久久精品女人天堂?V免费观看_精品少妇一区二区_欧美专区在线视频_日韩一区二区超清视频_欧美一级久久精品麻豆_国产成人一区二区三区免费AV_国产精品日本免费视频_亚洲精品免费第一页

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
日本久久久久久| 日本中文字幕在线播放| 中日韩一级片| 久久国产精品伦子伦网爆社区| 亚洲免费无码| 国产男女猛烈无遮掩视频免费网站| 日本性爱视频在线观看| 精品人伦一区二区色婷婷| 久久精品国产一区二区三区| 日韩美女一区二区三区| 高清欧美精品XXXXX在线看| 亚洲av播放| 日韩二区在线| 天堂网AV极品| 中文字幕一区二区三区| 亚洲高清一区二区三区| 安徽妇搡bbbb搡bbbb按摩 | 无码在线电影| 国产精品无码天天爽视频熟妇人 | 久久91精品| 亚洲一区二区在线播放| 欧美精品videos另类日本| 国产精品亚洲一区二区三区在线| 国产91在线视频| 一级av在线| 精品久久99| 日韩在线观看网站| 91AV亚洲| 国产精品内射婷婷一级二| 欧洲精品在线观看| 影音先锋成人AV| 无码国产精品一区二区色情男同| 无码国产精品一区| 大美女禁视频www| 国产成人精品久久二区二区| 国产精品第1页| 人妻中文在线| 狼友视频在线播放| 亚洲欧美激情小说另类| 91少妇精拍在线播放| 国产精品成人在线观看| 超碰av在线| 成人欧美一区| A片成人色色色网站在线播放| 亚洲综合色图| 天天射综合| 国产酒店3p| 人妻在线视频| 午夜激情AV| 无码人妻束缚av又粗又大| 翔田千里性爱视频| 久久人人爽人人| 黄色成人av| 国产第一页屁屁影院| 狠狠躁日日躁XXXXAAAA| 中文字幕第一区| 亚洲激情综合| 国产伦精品一区二区三区妓女下载| 欧美成人一区二免费视频苍井空| 国产三级精品三级在线观看四季网| 99精品久久| 人妻少妇精品视频免费看蜜桃| 婷婷一区二区| 国产美女裸体无遮挡,永久免费| 同桌用振动器玩我下面| 日韩无码成人| 亚洲综合激情| 91在线视频免费观看| 熟女91| 欧美黑人xxx| 欧美日韩免费在线| 五月婷婷大香蕉| 午夜男人视频| 国产精品久久影视| 国产精品黄色| 在线无码播放| 亚洲欧洲一区二区三区| 国产一级毛片av| 97久久精品| 久草人妻在线| 丰满人妻一区二区三区四区仙踪林 | 亚洲天堂av无码| 最新国产精品| 国产精品色哟哟| 久久中文视频| 天天干天天日天天射| 欧美XXXBBB| 日日夜夜草| 国产av一区二| 天天操夜夜操人人操| 欧美熟妇在线观看| 久久精品日韩| 欧洲av无码| 91丨九色丨熟女高潮| www亚洲午夜人美精片V区| 国产一级片在线| 女子初尝黑人巨嗷嗷叫| 国产欧美日韩综合精品| 欧美一区二区在线观看视频| 99热免费在线观看| 香蕉视频色| 爆乳熟妇一区二区三区爆乳漫画| 91视频播放| 久草国产在线| 亚洲一区二区三区视频| 久久久久久免费毛片精品| 黄网站免费看| 日本无码成人片在线观看波多| 一二三四无码| 久久亚洲一区二区三区四区| 免费视频成人| 国产91夫妻拳交| 热99视频| 一级内射片在线网站观看| 久久动态图| 黑人巨大精品欧美一区二区免费 | 精品无码一区二区| 亚洲精品无码18在线| 台湾精品久久久久久久| 91男女| 91亚洲视频在线观看| 国产三级日本三级在线播放| 国产后入清纯学生妹| 曰本无码人妻丰满熟妇啪啪| 91人妻无码一区二区三区| 色一情一伦一子一伦一区| 久久久久国产| 无码午夜精品一区二区三区视频| 免费精品一区二区三区视频日产| 日本精品视频在线观看| 国产综合在线观看视频| 人人干黄色| 三级片在线播放网站| 91国内自产精华天堂| 亚州AV| 波多野结衣一区| 精品中文字幕| 欧美精品久久久久久| 国产中文字幕免费| 日韩三级在线观看视频| 91激情视频| 中文字幕国产| 一级黄色A视频| 久久77| 国产情侣在线视频| 免费AV在线播放| 亚洲欧洲在线观看| 精品成人一区二区| 久久久久久中文字幕| 人人射人人操| 久热综合| 超碰人人人| av无码一区二区| 国产岛国A区一区| 精品乱子伦| 操逼免费| 无码深夜AAA片在线观看| 97伊人| 久久无码高清| 精品无码视频在线| 日韩三级在线| 黄色链接在线观看无码| 麻豆乱码国产一区二区三区| 国产黄色影院| 成人黄色一级片| 色香蕉视频| 偷看少妇自慰xxxx| 韩国精品视频在线观看| 国产成人91亚洲精品无码观看| 黄色链接在线观看无码| 国产女同| 欧美国产精品一区| 日韩美女在线| 91精品在线看| 欧美精品久久| 国产精品IGAO视频| 亚洲 欧美 自拍 另类 日韩| 乱色熟女综合一区二区三区 | 国内自拍偷拍视频| 91手机操逼视频| 国产一级毛片视频| 久久国产露脸精品国产| 国内精品一区二区| 亚洲福利网| 亚洲少妇一区二区| 日韩乱码一区二区三区| 精品综合网| 91麻豆精品国产| 国产精品久久久久久自浆Pr0m| 蜜桃久久久| 亚洲AV永久无码精品视色影视| 欧–美–性–交–黄–片| 少妇精品一二三区拳交| 麻豆精品视频| free性丰满69性欧美| 丝袜一区二区三区| 久久久久免费视频| 好屌妞视频这里只有精品| 欧美色图第一页| 99er在线| 岛国一级片视频在线免费观看| 精品视频一区二区| 中文字幕操逼| 8090操逼网| 日日夜夜草| 精品无码久久久久久国产牛牛影视| 欧美性爱一区二区三区| 欧美A级做爰片免费看红杏出墙| 日本一本视频| 免费观看黄色网址| 亚洲ⅴ国产v天堂a无码二区| 无码资源在线| 向日葵视频在线观看| 欧美性爱免费看| 黄色一级大片在线免费看国产一| 久久久夜夜夜| 亚洲性爱一区| 色欲AV伊人久久大香线蕉影院| 亚洲国产成人va在线观看天堂| 久久精品免费| 影音先锋男人av资源| 国产a一级| 亚洲中文字幕一区二区| 亚洲性爱av免费观看| 自拍偷拍一区| 国产视频二区| 国产一区不卡| 日韩毛片| 苍井空无码一区| 国内乱伦AV| 精产国产伦理一二三区| 97人伦影院A片在线观看97 | 日韩无码P| 国产福利一区二区三区视频| 国产乱来视频| 免费黄片毛片| 亚洲乱伦一区| a黄色澳门免费观看| 国产亚洲精久久久久久无码色戒| 伊人精品视频| 亚洲福利| 综合成人| a一级毛片| 精品伊人| 欧美乱妇狂野欧美在线视频| 色网站在线观看| 久久久久无码久久久| 秋霞午夜福利视频| 凹凸农夫导航十次啦| 亚洲毛片| 91日本| 国产免费自拍| 免费看操逼视频| 免费看黄色大片| 国产福利在线观看| 久久精品国产AV一区二区三区| 国产精品亚洲无码| 中文字幕一区二区三区日韩精品| 亚洲三级视频| 中文字幕无码在线观看| 久久亚洲欧美日韩精品专区| 女人扒开屁股桶爽30分钟| 国产一区a| 香蕉视频污版| 国产精品一区二区三区在线免费观看| 麻豆精品一区二区三区| 国产骚逼| 欧美一级黄色大片| 欧美一区二区三区视频在线观看 | 日韩无码操逼视频| 熟女视频91| 熟妇免费视频| 国产亚洲精品女人久久久久久| 久久精品国产亚洲av瑜伽仙踪林| 99视频在线免费观看| 人人搞人人操人人插人人摸| 精品一区二区在线播放| 俄罗斯电影一区二区| 国产欧美小视频| 亚洲视频不卡| 日韩视频精品| 欧美自拍视频| 被老头玩弄的漂亮人妻| 岛国视频一区在线| 久久久久国产视频| 精品乱伦| 麻豆精品一区二区三区av沈娜娜| 91免费在线| _中国一级特黄大片在线看| 美国一级黄色录像| 思思热视频在线观看| 国产91九色| 日韩二级片| 日本久草| 色牛Av| 人人摸人人搞| 蜜桃五月天| 色欲av永久无码精品无码蜜桃| 久久久精品人妻| 巨爆乳肉感一区三区三区夜本色| 一级做a爰性色黄A片小优视频 | 一级丰满老熟女毛片免费观看| 久久久久国产一级毛片| 日韩欧美黄色| caoprom人人| 欧美另类精品| 九九九国产| 口爆吞精视频| 国产黄片在线免费看| 国产高清一级毛片在线不卡| 自拍偷在线精品自拍偷无码专区| 天天插天天色| 欧洲精品视频在线观看| 丰满少妇伦精品无码专区| 无码国产| 亚洲AV伊人久久青青草原视色| 日韩操逼片| 精产国品一二三区| 超碰99在线| 在线免费黄片| 拳交美女A片大全| 麻豆久久| 片库| 日本无码在线| 久久精品国产AV一区二区三区| 日本精品久久久| 天天鲁一鲁摸一摸爽一爽| 精品国产乱码久久久久久婷婷| 日韩动漫无码| 国产毛片久久久久| 成人在线观看网站| 一区二区三区免费电影| 国产又粗又猛又大爽| 黄色亚洲视频| 一插菊花综合网| 午夜无码片在线观看影院| 久久伊99综合婷婷久久伊| 久久无码一区| 偷拍洗澡一区二区三区| 乱色熟女综合一区二区三区四| 爆乳一区| 嫩草视频在线观看| 爱草视频| 一区二区三区四区亚洲| 日韩午夜| 成人AV导航| 日韩欧美一区二区三区| 青青草成人网| 人妻专区| 精品国产自在精品国产精小说 | 好屌妞视频这里只有精品| 人人妻人人干| 麻豆久久久| 亚洲AV无码乱码| WWW插插插无码视频网站| 日本免费久久| 国产性爱一级片| 国产三级精品三级在线观看| 99精品久久久久久中文字幕| 亚洲狠狠爱| 伊人网在线观看| 亚洲男人天堂网| 懂色av一区二区三区| 一级a一级a爱片免免费香蕉精品| 亚洲喷水无码一区丰满爆乳少妇| 精品乱码一区内射人妻无码| www无码视频| 欧美MV日韩MV国产网站| 亚洲黄色小视频| 色久视频| 琪琪在线视频| 国产黄色一级片| 99欧美精品| 亚洲中文字幕一区二区| 熟女乱伦av| 免费国产一级| 超碰地址| 东北浓毛老妇国语对白| 国产 丝袜 另类 精品 综合| 国产色区| 探花日韩无码| 久久久久人妻| 无码免费一区二区三区| 99精品久久毛片A片| 婷婷色导航| 午夜一级片| 农村毛片| 少妇熟女视频一区二区三区 | 操逼一区| 午夜AV在线| 久久无码人妻| 亚洲成人av在线观看| 久久精品中文字幕| 亚洲黄色电影在线观看| 一级做a爰片久久毛片无码电影| 亚洲AV精色AV日韩大尺度| 一区二区三区视频在线观看| 亚洲精品一区三区三区在线观看| 福利视频导航大全| 日逼视频免费| 精品国产乱码| 91香蕉在线视频| 婷婷综合久久| 日本久久性爱| 欧美日韩操逼| 国产无码毛片| 香蕉视频免费| 大香蕉一区二区| 色鬼网站| 在线观看欧美日韩视频| 99re视频在线| 九九九九九九精品| 午夜想操你逼| 人人在操| 强奸乱伦1区2区3区| 无码成人一区二区三区入厕偷拍 | 在线观看无码电影| 99免费在线观看| 一级香蕉,黄色片| 久一在线| 亚洲色图乱伦av| 天天日天天操天天干| 色婷婷丁香五月| 国产伦精品一区二区三区妓国产 | 久久久精| 高清无码免费看| 亚洲视频在线免费观看| 99er热精品视频| 蜜桃av在线| 日韩视频在线观看免费 | 国产AV国产精品无套内谢下载| 在线观看中文国产探花| 青青草国产| 免费无码国产在线电影| 另类TS人妖一区二区三区| 国产精品久久久久久免费播放| 国产精品人妻无码久久久苍井空| 国产在线看av| 日韩精品人妻免费视频| 91久久久久无码精品国产| 欧美精品一区二| 国产主播99| 牲欲强的熟妇农村老妇女视频| 亚洲激情在线| 秋霞在线视频| 欧美五月婷婷| 日韩免费成人| 免费看黄网址| 久操视频在线| 小黄片高清| 狠狠综合久久AV一区二区老牛| 伊人婷婷| 秋霞在线无码| 韩国三级bd高清中字2021| 精品视频一区二区| 狼人综合网| 欧美性猛交99久久久久99按摩| 一级激情视频| 在线观看一级黄片| 日韩一级视频| 日韩精品久久久| 欧美精品一区二区三区A片| 天天干天天干天天干天天| 国产不卡视频一区二区三区| 无码视频在线| 在线视频一区二区三区| 人人操人人干人人摸人人色| 91九色在线| 国产精品免费无遮挡无码永久视频| 在线观看污污网站| 久久国产热视频| 精品国产乱码久久久久久图片| 日韩黄色网| 日韩一级毛卡片| 精品在线一区二区| 97精品人妻一区二区三区香蕉| 色婷婷精品久久二区二区密| 久久成人毛片| 三级片91| 黄网在线| 国精品无码一区二区三区三州| 亚洲91色图| 美女航空一级毛片在线播放| 狼人综合网| 成人蜜桃视频| 亚洲无码少妇| 久草人妻| 免费一级黄色录像| 亚洲欧美日韩在线播放| 无码人妻精品一区二区三区777| 蜜乳AV高清无码在线观看| 中文字幕日韩精品无码内射| 人妖AV| 日韩无套| 国产精品爽爽久久久久久| 不卡成人| 91久久精品日日躁夜夜躁欧美| 亚洲天堂av无码| 免费成人性爱| 岛国一区二区| 亚洲无码午夜福利| 国产AV一级| 日本高清久久| 国产一级a毛一级a| 超碰男人的天堂| 一级内射片在线网站观看| 婷婷国产| 亚洲无码专区在线观看| 婷婷伊人| www.-级毛片线天内射视视| 亚洲乱妇老熟女爽到高潮的片| av第一区| 成人网站在线进入爽爽爽| 少妇高潮喷水久久久久久久久| 最好看的2018中文2019| 日韩欧美国产高清| 国产精品一区在线播放| 久久久久18| 亚洲AV免费在线观看| 在线观看网站深夜免费| 国产一区二区无码| 精品自拍AV| 日本无码在线观看| 秋霞午夜国产精品成人片| 欧美激情中文字幕| 一级黄色片在线免费观看| 人妻中文无码| 激情久久久| 欧美性爱人人| 久久精品中文| 一级黄色电影网站| 天天天天天天中干| 色呦呦在线| 秋霞电影网一区二区三区| 丰满肥臀无码一区二区三区| 91在线视频播放| 国产精品一区二区电影| 黄aaaaaaaaaaaaaaaaaa色网站 | 天天操夜夜操| 午夜成人福利在线| 真实的和子乱拍视频| 国产精品无码永久免费不卡| 国产精品爽爽久久久久久| 性欧美精品| 日韩操逼片| 亚洲精品一二三四| 国产精品网址| 自拍偷拍网站| 97色综合| 国产一区观看| 国产古装又黄A片在线观看| 青青青视频在线| 久久一级| 欧美一级黄色网| 一级毛片在线免费观看| 欧美亚洲性爱| 国产一区无码| 超碰在线人人草| 久久久久亚洲| 亚洲无码免费在线观看| 五月社区| 欧美一区在线观看精品色欲| 国产永久精品| 天天干夜夜草| 大地资源免费视频观看| av电影资源| 黄色AV网| 秋霞在线影院| 无码精品一区二区免费JIZZ| 亚洲精品乱码久久久久久久久久| poronodrome极品另类| 久久免费视频6| 中文字幕乱偷无码av一区二区| 日韩欧美视频一区二区三区| 色哟哟国产精品色哟哟| 人与禽性视频77777| 蜜桃久久av无码牛牛影视| 影音先锋男人的天堂| 无码不卡在线| 久久久久一区| 日韩一区二区三区在线观看| 国产亚洲色婷婷久久99精品| 天天欧美| 狠狠操97操| AV肉肉| 在线观看免费高清无码| 久久精品成人一区二区三区蜜臀| 亚洲AA| 日韩精品影院| 日韩无码小电影| 久久高清内射无套| 少妇精品无码一区二区免费法国 | 国产免费乱伦| 91导航中文字幕| 久久免费小视频| 九九久久国产精品| 久久天堂av| 日韩黄色精品| 91com欧美乱伦| 狠狠操观看视频| 精品久久久久久久人人人人传媒| 久久国产亚洲精品| 中文无码电影| 亚洲精品乱| 国内精品国产三级国产在线专 | 国产真实乱全部视频| 91在线视频| 国产精品黄片| 一级久久| 日韩无码网址| 影音先锋中文字幕资源6| 无码av中文| 丰满人妻妇伦又伦精品APP| 欧美国产日韩在线观看成人| 午夜爱爱毛片XXXX视频免费看| 人人干黄色| 久久久久久久久久久99精品无码| 黄色不卡视频| 少妇又紧又深又湿又爽视频| 91大神精品| 久久精品熟女亚洲av麻豆| 一级a一级a爰片免费免免免下载| 日韩三级中文字幕| 久久加勒比| 日韩免费视频一区二区| 超碰人人妻| 超碰在线人人草| 丁香五月婷婷综合| 亚洲欧美日韩在线播放| 亚洲图片在线观看| 天天干在线观看| www毛片| 含着奶头搓揉深深挺进P漫画| 无码国产精品一区二区免费网站| 欧美日韩一级黄片| 国产一级特黄AAA大片| 在线观看成人电影| 国产操比一区| 国产SUV精品一区二区6| 香蕉国产2023| 国产精品成人在线| 人妻性爱网站| 亚洲精品影院| 久久精品超碰| 日韩 欧美 亚洲| 天天操天天干天天日| 97中文字幕在线观看| 亚洲第一中文字幕| 中文无码熟妇人妻AV在线| 中文一级片| 伊人久久免费视频| 国内少妇一区二区三区免费看| 国产黄色精品| AV无码免费| 嘿嘿射在线| 少妇人妻真实偷人精品视频| 99久久婷婷国产一区二区三区| 蜜桃AV丝袜一区二区三区| 成年人免费观看性爱视频| 无码精品人妻一二三区红粉影视| 久久精品影视| 亚洲A视频在线| 久去色| 一级特色黄大片| 三级在线观看| 免费国产精品视频| 成人动漫在线观看| 四色成人A片视频在线看| 日韩欧美一区在线观看| 影音先锋中文字幕资源6| 免费费一级黄色电影| 日韩欧美三级视频| 精品国产乱码久久久久电车痴汉久| 国产成人精品无码免费看点牛影视| 麻豆精品蜜桃视频网站| 一级特黄aa大片欧美| 国产精品久久久久无码AV八戒| 亚洲黄色小视频| 欧美精品一区二区视频| 国产成人在线免费视频| 女人爽到高潮免费视频| 欧美福利导航| 一级毛片久久久久久久18| 无码成人动漫| 久久久精品电影| 国产女主播在线| 国产无码观看| 成人做爰高潮片免费观看视频| 99自拍视频| 欧美一区二区三区在线观看| 午夜性色福利视频| 久久偷拍视频| 视频一区 91导航| 午夜秋霞| 国产三级视频| 国产伦精品一区二区三区视频金莲 | 成人精品视频在线| 中文字幕日韩在线| 国产一区在线免费| 亚洲三级片网站| 国产熟女鲁鲁视频| 欧美不卡一区| 亚洲熟女乱伦| 天堂综合网| 人人操人人搞| 99热免费观看| 亚洲精品一| 中文字幕成人电影| 日韩精品久久久久久久酒店| 国产在线91| 中文字幕第一区| 国产手机在线视频| 99久久国产热无码精品免费 | 亚洲精品一区二区三区成人片| 欧美亚洲天堂| 丰满少妇被猛烈进入| 国产高清无码一区| 又长又粗又爽美女高潮视频| 无码人妻少妇一区二区三区波多| 夜夜躁狠狠躁日日躁麻豆老人 | 婷婷五月天影视| 最新av在线| 五月天婷婷激情| 逼特逼视频在线观看| 福利姬在线观看| 99视频免费| 国产精品v欧美精品v日韩 | 凹凸精品熟女在线观看| 91精品在线观看视频| 亚州AV| 国产乱伦自拍视频| 一级操逼毛片| 国产人妻鲁鲁一区二区| 亚洲无遮挡| 国产一级做a爱片毛片A片男| 黄网站入口| 亚洲AV色一区二区三区精品| 国产一区福利| 亚洲福利一区二区| 岛国片在线观看| 97无码精品人妻一区二区三区 | 国产精品一区二区三区免费| 日韩AV无码专区| 伊人狼人综合| 国产性爱在线| 51ⅴ精品国产91久久久久久| 先锋影音一区二区日韩| 日本黑人乱偷人妻中文字幕| 久久久久国产精品免费免费搜索| 国产最新精品| 国产精品欧美在线| 久久亚洲视频| 亚洲午夜无码| 国产粗语刺激对白性视频| 久久久久久久亚洲| 手机在线无码视频| 无码精品一区二区三区四区色| 久久18| 国产一区二区电影| 高清无码小电影| 日韩视频中文字幕| 又大又粗又硬的视频| 亚洲AV二区| 人妻系列中文字幕| 这里只有精品视频| 国产精品一区二区在线观看| 国产在线网址| 黄色片网站在线| 丝袜制服大香蕉| 亚洲AV动漫| 免费看一级片| 久久久精品免费视频| 国产精品内射婷婷一级二| 婷婷五月天久久| 性爱导航综合| 欧美多毛熟妇| 国产精品日韩欧美| 亚洲三级网| 国产九九九| 成人毛片网| 狠狠人妻| 成人性生交大片免费看4| 熟妇熟女一区二区三区| www18禁| 又白又嫩毛又多12P| AV一二三区| 亚洲无码精品一区| 理论片琪琪午夜电影| 一级免费黄色片| 91视频色| 久久偷拍视频| 久久精品一区二区| 久久久久国产一区二区三区| 91天堂| 国产成人精品视频| 国产精品3| 欧美视频三区| 亚洲熟妇XXXXX| 久青操| 欧美日韩中文视频| 欧美在线中文字幕| 伊人久久久久久久久久久久 | 欧美激情精品久久久久久| 加勒比无码在线观看| 国产欧美日| 国产极品美女高潮无套在线观看| 亚洲熟女乱色一区二区三区丝袜| 色网在线播放| 亚欧洲精品视频在线观看| 草草网站| 天天日天天草| 高清无码免费看| 久久国产精品-国产精品| 日本无码精品| 明星A片无码一区二区| 91蜜桃在线| 91高清视频| 少妇xxxx| 日本三级少妇三级99夜在线观看| 军人野外吮她的花蒂| 久久久久亚洲AV无码换脸| 人人妻人人澡人人爽欧美一区双 | 91久久久| 国产精品香蕉| 日韩 欧美 亚洲| 久久久91人妻无码| 日韩精品一二三四区| 香蕉视频三级片| 中文天堂国产最新| 白浆一区| 日韩精品久久久| 国产成人精品一区二区| 亚洲Av无码午夜国产精品色软件| 精品欧美黑人一区二区三区| 亚洲熟妇一区| 国产乱伦一区| 高清无码视频在线播放| 国产视频网| 激情综合在线| 国产成人午夜视频| 国产无码在线看| 国产黄在线观看| 国产熟女一区二区三区浪潮97| 免费无码一区二区三区| 日本黄色一级| 免费黄片在| 欧美熟妇性爱视频| 久久天堂| 真实国产精品亲子伦视频对白| 夜夜操天天干| 性欧美另类| 一区二区三区三级片| 精品久久av| 操逼一| 国产亚洲精品女人久久久久久| 国产高清视频| 无码视少妇视频一区二区三区| 女同一区二区| 亚洲精品免费在线观看| 免费点击进入日韩| 乱伦中文| www.午夜| 一二三区在线视频| 一级毛片在线播放| xxxxx国产| 91精品无码国产在线观看一区| 丁香五月天AV| 国产又粗又大视频| 中文一区在线观看| 久久精品视频6| 亚洲自拍一区| 91插插插影库永久免费| 国内精品嫩模AV私拍在线观看| 国产中文字幕一区| 国产天堂网| 无码一区精品| 在线二区| 高清免费无码| 精品黄色片| 国产免费不卡视频| 成人做爰A片一区二区app| 无码专区视频| 久久久精品人妻一区二区三区色秀| 亚洲一级黄色| 久久欧美国产伦子伦精品按摩| 一区二区视频| 精品视频免费看| 99欧美| 欧美性视屏| 嫩草视频在线| 久久久久国产精品午夜一区| 日韩免费在线| 偷拍亚洲一区| 黄片软件在线下载| 自拍偷在线精品自拍偷无码专区 | 亚洲有码视频在线观看| 精品久久影院| 国产主播一区二区三区| 琪琪在线视频| 久久专区| 日韩精品在线一区| 欧美MV日韩MV国产网站| 久久99国产精品| 性做久久久久久久| 高清无码视频在线观看| 国产日韩视频在线| 亚洲精品久久久| 日本不卡一区二区三区| 欧美一区二区三区免费A片老妇人| 国产毛片在线| 国产又粗又硬又长又爽| 久久久久无码国产精品Sm高潮| 国产精品熟女一区二区不卡| 日韩精品一区二区三区中文字幕| 超碰公开人人操97| 亚洲熟妇AV乱码在线观看| 无码不卡一区二区| 亚洲第一区第二区| 中文字幕精品三区无码| 国产又色又爽又刺激在线观看| 一级a免一级a做免费线看内裤| 91天堂在线| 黄色黄片免费看| 国产精品www| 国产精品羞羞无码久久久| 久久黄色网址| 日韩无码乱伦视频| 国产AV黄色片|