后入欧美美女在线视频|?v在观线观看男人的天堂|国产美女高潮一区视频|久久精品国产av久|中日韩精品激情在线观看网站|国产高清在线在线视频|欧美成人午夜大片在线观看|欧美乱码一区二区三区在线

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
成年网站在线观看| 国产一级A片| 极品丰满少妇XXXHD剃毛| 国产激情视频一区| 91爱爱视频| 国产精品久久久久无码AV蜜臀| 亚洲欧美日韩精品久久亚洲区| 少妇高潮一区二区三区99刮毛 | 欧美精品在欧美一区二区少妇| 亚洲Av无码午夜国产精品色软件 | 国产精品久久久久久亚洲调教| 亚洲A级片| 无码专区一区| 玩弄白嫩少妇XXXXX性| 日韩av在线免费| 成人免费毛片AAAAAA片| 毛片在线免费| 中文字幕乱伦| 国产一级做a爰片久久毛片男| 国内精品写真在线观看| 国产精品99久久| 国产三级探花日韩| 中文字幕在线无码| 日韩无码网| 欧美性爱日韩高清| 亚洲w欧洲无码sss222| 最好看的2018中文2019| 我要看91大橾逼视频| 国产精品久久久久久久免费看| 久久99免费视频| 嫩草国产| 美女污污网站| 麻豆国产在线| 特级做a爰片毛片免费69| 欧美熟女一区二区三区| 久久久艹| 色综合天天综合网国产成人网 | 91精品在线视频| 亚洲欧美日韩精品久久亚洲区| 午夜国产在线观看| 91丝袜一区二区| 中文字幕在线观看日韩| 中国黄片免费看| 婷婷色九月| 日韩无码久久| 久久99精品国产自在现线| 草草影院ccyy国产日本第一页| 中文字幕国产传媒| 久久一区二区视频| 国产裸体永久免费无遮挡| 国产一区无码| 日本熟妇色日本免| 国产家庭性爰| 一区国产精品| 黑人精品XXX一区一二区| 免费在线看黄网站| 绯色av蜜臀一区二区中文字幕 | 人人操天天操| 欧美性视屏| 日韩欧美爱爱| 亚洲一区二区三区四区| av不卡在线| 日韩在线播放视频| 国产精品久久久久久模特| 在线播放成人A片麻豆网站| 日韩一区二区三区在线| 久久久久亚洲AV无码网站| 黄色无码在线观看| 高清在线无码视频| 欧美日韩国产中文字幕| 亚洲第一中文字幕| 亚洲精品91| 99re视频在线| 色婷婷又粗又长| 国产无码www| AV中文字| 全肉变态重口调教高辣小说| 亚洲国产精品自拍| 91麻豆精品国产91| 国产91视频| 日韩电影一区二区| 国产黄色影院| 欧美综合在线观看| 99精品欧美一区二区三区黑人| 国产日韩欧美一区| 日韩a在线| 米奇影视777| 天天看天天爽| 白嫩娇妻被交换经过| 一级a一级a爰片免费免免软件ww| 91香蕉视频在线| 狼友视频在线观看| 久久国产精品一区二区| 国产在线拍揄自揄拍无码视频| 日韩黄片| 国产人妻人伦精品久久| 一牛影视av| 亚洲日本精品| 国产一级性爱| 无码人妻一区二区三区线| 欧美性爱一区二区| 97精品视频| 91视频官网| 日韩免费视频一区二区| 久久人妻一区二区三区| 久久精品无码国产专区怎么用| 亚洲影音先锋在线| 97精品国产| 色噜噜在线视频| 蜜桃久久久| 精品少妇人妻| 久久77| 裸体久久女人亚洲精品| 久久这里有精品| 国产性爱AV| 又黄又大又爽A片三年片| 一区二区三区四区| 2018天天干天天操| 色色91| 亚洲一级黄色| 欧美五十路| 国产成人三级片| 97A片在线观看播放| 9l视频自拍九色9l视频| 国产精品毛片AV| 欧美一区二区无码三区有限公司| 亚洲中文字幕人妻| 日本黑人乱偷人妻中文字幕| 超碰激情| 午夜福利国产| 国内自拍视频在线观看| 调教她的尿孔(H)| 亚洲男人天堂视频| 色综合久久88色综合天天| 亚洲AV导航| 极品少妇XXXX精品少妇| 自拍视频一区二区| 日本黑人乱偷人妻中文字幕| 精品久久久久久久久久| 在线免费观看日韩| 日本无码免费| 亚洲欧洲强奸乱伦| 又爽又长又硬又大又粗又快| 亚洲成人精品在线| 欧美成人一区二免费视频苍井空| 亚洲成av人片在线观看| 国产一区二区无码| 精品一区二区三区四区| 国产精品久久久久久中文字| 亚洲精品无码AV中文永久在线| 久久噜噜噜| 亚洲一级毛片| 久久AV导航| 99精品免费久久久久久久久日本| 欧美亚洲一区二区三区| 一区二区三区性爱视频| 在线观看AV免费| 亚洲自拍中文字幕| 99国产在线| 欧美日韩国产精品一区二区| 无码视频一区二区| 懂色AV一区二区夜夜嗨| 九九色色| 五月婷婷六月丁香| 日韩精品无码一区二区| 欧美午夜三级| 亚洲 欧美 综合| 免费的黄色网址| 性免费视频| 亚洲巨爆乳一区二区三区四季网| 亚洲三级片在线观看| 免费操逼网站| 99久久人妻精品免费二区| 91插插插影库永久免费| 天天精品| 久久久久无码精品国产91福利| 欧美精品一区二区三区| 国产成人在线播放| 日韩性爱视频网站免费观看| 中文字幕永久在线| 日本在线观看不卡| 各种姿势玩小处雌女txt视频| 无码一区二区三区中文字幕| 国产无套内精一级毛片| 天堂资源在线| 朝桐光一区二区三区| 亚洲欧洲综合| 国产精品久久久久久久久久久新郎| 精品一区二区三区四区| 天天插天天干| 樱花动漫入口| 欧美天堂一区| 国产视频资源| 四季AV无码专区AV| AV网址在线| 国产熟女乱伦| 亚洲毛片| 国产无码AV| 香蕉久久久| 国产性爱一级| 制服丝袜在线视频| 青娱乐国产视频| 一区二区中文字幕在线观看| 中国娇小与黑人巨大交| 天天色色| 色婷婷一区二区| 凹凸视频国产日韩欧美小说| 久久国产精品久久| 精品导航| 亚洲AV永久纯肉无码精品动漫| 亚洲免费人妻视频| 国产精品久久久久久白浆| 黄色18禁| 色翁荡熄又大又硬又粗又视频| 久久瑟瑟| 亚洲精品视频免费在线观看| 国产高清av| 岛国无码AV| 日韩性爱一区二区三区| 懂色AV色窝窝无码久久免费| 国产aⅴ| 天堂一区二区| 亚洲一区二区三区四区的| 亚洲AV大香蕉| 最近中文字幕第一页| 日逼视频免费| 爆乳丰满熟妇一区二区三区爆乳 | 黄片影院| 日韩精品无码一区二区三区久久久| 国产免费一区二区三区免费视频| 日韩无码网址| 亚洲aV乱伦| 性色无码| 337p粉嫩大胆色噜噜噜| 国产强奸视频在线观看| 国产高清免费在线| 自拍偷拍一区| 91久久精品| 亚洲一区二区免费| 国产精品亚洲天堂| 国产在线无码视频| 蜜桃久久久| 亚洲熟妇无码AV| 天堂色av| 精品久久99| 国产深夜福利| 国产免费AV片在线无码免费看| 国产在线精品拍揄自揄免费| 亚洲AV无码片一区二区三区| 性欧美另类| 黄网站入口| 国产精品人妻无码久久久郑州天气网| 国产综合自拍| 亚洲三级片网站| 日韩AV天堂| 日韩午夜福利片| 国产高潮白浆无码| av资源网址| 色播AV| 日韩免费网站| 黄色三级在线视频| 99r在线视频| 一级国产精品| 中文在线最新版天堂| 欧美熟女性爱| 国产免费自拍视频| 国产无码www| 天天干天天日天天操| 欧美交换配乱吟粗大25P| www精品| 成人免费在线视频| 三个寡妇干柴烈火| 操逼强推视频| 国产视频一区二区三区四区| 国产精品主播一区二区主播| 天天综合网~永久入口红桃| av水蜜桃| 亚洲大片在线观看| 乱子轮熟睡1区| 九九国产视频| 你懂的电影| 人人摸免费视| 国产视频一区二区在线播放| 日本黄色三级片| 一级特黄AAAAA片免费| 人人摸人人上人人| 日韩在线| 99精品免费久久久久久久久| av无码aV天天aV天天爽| 精品视频99| 九九热在线视频| 日韩欧美中文| 中文字幕网址在线| a级黄毛片| 中文字幕无码在线观看| 动漫精品一区二区| 亚洲日本精品| 久久人妻无码一区二区美国快递| 三上悠亚中文字幕| 日本乱伦精品| 99精品人人A片免费看| 精品无码人妻一区二区| 色臀淫乱拳交| 五月丁香激情综合| 婷婷色视频| 国产乱伦免费视频| 毛片无码一区二区三区A片视频| 中文字幕人妻一区二区| 朝桐光一区二区三区| 五月丁香在线视频| 伊人久久五月天| AV无码一区二区三区| 线观看免费完整aaa| 亚洲乱强伦乂 乄乄乄乄9| 精品黄色片| 欧美91视频| 日韩三级一区二区| 久久99精品国产麻豆婷婷洗澡| 久久精品99国产| 亚洲AV电影免费在线观看| 日本一区不卡| 伊人久久艹| 亚洲成人精品| 人人妻超碰| 黄色av网站免费看| 思思热热思思| 亚洲男人的天堂av| 中国老熟女重囗味HDXX| 亚洲一区二区AV| 色翁荡熄又大又硬又粗又视频| 亚洲高清无码在线| 欧美少妇激情| 国产一区AV在线| 亚洲精品不卡| 精品久久久久高清无码| 91麻豆国产| 成人美女| 91午夜福利电影| 片库| 久久成人毛片| 国产精品一二| 黑人AV一区| 日韩av在线免费观看| 8090.aa| 欧美成人一区三区无码乱码A片| 欧美三级免费观看| 无码在线免费| 国产精品交换| 少妇导航福利| 日韩免费一区| 97人人爽人人爽人人爽人人爽| 凹凸视频极品人妻熟女| 熟女91| 一级黄片在线| 日本大学生三级三少妇| 亚洲二区在线| 尤物在线| 久久久久无码精品国产电影| 日韩无码成人| 欧美黄片在线| 国产精品第1页| 91无码人妻精品一区二区三区四| 欧美激情一区| 久久77| 少妇视频一区| 国产精品综合视频| 亚洲午夜精品一区二区三区电影院| 国模精品一区二区三区| 少妇Av导航| 天天草av| 日本伊人网| 国产欧美日韩一区二区三区| 天天色天天插| 亚洲无码一二三| 性欧美另类| 熟女91| 国产精品亚洲欧美在线播放 | 亚洲精品综合| 国产视频一区二区三区四区| 暗交老女一区二区三区| 日韩黄色网站| 国产成人精品一区二区| 亚洲91色图| 国产又大又粗视频| 青青草原亚洲| 毛片国产| 欧美激情精品久久久久久免费| 国产操比一区| 小俊┅┅快┅┅用力啊| 免费91视频| 视频一区二区在线| 91精品国产综合久久久久久漫画| 日本精品三区| 国产精品xx| 国产视频精品在亚洲| 极品人妻videosss人妻| 婷婷色视频| 中文字幕成人AV| 99re视频| 中文字幕视频在线| 国产污视频在线观看| 无码国产伦一区二区三区视频| 国产第一页屁屁影院| 国产精品二| 视频在线一区二区| 国产精品自在线拍| 爆乳一区二区| 黄色无码视频| japanese老熟妇乱子伦视频 | 欧美日韩系列| 国产精品自在线拍| 亚洲特级黄片| 久久久午夜精品福利内容| 男人的天堂无码| 丰满少妇被猛烈进入| 我和亲妺妺乱的性视频| 欧美极品少妇×XXXBBB| 国产成人精品一区二区三区| 夜夜操夜夜爽| 国产精品第1页| 日本黑人乱偷人妻中文字幕| jlzzjlzz国产精品久久 | 我要看黄色九九片| 亚洲一区中文字幕| 哪里可以看毛片| 中文无码熟妇人妻AV在线| 亚洲一级黄色电影| 色视频在线观看| a黄色片| 亚洲男人的天堂av| 亚洲精品变态另类虐交| 上国产操逼网| 欧美一区日韩一区| 人妻夜夜爽天天爽| 亚洲无码内射| 性无码专区| 国产麻豆一区二区三区| 日日躁夜夜躁狠狠躁aⅴ蜜 | 国产日韩欧美一区二区东京热| 久久久久99精品成人片直播| 久久午夜视频| 欧美熟妇另类久久久久久牛牛影视| 我与岳干柴烈火| 91Av导航| 国产精成人品日日拍夜夜免费| 伊人久久精品| AAA在线观看| aV男人的天堂在线| 2018天天干天天操| 无码人妻一区二区三区线| 国产真人真事一级A片| 99人妻碰碰碰久久久久禁片| 蜜乳av牢记| 亚洲自拍偷拍视频| 国产成人一区二区三区A片免费| 夜夜骚av| 日日躁久久躁熟妇高潮喷| 91天堂在线| 日本精品久久| 日本午夜视频| 最新无码视频| 久久久影院| 九九热免费| 午夜黄色一级片| 毛片无码一区二区三区A片视频| 一区二区AV| 国产一级片网站| 国产精品免费在线| 秋霞av无码| 中国老熟女重囗味HDXX| 99视频在线| 国产伦精品一级二级三级妓女| 成年免费视频黄网站在线观看 | 精品熟女| 免费高清无码| 欧美日本在线| 久久久久久一区| 视频一区欧美| 亚洲午夜精品一区二区三区电影院| 国产黄色片视频| 韩日无码视频| 黄色操日本| 成人三级片网站| 亚洲人成影院在线无码按摩店| 亚洲欧美一区二区三区不卡 | 欧美中文字幕在线观看| 欧洲AV无码精品色午夜飞机馆| 91麻豆精品国产91久久久久久| 国产熟女一区| 精品亚洲一区二区三区| 无码在线不卡| 亚洲自拍小说| 国产欧美日韩在线观看| 99视频免费看| 国产又粗又猛又黄| 狠狠人妻久久久久久综合蜜桃| 黄色在线网站| 岛国大片在线观看| 国产免费无码av| 先锋AV资源| 国产导航福利网| 日韩成人网站| 亚洲精品久久无码77777| 国产精品久久久久久久久免费看| 精品在线不卡| 午夜福利视频导航| 亚洲一级毛片| 中出无码| 成人网在线观看| 91九色首页| 亚洲毛片| 久久久久久久久久一级| 中文在线一区| 国产精品无码一区二区aⅴ污美国| 三级片免费网址| 免费无码电影| 国产精品一二三产区m553小说| аⅴ资源中文在线天堂| 天天夜夜操| 最新国产无码| 国产免费AV片在线无码免费看| 欧美日韩一区二区三区四区五区 | www毛片| 国产性爱一区二区三区| 精品一区二区AV国产精品探花| 精品国产网站| 91狠狠| AV牛牛| 日韩污视频| 午夜福利一区二区三区| 亚洲精品综合| 国产二区无码| 国产精品无码一区二区在线观软件| 精品久久BBBBB精品人妻 | 亚洲国产精品久久久| 人人操人人之| 最新中文无码| 一区二区视频| 精品无码一级毛片免费| 99久久久无码国产精品性九价| 国产一区二| 国产女人拳交视频| 天天夜夜操| 最近免费中文字幕MV在线视频3| 免费人妻性爱| 午夜视频免费在线观看| 99精品在线观看| 亚洲成人一区二区三区| 狠狠做六月爱婷婷综合aⅴ| 日日夜夜视频| 精品国产乱码久久久久久影片| 午夜成人在线| 色欲AV无码精品一区二区久久| 思思热视频在线观看| 麻豆射区| 青青国产精品| 国产午夜小视频| 伊人久久免费视频| 国产亚洲精品久久久久久牛牛| 色天堂视频| 欧美三日本三级三级在线播放| 中文字幕操逼视频| 欧美人妻曰韩精品| A片高潮狂喷白浆| AV在线毛片| 91精品国产高清91久久久久久| 免费一级a毛片免费观看欧美大片| 国产精品无码一区| 男人的天堂无码| 一区二区亚洲视频| 久久狠狠干| 日韩精品在线观看免费| 色情乱伦av| 国产精品国精产品一二三| 日本巜侵犯人妻人伦| 无码在线观看一区| 91麻豆视频| 国产精品农村妇女AAAA| 日本色色网| 91亚洲国产| 亚洲二区在线| 日本无码免费| 天天草夜夜草| av大香蕉| 一级全黄少妇性色生活片| 午夜电影网| 亚洲视频一区| 四季AV无码专区AV| 无码一区亚洲| 97中文字幕在线观看| 国产熟妇久久777777| 高清无码免费| 日本无码专区| 日逼视频免费| 丰满人妻老熟妇伦人精品| 日本三级精品| 围产精品久久久久久久| 亚洲精品电影| 91最新视频| 久久久影院| 黄色操日本| 91成人国产| 国产性爱一区二区三区| 日本特黄视频| 无套内谢波多野结衣| 精品国产乱码久久久久久影片| 先锋影音AV资源网| 无码视频免费看| 爆乳熟妇一区二区三区霸乳照片| 无码人妻束缚av又粗又大| 精品国产一区二区三区久久久蜜月| 成人在线小视频| 九九九国产视频| 伊人色吧| 天堂8在线| 久久思思热| 91人妻中文字幕在线精品| 美国一级黄色录像| 波多野结衣在线观看一区二区| 一级黄色电影免费看| 成人网站在线免费观看| 亚洲美女高潮久久久| 成人淫荡在线资源| 国产v精品| 久久久人妻| 超碰男人的天堂| 婷婷综合五月天| 熟女少妇内射日韩亚洲| 最新中文字幕在线| 精品人伦一区二区三区牛牛视频| 超碰97资源| 中文字幕一区二区三区乱码在线| 亚洲AV第二区国产精品| 精品一区二区三区中文字幕| 超碰天天操| 国产高清成人久久| 岛国av一区二区三区| 凹凸AV导航大全精品| 91精品国产综合久久久久久漫画| 久久久久久精品一级毛片免费按摩| αⅴ天堂αⅴ| 国产色无码精品视频国产| 久久综合婷婷国产二区高清| 欧美伊人影院| 日韩在线免费视频| 亚洲 欧美 综合| 一区二区中文字幕在线观看| 人人操人人摸人人看| 被调教的少妇雅芳1一19| 天天欧美| 色婷婷丁香五月| 在线免费国产| 超碰100| 日韩精品中文字幕一区二区三区| 丰满熟妇大号BBWBBWBBW| 国产精品久久久久永久免费看| 国产二区AV| 亚洲AV鲁丝一区二区三区| 国产欧美一区二区精品97| 国产精品VIDEOSSEX久久发布| 欧美乱码精品一区二区三| 亚洲三级在线观看| 成人在线性爱免费视频| av色在线| 国产精品久久久99| 一区二区三区日韩欧美| 国产欧美日韩在线观看| 欧美视频在线一区| 91麻豆视频| 国产裸体美女视频| 无码在线免费| 老熟妻内射精品一区| 97国产精品| 午夜av免费看| 成人毛片网| 亚洲蜜桃视频久久久| 女同一区二区| 熟女VS乱伦| 日屁视频| 一区二区自拍偷拍| 亚洲精品小视频| 国产中文字幕免费| 亚洲成a人片7777网站| 色综合图片| 91在线精品| 国产精品情侣呻吟对白视频| 国产成人久久| 99久久精品一区二区三区| 国产在线播放91| 中文字幕一区二区人妻电影 | 欧美三日本三级少妇三级在线播| 国产一级做a爰片久久毛片男| 无码人妻一区二区三区线| 国产成人在线播放| 精品国产99久久久久久| 躁躁躁日日躁| 亚洲欧洲无码AAA片在线观看| 成人激情在线| 超碰在线免费| 国产黄在线| 全部免费毛片免费播放| 蜜桃久久久| AV在线毛片| 亚洲欧美乱伦| 国产精品强奸乱伦| 国产精品18| 色噜噜噜| 999精品视频在线观看| 91无码人妻精品一区二区三区四| 久草资源在线| 99亚洲无码| 96精品无码一区二区动漫| 日本色色网| 污网站在线免费观看| 又粗又长又大手机福利视频| 高潮喷水波多野结衣在线观看| 国产精品一区二区三区免费| 人人爱人人摸人人要| 亚洲一区二区免费视频| 欧洲另类类一二三四区| 凹凸国产熟女精品福利11| 成人激情在线| 一区二区三区在线| 超碰96在线| 国产精品久久久人妻无码| 91人妻丰满熟妇Aⅴ无码| 国产精品1| 国产精选视频在线观看| 精品导航| 欧美日韩中文字幕| 高清无码小电影| 国产精品一二| 国产91丝袜在线播放九色| 小黄片高清| 国产A视频| 无码人妻熟妇av又粗又大| 无码成人精品区一级毛片| 国产无套白浆一区二区三区| 国产中文在线视频| 91丨九色丨熟女高潮| 激情欧美一区二区三区中文字幕| 久久久国产精品免费| 精品少妇爆乳无码av无码专区| 亚洲AV第二区国产精品| 成人色视频| 久草福利视频| 91精品国产91久无码网站| 欧美操逼网址| 琪琪在线视频| 黄网站在线观看| 久久99精品国产| jazzjazz国产精品麻豆| 小明看国产| 国产韩国日本欧美的品牌suv | 久久伊人免费| 亚洲精品免费视频| 国产午夜精品一区二区| 久久综合伊人| 亚洲另类激情综合偷自拍图| 中国黄片免费看| 日日干夜夜操| 超碰97资源| 国产免费操逼视频| 亚洲精品一区二区三区四区五区六| 国产强奸乱伦AⅤ| 精品视频在线观看99| 欧美精品一区二区在线| 日本久久无码高潮喷水电影| 欧美激情国产日韩精品一区18| A片软件| 亚洲精品在线视频| 九九综合久久| 亚洲AV精色AV日韩大尺度| 三级片网站在线观看| 日本黄色小视频| 少妇无码| 99精品国产91久久久久久无码 | 国产3级片| 中文字幕99| 亚洲一区二区在线播放| 综合网天天| 一级a一级a爰片免费啪啪女女| 天天搡天天狠天干天啪啪| 国产精品久久久一区二区| 一男一女一级一片| 黄片av免费观看| 人人摸人人干人人操| 亚洲综合无码一区二区毛片| a国产视频| 日本久久精品| 国产亚洲欧美一区二区| 国产真实乱了老女人视频| 黄色片视频网站| 国产精品女同| 免费看黄在线观看| 日韩三级免费| 丁香五月激情网| 国产女人18毛片水真多1| 欧美a在线| 久久久一级| 噜噜射尤物| 91国内自产精华天堂| AV在线免费观看网站| A级片免费看| 国产激情久久| 日本三级少妇三级99夜在线观看| 99久久精品免费看国产免费粉嫩 | 国产女人18毛片水真多| 91精品国产色综合久久不卡粉嫩 | 国产精品无码一区| 日本一区二区三区| 色婷婷又粗又长| 色欲色香天天天综合网WWW| 99精品免费久久久久久久久日本| 国产成人一区二区三区| 久久久久久久久久久国产| 一区高清无码| 国产精品视频免费观看| AV在线导航| 色欲无码精品一区二区三区99满 | 国产91精品在线| 国产电影一区二区| 国产一级无码| 人操人人视频| 午夜精品视频| 高清一区无码| 日韩三级片播放| 熟女作爱一区二区视频| 国产一级毛片av| 欧美日韩综合一区| 日本不卡在线| 国产chinasex对白videos麻豆| 国产夫妻av| 久久96国产精品久久99软件| 亚洲综合社区| 欧洲操逼视频| 一级片免费在线观看| 一区二区国产精品| 国产精品Av久久| 丝袜灬啊灬快灬高潮了AV| 亚洲AV色香蕉一区二区三区老师| 伊人婷婷| 日本三级网站| 日本少妇高潮日出水了| 熟妇免费视频| 91视频导航| 国产黄片在线免费看| 人人干人人摸人人操| 性一级视频| 欧美日韩中文| 久久窝窝| 91精品人妻一区二区三区| 免费观看黄| 一级A片黄女人高潮网站| 你懂的电影| 自拍偷在线精品自拍偷无码专区| 国产三级无码| 69av视频| 国产激情无码AV毛片久久| 欧美精品久久久久久| 五月丁香在线观看| 精品日韩| 久久18| 又硬又爽又长又粗又大毛片 | 久久午夜福利| 日韩一级无码| 中文字幕无码在线观看视频| 中文字幕在线观看一区二区三区 | 日韩欧美久久久| 三级无码| 人禽杂交18禁网站免费| 久久成人麻豆午夜电影| 琪琪女色窝窝777777| 久久亚洲一区二区三区四区五区高| 黄片在线免费观看视频| 日韩精品网| 亚洲精品视频在线播放| jzzijzzij国产乱熟无码| 亚洲欧美天堂| 欧美碰碰| 一级二级毛片| 91熟女视频| 牛牛影视一区二区| 亚洲中文字幕无码一区精品| 天天夜夜操| 色乱av| 久久久网| 人人摸人人操| 久久天堂av| 91aaa| 开心久久婷婷综合中文字幕| 国产精品久久久99| 熟女91| 无码人妻在线| 97人人人操| 久久久91人妻无码| 嫩草在线视频| 国产精品福利在线| 国产毛片毛片毛片| 无码一区二区在线观看| 伊人色吧| 久久久婷婷| 成人妇女免费播放久久久| 成年人免费观看性爱视频 | 亚洲国产精品自拍| 香蕉国产2023| 91麻豆精品秘密入口| 色呦呦在线观看视频| 国产亚洲精| 波多野结衣无码欧美在线播放69| 成人精品网| 久一在线| 最新国产在线| 亚洲av色图| 中文字幕无码日韩专区免费| 国产家庭性爱乱伦| 国产激情综合| 久久丫不卡人妻内射中出| 国产精品美女久久久久AV爽| 无码三级视频| 国产精品久久久久久久久久大尺度| 亚洲AV不卡无码| 91sese| 国产一级视频| 一级性爱视频| 一级毛片无套内谢免费视频| 亚洲蜜桃| 苍井空电影|