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Research progress of laser protection technology for optoelectronic imaging system (invited)
Li Yangliang, Ye Qing, Wu Yunlong, Sun Ke, Zhang Hao, Sun Xiaoquan
2023, 52(6): 20230192. doi: 10.3788/IRLA20230192
[Abstract](357) [FullText HTML] (72) [PDF 3008KB](106)
  Significance   Optoelectronic imaging systems, characterized by their compact size, light weight, high reliability, resolution, and dynamic range, have been extensively employed in various fields, such as medical imaging, media production, security management, high-resolution target reconnaissance, precision guidance, fire control and targeting, and flight assistance. However, with the rapid advancements in laser technology and the widespread use of laser weapon systems, the risk of optoelectronic imaging systems being blinded or dazzled by lasers has significantly increased, resulting in a substantial decrease in information acquisition capabilities. Consequently, investigating laser protection technologies for optoelectronic imaging systems has become increasingly vital.   Progress  The article initially provides a brief overview of the mechanisms and limitations of laser blinding protection technologies for optoelectronic imaging systems, focusing on linear and nonlinear materials. It then delves into laser blinding protection technologies employing phase-change materials, such as vanadium dioxide, discusses their mechanisms, fabrication methods, and application progress. Subsequently, the article explores the mechanisms and preliminary application studies of laser blinding protection technologies based on computational imaging, highlights the necessity and feasibility of researching laser dazzling protection technologies for optoelectronic imaging systems in relation to laser blinding. Finally, the advantages and disadvantages of various laser protection technologies for optoelectronic imaging systems are summarized, along with potential future development directions.   Conclusions and Prospects  The application of computational imaging technology for laser protection offers a groundbreaking technical solution, featuring a wide protective spectrum and exceptional adaptability. This approach eliminates the need for prior knowledge of interfering laser locations, wavelengths, or polarization states, as required by linear material protection, as well as considerations of response times and protection thresholds, as demanded by nonlinear or phase-change material protection. Computational imaging technology can defend against common continuous lasers, nanosecond pulse lasers, and emerging ultra-short pulse lasers, such as picosecond or femtosecond pulses. Designing and fabricating high-precision optical field control components and ensuring high-quality image restoration are crucial future development directions for this technology. As lensless imaging technology employing mask modulation, a key research area in computational imaging progressively matures, it may fundamentally resolve the high gain caused by the optical system structure in imaging systems, thereby effectively addressing the issue of laser blinding protection in such systems. Laser dazzling protection technology exhibits broader application scenarios compared to blinding protection technology; However, current research is relatively limited, and no groundbreaking solutions have been proposed. Based on the mechanisms of laser-induced blinding and dazzling in optoelectronic imaging systems, the seperate study on blinding and dazzling technologies is incomplete and unscientific. Future research should focus on integrating laser blinding and dazzling protection for optoelectronic imaging systems, examining protection mechanisms, technical approaches, and cost-effectiveness from multiple perspectives.
Review of laser Doppler velocimeter technology for navigation and localization
Chen Lanjian, Xi Chongbin, Zhou Jian, Nie Xiaoming, Wang Qi, Huang Rong, Xiang Zhiyi, Jin Shilong
2023, 52(6): 20230143. doi: 10.3788/IRLA20230143
[Abstract](199) [FullText HTML] (81) [PDF 2433KB](41)
  Significance   The technology known as the laser Doppler velocimeter (LDV) has gained widespread application in both scientific research and industrial production, following years of development. This technology offers an independent means of measuring velocity, which is especially useful for the navigation and localization of vehicles. Compared to traditional velocity measuring methods such as odometers, accelerometers, and global navigation satellite systems (GNSS), LDVs have high accuracy and reliability even in all-day, all-weather conditions. These features satisfy the requirement for precise navigation and localization, thus getting the focus of attention of the researchers in this field. In order to anticipate future progress, it is essential to review the current research.   Progress  The frequency shift of the Doppler effect in the probe beam of LDVs depends on the velocity of the vehicle which is based on the optical Doppler effect. When LDVs are installed on vehicles, the angle between the probe beam and the road surface remains constant. By measuring the frequency shift, it is possible to determine the velocity of the vehicles with accuracy. LDVs can be classified into two types based on their optical structure of dual-beam and single-beam. For the dual-beam type, two probe beams intersect each other, and the point of intersection is referred to as the control volume. When traveling over a bumpy road, dual-beam LDVs often lose the signal due to the limited depth of the control volume. The researcher has proposed a multipoint layer-type LDV to address the limitations of dual-beam LDVs. This type of LDV consists of multiple dual-beam probes that are distributed in the vertical direction. Each probe's small depth of field is combined to form a larger depth of field. For the single-beam type, there is only one beam containing the Doppler frequency shift during the measurement, which is different from the dual-beam LDV. The reflected light of the probe beam is transmitted back to the detector after illuminating the uneven road surface and is mixed with the reference beam without any Doppler frequency shift. The single-beam LDV has a broad depth of field, ensuring accurate and stable measurements. It is particularly suitable for use in ground vehicles compared to the dual-beam LDV. Improvements have been made for single-beam LDV to enhance its performance. The reuse-type single-beam LDV utilizes part of the reference beam power to illuminate the road surface, which would otherwise be wasted by an attenuator in the traditional single-beam LDV. The Janus configuration single-beam LDV eliminates the effect of vertical velocity on the velocity parallel to the direction of the vehicle's heading when ground vehicles experience vertical jolts. The speed component in the direction of the vehicle's heading cannot accurately reflect the actual state of a moving vehicle, as there are two components in the vertical and lateral directions. To deal with this, two-dimension (2D) and three-dimension (3D) LDVs are investigated by researchers. There are two probes in 2D LDV and four probes in 3D LDV. Each probe in these two multi-dimensional LDVs can be either dual-beam or single-beam type.   For years, researchers have been investigating the use of LDVs in the navigation and localization of ground vehicles. By integrating LDVs with inertial measurement units (IMUs), ground vehicles can achieve significantly improved localization and navigation precision. In particular, the highly accurate velocity data provided by LDVs can effectively suppress the measurement divergence of IMUs. As a result, the accuracy of dead reckoning has already reached an impressive 0.01%. However, to fully explore the potential of LDV technology for new applications such as high-speed trains, underwater vehicles, and aerial vehicles, further research is necessary. This will require optimization of LDV technology in terms of optical design, circuit design, and system architecture.   Conclusions and Prospects  This paper reviews the current research on LDVs for the navigation and localization of ground vehicles. It demonstrates the process of development and concludes that LDV plays a significant role in achieving precise navigation and localization of vehicles. Additionally, the paper provides an outlook on the development trend of LDV and its potential applications for high-speed trains, underwater vehicles, and aerial vehicles. The perspectives provided here can serve as a guide for future LDV research.
Rydberg atomic radio-optical measurement and spectrum processing techniques (invited)
Wu Jinyun, Yang Jian, Gao Weichao, Zhang Yinfa
2023, 52(6): 20230264. doi: 10.3788/IRLA20230264
[Abstract](356) [FullText HTML] (165) [PDF 12389KB](79)
  Significance   Rydberg atoms are highly excited atoms with large electric dipole moments. The energy difference between adjacent levels can cover an ultra-wide frequency spectrum range from DC to THz, making it possible to achieve high-sensitivity and ultra-wideband reception of electromagnetic fields. Radio-optical measurements based on Rydberg atoms are achieved by precisely controlling two laser beams, the probe laser and the control laser, to transform ground state alkali metal atoms into Rydberg atoms and induce Electromagnetic Induced Transparency (EIT) in the transmitted spectrum of the probe laser. Under the interaction of the input radio signal, Autler-Townes (AT) splitting occurs in the transparent EIT spectrum, completing the conversion of radio signals to optical signals (Fig.2-3), thereby extracting information such as frequency, amplitude, and phase of the radio signal. This technology has attracted great attention in electronic information fields such as electric field metrology, electromagnetic spectrum detection, communication, and radar in recent years. The physical implementation of this technology is simple and does not require strict physical conditions as usual quantum technologies such as single-photon sources or ultra-cold and superconducting conditions. It can be achieved at room temperature without being limited by the level of production technology. It is considered one of the fastest applicable quantum technologies with its high stability, accuracy, and repeatability that could partially replace existing radio reception technologies in the near future.   Progress  In the past decade, researchers have made significant progress in the study of radio-optical measurement techniques based on Rydberg atoms, from precise measurements of single-frequency static radio signals in electric field metrology applications to real-time reception of single-frequency dynamic radio signals in communication applications, and to spectrum detection and communication reception of complex multi-frequency radio signals. The key to this technology is how to quickly and accurately extract information about the radio signal from the output EIT spectrum of the atomic system. Different types of radio signals, such as static, dynamic, single-frequency, and multi-frequency radio signals, require different information extraction and spectral processing methods, as well as different experimental designs and implementations. For single-frequency static radio signals, researchers have already used Rydberg atoms in experiments to measure field strengths in the 0-320 GHz frequency range with a maximum coverage range of 780 pV·cm−1 to 50 V·cm−1. By using heterodyne technology (Fig.8) and critical phenomena in many-body Rydberg atomic system, the current sensitivity can reach as low as 49 nV·cm−1·Hz−1/2. Unlike measuring single-frequency static radio signals, for single-frequency dynamic radio signals, Rydberg atom systems are required to track and respond to rapidly changing radio signals in real-time and quickly read EIT spectral changes at the end point. Its primary application scenario is the communication reception. Since 2018, a large number of verification experiments on wireless communication reception principle have been carried out based on Rydberg atoms. This technology can directly convert intermediate frequency or baseband signals on the carrier into optical signals for direct demodulation. Verified communication methods include amplitude modulation (AM), frequency modulation (FM), and phase modulation (PM). When the input wireless signal becomes complex, especially for multi-frequency wireless signal input, the output EIT spectrum of the probe laser will become complicated. It will be a big challenge to quickly and effectively read and distinguish information from different frequency wireless signals. Currently, a small amount of research is focused on verifying dynamic multi-frequency wireless signals for communication reception, including using multi-harmonic Rydberg atomic level structures to finely adjust and optimize system parameters at the front end or using post-processing techniques such as deep learning at the back end to achieve recognition and reading of multiple frequency information. People have experimentally achieved simultaneous reception of five completely different frequency signals within a spectrum range of over 100 GHz (Fig.18) or 20 similar frequency signals within a range of 100 kHz (Fig.23).   Conclusions and Prospects  Through continuous research over the past 10 years, it has been experimentally verified that radio-optical measurements based on Rydberg atoms have unique quantum advantages in spectrum range, sensitivity, minimum field strength, signal demodulation mechanism, and other aspects. This technology has demonstrated promising prospects in applications such as electric field metrology, electromagnetic spectrum detection, communication, radar, and more. In order to further develop this technology to fully leverage the unique quantum advantages of Rydberg atoms and achieve practical applications as soon as possible, researchers need to deepen their research on the comprehensive performance improvement, anti-interference ability enhancement, miniaturization integration and simultaneously reduce the costs of radio-optical measurements based on Rydberg atoms.
Research progress of infrared stealth technology of micro-nano optical structure (invited)
Jiang Xinpeng, Du Te, Ma Hansi, Zhang Zhaojian, He Xin, Zhang Zhenfu, Chen Huan, Yu Yang, Huang Sha, Yang Junbo
2023, 52(6): 20230197. doi: 10.3788/IRLA20230197
[Abstract](638) [FullText HTML] (174) [PDF 4729KB](231)
  Significance   With the diversified development of infrared detection technology, the demand for infrared stealth technology is increasingly urgent. Infrared stealth technology aims to effectively control the infrared signature signals of weapons and equipment, reduce the operating range of enemy infrared detection systems, improve survival ability, penetration ability, and combat effectiveness. However, traditional infrared stealth technology is facing serious challenges of multi-band detection and multi-functional compatibility, making it of great significance to study the infrared stealth technology of micro-nano optical structure. Sub-wavelength micro-nano optical structures based on local resonance mechanism greatly enrich the modulation of light transmission behavior. They can be state-of-the-art in material and structure design for infrared radiation, so as to meet the demand of ideal emissivity spectrum for infrared stealth. It is foreseeable that infrared stealth technology based on the optical micro-nano structures will transform traditional infrared stealth technology and provide point-to-point spectral design for the multi-aspect demand, which makes the research progress of micro-nano optical structure infrared stealth technology meaningful.   Progress  Focusing on the progress of infrared stealth technology, this paper introduces the basic principles of thin film absorber, metal surface plasmonic, tunable absorber based on phase change materials (PCMs), and intelligent design for spectral response firstly. For example, the PCMs are widely used in tunable infrared absorbers by regulating resonance wavelength and changing infrared emissivity without the structural changes (Fig.4). And the innovatory field of the intelligent design has recently been transforming conventional micro-nano optical structure and allowing for the discovery of unorthodox optical structures via computer algorithms rather than engineered "by hand" (Fig.5-6). Secondly, the development status of optical micro-nano structure infrared stealth technology in the past decade is introduced. As an application technology driven by demand, infrared stealth technology faces many challenges such as multi-spectral compatibility, multi-functional integration, and complex changing environments. With the deepening optical micro-nano structures research, the application of infrared stealth technology has been expanding and showing the following new characteristics. (1) In order to deal with the thermal radiation detection of infrared atmospheric transparent window bands, infrared stealth technology is developing from single-band towards the multi-band infrared stealth; (2) On the basis of multi-band infrared stealth, balance and comprehensive design with infrared laser, visible light, radar and other multispectral stealth are required; (3) A new infrared stealth technology is developed that combines multiple functions such as thermal management, infrared sensor, and radiation regulation; (4) Adaptive infrared stealth technology is developed that integrates new materials such as phase change materials, two-dimensional materials of graphene, and vanadium oxides. To this end, the spectral tailoring design achieved through optical micro-nano structures endows infrared stealth technology with more new possibilities, including multispectral infrared stealth technology, multifunctional infrared stealth technology, and adaptive infrared stealth technology. According to the different requirements of multi-spectral compatibility, this paper summarizes the possible requirement of multispectral infrared stealth technology and current development status (Fig.7). Through the comprehensive survey, this paper reveals four development trends of micro-nano optical structure infrared stealth technology: multispectral compatibility, multi-function integration, large-area fabrication, and adaptive infrared stealth system.   Conclusions and Prospects  During the last decade, the micro-nano optical structure infrared stealth technology has made dramatic development. The multispectral infrared stealth technology has been extended from the single-band to the multi-band infrared stealth technology which is compatible with visible band, laser, and microwave. The multifunctional infrared stealth technology has been considered to integrate the thermal management, infrared encryption and infrared sensor, the adaptive infrared stealth technology has been widely studied in the dual-band infrared transparent atmosphere window by flourishing research of smart materials. The research of this paper aims to provide some reference for the infrared stealth technology of optical micro-nano structures in the future. It is expected that optical micro-nano structures will provide a promising way for the more multispectral, more versatile, and more adaptive infrared stealth technology.
Research progress of aerosol particle aggregation model (invited)
Gu Youlin, Zhang Xi, Hu Yihua, Meng Fanhao, Chen Guolong, Ding Wanying, He Haihao
2023, 52(6): 20230243. doi: 10.3788/IRLA20230243
[Abstract](176) [FullText HTML] (68) [PDF 1753KB](31)
  Significance   Aerosol particles refer to the solid, liquid or solid-liquid mixture particles suspended in the atmosphere caused by naturally formed or artificial factors, which are composed of metal powder, bioparticle, dust particle and so on. The analysis of the spatial structure and motion status of aerosol particles is of great significance for ecological environmental protection, climate change control and functional materials development. As an important means to study the spatial structure and motion status of aerosol particles, the aggregation model of aerosol particles is used to simulate the aggregated procedure of aerosol particles under different conditions, which is employed to explain its aggregation and physical mechanism. Aggregation models are widely used in optics, astronomical physics, dynamics and so on. The investigation on the mechanism, influential factors and application of aerosol particles aggregation model is beneficial to the optimization of aerosol particles aggregation model and the preparation of novel extinction materials.   Progress  Firstly, the mechanism and main influential factors of aerosol particle aggregations are analyzed, such as particle spatial structure characteristics, the interaction of particles, and atmospheric environment. The theory of fractal, mathematical statistics and molecular simulation used in the study of aerosol particle aggregation are summarized. Secondly, based on the implementation methods of aerosol particle aggregation simulation, the classifications and characteristics of aggregation models are described. In addition, the application of the aerosol particle aggregation model in optics, astrophysics, and dynamics is mentioned. The model optimization such as algorithm efficiency, simulation modes, and application errors reduction is analyzed. Finally, in view of the current application status and challenges faced by aerosol particle aggregation models, the trend of aggregation models is proposed, such as the construction of a non-spherical particle aggregation model, application of multi-factor coupled aggregation model and simulation of real-time spatial distribution of aggregation particles, etc.   Conclusions and Prospects  In recent years, the aerosol particle aggregation models have been used in a variety of areas. The aerosol particle aggregation model can be used to simulate the visual procedure of particle aggregation, study the formation mechanism and aggregation dynamics of particles, and carry out an in-depth analysis of aggregation characteristics. The aerosol particle aggregation model is important to analyze dynamics, morphology and other properties of aggregates. These models can be used to explain the phenomena such as gas mixture explosions and comet polarization. It can also provide a means for the screening and controllable preparation of extinction materials. However, there are still some shortcomings. Firstly, the complex morphology and structures of non-spherical particles are an important part of simulating and analyzing more realistic aerosol particle applications. The aggregation model of randomly oriented non-spherical aerosol particles with controllable particle shape and size has not yet been established. Secondly, the analysis of the aggregation mechanism of the model is relatively simple. To improve the accuracy of the simulation, the influence of multiple factors on the aggregation procedure needs to be considered. In addition, the simulation of real-time spatial distribution of the particles is acquired to further investigate in future. Therefore, the model can be optimized as followings. On the one hand, the aggregation models for of randomly oriented non-spherical aerosol particles can be analytically established. On the other hand, it can be revised in terms of multi-factor coupling and real-time spatial distribution of particles.
Research progress of low-quantum-defect fiber laser at 1 μm band (invited)
Xu Jiangming, Zhang Yang, Ma Xiaoya, Ye Jun, Ke Yanzhao, Li Sicheng, Liang Junrui, He Junhong, Huang Liangjin, Pan Zhiyong, Yao Tianfu, Leng Jinyong, Zhou Pu
2023, 52(6): 20230267. doi: 10.3788/IRLA20230267
[Abstract](152) [FullText HTML] (46) [PDF 3434KB](69)
  Significance   Power scalability of fiber lasers have attracted a great deal of attention for its remarkable features, such as excellent beam quality, high conversion efficiency, flexible operation, and wide applications in biomedicine, intelligent manufacturing, energy exploration, defense and security. However, there have been no reports of significant operation power breakthroughs of near-single-mode fiber laser since the first demonstration of 10 kW-level system in 2009. The wasted heat accumulation, which can induce thermal lens and transverse mode instability effects, is one of the most important limitation factors. Quantum defect, defined as (1-λp/λs), where λp is the pump wavelength and λs is the lasing wavelength, has always been a key parameter in high-power fiber lasers. High quantum defect not only limits the conversion efficiency but also increases the thermal load in fiber lasers. In hence, much research on low quantum defect fiber laser has been reported in the past decades.   Progress  This paper first introduces the performance exploration of high-power fiber laser at 1 μm band, including the power scaling and corresponding quantum defect decrease. It can be said that the power scaling progress of fiber lasers is also a continuous struggle against waste heat and other factors. As to low quantum defect fiber laser, the reported works mainly focus on two different technical schemes based on rare earth doped fiber and passive fiber. For the convenience of description, this article stipulates that the quantum defect of low quantum defect fiber lasers is ≤ 4.50%, and the quantum defect of ultra-low quantum defect fiber lasers is ≤ 1%.   Then, ytterbium-doped fiber lasers with low quantum defect are summarized. In 2011, Wirth et al. demonstrated a 2.9 kW fiber laser operating at 1071 nm that is tandem-pumped by a 1030 nm thin-disk laser, and the corresponding quantum defect is about 3.83% (Fig.1). In 2014, Chang et al. presented a fiber laser with a maximal output power of 5.7 W and a quantum defect of 1.9% (Fig.2). To further reduce the quantum defect of fiber lasers, some specially designed active fibers and high pumping intensity methods are adopted. For example, in 2018, Yu et al. demonstrated a 400 mW-level fiber lasers with less than 1% quantum defect via ytterbium-doped multicomponent fluorosilicate fibers (Fig.5).   Additionally, Raman fiber lasers with low quantum defect are reviewed. Based on common silicon fiber, a maximal power of 3 kW-level with a quantum defect of 4.42% (Fig.7) and a maximal power of 6.2 W with a quantum defect of 0.56% were achieved. To further improve the operation power of ultra-low quantum defect fiber laser, the scheme enabled by boson peak in phosphosilicate fiber was presented and realized by Zhang et al. in 2020 (Fig.14). In 2021, Ma et al. demonstrated a 100 W-level ultra-low quantum defect fiber laser with a quantum defect of 0.97%. What's more, cladding pump scheme was also been validated (Fig.15).   Conclusions and Prospects   The important progress of low quantum defect fiber laser operating at 1 μm band is reviewed. And the manuscript mainly focuses on two different technical schemes based on rare earth doped fiber and passive fiber. In rare earth doped fiber based lasers, the utilization of tandem-pumping, multi-component doping and strong pumping schemes can reduce the quantum defect, and the related ytterbium-doped fiber lasers with quantum defect ≤1% have achieved 400 mW-level output power. In Raman fiber lasers, the maximal output power of 100 W-level with a quantum defect of ≤1% has been demonstrated with the aid of techniques such as special doping, pump spectrum regulation, and gain competition suppression. The feasibility of cladding pumping scheme has also been verified successfully, indicating its significant potential in achieving high-power and low quantum loss output.