Brian Stern's research while affiliated with Columbia University and other places
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Publications (12)
Optical phased arrays are a promising beam-steering technology for ultra-small solid-state lidar and free-space communication systems. Long-range, high-performance arrays require a large beam emission area densely packed with thousands of actively phase-controlled, power-hungry light emitting elements. To date, such large-scale phased arrays have b...
Optical frequency combs are broadband sources that offer mutually coherent, equidistant spectral lines with unprecedented precision in frequency and timing for an array of applications¹. Frequency combs generated in microresonators through the Kerr nonlinearity require a single-frequency pump laser and have the potential to provide highly compact,...
Optical frequency combs are broadband sources that offer mutually-coherent, equidistant spectral lines with unprecedented precision in frequency and timing for an array of applications. Kerr frequency combs in microresonators require a single-frequency pump laser and have offered the promise of highly compact, scalable, and power efficient devices....
Chip-scale optical phased arrays could enable compact beam steering and LIDAR for autonomous vehicles, precision robotics, and free-space optical communications. Because these applications demand wide angle beam steering as well as high optical power in the output beam, a natural design choice would be to space the array emitters at a half-waveleng...
We demonstrate the first chip-based microresonator comb source consisting of a semiconductor laser integrated with a silicon nitride microresonator. For electrical powers as low as 130 mW, we generate a single-soliton comb spanning 90 nm.
We demonstrate an integrated silicon nitride/III-V laser leveraging the narrowband backreflection of a high-Q microring resonator for output coupling and feedback. We measure a 13 kHz linewidth with 1.7 mW output power around 1550 nm.
We demonstrate the highest yet-reported element count actively-steered optical phased array with record low array power consumption of <1.8W. We show 2D steering over a 70 x 14 degree field of view while pumped by an integrated InP/silicon laser.
We design and demonstrate a compact, narrow-linewidth integrated laser based on low-loss silicon nitride waveguides coupled to a III-V gain chip. By using a highly confined optical mode, we simultaneously achieve compact bends and ultra-low loss. We leverage the narrowband backreflection of a high- Q microring resonator to act as a cavity output mi...
The inability to efficiently tune the optical properties of waveguiding structures has been one of the major hurdles for the future scalability of integrated photonic systems. In silicon photonics, although dynamic tuning has been achieved with various mechanisms, even the most effective thermo-optic effect offers a refractive index change of only...
Citations
... By individually controlling the phase of light of wavelength λ, emitted from a sufficiently high number (10 2 < N ch < 10 4 ) of closely spaced (d < λ) emitters, a low divergence (<1 mRad) beam may be scanned at high frequencies (>1 MHz) over a wide (>90°) field of view (FOV) without the emergence of higher order beams and thus maintaining a high (>90%) power fraction in the main output beam 6 . Numerous proof-of-concept demonstrations based on silicon and/or siliconnitride photonics technology have been presented over the last decade, in general using wire-bonded chips with several tens or hundreds of electrical/ optical channels [7][8][9][10] . More recently, the application of more advanced electronic integration techniques shows a pathway to a low unit-cost device consisting of a one dimensional emitter array with N ch > 1000 and d < λ, allowing beam properties compatible with demanding applications such as automotive LIDAR [11][12][13] . ...
... The large mechanical steering solution is less desired because it is susceptible to vibration, temperature, acceleration, and inertial forces, and hence declines in performance. Moreover, they need a time-consuming construction and calibration process, resulting in a high unit price [9][10][11]. Furthermore, arbitrary pointing and quick steering, both of which are required for sophisticated communication and sensor applications, become difficult, if not impossible, to accomplish [12,13]. ...
... The on-chip optical-interconnect approach emerges as an attractive solution, having the advantages of large bandwidth and low power consumption. Silicon photonics (SiPh) is regarded as a promising technology to significantly enhance the transmission capacity [6][7][8][9][10][11][12]. High performance SiPh devices can be fabricated and manufactured by using complementary metal-oxide-semiconductor (CMOS) fabrication technologies at high yield and low cost. ...
... In this process, The survey of Si3N4 waveguide loss evolution over the years. The blue shaded elliptical area indicates prior work using EBL [4,7,10,12,[46][47][48][49][50][51][52][53][54][55], while the red shaded elliptical area highlights those using DUV lithography [9,[56][57][58][59]. The dashed red circle indicates the propagation loss of our device, the lowest recorded for the nonlinear Si3N4 waveguide, achieved with DUV stepper lithography and subtractive processing. ...
... In this regard, 1-D beam steering has been demonstrated with 1-D OPAs that can tightly assemble long and narrow radiators [26][27][28]. These systems are capable of steering the beam in one direction only, unless utilized with a highly precise tunable laser, making 2-D beam steering possible [29]. Furthermore, 2-D beam steering has also been shown by dispersive OPAs [30], circular OPAs [31], and planar OPAs [32]. ...
... Over the past few years, the global demand for bandwidth and capacity has increased exponentially (Ahmad et al. 2021). This rapid increase in data traffic is typically caused by the proliferation of various bandwidth-intensive applications, such as search engines, online combs are reported based on FWM in an optical parametric oscillator with silicon nitride ring resonator (Jacob et al. 2010), an integrated semiconductor laser (Stern et al. 2018), Kerr effect in micro-resonator (Xue et al. 2017) and lithium niobate on insulator modulators (Xu et al. 2022). ...
... Furthermore, a void-free encapsulation is critical in order to guarantee a reduced scattering at the coupling region, minimizing systematic excess losses due to the inter-mode interactions, and increasing the threshold power of failure events. This is of the utmost importance, especially in the perspective of the co-integration of III-V-based reflective semiconductor amplifiers (RSOAs) or even free-running multimode laser sources butt-coupled to ultra-high Q Kerr microresonators for compact, chip-based and power-efficient optical frequency comb sources [31][32][33][34][35][36]. ...
... Recently, integrated OPAs have garnered significant research interest [26][27][28][29][30][31][32][33][34][35][36][37][38][39]. Many researchers have demonstrated integrated OPAs on various platforms, such as silicon-on-insulator (SOI) [28, 29, 31, 33-35, 37, 39], silicon nitride ( Si 3 N 4 ) [26,27,31], and indium phosphide (InP) [40,41]. ...
... Nevertheless, achieving a large FSR necessitates adopting a small bend radius, potentially leading to increased bend losses and decreased Q factors. Consequently, these factors exert a detrimental influence on attributes such as laser linewidth [31] and the efficiency of nonlinear optical processes [32]. ...
... Modulators are indispensable in constructing an on-chip communication system. There are many on-chip modulation methods to implement optical signal processing such as electro-optic modulations 1, 2, 3 , thermo-optic modulations 4,5,6,7,8 and electro-absorption modulations 9 . Especially, thermo-optic modulations with advantages of easy fabrication, low cost and compactness have been applied in many optical devices 10,11,12,13 . ...