Optics (physics.optics)

Abstract: Integrated photonic devices have become pivotal elements across most research fields that involve light-based applications. A particularly versatile category of this technology are programmable photonic integrated processors, which are being employed in an increasing variety of applications, like communication or photonic computing. Such processors accurately control on-chip light within meshes of programmable optical gates. Free-space optics applications can utilize this technology by using appropriate on-chip interfaces to couple distributions of light to the photonic chip. This enables, for example, access to the spatial properties of free-space light, particularly to phase distributions, which is usually challenging and requires either specialized devices or additional components. Here we discuss and show the detection of amplitude and phase of structured higher-order light beams using a multipurpose photonic processor. Our device provides measurements of amplitude and phase distributions which can be used to, e.g., directly distinguish light's orbital angular momentum without the need for further elements interacting with the free-space light. Paving a way towards more convenient and intuitive phase measurements of structured light, we envision applications in a wide range of fields, specifically in microscopy or communications where the spatial distributions of lights properties are important.

Abstract: This work is inspired by recent experiments on the formation of vortices in exciton-polariton condensates placed in rotating optical traps. We study theoretically the dynamics of formation of such vortices and elucidate the fundamental role of the mode competition effect in determining the properties of stationary polariton states triggered by stimulated scattering of exciton-polaritons. The interplay between linear and non-linear effects is shown to result in a peculiar polariton dynamics. However, near the lasing threshold, the predominant contribution of the nonlinear effects is the saturation of the linear gain.

Abstract: When introducing a nanoparticle into an optical trap, its mass and shape are not immediately apparent. We combine a number of methods to determine the mass and shape of trapped nanoparticles, which have previously only been used separately. We demonstrate that the use of multiple classification techniques is in certain cases required to avoid incorrect or ambiguous results. The ability to identify these parameters is a key step for a range of experiments on precision measurements and sensing using optically levitated nanoparticles.

Abstract: Wave phenomena in bianisotropic media have been broadly studied in classical electrodynamics, as these media offer different degrees of freedom to engineer electromagnetic waves. However, they have been always considered to be stationary (time-invariant) in the studies. Temporally varying the magnetoelectric coupling manifesting bianisotropy engenders an alluring prospect to manipulate wave-matter interactions in new ways. In this paper, we theoretically contemplate electromagnetic effects in all classes of nondispersive bianisotropic media when the corresponding magnetoelectric coupling parameter suddenly jumps in time, creating a time interface in those bianisotropic media. We investigate scattering effects at such time interfaces, revealing new polarization- and direction-dependent phenomena. Hopefully, this work can pave the road for exploring bianisotropic time metamaterials (metasurfaces), and bianisotropic photonic time crystals, opening up interesting possibilities to control wave polarization and amplitude in reciprocal and nonreciprocal ways.

Abstract: Advances in optical imaging always look for an increase in sensitivity and resolution among other practicability aspects. Within the same scope, in this work we report a versatile interference contrast imaging technique, capable of sub-nm sample-thickness resolution, with a large field-ofview of several mm2. Sensitivity is increased through the use of a self-imaging non-resonant cavity, which causes photons to probe the sample in multiple rounds before being detected, where the configuration can be transmissive or reflective. Phase profiles can be resolved individually for each round thanks to a specially designed single-photon camera with time-of-flight capabilities and true pixels-off gating. Measurement noise is reduced by novel data processing combining the retrieved sample profiles from multiple rounds. Our protocol is specially useful under extremely low light conditions as require by biological or photo-sensitive samples. Results demonstrate more than a four-fold reduction in phase measurement noise, compared to single round imaging, and close valuesto the predicted sensitivity in case of the best possible cavity configuration, where all photons are maintained until n rounds. We also find a good agreement with the theoretical predictions for low number of rounds, where experimental imperfections would place a minor role. The absence of a laser or cavity lock-in mechanism makes the technique an easy to use inspection tool.

Abstract: Electron dynamics of anatase TiO$_2$ under the influence of ultrashort and intense laser field is studied using the real-time time-dependent density functional theory (TDDFT). Our findings demonstrate the effectiveness of TDDFT calculations in modeling the electron dynamics of solids during ultrashort laser excitation, providing valuable insights for designing and optimizing nonlinear photonic devices. We analyze the perturbative and non-perturbative responses of TiO$_2$ to 30 fs laser pulses at 400 and 800 nm wavelengths, elucidating the underlying mechanisms. At 400 nm, ionization via single photon absorption dominates, even at very low intensities. At 800 nm, we observe ionization through two-photon absorption within the intensity range of $1\times10^{10}$ to $9\times10^{12}$ W/cm$^2$, with a transition from multiphoton to tunneling ionization occurring at $9\times10^{12}$ W/cm$^2$. We observe a sudden increase in energy and the number of excited electrons beyond $1\times10^{13}$ W/cm$^2$, leading to their saturation and subsequent laser-induced damage. We estimate the damage threshold of TiO$_2$ for 800 nm to be 0.1 J/cm$^2$. In the perturbative regime, induced currents exhibit a phase shift proportional to the peak intensity of the laser pulse. This phase shift is attributed to the intensity-dependent changes in the number of free carriers, indicative of the optical Kerr effect. Leveraging the linear dependence of phase shift on peak intensities, we estimate the nonlinear refractive index ($n_2$) of TiO$_2$ to be $3.54\times10^{-11}$ cm$^2$/W.

Abstract: In recent years, there has been growing interest in using photonic technology to perform the underlying linear algebra operations required by different applications, including neuromorphic photonics, quantum computing and microwave processing, mainly aiming at taking advantage of the silicon photonics' (SiPho) credentials to support high-speed and energy-efficient operations. Mapping, however, a targeted matrix with absolute accuracy into the optical domain remains a huge challenge in linear optics, since state-of-the-art linear optical circuit architectures are highly sensitive to fabrication imperfections. This leads to reduced fidelity metrics that degrade faster as the insertion losses of the constituent optical matrix node or the matrix dimensions increase. In this work, we present for the first time a novel coherent SiPho crossbar (Xbar) that can support on-chip fidelity restoration while implementing linear algebra operations, realizing the first experimental demonstration of perfect on-chip arbitrary linear optical transformations. We demonstrate the experimental implementation of 10000 arbitrary linear transformations in the photonic domain achieving a record high fidelity of 99.997%+-0.002, limited mainly by the statistical error enforced by the measurement equipment. Our work represents the first integrated universal linear optical circuit that provides almost unity and loss-independent fidelity in the realization of arbitrary matrices, opening new avenues for exploring the use of light in resolving universal computational tasks.

Abstract: Cavity optomechanical sensors can offer exceptional sensitivity; however, interrogating the cavity motion with high accuracy and dynamic range has proven to be challenging. Here we employ a dual optical frequency comb spectrometer to readout a microfabricated cavity optomechanical accelerometer, allowing for rapid simultaneous measurements of the cavity's displacement, finesse, and coupling at accelerations up to 24 g (236 m/s$^2$). With this approach, we have achieved a displacement sensitivity of 3 fm/Hz$^{1/2}$, a measurement rate of 100 kHz, and a dynamic range of 3.9 $\times$ 10$^5$ which is the highest we are aware of for a microfabricated cavity optomechanical sensor. In addition, comparisons of our optomechanical sensor coupled directly to a commercial reference accelerometer show agreement at the 0.5% level, a value which is limited by the reference's reported uncertainty. Further, the methods described herein are not limited to accelerometry but rather can be readily applied to nearly any optomechanical sensor where the combination of high speed, dynamic range, and sensitivity is expected to be enabling.

Abstract: We present a detailed study of mechanically compliant, photonic-crystal-based microcavities featuring a quasi-bound state in the continuum. Such systems have recently been predicted to reduce the optical loss in Fabry-Perot-type optomechanical cavities. However, they require two identical photonic-crystal slabs facing each other, which poses a considerable challenge for experimental implementation. We investigate how such an ideal system can be simplified and still exhibit a quasi-bound state in the continuum. We find that a suspended photonic-crystal slab facing a distributed Bragg reflector realizes an optomechanical system with a quasi-bound state in the continuum. In this system, the radiative cavity loss can be eliminated to the extent that the cavity loss is dominated by dissipative loss originating from material absorption only. These proposed optomechanical cavity designs are predicted to feature optical quality factors in excess of 10^5.

Abstract: Many bosons can occupy a single quantum state without a limit, which is described by quantum-mechanical Bose-Einstein statistics and allows the formation of a Bose-Einstein condensate at low temperatures and high particle densities. Photons, historically the first considered bosonic gas, were among the last to show this phenomenon, which was observed in rhodamine-filled microlaser cavities or doped fiber cavities. These more recent findings have raised the natural question as to whether condensation is common in laser systems, potentially implying its technological application. Here, we show the Bose-Einstein condensation of photons in a semiconductor vertical-cavity surface-emitting laser with positive cavity-gain energy detuning. We observed a Bose-Einstein condensate in the ground mode at the critical phase-space density. Experimental results follow the equation of state for a two-dimensional gas of bosons in thermal equilibrium, although the extracted spectral temperatures were lower than those of the device. This is interpreted as originating from the driven-dissipative nature of the condensate being not in full thermal equilibrium with the device. In contrast, non-equilibrium lasing action is observed in higher-order modes in a negatively detuned device. Our work enables the potential exploration of superfluid physics of interacting photons mediated by semiconductor optical non-linearities. It also shows great promise for single-mode high-power emission from a large aperture device.

Abstract: Second-harmonic generation allows for coherently bridging distant regions of the optical spectrum, with applications ranging from laser technology to self-referencing of frequency combs. However, accessing the nonlinear response of a medium typically requires high-power bulk sources, specific nonlinear crystals, and complex optical setups, hindering the path toward large-scale integration. Here we address all of these issues by engineering a chip-scale second-harmonic (SH) source based on the frequency doubling of a semiconductor laser self-injection-locked to a silicon nitride microresonator. The injection-locking mechanism, combined with a high-Q microresonator, results in an ultra-narrow intrinsic linewidth at the fundamental harmonic frequency as small as 57 Hz. Owing to the extreme resonant field enhancement, quasi-phase-matched second-order nonlinearity is photoinduced through the coherent photogalvanic effect and the high coherence is mapped on the generated SH field. We show how such optical poling technique can be engineered to provide efficient SH generation across the whole C and L telecom bands, in a reconfigurable fashion, overcoming the need for poling electrodes. Our device operates with milliwatt-level pumping and outputs SH power exceeding 2 mW, for an efficiency as high as 280%/W under electrical driving. Our findings suggest that standalone, highly-coherent, and efficient SH sources can be integrated in current silicon nitride photonics, unlocking the potential of $\chi^{(2)}$ processes in the next generation of integrated photonic devices.