to achieve singlephoton level sensitivity the EMCCD camera operated at a low temperature of − 85 °C, which is typical for this type of cameras.
Progress on quantum imaging with cameras was achieved using intensified CMOS and CCD cameras^{16,17,18,19,20,21}. Flexible readout architectures allow kHz continuous framing rates in CMOS cameras. Additionally, nanosecond scale time resolution for single photons can be achieved by gating image intensifiers in the cameras. For example, an intensified sCMOS camera was used to observe HongOuMandel interference^{22}, where the entangled photons were collected on a 700 × 22 pixel area at a framing rate of 7 kHz, and their coincidence was ensured using a narrow 40 ns intensifier gate. Photon acquisition statistics can also be enhanced by using multiple triggers during a single frame, so the camera integrates multiple photons within a single acquired image. This approach was employed in^{19}, where the idler photon from an entangled pair was used to gate an intensified CCD camera. Although many thousands of photons were imaged in a single frame of the camera, allowing the spatial characterization of the photon’s angular momentum, the framingrate was only 4 Hz, and the spatial information of the idler photon was not available since it was used for triggering.
This low throughput remains a severe limitation to resolve spatial characterization of entanglement in realtime. Here we show how development from the highenergy physics community, the intensified Tpx3Cam camera^{23} can be converted into a quantum characterization device of photonic polarization entanglement. This setup allows for imaging and timestamping of a continuous stream of entangled photons with an excellent spatial and temporal resolution (55 × 55 μm^{2}, 1.5 ns), providing a high signaltobackground ratio. We emphasize that the Tpx3Cam readout is datadriven, with a high throughput of ≈ 10 M photons per second, which is several orders of magnitude higher than the conventional cameras discussed above. The main advantage of the camera is that it simultaneously gives access to the spatial and temporal information for each recorded photon and, hence, allows to study, at the same time, the spatial and temporal correlations of multiple photons (e.g. pairs, triplets), which was not the case for the experiments mentioned above. In the following, we demonstrate this for the case of spatial characterization of photonic polarization entanglement, which makes use of spatially resolved coincidences of photon pairs.
Experimental Setup
We study the characterization of SPDCbased quantum polarization entanglement using fast 2D imaging with a Tpx3Cam. The experimental layout is shown in Fig. 1.
Entangledphoton source
Our entanglement source (QuTools QuED^{24}) utilizes a blue pump laser diode tuned to wavelength λ = 405 nm, and a pair of Type I noncollinear BBO crystals with optical axes perpendicular to one another to generate signal and idler photons at wavelength λ = 810 nm. The first crystal optical axis and the pump beam define the vertical plane. Owing to Type I phase matching, an incoming photon which is vertically polarized gets downconverted and produces two horizontally polarized photons in the first crystal, whereas a horizontallypolarized photon going through these crystals would get downconverted in the second crystal producing two vertical photons. An additional pair of birefringent crystals ensures maximum spatial overlap of the downconverted photons by pre and postcompensating for differences in effective optical path lengths of signal and idler. The produced state has the form:
Signal and idler photons are spatially separated and collected using singlemode, polarization nonmaintaining fibers, with a linear polarizer, used for projective measurements, before each coupler.
Intensified fastcamera: Tpx3Cam
An intensified camera, Tpx3Cam^{23}, achieves imaging with singlephoton sensitivity when coupled to an image intensifier and allows timestamping of incident photons with 1.5 ns time granulation. The Tpx3Cam consists of a lightsensitive silicon sensor bumpbonded to Timepix3, a timestamping readout chip^{25}. The sensorchip assembly has 256 × 256 pixels of 55 × 55 μm^{2} each. The silicon sensor in the camera has a thin entrance window with an antireflective coating providing excellent quantum efficiency^{26}. The sensor is optimized for emission spectrum of the P47 scintillator^{27}. The nonintensified version of Tpx3Cam has been used before for the velocity mapped ion imaging^{28} while the intensified version of its predecessor, TimepixCam, has previously been used for fluorescent lifetime imaging, which required singlephoton sensitivity, similar to this application^{29}. This is the first time when Tpx3Cam is employed in the singlephoton regime.
The Timepix3 processing electronics in each pixel records the timeofarrival (TOA) of hits that cross a preset threshold and stores it as a timecode in a memory inside the pixel. The timeoverthreshold (TOT) is also recorded, serving as an estimate of the light flux seen by the pixel. The individual pixel dead time is caused by digitization and TOT of measured signal and is of the order of 1 μs. The hit pixel does not affect the performance of other pixels since all pixels in the chip function independently. The Timepix3 readout is datadriven, and only the pixels with signals above the threshold are recorded. The camera can operate continuously and does not require a trigger as the pixels transfer the data asynchronously within microseconds after being hit. The maximum camera throughput is 80 Mpix/s^{23,30}. SPIDR can also accept and time stamp an external trigger pulse, independent of the Timepix3 connection.
The intensifier in front of the camera is an offtheshelf vacuum device^{31}, which consists of a photocathode followed by a chevron microchannel plate (MCP) and fast P47 scintillator with a signal rise time of ~7ns^{32}. Photons are first converted to photoelectrons in the photocathode and then amplified in the MCP before producing a flash of light in the scintillator. The 18 mm diameter scintillator screen is projected on to the 14 × 14 mm^{2} sensor with a relay lens with no magnification^{33}. The quantum efficiency of the photocathode used for the experiments attains ≈ 18% at a wavelength of 810 nm.
The camera was calibrated to equalize the response of all pixels by adjusting the individual pixel thresholds^{34}. After this procedure, the effective threshold to fast light flashes from the intensifier is 600–800 photons per pixel depending on the wavelength. A small (≈0.1%) number of hot pixels was masked to prevent logging high rates of meaningless data.
Experimental Results
Benchmarking: entanglement characterization
Our procedure starts by evaluating the entangled state produced by the source. We assume the state to be in a superposition of two Bellstates of the form:
Using a density matrix \(\rho =\left\psi \right\rangle \left\langle \psi \right\), after projection of the two photons by polarizers with angles α and β, we obtain an expectation value for the measurements of coincidences:
here, the operator \({\widehat{M}}_{\alpha \beta }=\left{V}_{\alpha }{V}_{\beta }\right\rangle \left\langle {V}_{\alpha }{V}_{\beta }\right\) denotes the projection onto a vertical polarization state. In the basis of BBO crystal we have:
with \({c}_{0}=\frac{1\sin 2\theta \cos \delta \cos 2\alpha }{4},{c}_{1}=\frac{\cos (2\alpha )\cos \delta \sin 2\theta }{4}\) and \({c}_{2}=\frac{\cos 2\theta \sin 2\alpha }{4}\).
The incoming photon pairs from BBO crystal and background are indicated as N_{0} and N_{d} respectively. Then the total coincidence can be fitted as the equation:
where \({C}_{0}=\frac{{N}_{0}\cos \delta \sin 2\theta }{4}\cos 2\alpha +\frac{{N}_{0}+4{N}_{d}}{4},{C}_{1}=\frac{{N}_{0}}{4}\cos 2\alpha \frac{{N}_{0}\cos \delta \sin 2\theta }{4}\) and \({C}_{2}=\frac{{N}_{0}\cos 2\theta }{4}\sin 2\alpha \).
Experimentally, we evaluate the rate of coincidences using two singlephoton counting modules, as a dependence on the polarization angles α and β, which are set by rotating two polarizers (cf. Fig. 1). The coincidence data for different settings of the polarizers and the respective fitting curves are shown in Fig. 2, where we see the oscillation predicted by the simple theory described above. We numerically fit the parameters N_{0}, θ, δ and N_{d} to the experimental data, obtaining the following results: N_{0} ± ΔN_{0} = 47640 ± 2800, N_{d} ± ΔN_{d} = 380 ± 830, θ ± Δθ = −0.15 ± 0.10 and δ ± Δδ = 2.10 ± 0.48. Hence, the produced entangled state is: \(\left\psi \right\rangle =0.989\left{\phi }^{+}\right\rangle +(0.0760.130i)\left{\phi }^{}\right\rangle \).
Benchmarking: Bell inequality violation using SPCM
Our next step is to calculate the ClauserHorneShimonyHolt (CHSH) inequality violation^{35,36} using SPCM (Single Photon Counting Module). The inequality can be written as:
where \(E(\alpha ,\beta )=\frac{{N}_{VV}(\alpha ,\beta )+{N}_{HH}(\alpha ,\beta ){N}_{VH}(\alpha ,\beta ){N}_{HV}(\alpha ,\beta )}{{N}_{VV}(\alpha ,\beta )+{N}_{HH}(\alpha ,\beta )+{N}_{VH}(\alpha ,\beta )+{N}_{HV}(\alpha ,\beta )}\) from the fitted curves in Fig. 2. N_{xy}(α, β) with x, y = V, H are defined to represent counting schemes for linear polarizer angles such that N_{VV}(α, β) = N(α, β), N_{HV}(α, β) = N(α + 90°, β), N_{VH}(α, β) = N(α, β + 90°), and N_{HH}(α, β) = N(α + 90°, β + 90°). We obtain the values shown in Table 1.
Using these values, we calculate the S parameter S = 2.679 ± 0.007 > 2, demonstrating the violation of the CHSH inequality. The uncertainty is calculated using \(\Delta S=\sqrt{{\sum }_{\alpha ,\beta }\Delta E{(\alpha ,\beta )}^{2}}\) and
Entanglement Characterization with Tpx3Cam
Having set a benchmark for the measurements, we proceed to characterize the same entanglement source using the Tpx3Cam. Instead of being measured in the standalone singlephoton detectors, the entangled pairs are sent to another experimental setup where they are converted to photoelectrons, amplified in different regions of the intensifier and subsequentially timestamped in the fast camera.
The photon pairs were recorded continuously by the camera for a given period of 5 min, for each combination of polarizations. Figure 3a) shows five examples of individual singlephoton events in the camera with their time (TOA, right column) and amplitude (TOT, left column) information using raw data. Note that there is an anticorrelation of TOA and TOT for the same pixels, which can be used to improve the time resolution, as discussed later. The two beam spots coming from the optical fibers are visible in Fig. 3b), corresponding to the areas of highest occupancy. As expected, the intensity distributions in the fibers follow the Gaussian modes. The rate of photons in these regions was ≈ 20 kHz, determined primarily by the output rate of the photon source at the fiber end (typically ≈ 100 kHz) and the intensifier quantum efficiency.
The background, uniformly distributed over the photocathode surface in the occupancy map in Fig. 3b), is caused by spurious dark counts from the photocathode. This rate is ≈ 50 times smaller than the measured singlephoton rate in the fiber areas and could be further reduced by cooling the intensifier, which in our measurements was operated at room temperature. We also note that the background photoelectrons arrive at random times and thus suppressed by requiring coincidence between the two photons, as shown below.
Data processing
To perform a Bell’s inequality measurement using data from the fast camera, we gathered 72 fiveminute long datasets corresponding to different settings of the polarizers. The raw data is processed following several steps: i) timeordering of the hit pixels, ii) identification of the pixel clusters corresponding to the singlephoton hits, iii) centroiding of the pixel clusters, iv) TOT corrections to improve the time resolution, v) calculating the number of coincidences and vi) Bell analysis.
I. Timeordering
Tpx3Cam reads out the hit pixels asynchronously, which might alter the time order, especially at high rates. Thus, the first step of the data processing is to timeorder the pixels to prepare the data for the cluster finding.
II. Clustering
Clusters are groups of pixels adjacent to each other and within a preset time window. We used a recursive algorithm to look for the clusters: for a pixel, a 1 μs time window is applied to select other pixels close in space and time to the first one. Each pixel in a cluster should have a neighboring pixel separated not more than 300 ns apart. The algorithm then chooses another pixel, not contained in a cluster, shifting the time window and starting the process anew.
III. Centroid
A photon hit in the camera comprises, on average, ≈ 4 pixels with measured TOA and TOT, which allows applying a centroiding algorithm. The TOT information is used as a weighting factor, helping to define the geometrical center of the cluster, yielding an estimate of the coordinates x, y of the incoming singlephoton. The arrival time of the photon is estimated by using TOA of the pixel with the largest TOT in the cluster, correspondingly called TOA_{centroid} and TOT_{centroid}.
IV. TOT correction
Photons in the entangled pairs are simultaneous. Therefore, they will have the same timestamps within the time resolution. Precise timing is a powerful handle to reduce the random background, thus improving the camera time resolution and the signaltobackground ratio. For this, the timing information must be corrected to account for the socalled time walk. In the Timepix3 frontend electronics, within each pixel, the discriminator keeps a constant threshold, so larger signals cross the threshold earlier, producing smaller TOA and larger TOT values. The correlation of TOA and TOT allows to calibrate the constant threshold effect and, therefore, improves the timing resolution.
Typically, the correction requires a time reference, for example, from a laser, to determine the shift, as in the ion imaging experiments^{28}. Since, in these experiments, the entangled pairs are generated continuously, we had to develop a different procedure that does not rely on an external time reference. TOA_{centroid} was used as zero time reference for the cluster, giving a time difference defined by:
This can be calculated for each pixel within the cluster and associated with the pixel TOT and cluster TOT_{centroid} value. Combining the data from all runs a trend was observed that the value of dTOA(TOT,TOT_{centroid}) is constant for large TOT_{centroid} values (typically for TOT_{centroid} > 1500 ns), removing dependency on TOT_{centroid}. Thus a universal lookup table of dTOA(TOT) can be obtained. This procedure reduces the time difference between entries within a given cluster from ~ 100 ns down to a few ns and can be applied to TOA_{centroid}, improving the timing resolution.
The time resolution after the TOT correction is shown in the top graph of Fig. 4 as a function of TOT. The time resolution is determined from the distribution of time difference between two entangled photons. The distribution is fit with a Gaussian function, and the time resolution per photon is defined as the sigma of the fit divided by \(\sqrt{2}\) assuming equal resolution for each of the two photons. To determine the dependence of the resolution on TOT, we required that both photons have TOT greater or equal than a specific value on the TOT axis. The distribution of the TOT values is shown in the bottom graph of Fig. 4.
V. Time coincidences
To identify pairs of simultaneous photons, we selected areas of the sensor corresponding to regions illuminated by the fibers. The corresponding square areas were 42 × 42 pixels for the right fiber and 30 × 30 pixels for the left fiber, as shown in Fig. 3b). Then, for each photon detected in one region, we looked for its associated pair at the closest time in the second region. The time difference distribution for these detected pairs is shown in Fig. 5 for several settings of the polarizers, as defined in the Bell measurement above. The prominent peaks correspond to the pairs of entangled photons, while the small flat background corresponds to random coincidences of uncorrelated photons. Due to the finite quantum efficiency and other losses, not each photon from the source will have a detected synchronous partner in the other fiber. In this case, it will be paired with a random photon, either from the photon source (more likely) or the spurious photocathode counts, giving rise to the flat background.
Each distribution was fit to a function consisting of two Gaussians and a constant accounting for the flat background of random coincidences. The number of coincidences was estimated as the area under the Gaussian functions. The dependence of the number of coincidences on the polarizer settings indicates that the operation of the camera detection setup closely resembles the SPCM operation, despite the use of an entirely different registration scheme for single photons.
Bell’s inequality violation with a fast camera
The next step consists in studying the dependence of the coincidence measurements on the polarization projective measurements of the twophoton state. In the measurements, one polarizer was varied in 20° steps for four fixed values of the other polarizer: 0°, 45°, 90° and 135°. The dependence of the number of coincidences versus the polarizer angle is shown in Fig. 6. The data points were fitted with a sine function with the period, phase, amplitude and offset as free parameters. The fit results are shown in Table 2.
With these experimental parameters, we follow the procedure outlined in the benchmarking section, to obtain a Bellstate inequality Svalue with the Tpx3Cam setup. The obtained value is 2.78 ± 0.02, well above the classical limit of 2 and closer to the Tsirelson Bound of \(2\sqrt{2}\) (2.82) than with the SPCM measurements. We attribute this improvement to the better rejection of random background enabled by the fast camera. In these measurements, the signal is estimated with a fitting procedure described in the previous section. This procedure automatically accounts for the background and camera time resolution using the same dataset and gives a better estimate of the signal. We verified that the fast camera data presented in Fig. 6 have better visibility than the standard analysis data in Fig. 2, which should lead to higher Svalues.
Position dependent bell analysis
One of the clear advantages of using highspeed cameras for quantum state characterization lies in the capacity to analyze multiple processes simultaneously. In our final experiment, we probe the ability of the fast camera to analyze 81 entangled pairs in parallel. To simulate the latter, we divided the areas illuminated by the fiber’s output into nine subareas, forming a 3 × 3 matrix, as shown in the two fiber regions in Fig. 3. Then, we analyze each pairwise combination (81 total combinations) independently and reproduce the Bell analysis presented above for each of them. To accumulate enough statistics for these spatially resolved measurements, we took onehourlong extended datasets, corresponding to the 16 combinations of the polarizer settings, which are needed to calculate the Bell’s inequality violation. The total number of recorded photons was considerable, about 10^{9}, and required efforts to implement parallel processing of the data. The data analysis was performed within the scientific software framework ROOT developed at CERN^{37}. Figure 7 shows the results of the parallel evaluation of 81 Bell’s inequalities. Each box represents a specific spatial combination of subareas. The corresponding Svalue is colorcoded, with the corresponding uncertainty shown in the center of the box. The results show that the Svalue is uniform within the experimental errors with no apparent position dependence as expected. Figure 8 is a 3dimensional representation of the same information as in Fig. 7.
Discussion and Outlook
We have demonstrated that the spatial characterization of photonic entanglement can be performed employing the intensified Tpx3Cam camera. The camera can simultaneously timestamp multiple single optical photons with nanosecond timing resolution while capturing their spatial information. The Svalue results confirm that the fast camera spatial characterization of quantumstates in parallel is a viable alternative to be used in scaledup quantum systems. The photon rate in these experiments was limited by the photon source to about 100 kHz. This is a factor of 100 lower than the maximum rate allowed by the camera, which should be capable of working with much brighter sources of entangled photons. Another specification of the fast camera, the Quantum Efficiency (QE) of the image intensifier, remains another critical parameter for the efficient detection of entangled photons. This technology is moving forward benefiting from new photocathodes based on GaAs with better QE, up to 35% in the same wavelength range as used for these studies^{38}.
New imaging technologies based on monolithic silicon devices, such as singlephoton avalanche devices (SPADs), are rapidly improving and could soon become competitive. Since the devices have internal amplification, the image intensifier is not necessary, which is a considerable simplification. Additionally, SPADs could have better time resolution and, potentially, higher QE, compared to the intensified cameras. The SPAD imagers started to appear on the market, and the first applications for quantum information science (QIS) have been reported^{16,39,40,41}. Currently, the main limitation of the devices is the high dark count rate in the tens of MHz/cm^{2} range, which may saturate the readout and lead to low signaltobackground ratio. Another difficulty is the integration of the photon sensing SPAD pixels and sophisticated readout electronics in a monolithic device, which has many technical challenges. Also, in a SPAD, a singlephoton fires only one pixel producing a standard pulse, so no centroiding is possible, therefore rendering it also impossible to distinguish a noise hit from a useful signal.
From the QIS perspective, we have showcased the possibility of parallel processing of tens of entangled states in parallel by analyzing independent combinations of subareas illuminated by the two fibers, which is an unprecedented capability for quantum information processing. As all pixels of the Tpx3Cam sensor act independently of each other, the dimensionality of this processing can be scaled up manyfold, for example, employing the same camera setup with brighter photon sources and/or multiple photon beams. We estimate that Tpx3Cam can successfully process at least 10 × 10 = 100 photon beams, each with a photon rate similar to the one used in these experiments. This technique may become a crucial tool for the realtime characterization of the performance for sizable entanglementbased quantum networks or circuits. Furthermore, the camera also can count the number of simultaneous photons in the same fiber, given sufficient spatial separation. This offers the possibility of discerning an event with more than one photon pair, an effect of the statistical distribution of the number of photons at the output of the SPDC process.
We envision that our characterization setup can prove useful in other quantum information processing tasks, such as HongOuMandel interference^{22} and the characterization of entanglement encoded in orbital angular momentum (OAM) modes^{42}. Furthermore, it is well suited for the realtime benchmarking of quantum memories using OAM states^{43,44}, and for the parallel processing of the information in many memories systems^{45}. Lastly, it could also find a niche as a feedback tool in the positioning of longdistance freespace quantum communication channels forming intracity quantum cryptographic networks^{46}.
Data availability
The data that support the findings of this study are available upon request.
References
 1.
Kwiat, P. G., Mattle, K., Weinfurter, H., Zeilinger, A., Sergienko, A. V. & Shih, Y. New highintensity source of polarizationentangled photon pairs. Phys. Rev. Letters 75, 4337–4341 (1995).
 2.
Tittel, W., Brendel, J., Zbinden, H. & Gisin, N. Violation of bell inequalities by photons more than 10 km apart. Phys. Rev. Letters 81, 3563–3566 (1998).
 3.
Pan, J. W., Bouwmeester, D., Weinfurter, H. & Zeilinger, A. Experimental entanglement swapping Entangling photons that never interacted. Phys. Rev. Letters 80, 3891–3894 (1998).
 4.
Sherson, J. F. et al. Quantum teleportation between light and matter. Nature 443(7111), 557–560 (2006).
 5.
Ursin, R. et al. Entanglementbased quantum communication over 144km. Nature Phys 3(7), 481–486 (2007).
 6.
Hensen, B. et al. Loopholefree Bell inequality violation using electron spins separated by 1.3 kilometers. Nature 526, 682 (2015).
 7.
Choi, K. S., Goban, A., Papp, S. B., van Enk, S. J. & Kimble, H. J. Entanglement of spinwaves among four quantum memories. Nature 468(7322), 412–416 (2010).
 8.
Edgar, M. P. et al. Imaging highdimensional spatial entanglement with a camera. Nature Communications 3, 984 (2012).
 9.
Dada, A. C., Leach, J., Buller, G. S., Padgett, M. J. & Andersson, E. Experimental highdimensional twophoton entanglement and violations of generalized bell inequalities. Nature Physics 7, 677 (2011).
 10.
Howell, J. C., Bennink, R. S., Bentley, S. J. & Boyd, R. W. Realization of the EinsteinPodolskyRosen paradox using momentum and positionentangled photons from spontaneous parametric downconversion. Phys. Rev. Letters 92, 210403 (2004).
 11.
Walborn, S. P., Salles, A., Gomes, R. M., Toscano, F. & Ribeiro, P. H. S. Revealing hidden einsteinPodolskyRosen nonlocality. Phys. Rev. Letters 106, 130402 (2011).
 12.
Brida, G., Caspani, L., Gatti, A., Genovese, M., Meda, A. & Berchera, I. R. Measurement of subshotnoise spatial correlations without background subtraction. Phys. Rev. Letters 102, 213602 (2009).
 13.
Brida, G., Genovese, M. & Berchera, I. R. Experimental realization of subshotnoise quantum imaging. Nature Photonics 4, 227 (2010).
 14.
Kumar, A., Nunley, H. & Marino, A. M. Observation of spatial quantum correlations in the macroscopic regime. Phys. Rev. A 95, 053849 (2017).
 15.
Blanchet, J. L., Devaux, F., Furfaro, L. & Lantz, E. Measurement of subshotnoise correlations of spatial fluctuations in the photoncounting regime. Phys. Rev. Letters 101, 233604 (2008).
 16.
Unternährer, M., Bessire, B., Gasparini, L., Stoppa, D. & Stefanov, A. Coincidence detection of spatially correlated photon pairs with a monolithic timeresolving detector array. Optics Express 24(25), 28829–28841 (2016).
 17.
Jost, B. M., Sergienko, A. V., Abouraddy, A. F., Saleh, B. E. A. & Teich, M. C. Spatial correlations of spontaneously downconverted photon pairs detected with a singlephotonsensitive CCD camera. Optics Express 3(2), 81–88 (1998).
 18.
Just, F. et al. Detection of nonclassical spacetime correlations with a novel type of singlephoton camera. Optics Express 22(14), 17561–17572 (2014).
 19.
Fickler, R., Krenn, M., Lapkiewicz, R., Ramelow, S. & Zeilinger, A. Realtime imaging of quantum entanglement. Scientific Reports 3, 1914 (2013).
 20.
Reichert, M., Sun, X. & Fleischer, J. W. Quality of spatial entanglement propagation. Phys. Rev. A 95, 063836 (2017).
 21.
Reichert, M., Defienne, H. & Fleischer, J. W. Massively parallel coincidence counting of highdimensional entangled states (2017).
 22.
Michał, J. & Radosław, C. Shotbyshot imaging of hongoumandel interference with an intensified SCMOS camera. Optics Letters 40, 1540–1543 (2015).
 23.
 24.
Pomarico, E., Bancal, J. D., Sanguinetti, B., Rochdi, A. & Gisin, N. Various quantum nonlocality tests with a commercial twophoton entanglement source. Phys. Rev. A 83, 052104 (2011).
 25.
Poikela, T. et al. Timepix3 a 65k channel hybrid pixel readout chip with simultaneous ToA/ToT and sparse readout. Journal of instrumentation 9(05), C05013 (2014).
 26.
FisherLevine, M. & Nomerotski, A. Timepixcam a fast optical imager with timestamping. Journal of Instrumentation 11(03), C03016 (2016).
 27.
Nomerotski, A. et al. Characterization of Timepixcam, a fast imager for the timestamping of optical photons. Journal of Instrumentation 12(01), C01017 (2017).
 28.
Zhao, A. et al. Coincidence velocity map imaging using tpx3cam, a timestamping optical camera with 1.5ns timing resolution. Review of Scientific Instruments 88(9), 113104 (2017).
 29.
Hirvonen, L. M., FisherLevine, M., Suhling, K. & Nomerotski, A. Photon counting phosphorescence lifetime imaging with Timepixcam. Review of Scientific Instruments 88(1), 013104 (2017).
 30.
van der Heijden, B. et al. Spidr, a generalpurpose readout system for pixel ASICs. Journal of Instrumentation 12(02), C02040 (2017).
 31.
Photonis hiQE red intensifier, http://www.photonis.com/.
 32.
Winter, B., King, S. J., Brouard, M. & Vallance, C. A fast microchannel platescintillator detector for velocity map imaging and imaging mass spectrometry. Review of Scientific Instruments 85(2), 023306 (2014).
 33.
Photonis cricket advanced image intensifier adapter, http://www.photonis.com/.
 34.
De Gaspari, M. et al. Design of the analog frontend for the timepix3 and smallpix hybrid pixel detectors in 130 nm CMOS technology. Journal of Instrumentation 9(01), C01037–C01037 (2014).
 35.
Aspect, A., Grangier, P. & Roger, G. Experimental tests of realistic local theories via Bellas theorem. Phys. Rev. Letters 47, 460–463 (1981).
 36.
Aspect, A., Grangier, P. & Roger, G. Experimental realization of EinsteinPodolskyRosenBohm Gedanken experiment a new violation of Bellas inequalities. Phys. Rev. Letters 49, 91–94 (1982).
 37.
Brun, R. & Rademakers, F. ROOT  An ObjectOriented Data Analysis Framework. Nucl. Inst. & Meth. in Phys. Res. A 389, 81–86 (1997).
 38.
Glazenborg, R. et al. Imaging photon camera with high spatiotemporal resolution. European microscopy congress proceedings. Pages 471–472 (2016).
 39.
Boiko, D. L. et al. A quantum imager for intensity correlated photons. New Journal of Physics 11(1), 013001 (2009).
 40.
Burri, S. et al. Architecture and applications of a highresolution gated SPAD image sensor. Optics Express 22(14), 17573–17589 (2014).
 41.
Gasparini, L. et al. Supertwin towards 100kpixel CMOS quantum image sensors for quantum optics applications. Proc. SPIE, Quantum Sensing and Nano Electronics and Photonics XIV, 10111 101112L (2017).
 42.
Fickler, R. et al. Quantum entanglement of high angular momenta. Science 338(6107), 640–643 (2012).
 43.
Nicolas, A. et al. A quantum memory for orbital angular momentum photonic qubits. Nature Photonics 8, 234 (2014).
 44.
Ding, D. S. et al. Quantum storage of orbital angular momentum entanglement in an atomic ensemble. Physics Rev. Letters 114, 050502 (2015).
 45.
Parniak, M. et al. Wavevector multiplexed atomic quantum memory via spatiallyresolved singlephoton detection. Nature Communications 8(1), 2140 (2017).
 46.
Steinlechner, F. et al. Distribution of highdimensional entanglement via an intracity freespace link. Nature Communications 8, 15971 (2017).
 47.
Qutools GmbH, http://www.qutools.com/.
Acknowledgements
The authors thank A. Londono and J. Tsybysheva for their assistance with the measurements; H. Graafsma for providing the Timepix3 ASIC; M. van Beuzekom, B. Bouwens, and E. Maddox for their assistance with the fast camera; T. Tsang for assistance with the image intensifier. The Stony Brook team acknowledges the support from the National Science Foundation (grants PHY1404398 & PHY1707919) and the Simons Foundation (grant SBF241180). The Czech Ministry of Education also supported this work, Youth and Sports (grant LM2015054), and by the LDRD grant 18051 of Brookhaven National Laboratory. A.H. acknowledges support under the Science Undergraduate Laboratory Internships Program (SULI) by the U.S. Department of Energy.
Author information
Affiliations
Contributions
C.I., P.S., M.F., A.H., G.C., A.N. and E.F. all contributed to the implementation and modelling of the experiment, interpretation of the results, and the writing of the manuscript.
Corresponding author
Correspondence to Eden Figueroa.
Ethics declarations
Competing interests
M.F. and E.F. have shares of Qunnect Inc., a quantum technology company based in NY. All other authors declare no competing interests.
Additional information
Publisher’s note Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Rights and permissions
Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/.
About this article
Cite this article
Ianzano, C., Svihra, P., Flament, M. et al. Fast camera spatial characterization of photonic polarization entanglement. Sci Rep 10, 6181 (2020). https://doi.org/10.1038/s4159802062020z
Received:
Accepted:
Published:
Further reading

Multidimensional quantumenhanced target detection via spectrotemporalcorrelation measurements
Physical Review A (2020)
Comments
By submitting a comment you agree to abide by our Terms and Community Guidelines. If you find something abusive or that does not comply with our terms or guidelines please flag it as inappropriate.