青青青爽在线视频免费观看-在线国产日韩欧美播放精华一-日韩综合第二区2区3一区-亚洲av永久无码精品欣赏-成人精品午夜在线观看-婷婷五月深深久久精品-久青草国产高清在线视频-国产成人免费片在线观看 亚洲欧美动漫中文字幕-国产视频精品久久久久不卡-久久?v不卡人妻一区二区-中文字AV字幕在线观看-久久99中文字幕久久-亚洲欧美综合图片-国产精品视频福利-国产亚洲欧美人伦

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
久久精品—区二区三区舞蹈 | 午夜无码免费视频| 成人综合网站| 91人人爽人人爽人人精88V| 一级a毛片免费观看久久精品| 免费国产精品视频| 99视频99| 国产精品操逼视频| 99自拍视频| 99视频在线看| 天天做天天爱天天爽综合网| 亚洲视频中文字幕| 人妻精品| 清纯唯美亚洲经典中文字幕| 九九超碰| 免费看一级一级人妻片| 亚洲性爱无码| 亚洲天堂视频在线观看| 91蜜桃婷婷狠狠久久综合9色| 天天综合久久综合| 国产性―交―乱―色―情人| 98年欧美综合性爱| 成人免费毛片足控| 黄色一级视频免费观看| 欧美bbbwbbwbbwbbw| 婷婷在线视频| 熟女天堂| 中文熟妇人妻又伦精品| 久久国产一区二区三区高清视频| 国产伦对白刺激精彩露脸| 青青草97国产精品免费观看| 成人7777| 国产午夜伦鲁鲁| 人人摸人人摸| 丰满人妻一区二区三区免费视频棣| 国产九色| 亚洲一区二区三区| 久久精品黄片| 国产精品国产自产拍高清av水多| 一区二区三区久久| 国产成人99久久亚洲综合精品| 中文字幕第四页| 国产免费AV片在线无码免费看| www香蕉| 久久精品国产亚洲AV超碰| 色妞WW精品视频7777| 免费观看黄片| 国产精品毛片久久久久久久| 亚洲精品国产一区二区三区三州4点 | 国产网址在线观看| 一区二区亚洲视频| 宅男666| 日逼视频免费| 精品国产AV色一区二区深夜久久 | 国产真实生活伦对白| 国产成人精品水| 色九九| 久久99精品久久久久久园产越南| 亚洲高清在线无码| 99大香蕉| 天天干天天爽| 大地资源二中文在线观看官网| 色吧在线无码| 国产精品一区二区三区AV| 国产高清视频在线观看| 久久福利精品| 另类无码| 在线观看91| 美女裸体久久久久久久久| 国产一区a| 日韩人妻系列| 99久久久久久久| 国产一级免费视频| 国产 亚洲 激情 小说| 久久精品99| 日韩视频免费观看| 成人日本A片无码| 色91精品久久久久久久久| 国产午夜精品无码一区二区| 国产成人精品无码免费播放精品 | 国产精品久久久久的角色| 水蜜桃久久| 熟女一二三| 国产–第1页–屁屁影院| 欧美精品 - 色哟哟| 中文字幕乱伦视频| 秋霞三级伦电影| 麻豆乱码国产一区二区三区| 午夜一区二区三区在线观看| 91精品国产高清一区二区三区蜜臀| 黄色在线网站| 天天操人人爽| 日韩欧美中文| 天天干天天色天天射| 一本无码视频| 在线黄色网| 亚洲成人精品一区二区三区| 久久福利网| 疯狂的交换1—6真实交换3和2| 欧美视频一区二区三区四区| 国产精品二区| 91视频网站入口| 香蕉视频一区二区| 中文字幕精品一区久久久久| 亚洲国产欧美日韩| 国产精品永久久久久久久久久| 无码高清成人| 免费毛片网址| 国产精品一区二区在线免费观看| 一级操逼毛片| 国产精品黄色| 国产精品中文字幕在线观看| 台湾无码A片一区二区| 一级做a爰片毛片| 日本美女内射| 欧洲熟妇的性久久久久久| 久久亚洲精少妇毛片午夜无码| 麻豆三级视频| 国产人妻一区二区三区四区五区六| 日本护士毛茸茸| 麻豆视频免费在线观看| 韩国无码视频| 天天干天天操天天干| 亚洲AV日韩AV永久无码网站| 天天色天天日| 奇米久久| 黄页无码| 国产va在线观看| 99中文字幕| 制服丝袜在线视频| 秋霞久久| 色婷婷在线播放| 在线国v免费看| 国产精品1| 人妻,精品中区| A级片免费看| 春色AV| 久久成人麻豆午夜电影| 操逼免费| 国产一区二区视频在线| 久久精品国产精品| 天天操天天艹| 91Av导航| 成人国产色情无码视频网站代码| 日韩无码| 少妇交换HD中文| 91麻豆精品国产91久久久久久| 99久久综合国产精品二区| 欧美视频一区| 午夜视频网站| 夜夜草天天干| 欧美国产在线视频| 永久免费av网站| 无码人妻AV一区二区| 亚洲操逼网| 丁香激情五月天| 99re热精品视频| 国产AV地址| 久久久久人妻| 黄色片免费观看| 99精品久久毛片A片| 伊人久久大香线蕉| 国产美女裸体无遮挡,永久免费| 黄色一级毛片| 久草中文在线| 久草精品在线| 内射干少妇亚洲69XXX| 欧美第二页| 小小拗女一区二区三区| 欧美日韩国产精品| 激情久久AV一区AV二区AV三区 | 久久久久国产精品免费免费搜索 | 亚洲综合国产精品| 中国免费一级片| 国产粉嫩呻吟一区二区三区| 青青久操视频在线观看| 久久久大香蕉| 操逼视频无码免费看| 午夜在线小视频| 国产精品福利网站| 天天天天天天中干| 青娱乐加勒比| 二区三区视频| 校花被网站免费看视频| 日本东京热视频| 99国产精品免费视频观看8| 无码白丝强行免费| 精彩无码艹逼视频| 日韩免费操逼视频| 美女喷潮视频| 无码人妻精品一区二区三区不卡 | 99久久这里只有精品| 欧美大黄| 少妇人妻偷人精品无码视频新浪| 欧美黄片在线看| 乱伦熟妇| 久久亚洲国产精品无码一区| jizz国产| 3d动漫精品一区二区三区| 亚洲欧洲一区二区三区| 午夜精品美女久久久久av福利| 贵妇情欲按摩a片| 国内精品视频在线观看| 国产精品久久一区二区三区影音先锋| 伊人久久超碰| 国产精品无码一区二区三区 | 日韩无码视频一区二区| 精品无码黑人又粗又大又长| 欧美爱爱视频| 51无码| xxxxx国产| 黄片在线视频| 岛国激情一区二区三区| 操逼喷水无码| 伊人久久亚洲| 草逼电影| 91爽爽| 日韩无码精品视频| 伊人久久久久久久久| 国产在线网址| 国产精品一级| 免费伦片A片在线观看警官| 福利导航站| 91久久久久久久久| 亚洲三级网站| 欧美无线码| 日本熟女一区| 91精品国自产在线偷拍蜜桃| 办公室揉弄震动嗯~动态图| 国产特黄一级片| 欧美日韩在线视频播放| 亚洲精品无| 老熟女露脸泻火专区| 欧美日韩三级视频| 国产精品久久久久久一级毛片| 国产无码日韩| 免费特级黄色片| 波多野结衣网址| 99人妻碰碰碰久久久久禁片| 国产一级毛片精品A片在线美传媒| AV狠狠干| 欧洲av在线| 亚洲精品毛片| 最好看的2018中文2019| 国产又粗又大又黄| 国产品无码一区二区三区在线妖精| 亚洲视频入口| 日本熟妇色| 天天撸天天操| 性无码一区二区三区在线观看| 亚洲十八禁| 一区二区三区国产精品| 四虎欧美| 做受无码免费一区二区| 黄色网页免费| 亚洲AV高清无码| 三级精品在线| 中文字幕手机在线视频| 99精品国产91久久久久久无码| 黄色免费网站在线观看| 伊人色色| 日本人妻中文字幕| 日韩欧美在线一区二区三区| 亚洲尺码一区二区三区| 久久国产精品-国产精品| 人人操人人摸人人爽| 人人操人人爽| 国产SUV精品一区二区69| 国产丝袜视频| 欧美A级做爰片免费看红杏出墙| 亚洲熟女乱伦| 色噜噜狠狠一区| 国产精品天堂一区二区在线观看| 麻豆精品国产| 国产三级网站| 美女超碰| 亚洲啪啪| 欧美日韩一区二区在线观看| 日本一巨二巨三巨爆乳| 人妻免费视频| 一区二区三区xxx| 天天干天天日天天射| 午夜黄色一级片| 国产精品无码AV在线有声小说| 日本黄色高清视频| 三级久久| 成人高清无码在线观看| 乱伦激情视频| 91天天综合| 九九热视频在线| 中字一区| 欧美A级视频| 99热导航| 国产精品无码不卡| 欧美视频第一页| 国产一级二级三级视频| 婷婷中文字幕| 日韩无码看片| 国产视频无码| 国产精品一级AAAA片在线观看| 超碰蜜桃| 国产淑女操逼| 精品国产乱码久久久| 色资源网| 色一色操一操| 亚洲av无码天堂| 精品一区二区在线观看| 国产午夜片| 亚洲成人av在线观看| 波多野结衣无码在线播放| 91中文字幕在线| 色图无码| 久久无码影视| 污视频下载| 91久久国产综合久久| 国产一级A片夜天码免费看| 熟女导航| 加勒比无码在线观看| 91在线视频| 中文熟妇人妻又伦精品| 国产丰满乱子伦无码| 性一交一乱一透一A级| 日韩一级精品| 久久久熟妇熟女| 亚洲AV无码一区| 亚洲AV成人无码久久精品| 国产AV无码电影| 失眠是什么原因引起的| 久久久婷婷| 国产真实乱全部视频| 欧美一区二区三区四区在线观看| 日韩三级免费观看| 啊v在线观看视频| wwwxxx国产| 无码人妻熟妇av又粗又大| 欧美a视频| 亚洲操逼片| 岛国三级片在线观看| 国产av网页| 白洁性荡生活第90章| 99久久人妻精品免费二区| 无码中文av| 天天干天天色天天射| 一区二区激情| 精品无码久久久久| 91亚洲精品国偷拍自产乱码| 人人弄人人摸| 日韩两人性爱免费视频| 久久久逼逼| 永久成人无码激情视频免费| 秘书喂奶好爽一边吃奶一| 午夜精品国产| 欧洲av无码| 精品欧美一区二区三区| 青娱乐国产视频| 日韩AV无码电影| 国产精品久久久久久久久无码消赢| 欧美一a一片一级一片| 亚洲欧洲一区二区| 日韩欧美视频| 国产一级a毛一级a在线播放| 国产无码一区二区| 成人精品视频| 国产精品亚洲精品| 免费看黄视频| 日本在线一区二区三区| 无码国产精品96久久久久孕妇| 亚洲iv一区二区三区| 亚洲天堂男人天堂| 午夜福利视频一区| 99国产精品久久久久久| 黄aaaaaaaaaaaaaaaaaa色网站 | 中文无码二区| 色情无码片a一区二区| 综合另类| 欧美高清一区二区| 性爱视频操| 懂色AV一区二区夜夜嗨| 人妻自拍偷拍| 久久精品熟女亚洲av麻豆| 日韩精品在线看| 亚洲精品中文字幕乱码三区91| 久久天天躁狠狠躁夜夜AV| 欧美日韩三级片| AV网址在线| 亚洲综合激情| 特黄99视频| 久久精品无码一区| a视频在线| 性爱福利视频| 亚洲精品午夜福利| 日韩黄视频| 中文字幕第一区| 日韩毛片视频| 久久久精品欧美一区二区白云视色| 波多野结衣性爱视频| 欧美a级黄片| 理论片琪琪午夜电影| 极品视频在线| 无码少妇一区二区三区| 91色色色| 日韩久久人妻| 日韩在线免费播放| 国产精品美女久久久久AV爽| 999国产精品永久免费视频APP| 成人免费网站www网站高清| 欧美亚洲精品在线| 精品视频一区二区| 亚洲 欧美 综合| 无码三级视频| av影音先锋| 精品人妻无码一区二区三区淑枝| 亚洲精品在线视频| 友田真希一区| 无码做爰内谢免费视频| 天堂网无码| 欧美久久一区二区| 欧美性猛交99久久久久99按摩| 国产a毛片一级二级真人| 人人摸人人干人人色| 超碰影视| 在线观看视频一区二区三区| 国产美女裸体无遮挡免费播放网站| 特黄一级毛片| 无套内射在线观看| 久久午夜影院| 国产xxxxx| 国产精品久久影院| 亚洲精品国产一区二区| 午夜黄片| 国产内射一区| 99久久99久久精品国产片果冻| 黄片免费的| 国产在线精品一区二区| 精品蜜桃一区二区三区| 91精品国啪老师啪| 中文字幕www| 99国产精品久久久久久| 亚洲有码视频在线观看| 国产在线激情| 中文字幕免费在线观看| 精品久久久久久久久| 搞黄无遮挡| 一级片在线播放| 日韩精品无| 国产黄在线观看| 一级特黄大片69| 日本黄色免费看| 国产中文字幕免费| 无码在线一区二区三区| 亚洲αv| 蜜桃AV丝袜一区二区三区| 国产无套内射又大又猛又粗又爽| 亚洲精品无码在线观看| 国产一二三内射在线看片| 欧美三级片免费观看| 2024狠狠爱| 色七影院| 精品一区精品二区| 欧美a在线| 自拍视频第一页| 高清免费无码| 少妇粉嫩小泬喷水视频WWW| 最新中文字幕在线| 久久久久久久久久一级| 黄色免费一级视频| 一级片免费在线观看| 国产一毛不卡| 青草视频在线| 亚洲AV无码久久精品狠狠爱浪潮| 欧美日韩网| 高清无码操逼| 欧美日韩在线精品| 国产免费AV片在线无码免费看| 99精品久久毛片A片| 暗交老女一区二区三区| 91丨露脸丨熟女| MM1313亚洲精品无码小说| 亚洲一级黄色录像| 狠狠操影院| 性爱视频操| 69av在线| 国产精品毛片一区视频播| 国产人妻无套17p| 午夜无码在线观看| 黑人极品videos精品欧美裸| 99视频国产精品免费观看A| 久久久久久精品无码一区二区三区| 天天干夜夜爱| 五月丁香伊人网| 米奇影视777| 少妇人妻偷人精品无码视频新浪| 国产网友自拍视频| 日韩一级精品| 人妻体内射精一区二区| 欧美日本一区二区| 欧美成人性爱视频在线观看| 亚洲制服丝袜在线观看| 国产黄网站| 丰满熟妇大号BBWBBWBBW| 一区二区三区无码按摩精电影| 国产精品二区| 亚洲人成色777777精品音频| 无码视频免费观看| 日美免费黄片| 欧美亚洲一区二区三区| 青青草91| 91精品国产aⅴ一区二区| 亚洲成人精品一区| 国产精品偷伦视频免费观看国产| 高清不卡一区二区| 日韩毛片无码| 青娱乐国产视频| 少妇一级淫片免费放| 精品欧美一区二区三区免费观看 | 久久人妻一区二区三区| 午夜精品A片一二三区蜜臀| 国产色色视频| 日韩精品一区二区三区在线观看视频网站 | 国产乱人乱偷精品视频a人人澡| 日本在线不卡视频| 亚洲乱色熟女一区二区三区| 国产日韩欧美高潮无码一区二区| 色老头久久综合网| 精品综合久久久| 视频一区二区在线观看| 国产日韩在线播放| 国产91清纯白嫩初高中在线观看| xxxxx欧美| 久久久一区二区三区| 99久久中文字幕| 色九月婷婷| 亚洲精品无码久久久苍井空| 久久久精品人妻| 国产精品JIZZ久久久久久久| 久久无码影视| 日本性爱视频在线观看| 国产成人在线播放| 超碰这里只有精品| 欧美视频亚洲视频| 久久久久性色av无码一区二区| 中文字幕乱偷无码av一区二区| 在线一区| 国产一区二区免费视频| 欧美A级视频| 色综合天天综合网天天狠天天| 三级片在线观看网站| 中文字幕综合网| 久久一道本| 日本一区免费| 亚欧无码在线观看| 国产成人精品久久久| 99爱免费视频| 国产精品久久久久久久久久免费看| 色哟哟一一国产精品| 在线观看亚洲视频| 91极品人妻| 国产一区二区三区| 国产色视频一区二区三区qq号| 久久久91精品国产一区苍井空| 亚洲AV永久无码精品| 天天日天天日天天日| 成人欧美一区二区三区黑人免费| 成人片网址| 亚洲日本精品| 97在线观看| 扒开双腿猛进入的视频免费| 亚洲肏屄性爱图片| 懂色aⅴ精品一区二区三区蜜月| 九色在线视频| 蜜臀AV在线播放| 久久久久久av| 三级视频在线| 久久久影院| 久久久欧韩成人看片| 五月天狠狠爱| 久久精品国产亚洲av丁香| 熟妇人妻系列aⅴ无码专区友真希 影音先锋成人资源AV在线观看 | 久久国产一区二区三区高清视频| 91精品欧美| 黄色av网站在线免费观看| 国产一级a毛一级看免费视频| 国产一区二区三区中文字幕| 国产精品观看| 超碰不卡| 日本免费在线| 无码免费毛片| 日本在线视频一区二区| 亚洲一区电影| 中文字幕在线观看av| 日韩精品一级| 成人精品网| 91精品一区二区三区在线观看| 色婷婷色| 综合激情久久| 日韩精品在线视频观看| 九九视频免费看| 免费毛片基地| 久操精品| 日韩欧美中文| 国产一区二区视频免费| 一级做a爰片久久毛片A片冒白浆| 国产内射视频| 在线播放高清无码| 欧美日韩毛| 2014av天堂| 做受无码免费一区二区| 国产强奸乱伦精品| 日日天天| 欧美MV日韩MV国产网站| 亚洲一区无码视频| 影音先锋女人av鲁色资源久久| 国产一区AV在线| 亚洲国产网站| 国产成人久久| 日韩欧美一级片| 国产精品久久久久毛片大屁完整版| 午夜欧美一区二区三区在线播放| 99人妻| 久久精品国产亚洲A| 人人操人人爱人人乐人人操人人摸| 日韩成人高清视频| 激情欧美一区二区三区中文字幕| 黄色无码视频网站| 日本嫩草影院| 欧美激情一区二区| 色99视频| 国产无码免费视频| 黄色电影免费看| 高h小月被几个老头调教| 91偷拍一区二区三区精品| 国产三级探花日韩| 亚洲香蕉在线观看| 少妇一区二区三区| 免费在线观看成人网站| 国产一区在线午夜福利影片观看| 嫩草影院入口一二三免费| 人妻二区| 三级网站在线| 免费在线观看的黄片| 岛国大片在线观看| 亚洲激情黄色| 在线日韩国产| 国产高潮白浆无码| 久久国产精品无码| 国产无码久久久| 中文字幕亚洲综合| 欧美另类精品| 亚洲国产高清在线观看| 日韩欧美中文字幕在线观看| 天天操天天干| 免费看一级高潮毛片2023| 亚洲精品国产一区二区三区三州4点 | 秋霞AV国产精品一区| 亚洲精品无码久久久久| 久久给综久久线| 天天日狠狠干| 18禁美女网站| 午夜精品视频在线观看| 91高清视频| 无码人妻少妇| 无码精品一区二区三区潘金莲| 国产精品一级二级三级| 干爽人妻| 亚洲美女一区| 国产三级片在线看| 亚洲国产成人精品无码区二本| 99久久99久久精品国产片果冻| 国产夫妻性爱自拍| 熟妇熟女一区二区三区| 国产在线a| 午夜精品久久久久久久| 偷拍区小说区| 亚洲欧洲精品一区二区| 在线中文字幕视频| 92国产精品| 日韩操逼逼| 午夜福利精品| 91亚洲精品乱码久久久久久蜜桃| 哦┅┅快┅┅用力啊熟妇在线视频| 人人九九精品| 国产伦乱| 在线小视频| 国产自慰网站| 精品一区国产| 黄色在线观看国产| 国产精品乱码| 精品久久ai| 夜夜草影院| 午夜av污污污羞羞影院| 欧美午夜精品久久久久久浪潮| 日韩熟女一区| 视频操逼| 国产午夜精品在线| 校园春色亚洲无码| 亚欧无码| 国产精品一区二区三区免费| 日本三级视频| 色先锋资源| 国产精品毛片AV| 欧美黄色三级片| 人人人操| 8050午夜| 国产第一页屁屁影院| 毛片99| 成人A视频| 国产香蕉视频在线观看| 超碰999| 国产精品天天狠天天看| 国产精品免费在线| 中文无码在线视频| 成人高清无码在线观看| 日韩在线视频精品| 乱熟女高潮一区二区在线 | 成人在线性爱免费视频| 乱伦精品| 欧美日韩精品一区二区三区| 国产精品欧美日韩| 中文字幕亚洲中文精品乱码在线| 人妻少妇一区二区三区| 色综合天天综合| 最新高清无码专区| 深夜福利无码| 91成人国产| 亚洲无码爱爱| 久久国产高清视频| 日韩精品一区二区三区电影| 日韩欧美一区二区三区| 三级无码| 日韩在线精品| 中文字幕丰满人妻无码区隔壁人爱| 国产超碰在线| 高清无码毛片| 91人妻无码一区二区三区| 久久久精品国产sm调教网站| 黄视频网站| 最新无码视频| 国内精选免费大片在线观看| 国产精品精品| 久久久久久精品一级毛片蜜| 亚洲精品中文字幕| 国产精品久久久久久精| 亚洲网站在线观看| 国产熟女乱伦文学| 色综合天天综合网天天看片| 日本一区久久| www国产视频| 亚洲高清毛片| 91小视频在线观看| 日韩av电影在线观看| 久久精品一区| 黄色一级片视频| 熟女一区| 日本免费高清视频| 国产亚洲精品久久19p| 水蜜桃成人| 潮喷在线| 国产极品在线观看| 国产色视频一区二区三区qq号| 色婷婷精品久久二区二区密| 亚洲国产综合在线| 国产熟女视频| 黄片AV在线| 亚洲视频欧美视频| 精品久久久久久久久久| 亚洲国产视频中文字幕| 日本精品三区| 乱熟女高潮一区二区在线观看| 国产精品国产三级国产三级人妇| 久久久国产视频| 欧美日韩俄乌国产男女操逼逼视频| 欧洲高清转码区一二区| 欧美一级性爱| 乱伦五月天| 亚洲熟妇综合久久久久久| 国产精品美女久久久久久久久久久| 欧美一区二区三区免费细高跟视频| 亚洲性爱片| 亚洲成人无码在线观看| 欧美一区二区在线| 黄页网站免费观看| 精品欧美一区二区精品久久久| 色姑娘综合网| 三年片观看免费观看大全| 99久久精品免费看国产免费粉嫩| 国产午夜福利| 国产综合精品| 国产精品久久久久久久久| 黄色av网站在线观看| 欧美日日干| 国产乱伦小说| 午夜无码免费视频| 日韩无码第二页| 国产三级自拍| 亚洲AV无码牛牛影视| 人妻二区| 国产精品爽爽久久久久久豆腐| 国产又粗又爽又黄的视频| 五月婷婷综合网| 国产欧美另类| 91精品国产| 精品二区在线观看| 精品国产一区二区三区久久久蜜月| 国产精品成人在线观看| 99精品无码扒开猛进自慰| 男人天堂亚洲| 乱女乱妇熟女熟妇综合网网站| 天堂在线一区| AV在线无码| 丰满人妻妇伦又伦精品APP| 国产伦精品一区二区免费| www超碰| 大香蕉福利视频| 一区二区三区欧美| 免费国产乱伦| 亚洲无码高清视频| av第一福利导航| 搡老熟女老女人一区二区| 久久精品午夜| 午夜操逼| 亚洲日本精品| 九九在线精品视频| 狠狠操影院| 青青草一区二区| 欧美视频一区二区三区| 青青国产| 国产无套内谢国语对白| 久久亚洲国产精品无码一区| 国产一区精品| 乱熟女高潮一区二区在线| 无人码人妻一区二区三区免费| 色牛Av| 99热视| 夜夜看av| 性无码一区二区三区| 激情内射人妻1区2区3区| 欧美电影一区二区三区| 国产老熟女一区二区三区仙踪密林| 99国产精品一区二区| 国产综合在线观看| 久久日本无码中文字幕三级伦| 日韩免费网站| 啤酒色 无码| 亚洲av一级| 国产乱伦免费| 婷婷久久五月天| 亚洲中文字幕无码AV| 日本三级日本三级日本产国| 91在线无码| 深夜福利无码| 亚洲中文字幕一区二区| 国产精品一区二区三| 欧美三日本三级少妇三级在线播| 欧美一级在线观看| 超碰在线中文字幕| 久久久精品一区二区三区| 国产女主播一区| 操逼视频无码免费看| 无码人妻少妇一区二区三区波多| 精品人伦一区二区色婷婷| 91精品丝袜国产高跟在线| 亚洲国产精品自拍| 夜夜躁狠狠躁日日躁麻豆老人| 精品国产乱码久久久久久浪潮| 免费视频无码| 成人高清| 无码手机在线观看| 二区三区无码| 欧美伊人| 亚洲无码校园春色| AV电影在线免费观看| 国产麻豆视频| 特级无码| 成人免费毛片足控| 国产丨熟女丨国产熟女| 日韩欧美综合| 丁香七月婷婷| www.人妻| 久久久久国产一区二区三区| 精品免费国产| 三级网站在线| 日韩av毛片| 91麻豆视频| 亚欧AV| 成人第一页| 亚洲强奸视频网站| 白浆一区| 婷婷视频在线| 日本久久久久久| 中文字幕日本最新乱码视频| 巨爆乳肉感一区三区三区夜本色| 国产成人精品视频| a级片网站| 国内乱伦视频| 亚洲精品影院| 五月婷婷丁香| se综合网站| 精品无码视频| 高清无码小电影| 亚洲一区二区免费视频| 午夜操逼逼| 午夜精品久久久久久久男人的天堂 | 亚洲AV无码一区二区三区蜜柚| 国产网友自拍视频| 午夜爱爱毛片XXXX视频免费看| 国产精品成人一区二区网站软件| 亚洲精品少妇| 国产精品久久久久av| 欧美草逼网| 中文字幕www| 丁香五月天狠狠操| AV天堂久久| 一级毛片久久久久久久18| 国产色在线| 变态另类第一页| 婷婷大香蕉| 99精品成人无码A片观看金桔| 亚洲中文字幕在线观看| 久久精品不卡| 人妻少妇精品中文字幕AV蜜桃| 天天射日日| 超碰九九| 日韩中文字幕网| 91手机在线视频| 成人午夜毛片| 亚洲大片在线观看| 亚洲精品v日韩精品| 嘿嘿射在线|