Dheera Venkatraman

First-Photon Imaging

Computing an Image Firing off a burst of laser pulses and detecting the back-reflected photons is a widely used method for constructing three-dimensional (3D) images of a scene. Kirmani et al. (p. 58, published online 29 November) describe an active imaging method in which pulsed laser light raster scans a scene and a single-photon detector is used to detect the first photon of the back-reflected laser light. Exploiting spatial correlations of photons scattered from different parts of the scene allows computation of a 3D image. Importantly, for biological applications, the technique allows the laser power to be reduced without sacrificing image quality. A computational imaging method based on photon timing enables three-dimensional imaging under low light flux conditions. Imagers that use their own illumination can capture three-dimensional (3D) structure and reflectivity information. With photon-counting detectors, images can be acquired at extremely low photon fluxes. To suppress the Poisson noise inherent in low-flux operation, such imagers typically require hundreds of detected photons per pixel for accurate range and reflectivity determination. We introduce a low-flux imaging technique, called first-photon imaging, which is a computational imager that exploits spatial correlations found in real-world scenes and the physics of low-flux measurements. Our technique recovers 3D structure and reflectivity from the first detected photon at each pixel. We demonstrate simultaneous acquisition of sub–pulse duration range and 4-bit reflectivity information in the presence of high background noise. First-photon imaging may be of considerable value to both microscopy and remote sensing.

Phase-conjugate optical coherence tomography

We demonstrate a new type of optical coherence tomography using only classical resources to achieve results that are typically associated with quantum-enhancedmetrology: factor-of-two axial resolution enhancement and even-order dispersion cancellation.

Experimental realization of phase-conjugate optical coherence tomography

We demonstrate phase-conjugate optical coherence tomography (PC-OCT) using a classical source of phase-sensitive cross-correlated beams to achieve measurement improvements shared by quantum OCT (Q-OCT): a factor-of-2 enhancement in axial resolution and even-order dispersion cancellation. Compared with coincidence counting used in Q-OCT, PC-OCT employs standard photodetection that results in much faster data acquisitions. This work belongs to a new class of classical techniques inspired by quantum methods that have advantages once thought to be exclusively quantum mechanical.

Ghost Imaging without Discord

Ragy and Adesso argue that quantum discord is involved in the formation of a pseudothermal ghost image. We show that quantum discord plays no role in spatial light modulator ghost imaging, i.e., ghost-image formation based on structured illumination realized with laser light that has undergone spatial light modulation by the output from a pseudorandom number generator. Our analysis thus casts doubt on the degree to which quantum discord is necessary for ghost imaging.

Classical far-field phase-sensitive ghost imaging.

We report the first (to our knowledge) far-field ghost images formed with phase-sensitive classical-state light and compare them with ghost images of the same object formed with conventional phase-insensitive classical-state light. To generate signal and reference beams with phase-sensitive cross correlation, we used a pair of synchronized spatial light modulators that imposed random, spatially varying, anticorrelated phase modulation on the outputs from 50-50 beam splitting of a laser beam. In agreement with theory, we found the phase-sensitive image to be inverted, whereas the phase-insensitive image is erect, with both having comparable spatial resolutions and signal-to-noise ratios.

Classical low-coherence interferometry based on broadband parametric fluorescence and amplification

We demonstrate that single-mode broadband amplified spontaneous parametric downconversion, combined with optical parametric amplification, can be used as a classical source of phase-sensitive cross-correlated beams. We first study the single spatial mode emission and the spectral brightness properties of the parametric fluorescence, produced in periodically poled MgO-doped lithium niobate. Using the same single-pass bulk-crystal configuration for a pulsed optical parametric amplifier, we achieve a gain of approximately 20 dB at an average pump power of 2W, and explain the pulse narrowing observed at the output of both parametric fluorescence and amplification in the regime of high gain. Combining these two nonlinear processes, we measured optical coherence tomography signals with standard InGaAs photodiodes, thus realizing the first classical interferometer based on amplified parametric fluorescence. The results suggest their utility for demonstrating phase-conjugate optical coherence tomography.

Classical Imaging with Undetected Photons

We describe a classical-state system capable of mimicking the essential features of Barreto Lemos et a/.s quantum imaging with undetected photons [Nature, 512, 409-412 (2014)]. but with a much higher signal-to-noise ratio.

High photon efficiency computational range imaging using spatio-temporal statistical regularization

We demonstrate 1 photon-per-pixel photon efficiency and sub-pulse-width range resolution in megapixel laser range imaging by using a joint spatio-temporal statistical processing framework and by exploiting transform-domain sparsity.

Photon-efficient computational imaging with a single-photon camera

Using a photon-efficient reconstruction algorithm and a single-photon camera prototype, we demonstrate accurate depth and reflectivity imaging of natural scenes from an average of ~1 detected signal photon per pixel.

Classical imaging with undetected photons

We describe a classical-state system capable of mimicking the essential features of Barreto Lemos et a/.s quantum imaging with undetected photons [Nature, 512, 409–412 (2014)]. but with a much higher signal-to-noise ratio.