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Optical and Quantum Sensing and Precision Metrology II

3D quantum ghost imaging microscope

Dominique Davenport, Audrey V. Eshun, Brandon J. Demory, Shervin Kiannejad, Paul Moş, Lin Yang, Edoardo Charbon A, Tiziana Bond, Mike Rushford, Claudio E. Bruschini, Ted A. Laurence

Published Mar 19, 2025• 0 citations
Publisher

Abstract

We present a 3D quantum enhanced microscope which utilizes the principles of quantum ghost imaging (QGI) to produce volumetric images. This tool is developed to address current challenges in 3D microscopy which include the volumetric capture and tracking of photosensitive samples. Much of the active research on QGI are focused on exploiting the correlative behaviors of the quantum light sources, to obtain higher dimensional data than can be achieved with traditional imaging; in this vein, our study is similar. Where we believe our approach deviates, even from current research in QGI, is that we demonstrate that perpendicularly scattered light from the sample can still be correlated to generate a ghost image from a different perspective plane. Using two state-of-the-art single photon avalanche diode (SPAD) array detectors, this achievement allows us to generate, for each count, positional coordinates from two perpendicular planes. We present this novel 3D QGI approach along with initial 3D images of silver nanoclusters, followed with a discussion on how the results can impact biological imaging applications. Prepared by LLNL under Contract DE-AC52-07NA27344

DOI
10.1117/12.3043888

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We present a 3D quantum enhanced microscope which utilizes the principles of quantum ghost imaging (QGI) to produce volumetric images. This tool is developed to address current challenges in 3D microscopy which include the volumetric capture and tracking of photosensitive samples. Much of the active research on QGI are focused on exploiting the correlative behaviors of the quantum light sources, to obtain higher dimensional data than can be achieved with traditional imaging; in this vein, our study is similar. Where we believe our approach deviates, even from current research in QGI, is that we demonstrate that perpendicularly scattered light from the sample can still be correlated to generate a ghost image from a different perspective plane. Using two state-of-the-art single photon avalanche diode (SPAD) array detectors, this achievement allows us to generate, for each count, positional coordinates from two perpendicular planes. We present this novel 3D QGI approach along with initial 3D images of silver nanoclusters, followed with a discussion on how the results can impact biological imaging applications. Prepared by LLNL under Contract DE-AC52-07NA27344
Quantum ghost imaging uses quantum-entangled photons to generate a two-dimensional image with only a bucket detector at the sample. Here we expand on this approach to generate a three-dimensional image without scanning. A quantum-entangled light source directly links information between a pair of 2D sensors, one of which captures a standard image from one perspective and a second sensor which captures a ghost image from a perpendicular perspective. By correlating the spatial information from the two detectors for each photon pair, we obtain three dimensions of spatial information ( x , y , and z ) for each scattered photon. We demonstrate that this system can study microscopic environments by imaging scattering from metallic nanoparticle clusters. This approach has the potential to greatly reduce the flux of light required to obtain a 3D image of a biological sample and thereby extend the number of images that can be obtained before photodamaging the sample.
Quantum ghost imaging (QGI) is an intriguing imaging protocol that exploits photon-pair correlations stemming from spontaneous parametric down-conversion (SPDC). QGI retrieves images from two-path joint measurements, where single-path detection does not allow us to reconstruct the target image. Here we report on a QGI implementation exploiting a two-dimensional (2D) single-photon avalanche diode (SPAD) array detector for the spatially resolving path. Moreover, the employment of non-degenerate SPDC allows us to investigate samples at infrared wavelengths without the need for short-wave infrared (SWIR) cameras, while the spatial detection can be still performed in the visible region, where the more advanced silicon-based technology can be exploited. Our findings advance QGI schemes towards practical applications.
Quantum Ghost Imaging (QGI) is a scheme which uses the temporal correlation of entangled photon pairs (signal and idler) to identify detections belonging to actual entangled pairs and separate them from uncorrelated detections. By also exploiting the spatial correlation of the photon pair, this identification allows to extract image information of the idler photons by imaging the signal photons. This can even be done for non-degenerate photon pairs, allowing imaging at wavelengths without sophisticated cameras in this regime. Recent advances in detector technology, especially single photon avalanche diodes (SPADs), allow the design for new cameras capable of single photon detection with both high spatial and temporal resolution. These new detectors are especially useful for application in QGI, allowing to detect each photon individually and identify the correlated pairs after the measurement. It further allows to analyse the time-of-flight of photons and thus enables 3D imaging, the first realization of which will be presented here.
Low-light-level imaging in the infrared regime could find applications in areas ranging from technological to biological. Still, its development is limited by the inefficiency of silicon-based detectors in this regime. Quantum Ghost Imaging (QGI) can address this limitation by allowing the separation of illumination and imaging [1]. This is accomplished by generating non-degenerate correlated photon pairs, whose infrared photon probes the object and is detected by an InGaAs bucket detector, while the spatial distribution of the visible one is collected by a single-photon sensitive silicon camera. Traditional QGI setups evaluate photon correlations through “heralding”, by triggering the camera upon idler detection and thus require an image-preserving delay-line, which limits their use for remote sensing [1]. In asynchronous QGI (aQGI) cameras are replaced with SPAD arrays [2] able to record photon timestamp with picoseconds precision. By identifying pairs through timestamps comparison, the mentioned limitations are resolved [3], enabling applications with reflective or diffusive objects where the timestamp delay depends on the object's position. In this work, we propose and demonstrate an experimental QGI setup for remote sensing in reflection configuration (Fig. 1). Collinear non-degenerate pairs of single-photons at 550 nm and 1550 nm are generated by pumping a 2 mm-long type-0 ppKTP crystal with a 405 nm laser. To enable imaging of objects at varying distances, we implemented a momentum-correlation-based setup. Infrared photons interacting with the object were collected by commercially available InGaAs SPAD detectors, while the visible photons were directly captured using a prototype silicon SPAD array developed by Politecnico di Milano [4]. It is based on a 32×32 SPAD, with in-pixel TDCs, and on-chip microlenses are employed to reach a fill factor of 78%. The time resolution is adjustable down to 250 ps, with 1 μs Full Scale Range (FSR). The measurement duty cycle (i.e. the ration of the TDC FSR and the frame time) can be increased with a multi-gate acquisition scheme. To validate the efficiency of our setup, we tested it using a proof-of-principle object, as shown in Fig. 1b. The reconstructed images, captured with the object placed at 30 cm intervals in an acquisition time of only 30 s, are shown in Fig. 1c. In summary, the shown results confirm the potential of the proposed setup for remote sensing applications, particularly for reflective or diffusive objects. Moreover, the proposed approach could offers the possibility of significantly reduce acquisition times compared to standard QGI setups.
Quantum ghost imaging approaches have been proposed to enhance biological microscopy, for example, using 2D visible detectors to provide IR images or providing additional dimensions of spatial or spectral information. Toward the goal of making such imaging schemes practical, we compare image quality and depth-of-field between traditional images and ghost images at the same excitation levels. We measure how image quality and depth-of-field depend on the parameters of the entangled light produced using type-I spontaneous parametric down-conversion (SPDC). We use a pair of time-synchronized, photon-timing single-photon avalanche diode (SPAD) array detectors to capture two distinct microscope imaging paths simultaneously on a photon-pair-by-photon-pair basis: one in a traditional imaging pathway and the other a quantum ghost imaging pathway. We calculate the depth-of-field, resolution, contrast, and signal-to-noise ratio (SNR) through the parameter space of a β-Barium Borate (BBO) type-I bulk non-linear crystal length and angle. Our results provide a basis for choosing parameters for quantum ghost imaging with type-I SPDC sources.
Quantum Ghost Imaging (QGI) is a scheme using entangled pairs of photons (signal and idler) in order to perform imaging with both single photons and with only a single-element detector in the spectrum of interest. It utilises the temporal coincidence of the photons to identify associated pairs, while their spatial correlation allows to obtain image information from of the idler photon from the measurement of the signal photon. It is especially useful when using nondegenerate photon pairs, allowing to keep the signal photon in the silicon detection window, while the interacting wavelength can be freely chosen.However, current schemes are limited, as they rely on time-gating and heralding. Recent advances in single photon avalanche diodes (SPADs) allow the design of new single photon cameras, which can be outfitted with dedicated in-pixel timing circuitry. This allows to register single photons in both time and space. These detectors allowed us to design a new scheme for QGI, in which the coincidence is evaluated after the measurement. It also allows us to perform depth-resolved 3D imaging based on the time-of-flight of photons, first results of which are presented here.