In traditional imaging, one tries to create a perfect image directly. In computational imaging, a distortion is added to the optical path, so that the recorded picture no longer resembles the object. Since the distortion is known, however, an image can be reconstructed numerically. This a priori information can be used to obtain "extra" information about the object, such as increased resolution and depth. We have generalized computational imaging to include nonlinear dynamics and are applying it to super-resolution microscopy, phase retrieval, and biomedical imaging.
Classical optics treats light as a smooth continuum. Quantum optics introduces new effects, and can surpass classical limits, by exploiting the discrete nature of photons (and their correlations). Historically, quantum opitcs experiments used single-point detectors and scanning, which limit the possible outcomes and inhibit true quantum imaging. In contrast, we use megapixel cameras that record an entire image at once. The resulting pictures open up new applications in quantum sensing, imaging, and information processing.
Ultrasound operates like radar, with a probe beam sent to the object and an echo recorded. In the simplest case, the reflected signal is at the same frequency as the probe, and the return signal gives the distance of the object. In more advanced cases, the response is at a different frequency. Measuring these frequencies gives extra information about the sample but is complicated by material properties, scattering, and noise. We are working to overcome these issues, particularly for tissue and biomedical ultrasound.
Microfluidics is becoming increasingly useful for transporting and sorting biological objects. In this research, we use the flow as a new degree of freedom for imaging. Examples include tilting the fluid channel for focus at different depths and cell tomography by recording different perspectives. This integrated approach provides high-speed 3D imaging with no mechanical movement of the microscope, minimal stress on the biosamples, and small computational overhead.
Intuitively, the propagation of light can be considered as the flow of a “fluid” from high-intensity to low-intensity, e.g. a candle illuminating the shadows of a room. Standard fluid behavior, such as flow around objects, shock waves, and turbulence, are all possible with light. New features arise, however, as wave diffraction (rather than viscosity or surface tension) moderates the dynamics. This difference leads to new mathematics and gives insight into both traditional and quantum fluids.
When the light is partially incoherent, then its propagation can be treated as a statistical fluid, i.e. as a plasma. In this photonic plasma, nonlinearity creates an effective plasma frequency, while the finite correlation length creates an effective Debye length. This formalism unifies all previous treatments of nonlinear statistical optics and predicts fundamentally new dynamics for nonlinear light propagation. It also allows observation of phenomena that are difficult, if not impossible, to observe in material plasma.
Photonic lattices, such as waveguide arrays, facilitate the guiding and control of light. Typically periodic structures, they are difficult to fabricate, especially in a nonlinear medium. We bypass these difficulties by holographically inducing photonic structures in a photosensitive material, e.g. a photorefractive crystal. The waveguides then acquire the nonlinearity of the medium, allowing studies of wave mixing constrained by geometry. Applications include all-optical material modeling, nonlinear spectroscopy, and spectral filtering.