亚洲中文字幕人妻在线观看|欧美日韩精国产无套粉嫩白浆在线观看|91麻豆精品国产自产|亚洲精品?Ⅴ无码精品丝袜足|最近免费韩国高清在线观看|国产亚洲精品观看91在线|国产亚洲成aⅴ人片在线观看|欧洲极品无码一区二区三区|亚洲中文字幕人妻在线观看|日本久久亚洲精品

2022

2022

  • Record 49 of

    Title:Laser Active Fusion Trajectory Measurement Technology in Rocket Take-off Phase
    Author(s):Shi, Heng(1,2,3,4); Gao, Xin(1); Li, Xiyu(1); Lei, Chengqiang(1); Hu, Lei(1); Zong, Yonghong(1); Zheng, Donghao(1); Sun, Rui(1)
    Source: Guangzi Xuebao/Acta Photonica Sinica  Volume: 51  Issue: 12  DOI: 10.3788/gzxb20225112.1212001  Published: 2022  
    Abstract:The high-precision trajectory data of the rocket vertical take-off phase can be used to evaluate the technical performance and accuracy of the rocket,provide data reference for the improved design and finalization of the rocket,and also provide important trajectory reference data for the rocket take-off safety control system. The trajectory of the rocket in the vertical take-off phase changes greatly in the vertical rising direction,while the theoretical trajectory in both directions of the horizontal plane does not change. However,in the actual launch process,due to various interferences and certain delays and deviations in the real-time control of the rocket,the actual trajectory of the rocket in the horizontal plane will inevitably have a certain offset. The traditional trajectory measurement methods in the vertical take-off phase of rocket mainly include telemetry,optical and radio radar measurement. Due to the vibration caused by rocket launch,the trajectory measurement accuracy of telemetry system is not high,and it is difficult to obtain effective original analysis data after rocket failure. The optical measurement system uses images taken by multiple stations to obtain the rocket trajectory data after the rendezvous,but it is easily affected by the weather and has poor real-time performance. Due to the interference of ground clutter,it is difficult for radio radar to obtain effective trajectory data at this stage. It can be seen that there is no real-time trajectory measurement data in the vertical take-off phase of the rocket at present,and it is urgent to fill the data gap in this phase through new measurement methods.A single lidar can be used to measure the rocket trajectory in the take-off phase,but the trajectory data of the rocket in both directions of the horizontal plane in the vertical take-off phase changes very little,and only relying on a single lidar to measure the trajectory in the two directions will cause large errors. Compared with a single lidar measurement system,the field of view of the two multi-line lidars in the vertical direction can reach 25°,and a total of 128 laser scanning lines scan the rocket target area at the same time. In addition,the two lidars conduct fusion measurement at an intersection angle of 70°,which can cover the target area of the rocket with a larger angle range. Therefore,more target measurement points can be scanned,which can not only improve the fitting accuracy of the center of the ellipse ,but also effectively ensure the reliability of the data measurement. In view of the difficult technical problem of obtaining real-time high-precision trajectory data in the rocket vertical takeoff phase,a new rocket take-off phase trajectory fusion measurement system based on lidar is proposed in this paper,which has the advantages of convenient station layout,easy installation and low power consumption. At the same time,it is less affected by weather,ground clutter signals and rocket vibration,and can effectively obtain the rocket real-time trajectory data. Two lidars are installed on a two-dimensional precision turntable to form a fusion measurement system. Before the launch of the rocket,the two lidars jointly scan the middle and upper target areas of the rocket. Based on the proposed algorithm of laser point cloud data correction,the initial value solution of rocket target area trajectory and data fusion processing of the two trajectory data,the static and dynamic trajectory measurement accuracy of the lidar are calculated and analyzed to be 0.023 5 m and 0.036 6 m respectively. In the process of rocket vertical take-off,the two-dimensional precision turntable receives the trajectory data of the rocket target area in real time,guides the lidar to track and scan the whole process of the rocket vertical take-off phase with high precision according to the rocket position information,and completes the real-time and high-precision trajectory measurement of the rocket vertical take-off phase,which effectively fills the gap of the trajectory measurement data of the rocket at this stage and ensures the safety of rocket launch. Up to now,the rocket real-time trajectory measurement system based on lidar has successfully completed many test tasks in a satellite launch center. Under the conditions of vibration,tail flame and other environmental interference in the rocket take-off phase,the real-time dynamic trajectory measurement accuracy can be better than 0.05 m. It is verified that the measurement system and method proposed in this paper can effectively improve the measurement accuracy and reliability of rocket trajectory,which has important engineering application value. ? 2022 Chinese Optical Society. All rights reserved.
    Accession Number: 20230813622786
  • Record 50 of

    Title:Theoretical Model of Thermal Stress in the Film-Substrate System of Optical Thin Film
    Author(s):Shi, Yunyun(1,2); Xu, Junqi(1); Li, Yang(1); Liu, Zheng(2); Zhang, Kaifeng(3); Su, Junhong(1)
    Source: Journal of Electronic Materials  Volume: 51  Issue: 10  DOI: 10.1007/s11664-022-09819-w  Published: October 2022  
    Abstract:A model of thermal stress in double-layer optical dielectric films on circular substrates was established based on the theory of double-layer composite beams. Here, considering the boundary conditions including force balance and bending moment balance, the distribution of stress and strain in the double-layer film-substrate system was analyzed following equivalence manipulation to determine a detailed formula for calculating the thermal stress in the equivalent film and substrate. The derived formula was not only effective in analyzing the stress and strain of the double-layer film-substrate system but was also applicable for predicting the distribution of thermal stress in the periodic elastic multilayer film-substrate system. According to the actual radius of curvature of the substrate measured via a profilometer before and after the deposition of the HfO2/SiO2 double-layer films, the obtained residual stress of the film was ? 79.33 MPa, whereas the thermal stress of the film was calculated to be ?52.59 MPa using the theoretical formula. The calculations of the theoretical model were similar to the experimental results when the smaller intrinsic stresses were neglected and the double-layer film was only of nanometer thickness, thus verifying the effectiveness of the double-layer film-substrate model. ? 2022, The Minerals, Metals & Materials Society.
    Accession Number: 20223412602126
  • Record 51 of

    Title:Large-field structured illumination microscopy based on 2D grating and a spatial light modulator
    Author(s):Wen, Kai(1,2); Fang, Xiang(1); Ma, Ying(1); Liu, Min(1); An, Sha(1); Zheng, JuanJuan(1,3); Kozacki, Tomasz(2); Gao, Peng(1)
    Source: Optics Letters  Volume: 47  Issue: 11  DOI: 10.1364/OL.460292  Published: June 1, 2022  
    Abstract:Structured illumination microscopy (SIM) has been widely used in biological research due to its merits of fast imaging speed, minimal invasiveness, super-resolution, and optical sectioning imaging capability. However, the conventional SIM that uses a spatial light modulator (SLM) for fringe projection often has a limited imaging field of view. Herein, we report a large-field SIM technique that combines a 2D grating for fringe pattern projection and an SLM for selecting fringe orientation and performing phase shifting digitally. The proposed SIM technique breaks the bottleneck of fringe number limited by the digital projection devices, while maintaining the advantage of high-speed (digital) phase shifting of conventional SIM. The method avoids the pixilation and dispersion effects of the SLMs. Finally, a 1.8-fold resolution enhancement in a large field of 690 × 517 μm2 under a 20×/NA0.75 objective is experimentally demonstrated. The proposed technique can be widely applied to biology, chemistry, and industry. ? 2022 Optica Publishing Group
    Accession Number: 20222212182743
  • Record 52 of

    Title:Secondary electron emission of Al2O3 and MgO nanofilms fabricated by atomic layer deposition
    Author(s):Zhu, Xiangping(1,2); Wang, Dan(3); Wang, Hui(4,5); Zhou, Rundong(1,2); Li, Xiangxin(1); Hong, Yunfan(1); Jin, Chuan(1); Wei, Yonglin(1); Luo, Chaopeng(4,5); Zhao, Wei(1,2)
    Source: Kexue Tongbao/Chinese Science Bulletin  Volume: 67  Issue: 23  DOI: 10.1360/TB-2022-0175  Published: 2022  
    Abstract:Electron multiplier devices are widely applied in many electronic instruments like mass spectrometers and atomic clocks. It is considerably crucial for a multiplier to possess a high electron gain, and this index can be directly determined by secondary electron yield (SEY) of the dynodes. Al2O3 and MgO possess a relatively high SEY level among majority of dynode materials, and their film products are excellent dynode candidates. Whereas, for some multipliers like microchannel plate (MCP), only an ultrathin film of several nanometers is allowed to be coated onto the inner wall of the micro channels to avoid the variation of the channel diameter. Therefore, SEY characteristics of the ultrathin films are necessary to be figured out. Here, by using the technology of atomic layer deposition, 7 groups of ultrathin Al2O3 and MgO nanofilms with increase thickness (1, 3, 5, 7, 10, 30, and 50 nm) are fabricated on silicon (Si) substrates. As well as, 5 groups of Al2O3 nanofilms (1, 2, 3, 4, and 20 nm) are deposited on MgO film (20 nm) substrate. Surface composition, morphology, film thickness, and SEY have been characterized in detail. Via the experiments, it is found that SEY of the Al2O3/Si and MgO/Si samples largely depends on the film thickness, namely, SEY increases obviously as the film thickness rises, meanwhile, the increment of SEY decreases gradually. The SEY tendency indicates that the effect of top film on SEY becomes enhanced, and the influence of bottom substrate on SEY becomes weakened. When the film thickness increases beyond 30 nm, SEY increment approaches to 0, and SEY tends to be saturated. This phenomenon demonstrates that the penetration depth of incident electrons is less than the film thickness under the circumstances. To interpret the experimental results, the SEE semi-physical theory developed for double layer structures is utilized. The calculation results indicate that the film thickness has a remarkable impact on SEY, especially when the incident energy becomes lower and the film becomes thicker, the results also reveal that the dielectric surface film possesses a great ability to modulate the surface SEY. However, SEY becomes less dependent on film thickness as the incident energy increases, and it results from the increase of penetration depth for the incident electrons. This work reveals the mechanism of the SEE characteristics for ultrathin Al2O3 and MgO nanofilms, which is of great significance for the subsequent research on the use of nanoscale high SEY dielectric films as the SEE functional layer in electron multipliers. ? 2022 Chinese Academy of Sciences. All rights reserved.
    Accession Number: 20223712734072
  • Record 53 of

    Title:Broadband Fiber Chirped-pulse Amplification System Based on Parabolic Evolution
    Author(s):Du, Li(1); Jin, Cuihong(1); Yang, Zhi(2); Cui, Yudong(1,3)
    Source: Guangzi Xuebao/Acta Photonica Sinica  Volume: 51  Issue: 11  DOI: 10.3788/gzxb20225111.1114002  Published: November 2022  
    Abstract:Fiber lasers have attracted substantial research interest due to their high stability, excellent beam quality and system compactness. Furthermore, lasers generating high-energy ultrafast pulses and operating at the 1 550 nm region are widely developed due to the low optical attenuation at the first communication window and more cost-effective than other laser sources in a variety of applications such as ultrafast spectroscopy, precision material processing and terahertz-wave generation. To achieve high-energy pulses, an Erbium-doped fiber amplifier was employed to amplify seed pulses. However, pulses will accumulate large nonlinear effects such as Self-Phase Modulation (SPM) and Stimulated Raman Scattering (SRS) during direct amplification, thus degrading the pulse quality. One common solution is to widen the pulse width by introducing a chirp before amplification. The peak power intensity is significantly attenuated, avoiding excessive nonlinearity. The amplified pulse is then de-chirped by a compressor. This method is called chirped pulse amplification (CPA). Several high-power CPA systems operating at 1.56 μm have been demonstrated in recent years. However, all of these sources produced a pulse with spectral width between 5 nm and 15 nm. Broadband fiber laser plays an important role in optical frequency combs, optical coherent tomography, optical coherence radar and fiber optical sensing systems. There is a lack of high-energy devices capable of generating pulses with spectral width above 30 nm. Several approaches have been utilized to generate broadband pulses. A noise-like mode-locked fiber laser was demonstrated based on the precise adjustment of intracavity dispersion. However, this laser regime was seldom applied in ultrashort pulses due to its incompressibility. A Mamyshev oscillator is able to generate broadband pulses as shorter than 100 fs at the expense of complicated intracavity structure and accurate pulse evolution. The extra-cavity generation method relies on Highly Nonlinear Fibers (HNLFs), such as photonic crystal fibers, whose complexity of design is increased by demanding careful selection of parameters for the seed pulse. In addition, the nonlinear effect induced by SPM generates a nonlinear chirp on both sides of pulses which degrades the beam quality in CPA systems. Note that self-similar pulses are nonlinear optical structures whose amplitudes and widths could be altered by dispersion, nonlinearity, gain and other system parameters, while maintaining the overall shapes. Since the self-similar pulse has a strict linear frequency chirp induced by the balance between SPM and normal group velocity dispersion in the erbium-doped fiber, it could be effectively compressed by grating pairs to obtain a high-power ultrashort pulse. Therefore, the combination of self-similar amplification and CPA is a promising solution to generating broadband watt-level pulse. High-energy ultrafast pulses based on parabolic evolution in ytterbium-doped lasers have been reported. Nevertheless, the Erbium-Doped Fiber Amplifier (EDFA) based on self-similar amplification operates at an anomalous dispersion region, which is less applicable to generating pulses with the average power above watt-level high-energy pulses comparing to Ytterbium-Doped Fiber Amplifier (YDFA). At the same time, high-energy CPA systems operating at 1 550 nm significantly lag behind Yb-doped lasers due to high quantum defect, thermal effects and nonlinearity. At present, there is no report on a broadband high-energy CPA system based on parabolic evolution operating at 1 550 nm. Here, we demonstrated an all-fiber Er-doped chirped-pulse amplification laser, which generates Watt-level broadband pulse with the application of self-similar amplification. Numerical simulations of the model laser were performed by following the propagation of the pulses and considering every action of cavity components on the pulses. We use the results of one round-trip circulation as the input of the next round of calculation until the optical field becomes self-consistent. For this context, pulse propagation equation is given by the nonlinear Schrodinger equation. The parameters of each element of the laser are optimized according to theoretical simulations. In our experiment, the seed source is a dispersion-managed passively mode-locked fiber laser with a Gaussian-spectral profile, which evolves into a parabolic shape after self-similar amplification, achieving a broadband pulse bandwidth with the full-width at a half-maximum of 44.8 nm under 400 mW pump power. The spectral width and energy of the pulse increase rapidly during amplification. The pulses are stretched in Dispersion Compensating Fiber (DCF) to reduce peak power, avoiding excessive nonlinearity. Then a Double-Clad Er/Yb co-Doped Fiber (DC-EYDF) is used as the main amplifier. The spectral width of the pulse is narrowed down to 30 nm with the effect of gain filtering during amplification. The pulse is amplified to 1.3 W with the pump power of 9 W. The amplifier delivers 32 nJ pulses at a repetition rate of 40.1 MHz, which can be compressed down to 587 fs through a pair of transmission gratings. We believe that the narrower pulses could be achieved by switching to fiber Bragg gratings to adjust the dispersion between the stretchers and compressors precisely. The robust, broadband, and watt-level 1 550 nm fiber laser source can be used for nonlinear frequency conversion, solar cell micromachining and ophthalmology due to its compact size. ? 2022 Chinese Optical Society. All rights reserved.
    Accession Number: 20224513074550
  • Record 54 of

    Title:Enhancement of Fiber-to-Waveguide Coupling Efficiency of Silicon Nitride Integrated Optical Circuits
    Author(s):Zhu, Xiaotian(1); Li, Guangkuo(1); Li, Yuhua(4); Wang, Xiang(2); Davidson, Roy(2); Little, Brent E.(2,3); Chu, Sai T.(1)
    Source: 2022 Conference on Lasers and Electro-Optics Pacific Rim, CLEO-PR 2022 - Proceedings  Volume:   Issue:   DOI: 10.1109/CLEO-PR62338.2022.10432431  Published: 2022  
    Abstract:A hybrid approach for the enhancement of the fiber-to-silicon nitride waveguide coupling efficiency is proposed. It shows the coupling efficiency of lower than 0.7 dB/facet across the C band can be achieved. ? 2022 IEEE.
    Accession Number: 20241115716953
  • Record 55 of

    Title:The complex Maxwell stress tensor theorem: The imaginary stress tensor and the reactive strength of orbital momentum. A novel scenery underlying electromagnetic optical forces
    Author(s):Nieto-Vesperinas, Manuel(1); Xu, Xiaohao(2,3)
    Source: Light: Science and Applications  Volume: 11  Issue: 1  DOI: 10.1038/s41377-022-00979-2  Published: December 2022  
    Abstract:We uncover the existence of a universal phenomenon concerning the electromagnetic optical force exerted by light or other electromagnetic waves on a distribution of charges and currents in general, and of particles in particular. This conveys the appearence of underlying reactive quantities that hinder radiation pressure and currently observed time-averaged forces. This constitutes a novel paradigm of the mechanical efficiency of light on matter, and completes the landscape of the optical, and generally electromagnetic, force in photonics and classical electrodynamics; widening our understanding in the design of both illumination and particles in optical manipulation without the need of increasing the illuminating power, and thus lowering dissipation and heating. We show that this may be accomplished through the minimization of what we establish as the reactive strength of orbital (or canonical) momentum, which plays against the optical force a role analogous to that of the reactive power versus the radiation efficiency of an antenna. This long time overlooked quantity, important for current progress of optical manipulation, and that stems from the complex Maxwell theorem of conservation of complex momentum that we put forward, as well as its alternating flow associated to the imaginary part of the complex Maxwell stress tensor, conform the imaginary Lorentz force that we introduce in this work, and that like the reactive strength of orbital momentum, is antagonistic to the well-known time-averaged force; thus making this reactive Lorentz force indirectly observable near wavelengths at which the time-averaged force is lowered. The Minkowski and Abraham momenta are also addressed. ? 2022, The Author(s).
    Accession Number: 20224212968254
  • Record 56 of

    Title:An Optimization Algorithm for Optical Gain in the Multi-EDFAs-based Fiber-optic Time Synchronization
    Author(s):Liu, Bo(1,2); Kong, Weicheng(3,4); Guo, Xinxing(3,4); Li, Bo(3,4); Zhang, Shougang(3,4); Dong, Ruifang(3,4); Liu, Tao(3,4)
    Source: 2022 Joint Conference of the European Frequency and Time Forum and IEEE International Frequency Control Symposium, EFTF/IFCS 2022 - Proceedings  Volume:   Issue:   DOI: 10.1109/EFTF/IFCS54560.2022.9850958  Published: 2022  
    Abstract:This article reports an optimization model of optical fiber time synchronization EDFA gain coefficient based on genetic algorithm (G A). According to a series of parameters such as the distance and attenuation of each section of optical fiber, the EDFA gain coefficient of each node is obtained for the purpose of maximizing the signal-to-noise ratio, SNR. This algorithm is further exploited for regulating the gains of bidirectional amplifiers, allowing optimization of the performance of the link. The developed algorithm was tested experimentally done with 210-and 300-km-long links in the laboratory, incorporating three and four amplifiers. The results suggest that, comparing with the fixed gain coefficient setting, the proposed solutions allow optimizing the SNR by 3-5 dB and reduce the phase jitter by about 20%. ? 2022 IEEE.
    Accession Number: 20223712712947
  • Record 57 of

    Title:The route to a 200 MHz, all-PM femtosecond Yb-doped fiber laser with a high output coupling ratio
    Author(s):Zhang, Zhao(1,2); Zhang, Tong(1,2); Lv, Zhiguo(3); Zhang, Ting(1,2); Cheng, Haihao(1,2); Hu, Xiaohong(1); Pan, Ran(1); Feng, Ye(1); Wang, Yishan(1)
    Source: Applied Optics  Volume: 61  Issue: 28  DOI: 10.1364/AO.472038  Published: October 1, 2022  
    Abstract:Based on the time-independent rate equations and nonlinear Schr?dinger equation, we simulate a 200 MHz all-polarization-maintaining (PM) mode-locked Yb-doped fiber laser. The cavity round trip evolution toward stable mode locking is present. Additionally, the gain coefficients along the gain fiber as well as the pulses, chirp, and spectra at different locations in the cavity are examined. The effects of chirped fiber Bragg grating parameters on the pulse shape and spectrum profile are also investigated. According to the calculations, we experimentally realize a 200 MHz femtosecond fiber laser with 115 mW output power. The timing jitter and integrated relative intensity noise are measured as 158 fs (1 kHz to 10 MHz) and 0.0513% (1 Hz to 300 kHz), respectively. Eventually, an amplified average power of 610 mW and 79 fs compressed pulses with a peak power of approximately 28 kW are obtained. The exhibited all-PM femtosecond fiber laser system can be adopted as the foundation for an optical frequency comb. ? 2022 Optica Publishing Group.
    Accession Number: 20224212986017
  • Record 58 of

    Title:Eagle-Eye-Inspired Attention for Object Detection in Remote Sensing
    Author(s):Liu, Kang(1,2); Huang, Ju(1,2,3); Li, Xuelong(1,2)
    Source: Remote Sensing  Volume: 14  Issue: 7  DOI: 10.3390/rs14071743  Published: April-1 2022  
    Abstract:Object detection possesses extremely significant applications in the field of optical remote sensing images. A great many works have achieved remarkable results in this task. However, some common problems, such as scale, illumination, and image quality, are still unresolved. Inspired by the mechanism of cascade attention eagle-eye fovea, we propose a new attention mechanism network named the eagle-eye fovea network (EFNet) which contains two foveae for remote sensing object detection. The EFNet consists of two eagle-eye fovea modules: front central fovea (FCF) and rear central fovea (RCF). The FCF is mainly used to learn the candidate object knowledge based on the channel attention and the spatial attention, while the RCF mainly aims to predict the refined objects with two subnetworks without anchors. Three remote sensing object-detection datasets, namely DIOR, HRRSD, and AIBD, are utilized in the comparative experiments. The best results of the proposed EFNet are obtained on the HRRSD with a 0.622 AP score and a 0.907 AP50 score. The experimental results demonstrate the effectiveness of the proposed EFNet for both multi-category datasets and single category datasets. ? 2022 by the authors. Licensee MDPI, Basel, Switzerland.
    Accession Number: 20221712029080
  • Record 59 of

    Title:Staging of Skin Cancer Based on Hyperspectral Microscopic Imaging and Machine Learning
    Author(s):Liu, Lixin(1,2); Qi, Meijie(1,2); Li, Yanru(1); Liu, Yujie(1); Liu, Xing(3); Zhang, Zhoufeng(2); Qu, Junle(4)
    Source: Biosensors  Volume: 12  Issue: 10  DOI: 10.3390/bios12100790  Published: October 2022  
    Abstract:Skin cancer, a common type of cancer, is generally divided into basal cell carcinoma (BCC), squamous cell carcinoma (SCC) and malignant melanoma (MM). The incidence of skin cancer has continued to increase worldwide in recent years. Early detection can greatly reduce its morbidity and mortality. Hyperspectral microscopic imaging (HMI) technology can be used as a powerful tool for skin cancer diagnosis by reflecting the changes in the physical structure and microenvironment of the sample through the differences in the HMI data cube. Based on spectral data, this work studied the staging identification of SCC and the influence of the selected region of interest (ROI) on the staging results. In the SCC staging identification process, the optimal result corresponded to the standard normal variate transformation (SNV) for spectra preprocessing, the partial least squares (PLS) for dimensionality reduction, the hold-out method for dataset partition and the random forest (RF) model for staging identification, with the highest staging accuracy of 0.952 ± 0.014, and a kappa value of 0.928 ± 0.022. By comparing the staging results based on spectral characteristics from the nuclear compartments and peripheral regions, the spectral data of the nuclear compartments were found to contribute more to the accurate staging of SCC. ? 2022 by the authors.
    Accession Number: 20231213758750
  • Record 60 of

    Title:Large aperture phase-coded diffractive lens for achromatic and 16° field-of-view imaging with high efficiency
    Author(s):Ma, Gu(1,2); Zheng, Peng-Lei(1,2); Hu, Zheng-Wen(1,2); Ma, Suo-Dong(1,2,3); Xu, Feng(1,2); Pu, Dong-Lin(1,2); Wang, Qin-Hua(1,2)
    Source: Chinese Physics B  Volume: 31  Issue: 7  DOI: 10.1088/1674-1056/ac560c  Published: July 1, 2022  
    Abstract:Diffractive lenses (DLs) can realize high-resolution imaging with light weight and compact size. Conventional DLs suffer large chromatic and off-axis aberrations, which significantly limits their practical applications. Although many achromatic methods have been proposed, most of them are used for designing small aperture DLs, which have low diffraction efficiencies. In the designing of diffractive achromatic lenses, increasing the aperture and improving the diffraction efficiency have become two of the most important design issues. Here, a novel phase-coded diffractive lens (PCDL) for achromatic imaging with a large aperture and high efficiency is proposed and demonstrated experimentally, and it also possesses wide field-of-view (FOV) imaging at the same time. The phase distribution of the conventional phase-type diffractive lens (DL) is coded with a cubic function to expand both the working bandwidth and the FOV of conventional DL. The proposed phase-type DL is fabricated by using the laser direct writing of grey-scale patterns for a PCDL of a diameter of 10 mm, a focal length of 100 mm, and a cubic phase coding parameter of 30π. Experimental results show that the working bandwidth and the FOV of the PCDL respectively reach 50 nm and 16° with over 8% focusing efficiency, which are in significant contrast to the counterparts of conventional DL and in good agreement with the theoretical predictions. This work provides a novel way for implementing the achromatic, wide FOV, and high-efficiency imaging with large aperture DL. ? 2022 Chinese Physical Society and IOP Publishing Ltd.
    Accession Number: 20223012413010
精品一区二区在线播放| 久久久国产精品一区二区白洁老师| 亚洲国产区| 亚洲中文字幕在线观看| 国产AV无码电影| 欧美精品一卡二卡| 国产AV视屏| 亚洲综合一区二区| 欧美另类交在线观看| 婷婷超碰| 久久性爱视频| 日本不卡视频| 蜜乳av一区二区| 性色一区| 国产精品一区二区三区久久| 人人干人人爽| 乱色熟女综合一区二区三区四 | 中国少妇XXXX| 一级内射片在线网站观看| 一区二区三区在线| 性免费| 亚洲国产二区| 亚洲无码一区在线| 国产色图乱伦| 久久久久99| 国产永久精品| 欧美三级片在线| 午夜福利视频免费看| 日韩一级电影在线观看| 天天精品| 免费黄色在线视频| 操逼.com| 欧美精品一区二区三区| 久久久网| 性爱导航综合| 亚洲乱伦网| 久久久91人妻无码精品蜜桃观看| 亚洲自拍偷拍视频| 欧美日韩精品一区二区三区四区| 黑人AV无码| 欧美第二页| 欧美肏屄视频| 久久精品一区二区三区四区| 91精品中文字幕| 免费无高潮片60分钟观看| 亚洲狼人| 97国产| 国产情侣小视频| 日本三日本三级少妇三级66| 在线国v免费看| 精品人妻熟女一区二区三区免费看 | 91精品免费视频| 成人高清无码| 欧美不卡视频| 无码不卡在线| 国产AV不卡一区二区| 91人妻人人操| 天天草视频| 91综合福利导航| 国产学生妹在线观看| 一级毛片在线| 国产乱码精品一区二区三区中文 | 色综合精品| 夜夜久久| 日韩无码精品电影| 国产伦精品一区二区三区视频新| 五月婷婷色色午夜| 久久伊人精品视频| 午夜国产精品视频| 精品视频在线观看99| 日本欧美一区二区| 国产欧美又粗又猛又爽| 亚洲Av无码一区二区三区在线播放| 天天日天天插| 国产激情综合| 欧美小视频在线观看| 毛片一区二区| 午夜精品福利在线观看| www.人妻| 免费国产网站| 国产日本欧美一区二区| 国产成人精品AA毛片| 人妻互换一二三区免费| 国产欧美精品一区二区三区色大师| 欧美一级黄片免费观看 | 婷婷综合色| av色综合| 免费观看av网站| 玖草在线| 人人爱人人插| 久久久久久久久久久高清毛片一级| 国产毛片在线看| 深夜成人视频在线| 亚洲日韩激情无码| 久久婷婷国产综合精品简爱Av| 日韩免费操逼视频| 中文欧美日韩| 黄色av网站在线免费观看| 中国免费一级片| 国产精品久久久久永久免费观看| 国产电影一区二区三曲| 久久久久久人妻精品一区二百内谢| 特级全黄一级毛片| 图片区偷拍区小说区| 一级大片网站| 一道本在线视频| 精品人妻一区| 天天干,夜夜操| 三上悠亚中文字幕| 人妻精品| 高清无码一区二区三区| 色色视频区| 日韩免费看| 熟妇高潮一区二区在线播放| 国产激情一级毛片久久久| 岛国大片在线一区二区三区在线免费观看| 天堂中文在线视频| 99热这里有精品| 天天躁日日摸久久久精品| www.午夜| 99久久这里只有精品| 欧美精品久久久| 成人性爱视频免费观看| 日韩一级黄色| 亚洲精品区一区二区三区四区五区高 | 欧洲操逼视频| 精东粉嫩av免费一区二区三区| 啪啪免费网站| 欧美成人社区| 免费在线看黄网站| 欧美精品四区| 超碰导航| 国产福利小视频在线观看| 日本久久三级片| 亚洲成人毛片| 亚洲91色图| 国产三级片在线看| 欧美区日韩区| 屁屁影院第一页| 日本欧美一区二区三区| 色婷婷精品| 欧美大黄| 国产麻豆一区二区三区| 国产成人精品自拍| 日韩欧美中文| 亚洲五码在线| 蜜桃AV丝袜一区二区三区| 婷婷国产精品| 91精品视频网| 亚洲Av无码午夜国产精品色软件| 日韩无码| 女人高潮抽搐喷液30分钟视频 | 91精品久久人妻一区二区夜夜夜| 日本少妇一级片| 奇米狠狠| 91精品久久久久久粉嫩| 欧美精品一区二区在线| 日本久久久久| 碰碰人人| 中文字幕精品一区二区三区精品| 亚洲一区免费| 国产视频精品一区二区三区| 青娱乐91| 丰满熟妇大号BBWBBWBBW| 久久成人毛片| 免费看黄网址| 五月天青青草| 中文人妻| 免费看黄色大片| 99在线视频精品| 欧美怡春院| 免费午夜视频| 老熟妇午夜毛片一区二区三区| 黄色三级片在线观看| 噜噜噜久久久| 亚洲无码TV| 青青草视频在线观看| 日韩精品1| 午夜无码视频| AV无码一区二区三区| 超碰免费人妻| 一级肉体AAAA片免费看| 三级中文字幕| 亚洲熟人妇一区二区三区| 伊人色综合久久久天天蜜桃| 黄色AV免费看| 亚洲av免费在线| 天天操天天日天天射| 色爱a∨综合区| 欧洲-级毛片内射| 操逼无码视频13p| 欧美视频精品| aaa无码| 道日本一本草久| 人妻毛片| 麻豆精品无码国产在线| 久久成人网站| 毛片免费播放| 国产精品视频免费观看| 国产一区精品在线| 日本一二三区欧美色欲| a片在线播放| 九色人妻| 午夜男人天堂| 中文字幕一区二区人妻电影| 亚洲精品一区三区三区在线观看 | 91九色视频在线| 国产香蕉视频在线观看| 午夜精品福利在线观看| 亚洲AV无码久久久久精品同性| 岛国无码在线| 国产精品久久欧美久久一区| 欧美一级大黄片| 亚洲视频入口| 日本三级久久| 热99热| 人人摸人人上人人| 国产思思久久| 啪免费视频久久| 99热精品免费| 91免费看片| 奇米影视第四色777| 久久五月婷| 国产亚洲AV| 一级做a爰片久久毛片无码电影| av一级毛片| 久久大香蕉| 国产一级特黄大片视频播放| MM1313又粗又大受不了| 少妇被躁爽到高潮无码文| 男女无遮挡网站| 亚洲精品欧美日韩| 波多野吉衣一区二区| 99热在线播放| 天天干天天狠| 国产做a爱一级毛片| 最好看的2018中文2019| 国产精品久久久久永久免费看| 日韩福利视频| 美女裸体无遮挡免费网站| 欧美乱妇狂野欧美在线视频| 人妻无码专区| 一级特黄60分钟免费看| 肉肉AV福利一精品导航| 人妻体内射精一区二区| BAOYU| 秋霞AV国产精品一区| 性久久久久久久久久久久久久| 乱伦熟女肉妇| 99大香蕉| 亚洲国产精品无码久久久| 一级性爱毛片| 麻豆精品视频| 91av在线免费观看| 日韩精品久久久| 国产毛片毛片精品天天看软件| 18禁无遮挡网站| 麻豆精品一区二区三区| 亚洲精品免费视频| 国产激情在线| 久久性爱免费的| 亚洲天堂无码| 99人妻碰碰碰久久久久禁片| 91精品91久久久中77777| 在线视频午夜| 中文无码在线| 加勒比一区| 成人免费性爱视频| 伊人色吧| 久久官网| 在线观看日韩AV| 91囯在线啪无码| 日韩欧美在线一区| 欧美午夜理伦三级在线观看| 国产成人91亚洲精品无码观看| 国产九九九九| 91无码| 久久亚洲AV日韩AV无码A| 99精品免费观看| 中文字幕婷婷| 99久久久国产精品无码免费 | 中文字幕日韩三级片| 91亚洲国产成人久久精品网站| 禁果AV一区二区夜夜嗨| 国产黄片在线视频| 日本精品久久| 免费无码国产精品一区二区| 国产无码精品在线| 精品婷婷| 四虎久久| 日韩精品影院| 九色影院| 亚洲AV无码久久久久精品同性| 国产一级av在线| 国产流白浆| 日本一级A片| 亚洲色无A片一区二区夜夜嗨| 特级无码| 丁香五月天在线观看| AV在线免费播放| 日韩无码影院| 久草福利在线视频| 人妻中文无码| 免费观看操逼| 亚洲理伦| 波多野结衣网址| 国产一区高清无码| 亚洲免费精品| 国产午夜片| 欧美特黄一级| 污视频在线| 无码专区AV| 国产乱人伦| 国产精品三级| 97碰碰碰| 国产一级自拍| 亚洲国产精品无码久久久久久久久| 一级操逼毛片| 国产无码电影| 亚洲少妇无套内射激情视频| 欧美精品第一区| 亚洲无码精选| 变态另类zoz0另类| 亚洲一区中文字幕| 无码aⅴ一区二区三区门票价格表| 黄色三级片视频| 黄色网在线播放| 国产成人久久| 亚洲欧洲在线观看| 国产三级在线观看视频| 欧美亚洲中文字幕| 毛茸茸性XXXX毛茸茸| 国产精品igao视频网网址| 91导航中文字幕| 午夜成人免费视频| 国产午夜片| 被体育老师抱着c到高潮| 色欲影视综合网| 欧美日韩精品国产| 乱伦熟妇| 欧美老少交| 久久蜜桃AV一区二区天堂| 国产精品伦子伦免费视频| 在线观看第一页| 亚洲av无码一区二区三| 国产精品一区在线| 免费观看黄色大片| 欧美精品videossexohd| 在线观看亚洲AV| 欧美高清a| 91九色国产| 国色天香一区二区| 日韩Av免费| 国产免费一区二区三区在线观看| 欧美黄片儿| 国产伦精品一区二区三区免费迷奷| 国产三级在线观看| 国产一级a毛一级a| 婷婷综合五月天| 少妇放荡的呻吟干柴烈火| 亚洲二区在线| 日韩A级片| 天天综合网在线观看| 开心激情综合| 国内精品国产三级国产在线专 | 欧美香蕉视频| 女性一级裸体片| 一级α片免费看刺激高潮视频| 乱伦天堂| 搡老女人老91妇女老熟女| 人人操人人干人人操| 99久久国产视频| 精品国产日韩亚洲| 看操逼的视频| 国产黄色录像| 国模私拍| 真人视频直播app免费观看| 线观看免费完整aaa| 99热在线观看| 91在线视频| 91在线视频免费的| 黄片在线免费观看视频| 亚洲AV无码乱码国产精品牛牛| 美女黄片免费看| 精品国产99久久久久久影视吊车| 91色逼资源| 拳交美女A片大全| 在线中文无码| 国产乱国产乱300精品| 天天干夜夜欢| 无套内谢少妇高潮免费| 秋霞影院午夜丰满少妇在线视频| 亚洲性天堂| 一级毛片视频免费看| 精品国产亚洲AV| av免费网址| 国产三级网站| 在线视频午夜| 91丨九色丨国产熟女软件| 成年人在线观看| 成人在线视频app| 国产网曝门事件福利视频| 影音先锋中文字幕资源6| 四虎精品视频| 亚洲视频www| 欧美中文在线观看| 中国黄片免费看| 天天操操| 日韩AV在线免费| 日本伊人网| 精品福利在线| 高清无码视频在线看| 8090.aa| 亚洲喷水无码一区丰满爆乳少妇| 电家庭影院午夜| 91aaa| 国产麻豆视频| 精品视频一区二区| 99视频精品全部在线观看下载| 人体人人摸人人插| 欧洲AV一区二区三区| 欧美日韩视频一区二区| 无码高清一区| 亚洲无码视频在线观看| 91AV亚洲| 黄片在线免费视频| 精品69| 成人伊人| 香蕉福利视频| 日本东京热视频| 国产成人无码www免费视频播放| 天天干天天干天天干| 日韩欧美中文| 鲁鲁狠狠狠7777一区二区| 日韩欧美在线一区| 人人看人人干| 欧美性受XXXX黑人XYX性爽| 久久久久久久久久久高清熟女av粉嫩AV| 欧美天堂在线观看| av无码天堂| 欧洲精品无码一区二区三区在线| 久久久久久国产精品三区| 日韩精品欧美精品| 免费观看又色又爽又黄的忠诚| 国产精品女| 亚洲无码专区在线观看| 欧洲-级毛片内射| 看免费毛片| 日韩中文字幕人妻在线| 国产精品一区二区三区免费| 欧美日韩一| 密乳av免费在线| 熟女少妇内射日韩亚洲| 国产日韩成人| 国产精品国产三级国产专播品爱网| 欧–美–性–交–黄–片| 99人妻碰碰碰久久久久禁片| 无码国产精品一区| 99久久精品国产一区二区三区| 色爱a∨综合区| 999久久久| 久久无码一区| 久久久久久久久久一级| 成 人 黄 色 免费 观 看| 亚洲精品无码AV中文永久在线 | 国产黄片在线免费看| 成人黄色一级片| 精品2022露脸国产偷人在视频| 人人搞人人干| 无码精品一区二区三区潘金莲| 国产激情91| 无码中文字幕| 日本www色视频| 精品国产在热久久婷婷人妻AV综| 国产伦精品一区二区三区四区免费| 国产精品亚洲一区| 中文字幕人妻视频| 国产伦精品| 亚洲精品视频在线播放| 久久久三级片| 色视频在线观看| 成人伊人| 久久九九视频| 日韩无码一区二区三区| 国产精品久久久久久久久久10秀| 不卡无码AV| 看片网址国产福利av中文字幕| 日韩欧美亚洲国产精品字幕久久久| WWW插插插无码视频网站 | 91视频色| 亚洲一区二区三区四区| 亚洲精品久久久久玩吗| 天天爽夜夜爽| 少妇高潮喷水惨叫久无码一区二区| 国产三级国产精品国产专区50| 精品少妇人妻av无码中文字幕| 91麻豆精品秘密入口| 精品导航| 亚洲乱伦图片| 国产精品毛片一区二区| 在线中文AV| 九九热视频在线| 国产超碰人人| 国产99自拍| 欧美视频第一页| 无码成人精品区一级毛片| 日本精品无码aⅴ片视频| 五十路熟女乱伦| 日韩在线视频免费| 午夜一级黄色片| 午夜在线影院| 午夜福利视频| 黄色网页免费| 日韩操逼逼| 日韩人妻视频| 99re在线观看| 爆乳一区二区| 探花日韩无码| 国产刺激对白| 免费看黄色大片| poronodrome极品另类| 亚洲色无A片一区二区夜夜嗨| 一区二区三区亚洲| 亚洲AV无码乱码精品护士岛国| 91九色在线| 91精品国产综合久久香蕉922| 国产免费A∨片在线观看不卡| 精品第一页| 日本熟女一区二区| 强奸乱伦亚洲无码第一页| 一本无码视频| 国产成人91亚洲精品无码观看| 少妇人妻偷人精品无码视频新浪| 久久黄色三级片| 逼操逼操逼操逼操| 国产3p露脸普通话对白| 91丝袜一区二区| 中文字幕在线一区| 国产偷自拍| 色九九九| 成人精品一区| 国产欧美日| 久草青青视频| 欧美日韩操逼| 欧美日韩高清丝袜| 欧美久久免费| 亚洲欧美在线视频| 亚洲无码视频专区| 亚洲精品一区二区三区中文字幕| 亚洲AV无码成人精品区国产| 一级片在线播放| 国产熟女自拍| 日本一级A片| 亚洲人妻中文字幕| 国产人妻人伦精品1国产盗摄| 加勒比一区| 一区二区视频在线| 亚洲一区亚洲二区| 三级片无码| 亚洲午夜福利| 一区二区三区免费| 91福利网| 黄片AV在线| 熟女一区| 亚洲熟妇AV乱码在线观看| 人人草人人摸| 亚洲A√| 国产福利一区二区| 精品av| 3d动漫精品一区二区三区| 国产精品久久久久久电影| 91精品啪在线观看国产| 免费无码国产免费| 亚洲欧洲一区| 亲嘴视频| 色婷婷精品| 国产熟女乱伦文学| 人妻少妇一区二区| 国产一级性爱| 久久精品国产精品| 在线无码视频| 亚洲一级特黄大片| 国产精品亚洲一区二区三区在线| 亚洲午夜av一二三区熟女| 高清无码91| 99久久国产| 久久99国产精品| 最新亚洲中文字幕| 红桃AV| 一级黄片免费| 18无码国产在线看不卡动漫| 蜜臀导航| 影音先锋一区| 日韩高清一区| 久久午夜影院| 国产高清精品无码| 精品无码成人| 91精彩刺激对白露脸偷拍| 草草视频在线观看| 亚洲中文在线观看| 久久精品香蕉| 二区三区无码| 久久av一区二区三区| 91视频官网| 免费AV在线网址| 嫩呦国产一区二区三区AV| 五月婷婷在线观看视频| 熟女91| 精品无码黑人又粗又大又长| 国产夫妻av| 国产免费一区二区三区在线观看| 一区二区三区影院| 疯狂的交换1—6真实交换3和2| 久久精品成人| 日日碰碰| 国产无码AV| 国产精品三级在线| 加勒比一区| 国产中文字幕一区| 91久久人人操人人爱人人摸| 99er在线| 国产免费一区二区三区| 秋霞午夜一区二区三区视频| 毛片无码免费| 国产熟女AV| 欧美操逼网址| 黄色小视频网站在线观看| 欧美人与物videos另类| 男女无套 在线观看网站| 成人在线小视频| 理论片琪琪午夜电影| 日逼视频xxxxxXxXX| 久久人妻少妇嫩草AV无码专区| 丝袜乱伦视频| 国产手机在线视频| 亚洲一区二区久久| 末成年女AV片一区二区三区| 久操国产视频| 三年片在线观看大全中国| 高清国产一区二区三区四区五区| 国产无码免费| 精品视频导航| 熟妇人妻一区二区三区四区| 国产黄色影院| 99亚洲无码| 亚洲午夜精品一区二区三区电影院| 午夜成人毛片| 91麻豆精品秘密入口| 新疆啪啪啪啪视频| 亚洲精品www| 蜜乳av不忘| aaa无码| 国产一区福利| 99热精品在线观看| 一区二区三区三级片| 久久久精品国产sm调教网站| 日韩无套| 国产成人精品在线| 久久99精品久久久水蜜桃| 中文字幕精品一区二区三区精品 | 老女人性生交大片免费| 人妻互换一二三区激情视频| 日韩成人中文字幕| 人人狠狠| 精品国产Av无码久久久影音先锋| 一插菊花综合网| 色婷婷九月天天综合| 久久亚洲无码| 色噜噜综合网| 亚洲国产毛片| 后入内射欧美99二区视频| 国产精品无码一区二区桃花视频| 97久久精品| 色综合天天综合网天天看片 | AV一区二区三区在线| 色色91| 1769视频精品| 亚洲AV无码久久久久网站飞鱼| 欧美久操| 真实的和子乱拍视频| 色哟哟av| 久久九九精品视频| 一级毛片久久久久久久女人18| 7777精品久久久久久| 一区高清无码| 欧美日韩中文字幕| 亚洲黄色网址| 欧美一级性爱视频| 91在线成人| 国产91丝袜在线播放九色| 日日操日日爽| 欧洲亚洲一区二区三区四区五区| 中日无码| 狠狠干网址| 麻豆乱伦AV| 精品中文字幕| 欧美不卡在线| 亚洲国产91| 激情内射亚洲一区二区三区爱妻| 中文字幕天堂网| 自拍偷拍第一页| 国产一区二区不卡| 亚洲性爱av免费观看| 国产精品久久久久久电影| 日本一区二区不卡| 伊人网综合| 九色在线视频| 理论片琪琪午夜电影 | 看一区二区三区性爱精品| 午夜精品视频在线观看| 亚洲永久无码7777kkkk| 91丝袜视频| 欧美久久一区二区| 久久另类TS人妖一区二区| 亚洲欧洲一区| 欧美色逼| 91性视频| 无码视频免费观看| 伊人三级| 男女猛烈无遮挡| 国产精品无码午夜福利免费看 | 精品无码国产一区二区三区高跟 | 黄色A级大片| 玖玖在线| 无码入口| 无码三级片视频| 欧洲亚洲AV无码国产精品成人 | 免费精品人在线二线三线区别| 色婷婷精品久久二区二区蜜臂av| 亚洲国产区| 日本福利视频| 精品人妻码一区二区三区红楼视频 | 波多野结衣中文字幕一区二区三区| 欧美边做饭边被躁BD在线看| 啪啪一区二区| 国产a一区| 亚洲w欧洲无码sss222| 欧美亚洲一区二区三区| 中文字幕乱妇无码Av在线| 人妻少妇精品| 国产成人毛片| 人妻少妇视频| 黄色网页在线观看| 人妻少妇精品| 日本熟妇乱伦| 日韩无码电影| 热re99久久精品国产99热| 99无码视频| 91九色国产| 日韩激情无码| 精品视频在线播放| 一区二区无码在线观看| 国产一国产一级毛片视瓶| 久久国产一区二区| 熟女乱伦视频| 久久这里都是精品| 久久精品午夜| 欧美视频| 岛国网站在线观看| 无码白丝强行免费| 啪啪啪精品| 国产一区二区不卡| 91麻豆精品秘密入口| 无码中文av| 久久久国产精品视频| 99久久99久久精品国产片果冰| 成人深夜福利| 一区在线看| 天天做夜夜爱| 成人精品在线播放| 老熟妻内射精品一区| 国产原创精品| 人妻毛片A一级毛片免费看| 成人午夜福利视频| 欧美精品在线视频| 欧美熟妇色| 日韩天天搞| 亚洲免费黄色网址| 国产精品一区二区三区免费观看| 一区二区在线观看视频| 成人乱人伦一区二区三区| 亚洲w欧洲无码sss222| 国产av日韩一区二区三区精品| 最近中文字幕在线观看视频| 五月婷婷av| 亚洲va韩国va欧美va精品| 色播AV| 免费黄网站| 国产无套内精一级毛片| 亚洲精品无码AAA在线播放| 国内精品一区二区三区| 免费看一级高潮毛片2023| 中文字幕专区| 99久99| 国产欧美日韩在线| 黄页网站视频| 欧洲另类类一二三四区| 久久精品国产亚| 天天干天天狠| 91久久久久久久| 人妻99| 国产欧美在线播放| 黄色片网站在线观看| 久久久久久人妻| 国产黄色成人网站| 999久久久免费精品国产| 亚洲1区2区| 免费观看黄| 午夜成人网址| 国产视频久久久| 蜜乳在线| 一区二区三区中文字幕| 亚洲视屏| 91人人操人人摸| 婷婷五月天综合| 国产精品久久久久久久久久久久久四虎| 国产精品系列视频| 性爱国产| 亚洲精品第一页| 国产精品无码在线播放 | 激情图片激情小说| 免费观看国产精品| 国产精品成人亚洲一区二区| 亚洲精品国产无码| 精品乱伦3p| 精品久久一区二区三区| 国产熟女网站| 久久综合伊人| 97超碰免费在线观看| 91五月天| 国产精品天天狠天天看| 91免费在线看| 国产三级午夜理伦三级| 国产精品婷婷| 免费三级片网址| 久久久久久亚洲AV无码| 草草网站| 日韩av毛片| 青青草视频在线免费观看| 门卫老董| 久久婷婷五月天| 日韩黄色精品| 日本免费在线| 无码精品久久久久久亚洲| 成年免费视频黄网站在线观看| 91精品91久久久中77777| 少妇又紧又深又湿又爽视频| 亚洲免费av网| 中文字幕在线观看一区二区三区| 国产69精品久久久久孕妇大杂乱| 老外和中国女人毛片免费视频| 欧洲精品无码一区二区三区在线| 天天综合永久| 久久久黄色网| 国产欧美一区二区三区在线| 国产一区不卡在线| 毛片免费播放| 久久99电影| 亚洲精品无| 中文字幕乱码亚洲精品一区| 3d动漫精品一区二区三区| 中文字幕一区二区三区日韩精品| 亚洲精品午夜福利| 中文有码| 久久国产露脸精品国产| 超碰亚洲| 免费精品一区二区三区视频日产| www.人妻| 一级做a爱全过程| 午夜成人网址| 中国少妇XXXX| 久久精品一区二区三区免费播放| 毛色毛片免费看| 欧美亚洲一区二区三区| 中文字幕一区二区人妻电影| 欧美午夜在线视频| 久久国产精品一区| 国产一区二区在线免费观看| 91午夜福利视频| 日本综合久久| 国产女人水真多18毛片18精品视频| 欧美性爱一级免费| Av天天有| 亚洲男人天堂| 91国自产精品中文字幕亚洲 | 黑人巨大精品欧美一区二区免费 | 亚洲AV无码成人精品区明星蜜乳| 国产精品久久久久久免费播放| 国产精品久久久久久久下载地址| 亚洲色一色| 色综合网色综合| 无码精品人妻一区二区三区综合部| 国产又爽又黄无码无遮挡在线观看| 欧洲高清转码区一二区| 国产精品久久精品| 91精品视频在线| 国产精品资源| 毛片毛片毛片毛片| 精品无码国产AV一区二区三区| A片软件| 国产粉嫩| 69堂在线| 91精品在线看| 中文字幕少妇交换乱吟HD免费看 | 国产精品色视频| 国产精品久久久久久亚洲调教| 午夜高清无码| 黄色国产视频| 露脸丨91丨九色露脸| 亚洲熟女乱伦| 无码电影院| 亚洲精品国产一区二区三区三州4点 | 日韩在线精品视频| av免费在线观看网站| 国产精品日韩精品| 久久九九免费观看网站| 中文字幕在线观看av| 一级av在线| 日韩无码不卡| 国产一区二区成人久久919色 | 国产三级片一区二区| 日韩一区在线播放| 九九精品在线| 精品www| 九色在线| 精品福利导航| 久久99精品久久久久久清纯直播| 欧美一区二区三区在线视频|