Lidar, radar, optical imaging and ultrasonic are important environmental sensing technologies in the field of autonomous driving. Among them, the radar can perform long-distance sensing, however it is limited by the resolution and cannot distinguish objects. Optical images have clear object resolving power, but hardly to get distance information. Ultrasonic only detect objects that are in very short distances. Therefore, it is necessary to have a technique that can clearly distinguish the objects and get the object information such as speed and distance at medium-range (100-m) for autonomous driving scheme entering level 4 and level 5.
The existing light technology in the autonomous driving is to place the Lidar module on the roof of a car and perform environment sensing in a rotating manner. Such technology has low sensing capability and is not conform to the development direction of the vehicle industry that not fulfill the demand of autonomous car. In contrast to Lidar module on the roof, placing the Lidar on the front of the car has many advantages, such as easy to collect dust, suffer water corrosion and difficult to set up the electrical system. Integrating the Lidar with headlight system is a feasible direction to solve the aforementioned problems. In this study, we will develop laser headlights system with Lidar module by integrating the optical system of Lidar into headlight a unit, in which the smart laser headlight was achieved by feedback control orders system.
The laser headlight will focus on the development of smart headlights with laser as the light source. With the feedback of the system, it can control the car's light field, avoid high-reflection areas at night. The integrated Lidar module will develop a quasi-static optical scanning system with a wavelength of 1550 nm and embed it in the optical path of the laser headlight. By wavelength differences, the optical path of Lidar does not interfere with headlight and high quality optical data could be obtained. Despite adapting 905 nm as optical wavelength in the current technology, the 1550 nm wavelength selected by this study meets the safety regulations and will not cause damage to the human eye at night or during the day. In this study, we will develop a Lidar module attached to a 10W laser headlight for autonomous driving. The simulation and optical performance of integration of Lidar module with laser headlight will be presented.
Light detection and ranging (LiDAR) is an important technique for three-dimensional environment reconstruction that is useful for self-driving car, robotic vehicle, agriculture detection and blind guidance. Beam steering in the current LiDAR is accomplished by a mechanical spinning architecture, which is heavy, slow and expensive. Micro-electrical-mechanical system (MEMS) built mirror is an alternative solution to reduce size and cost. However, the mechanical beam steering in both techniques cause reliability issues in long-term precise beam positioning that limit the broad application of the LiDAR.
Optical phased arrayed (OPA) comprise periodic placed emitters with coherent light output by using Silicon photonics. The beam steering in the OPA is accomplished by the interference of coherent light that has no moving parts. Each emitter is modulated and delayed by a pre-determined phase that cause the maximum light intensity has an angle to the emitter plane. This angle is determined by the phase difference in each emitter. Therefore, the beam steering is implemented and controlled by the phase adopted. However, according to the interference theory, second and high-order maximum, the side-lobes, appear at different angles that confuse the LiDAR system by multiple positioning at the same time. In addition, to implement wide angle beam steering, the large amounts of arrayed emitters should be applied. To keep coherent, multiple -3dB light coupling structure were applied. The wide distributed and non-uniform light output between emitters cause the beam steering disturbed.
In this work, instead of wide angle beam steering, we design a linear optical phased array (LOPA) with limited number and closed-distance emitters for small angle beam steering. Practical-wise, multiple LOPA modules could be integrated to implement wide angle beam steering. Finite-element method was used to simulate the 1550 nm beam steering behavior in LOPA. With proper and minimal phase delayed, the intensity of the side-lobes was largely suppressed to the primary light. With proper tuning on the sensitivity of the receiver, the high-order disturbance in the LOPA for LiDAR could be eliminated.
In this work, the polymer was incorporated into the luminescent materials to form many encapsulated domains that could possible limit the forming of positive and negative charged layer inside each domain. This was expected to increase the luminescent area and hence the efficiency. Several polymers were used, including Poly(4-vinylphenol) (PVP), Poly (vinyl alcohol) (PVA), Poly (methyl methacrylate) (PMMA), Poly (ethylene Oxide) (PEO) and Poly(3,4- ethylenedioxythiophene) (PEDOT). To understand the effect of these polymers to the efficiency. The OLEC devices with Ru(bpy)3(PF6)2, red-emitting materials, were made. Red light emitting was found in the OLEC devices with PVA, PMMA, and PEO polymer matrix. The highest efficacy of approximately 0.3 lm/W was obtained in the Ru (bpy)3 OLEC with PEO as matrix, which is almost 100 times higher than the device with PVA as matrix. The reason of high luminescent efficiency was primary attributed to the low injection barrier for carrier from PEO into encapsulated Ru(bpy)3(PF6)2. The result of this work indicates the forming of micro-encapsulated domain in the OLEC could enhance the luminous and the efficacy effectively.
The organic material based thin film transistors (TFTs) are attractive for flexible optoelectronics applications due to the ability of lager area fabrication by solution and low temperature process on plastic substrate. Recently, the research of organic TFT focus on low operation voltage and high output current to achieve a low power organic logic circuit for optoelectronic device,such as e-paper or OLED displayer. To obtain low voltage and high output current, high gate capacitance and high channel mobility are key factors. The well-arranged polymer chain by a high temperature postannealing, leading enhancement conductivity of polymer film was a general method. However, the thermal annealing applying heat for all device on the substrate and may not applicable to plastic substrate. Therefore, in this work, the low operation voltage and high output current of polymer TFTs was demonstrated by locally electrical bias annealing. The poly(styrene-comethyl methacrylate) (PS-r-PMMA) with ultra-thin thickness is used as gate dielectric that the thickness is controlled by thermal treatment after spin coated on organic electrode. In electrical bias-annealing process, the PS-r- PMMA is acted a heating layer. After electrical bias-annealing, the polymer TFTs obtain high channel mobility at low voltage that lead high output current by a locally annealing of P3HT film. In the future, the locally electrical biasannealing method could be applied on plastic substrate for flexible optoelectronic application.
Either nanowire or nanohole array for semiconductor were proved to be an efficient nanostructure to harvest solar light. However, for Si, the length of nanostructure about several micrometers is required to have acceptable absorption. Although this length already far less than the bulk Si in which hundred micrometers are required, the micrometers length still not feasible for Si nanostructure. High density nanostructures will cause extensive surface recombination that reduces the power conversion efficiency. Therefore, explore the dependence of light absorption to the length of Si nanostructure is very important to design an efficient solar cell. In this work, the Si nanohole array was fabricated in several depths from 110 to 960 nm. The total reflection was less than 1% at visible regime for 960 nm depth hole. The Ag nanoparticles were put at the bottom of the nanohole to explore the light absorption by plasmonic enhanced Raman scattering. A chemical, pNTP, was cover Ag nanoparticle as the prober for the plasmonic effect. As the laser light incident to the Ag nanoparticle, the surface plasmonic effect will enhance the Raman scattering of the pNTP. The enhanced Raman signal obtained from pNTP indicates the incident light could penetrate into the bottom of the Si nanohole array without significant absorption. The experiment result indicate the Raman signal decay fast after the depth of nanohole exceed 240 nm. This result indicate, the length of Si nanostructure may not need micrometers length to harvest incident solar light. This finding pave a bright route for design of Si solar cell with nanostructures.
Access to the requested content is limited to institutions that have purchased or subscribe to SPIE eBooks.
You are receiving this notice because your organization may not have SPIE eBooks access.*
*Shibboleth/Open Athens users─please
sign in
to access your institution's subscriptions.
To obtain this item, you may purchase the complete book in print or electronic format on
SPIE.org.
INSTITUTIONAL Select your institution to access the SPIE Digital Library.
PERSONAL Sign in with your SPIE account to access your personal subscriptions or to use specific features such as save to my library, sign up for alerts, save searches, etc.