亚洲精品?Ⅴ无码精品丝袜足-亚洲中文字幕在线网站-久久精品aⅴ无码中文字幕不卡-久久精品免费首页-国产高清欧美亚洲-少妇人妻精品毛片一区二区-久久国产精品亚洲艾草网-国产三级精品国产三级人妇在线-中文字幕日韩精品内射

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
国产一级a毛一a毛免费视频| 国产精品福利一区| 日本无码熟妇五十路视频| 男人资源站| 欧美日韩性爱在线| 91精品无码在线观看| 99国产精品久久久久99打野战| 国产黄片高清无码| 思思热在线视频精品| 国产伦精品一区二区三区妓国产 | 国产精品久久久久久久久晋中| 乱女乱妇熟女熟妇综合网网站| 久久熟妇五十路一区| 成人三级在线观看| 一本无色道高清码| 国产亚洲91| 波多野结无码中文在线| 在线日韩国产| 亚洲欧洲一区| 国产熟女乱伦| 亚洲无码三级片| AV在线无码| 亚洲综合无码| 国产黄色在线视频| 国产精品黄色| 日韩av在线免费观看| 肉大捧一进一出免费视频| 亚洲抽插| 日韩精品在线视频| 成人免费毛片视频| 国产妓女一级在线| 激情久久AV一区AV二区AV三区| 丝袜乱伦视频| 精品无码区| 精品视频导航| 亚洲欧美国产一区二区| 久久久久久影院| 久久五月天婷婷| 日日干天天干| 久久国产高清视频| 91丝袜一区二区| 婷婷色一二三区波多野结衣| 亚洲精品亚洲人成人网裸体艺术| 亚洲无码网址| 亚洲熟女性爱| 日本三级视频在线| 国产激情在线| 狠狠干av| av免费在线观看网站| 无码午夜视频| 日韩免费视频一区二区| 欧美色影院| 五月天婷婷在线播放| 北条麻妃视频在线观看| 日韩视频一区| 国产精品一级毛片在码A片| 成人电影一区| 一级毛片免费播放视频| 国产精品―色哟哟| 超碰国产在线| 欧美在线视频免费播放| 日韩亚洲一区二区| 国产精品久久精品| 午夜精品久久久久久| 国产AV一区二区三区| 久久性爱视频| 邻居少妇张开双腿让我爽一夜| 久久久亚洲一区二区三区| 黄片com| 无码人妻在线| 国产女人18毛片水真多1| 自拍偷拍专区| 一级外国欧美性爱黄色录像| 在线中文AV| 秋霞免费视频| 欧美地区一二三不播放| 麻豆一级片| 夜夜操天天干| 免费精品视频| 国产一级内射| 性色AV一区二区三区| 日韩三级中文字幕| 五月天婷婷丁香花| 亚洲啪啪综合| 国产香蕉视频| 中字幕视频在线永久在线观看免费| 高清无码成人片| 丁香五月综合| 精品无人区一区二区三区蜜桃小说 | 国产人妻无码一区二区三区不卡| 日本熟妇视频| 亚洲精品www| 成人三级片在线观看| 日本免费一区二区三区| 秋霞无码| 国内自拍第一页| 国产欧美一区二区精品97| 一级黄色网址| 无码AV电影| 国产av成人| 囯产精品久久| JDAV视频在线观看免费| 无码无卡| 欧美丝袜乱伦| 久久精品不卡| 亚欧洲精品视频| 又长又粗又爽美女高潮视频| 91精品91久久久中77777| 伊人久久久久久久久| 码人妻免费视频| 国产aaaa| 91成人无码看片在线观看网址| 一道本在线视频| 国产精品久久久久久一级毛片探花| 拍国产真实乱人偷精品| 性无码一区二区三区| 亚洲天堂av无码| 琪琪在线视频| 国产免费一级黄片| 国产欧美一区二区三区在线看蜜臂| 亚洲午夜无码AV毛片久久| 国产不卡在线观看| 亚洲精品久久无码77777| 给我免费观看片在线观看中国| 波多野吉衣一区二区| 青青草无码视频| 色欲影视综合网| 久久无码人妻| 成年人免费视频网站| 老女人做爰全过程免费的视频 | 丁香激情五月天| 欧美熟妇乱伦| 国产欧美在线| 欧美一区永久视频免费观看| 亚洲成人无码网站| 91在线视频免费的| 精品久久久久久久久久久下载| 午夜成人app| 奶乳咪咪人无码AV网址| 亚洲国产精品无码久久久秋霞1| 综合成人| 国产女人水真多18毛片18精品视频| 久色91| 国产裸体免费无遮挡| 亚洲乱码一区二区三区| 日韩无码一区二区| 国产亚洲91| 中文字幕在线视频网站| 日韩中文字幕一区二区| 成人AV一区二区三区无码金桔| 狠狠爱69AV| 亚洲网站视频| 熟女乱伦视频| 三级网站在线| 亚洲av一级| 亚洲精彩视频在线观看| FREEZEFRAME丰满少妇| 国产精品一二三| 亚洲最大激情网| 亚洲国产成人va在线观看天堂| 中文字幕在线无码| A一级黄色片| 污网站在线观看| 99久久久无码国产精品怎么下载| 偷拍自拍网| 久久久亚洲一区二区三区四区五区 | 91久久免费视频| www.久久AV| 国产精彩视频| 人妻在线视频播放| Av人体片| 妞干网视频| 久久精品99北条麻妃| 91久久久久久久久| 国产精品久久久久无码AV绿帽男| 亚洲熟女乱色一区二区三区久久久| 毛片黄色| 国产一级黄色大片| 福利120无码| av大片在线观看| 高清无码操逼视频www| 婷婷中文字幕| 人体人人摸人人插| 国产中文字幕在线| 午夜色色视频| 亚洲欧洲一区| 二区三区无码| 中文字幕日韩一区二区| 我与岳干柴烈火| 久久蜜桃AV一区二区天堂| 国产精品自拍一区| 欧美日韩免费| 久草视频在线播放| 国产手机在线视频| 女同啪啪免费网站www| 一区二区人妻| 美女视频一区二区三区| 婷婷在线观看视频| 免费无码一级A片大黄在线观看| 激情影院内射美女| 亚洲精品无码AV中文永久在线| 国产不卡在线| 色橹橹欧美在线观看视频高清| 91蜜桃婷婷狠狠久久综合9色| 99热精品在线观看| 中文字幕操逼视频| 精品久久国产| 精品在线一区| 成人区精品一区二区| 亚洲精品一区二区三区四区五区六| 日本A片在线观看| 狠狠干天天日| 国产精品视频无码| 欧美黑人少妇高潮喷水| 欧美高清视频| 黄色网址免费在线观看| 欧美一级特黄A片免费看视频小说| 久久99com| 欧美性爱一级视频| 一级黄色无码| 26AU欧美| 91久久精品国产91性色tv| 国产精品视频网站| 欧美日韩一区在线| 大美女禁视频www| 在线观看91| 成人日本A片无码| 在线看91| 成人免费毛片足控| 激情成人综合网| 国产性爱乱伦网站| 婷婷五月综合在线| 女人18片毛片90分钟| 欧美三级片免费观看| 久久久国产一区二区三区| 91精品免费视频| 日本三级电影中文字幕| 综合色网址| 欧美熟妇在线观看| 亚洲精品白浆高清久久久久久| 国产h片在线观看| 亚洲精品乱码久久久久久久| 免费看一级片| 成人性生交大片免费看4| 免费不卡av| 欧美熟妇A片在线观看麻豆| 欧美老熟妇又粗又大| 亚洲视频在线播放| 中文字幕日产A片在线看| 日韩一区二区在线| 日韩成人中文字幕| 久久AV秘一区二区三区| 亚洲AV综合色区无码| 无码三级| 大地资源二中文在线观看官网| 亚洲AV不卡无码| 少妇高潮喷水久久久久久久久| 国产成人精品亚洲男人的天堂| 久久精品综合视频| 日日朝屄| 欧美国产黄片| 亚洲av最新在线网址| 无码人妻一区二区三区免水牛视频 | 免费毛片在线| 久久精品嫩草影院| 国产性爱片| 亚洲视频一区二区三区| 欧美在线观看一区二区| 欧美三级免费观看| 玖玖资源在线观看| 午夜不卡视频| 久99综合婷婷| 欧美无砖砖区免费| 一级国产| 草视频黄在线| 日韩啪啪啪网站| 中文字幕在线观看一区二区三区 | 插插插毛片黄片免费视频导航| 亚洲精品无码久久久苍井空| 黄色无码| 日韩欧美一区二区在线观看| 一区二区三区在线视频观看| 日韩人妻在线视频| 国产精品久久久久久妇女6080| 亚洲操逼网| 91熟妇| 一色一伦一区二区三区| 台湾超碰| 国产熟女真实乱精品91| 日日夜夜视频| 亚洲精品在线视频| 激情淫荡视频| 色婷婷一区二区| 亚洲a视频| 久久人妻少妇嫩草av| 91亚色在线观看| 91精品国产色综合久久不卡蜜臀| 人妻超碰| 国产熟女一区二区三区浪潮97| 日韩一区二区精品| 免费视频成人| 91高清无码视频| 中文字幕在线免费视频| 国产色在线| 欧美成人社区| 亚洲av成人精品一区二区三区| 欧美日韩一二三| 日韩二三区| 欧洲AV无码精品色午夜飞机馆| 成人免费观看网站| wwwxxx国产| 嫩草影院一区二区| 国产成人精品三级麻豆| 国产乱国产乱老熟300部| 国产AAA毛片| 色色视频网站| 日本老熟妇视频| 天天躁日日躁狠狠躁av无码老牛| 日韩欧美亚洲| 极品白丝 国产| 奇米四色影视| 亚洲自拍三区| 亚洲xx网| 精品成人一区二区| 黄色国产| 国产又黄又粗又爽| 日本a免费| 人妻日韩中文字幕| 国产精品一二| 成人免费无遮挡无码黄漫视频 | 亚洲熟妇无码AV无码| 天天精品| 黄网站入口| 下载日韩黄片| 亚洲无码影院| 中文字幕精品人妻| 黄片免费下载| 国产日韩视频在线观看| 日韩无码视屏| 国产精品久久久久野外| 欧美伦妇AAAAAA片| 国产喷白浆一区二区三区| 强奸乱伦视频第二页| 乱伦熟妇| 香蕉久久夜色精品国产更新时间| 伦乱视频| 亚洲资源网| 91麻豆精品视频| 九色人妻| 国产精品久久久久久久久久九秃| 精品久久久久久久人人人人传媒| 日韩 精品 无码 系列 另类| 国产逼操| 91久久国产| 亚洲熟女乱综合一区二区| 潘金莲一级特黄大片| 高清无码在线看| 欧美日韩俄乌国产男女操逼逼视频| 成人网站在线免费观看| 风间由美一区二区| 天堂中文字幕在线| 久久黄色大片| 日韩裸体视频| 欧美日韩爱爱| 国产精品久久精品| 亚洲三级片在线| 国产黄色片在线观看| 精品999久久久一级毛片| 国产一区二区免费| 91av在线播放| 国产精品麻豆| 久久综合一区| 色妞WW精品视频7777| 欧美一级成人| 日本三级影院| 黄色国产| 亚洲AV无码乱码精品护士岛国| 人人干人人爽| 久久久久国产精品视频| 国产精品一区二区黑人巨大| 亚洲免费在线| 欧美国产一区二区三区激情无套| 岛国视频一区在线| 日韩欧美在线不卡| 国产免费AV片在线无码免费看| 日韩欧美久久久| 天肏AV| 一本久久精品久久综合桃色| 高清无码一区二区三区| 亚洲第一影院| 婷婷色一二三区波多野结衣| 苍井空无码一区二区三区| 精产国品一二三区| 中文字幕精品无码| 一级日韩| 久久精品熟妇丰满人妻99| 亚洲无码视频一区| 久久久无码电影| 国产女人18毛片水真多1KT∧| 亚洲永久无码7777kkk| 日韩人妻系列| 亚洲精品久| 精品久久久久久久久久久久| 思思热在线观看视频| 爱看男人视频午夜日韩| 亚洲无码免费网站| 黄色无码在线| 女同啪啪免费网站www| 亚洲精品系列| 日韩天天搞| 久久久国产无码精品| 国产一页| 色鬼网站| 99人人操| 香蕉在线影院| 久久亚洲网站| 国产午夜一区| 26uuu欧美| 国产成人97精品免费看片| 一道本无码一区| 国产伦精品一区二区三区二区| 欧洲无乱码一二三区| 国产精品观看| 久久久久久亚洲综合影院红桃| 日本免费高清| 免费h片| 亚洲一区二区三区四区的 | 欧美狠狠干| 日本在线观看| 五月天婷婷激情| 日本无码高清| 三级片在线观看网站| 一区二区三区四区无码| 亚洲黄色一区二区| 久久久久国色AV免费观看麻豆| 亚洲欧美激情小说另类| 黄色一级视屏| 国产女主播在线| A级a做爰片成人毛片入口| 日本污网站| 欧美操逼片| 一级做a爰片久久毛片无码电影 | 久久久婷婷| 秋霞视频在线观看| 国产精品久久久久久久久久久新郎 | 久久岛国| 中文字幕人妻AV| 久久精品国产亚| 欧美天堂在线观看| 亚洲A级片| 亚洲成人自拍| 国产永久精品| A之v在线| 国产精品久久久久久久久免费桃花| 久久精品国产亚洲AV高清色欲| 九九热国产| 九色人妻| 香蕉福利视频| 国产免费看黄| 亚洲精品一区二三区不卡| 欧美日韩精品一区二区三区| 欧美怡春院| 国产精品99精品久久免费| 天天操夜夜爽| 日韩欧美一区二区三区| 岛国激情一区二区| 天天射影院| 超碰98| 亚洲精品乱码久久久久久蜜桃91| 日日干夜夜操| 黄片在线免费播放| 国产精品国产三级国产普通话蜜臀| 强奸乱伦首页av| 中文字幕在线视频网站| 欧美操操操| 欧美91| 久久精品国产亚洲AV麻豆图片| 国产精品久久一区二区三区| 日韩无码视屏| 国产白浆视频| 人妻专区| 国产主播99| 亚洲性爱网站| 熟女乱一区二区三区四区| 人妻体内射精一区二区三区| 韩国免费一级a一片在线播放| 在线不卡av| 在线视频福利| 亚洲人妻中文字幕| 91久久人人操人人爱人人摸| 欧–美–性–交–黄–片| 日本一本视频| 少妇人妻偷人精品无码视频新浪| 国产女人18毛片水真多1KT∧| 天天操天天插天天干| 日本高清视频在线观看| 久久精品国产亚洲AV无码偷| 免费毛片一区二区三区久久久| 制服丝袜在线播放| 人人插人人爱| 亚洲精品视频免费在线观看| 中文字幕三级片| 高清无码不卡视频| 日韩三级免费观看| 日韩精品极品视频在线观看免费| 美女掰穴| 精品国产乱码久久久久电车痴汉久| 夜夜操夜夜操| 无码人妻一区| 国产自慰网站| 人人操人人爱人人色| 精品乱子伦一区二区三区| 久久九九性免费视频| 成人免费网址| 欧美精品午夜| 四季AV无码专区AV| 亚洲国产综合在线| 四虎少妇做爰免费视频网站四| 日韩精品专区| 九九精品久久| 一区二线视频| 国产伦精品一区二区三区照片| 亚洲午夜福利精品国产字幕制服| 亚洲无遮挡| 五月综合在线| 欧美黄色小视频| 色色天堂| 日本韩国啪啪视频| 午夜福利视频一区| 国产黄色在线视频| 亚洲伦理一区二区| www.人妻| 国产精品国产精品国产专区不卡 | 中国无码区| 午夜高清无码| 久久久久99人妻一区二区三区| 麻豆精品无码国产在线| 99久久99久久精品国产片果冻 | 久久久久久久久影院| 国产精品一区在线| 大香蕉大香蕉一级黄色片| 国产精品v| 国产欧美精品| 91蜜桃网| 成人日本A片无码| 97资源超碰| 美女十八禁网站| 青青草精品视频| 亚洲自拍偷拍一区二区三区| 久在线视频| 91久久免费视频| 激情偷乱人成视频在线观看| 亚洲精品无码成人片在线观看| 色香蕉av| 成人黄色免费看| 色欲无码精品一区二区三区99满| 中文一级片| 午夜精品福利一区二区三区蜜桃| 日日干日日射| 欧美午夜激情| 97国产精品| 亚洲国产欧美日韩在线观看第一区| 国产精品偷窥探花在线| 欧洲精品无码一区二区三区在线| 亚洲一区在线播放| 欧美日韩精品一区| 麻豆精品一区二区三区| 中文字幕一区三区| 国产色图乱伦| 九九偷拍视频| 亚洲精品白浆高清久久久久久| 国产伦精品一区二区三区妓女| 一级内射| 伊人久久精品| 日韩一区无码| 国产日韩亚洲欧美| 国产精品视频无码| 影音先锋乱伦强奸| 亚洲无码短视频| 国内精品国产三级国产在线专| 国产操片| 国产伦精品一区二区三区妓国产| 天天操夜夜操免费视频| 人妻免费视频| 亚洲一级AV无码毛片| 国产真实伦在线观看视频第1集| 91久久精品一区二区| 国产精品久久久久久久久无码ⅴa| 91国内揄拍国内精品对白 | 女人AV在线| 成人在线免费观看av| 豪妇荡乳1一5潘金莲| 亚洲欧洲一区| AV无码专区亚洲AV毛片不卡| 最新国产精品视频| 黄色免费AV| 欧美电影一区二区| 无码人妻束缚av又粗又大 | 超碰人人网| 国产伦精品一区二区三区照片 | 国产在线拍揄自揄拍无码| 人人操免费| 丰满岳跪趴高撅肥臀尤物在线观看| 久久久精品人妻| 乱伦熟妇| 久久久久久影院| 国产三级片网址| 操熟女视频| 一级内射片在线网站观看| 黄色网址免费| av自拍偷拍| 爱爱视频网址| 天天操狠狠干| 精品自拍AV| 视频一区二区无码| 96国产精品久久久久aⅴ四区| 国产精品色悠悠| 人人操人人搞97| 免费看成人毛片| 国产淑女操逼| 热久久91| 国产一级a| 秋霞三级伦电影| 日韩专区中文字幕| 一本一道久久综合狠狠躁牛牛影视| 午夜国产视频| 久热国产精品视频| 精品黄色片| 日本理伦片午夜理伦片| 国产精品一线| 免费人成视频在线| 91在线色| 国产精品一区二区三区不卡| 爱爱综合| 亚洲国产精品毛片AV不卡下载| 国产精品黄色| 国产内射一区| 天天日夜夜| 日韩在线免费观看视频| 97在线观看| 午夜视频网站在线观看| 日韩视频精品| 日韩无码成人| 亚洲无码网址| 国产精品激情偷乱一区二区∴| 日韩免费在线视频| 欧美操逼精品| 超碰免费人妻| 黄网站入口| 高清不卡一区二区| 欧美视频精品| 免费一级A片| 国产女人18毛片水真多14| 久久99免费视频| 久久露脸国语精品国产91| 国产性爱网| 久久亚洲网站| 无码电影院| 久久久久久久久久久久久久免费看| 亚欧专区| 国产精品一区二区AV白丝下载| 久久激情综合| 中文写幕一区二区三区免费观成熟| 日韩黄色无码| 精品九九| 婷婷色导航| 中文无码免费视频| 人人操99| 黄色一级无码| 天天看天天操| 色视频一区二区三区| 夜夜躁狠狠躁日日躁| 日韩黄色精品| 国产激情在线| 欧美一级在线| 久久午夜精品| 国产麻豆精品| 黄色性爱网| 大香蕉欧美| 永久精品| 日本黄色免费看| 亚洲天堂无码一区| 99精品在线观看| 国精品伦一区一区三区有限公司| 国内乱伦视频| 亚洲自拍偷拍一区二区三区| a视频在线| av成人导航| 性生交大片免费看无遮挡网站| 香蕉久久精品| 无码一区二区在线观看 | 在线观看色| 人妻系列在线| 国产91在线播放| 天天操天天日天天爽| 校园春色亚洲无码| 亚欧AV| 国产人妻777人伦精品HD| 国产黄片在线免费观看| 久久精品久久久久久久| 国产一级做a爱片久久毛片A| 精品av| 亚洲Av无码午夜国产精品色软件| 天天日天天搞| 欧美人与性动交α欧美精品| 国产精品久久久久久久久久久久| 亚洲电影在线| 天天干天天干天天干天天 | 成人免费在线视频| 国产色午夜婷婷一区二区三区| 狠狠人妻久久久久久综合蜜桃| 国产无码三级| 99精品免费观看| 懂色av蜜臀av粉嫩av分享吧| 人妻熟妇视频| 国产精品视频一| 日韩性爱无码| 一级毛片国产| 经典三级在线观看| 福利久久| 国产无码精品在线播放| 亚洲AV无码久久国产精品| 国产女同互慰在线观看| 精品成人| 青青国产精品视频| 中日韩无码视频| 国产欧美一区二区三区鸳鸯浴| 国产变态操逼视频| 中文字幕精品久久久久人妻红杏1| 综合激情五月天| 欧美日韩黄片| 久久综合一区| 日韩二区在线| 狠狠躁夜夜躁XXXXAAAA| 精品亚洲国产成人AV制服丝袜| 欧美性另类| 日本黄色高清视频| 五月天天天操| 国产电影精品一区| 日韩AV无码专区| 日韩视频第一页| 国产精品一区揄拍无码免费| www亚洲午夜人美精片V区| 91精品人妻人人做人碰人人爽| 最新国产视频| 污视频网站在线观看| 国产精品99在线观看| 亚洲精品无码AV中文永久在线| 午夜啪啪视频| 精品一级毛片| 国产精品色片| 亚洲精品v日韩精品| 噜噜噜噜人人澡夜夜天堂| 成人欧美一区二区三区黑人动态图 | 日韩欧美在线观看视频| 日日夜夜爽| 4388国产成人无码| 超碰在线国产| 久久性爱综合网| 黄aaaaaaaaaaaaaaaaaa色网站| 日本人妻丰满熟妇久久久久久| 国产精品久久久久久亚洲色| 躁躁躁日日躁2020麻豆| 国产三级视频| 欧美一区二区三区婷婷五月老人| 人人操人人| 国产青青草| 黄片下载软件| 日日视频| 玩弄白嫩少妇XXXXX性| 久久亚洲一区二区| 黄色一区二区三区四区| 国产伦精品一区二区三区二区| 91婷婷国产欧美一区二区| 欧美群妇大交群| 亚洲福利视频一区| 特级黄色网站| 超碰九九| 夜夜草影院| 国产伦精品一区二区三区妓女下载 | 欧美精品久久久久A片| 亚洲成人av在线观看| 一级片国产| 欧美精品少妇| 操逼无码免费视频| www99热| 综合久久亚洲| 久久人人网| 自拍视频第一页| 999久久久| 丰满白嫩大尺度裸体尤物免费视频| 亚洲国产精品成人va在线观看| 精品久久九九| 国产一区二区无码| 亚洲av网站| 日本国产欧美| 五月天丁香| 亚洲一区二区三区在线视频| 被体育老师抱着c到高潮| 日韩精品在线视频观看| 91小视频| 成年人性爱视频免费看| 午夜日韩无码| 手机在线精品视频| 三级片在线观看网站| 国产无码精品电影| 一级片黄片| 欧美一区二区三欧A片直播| 婷婷五月天丁香| 九色影院| 色婷婷香蕉| 久久精品国产亚洲AV超碰| 亚洲三级无码| av天堂资源在线观看| 99久久99久久免费精品不卡 | 在线观看av的网站| 九草在线视频| 亚洲视频免费观看| 日韩在线一区二区| 久久久久国产一区二区三区| 奇米影视第四色777| 久久另类TS人妖一区二区| 在线观看的黄网| 少妇人妻偷人精品无码视频新浪| 91人人妻人人做人人爽男同| 午夜成人在线| 一二区无码| 国产凹凸熟女一区二区三区| 大鸡巴操我视频| 色综合天天综合网国产成人网| 一区二区三区视频在线观看| 国产精品久久久久久久久久久久久四虎 | 日日躁夜夜躁狠狠躁aⅴ蜜| 精品无码三级在线观看视频| 熟女一区二区三区| 日本高清久久| 国产成人午夜| 躁躁躁日日躁网站| 日韩AV专区| 高清无码电影| 国产乱轮视频| 亚洲中文av| 一区二区三区黄片| 无码人妻一区二区三区在线| 免费一区视频| 熟妇人妻一区二区三区四区| 天天操天天日天天干| 国产一区二区视频在线| 国产午夜精品无码理伦片| 日本XXX护士18一19高潮| 亚洲精品国产| 国产v精品| 久久免费精品| 国产精品久久久久久久久久尿| 国产嫩草一区二区三区在线观看| 一级a一级a爱片免费视频| 可以看啪啪视频的网站| 日韩无码小电影| chinese偷拍一区二区三区| 无码资源在线| 国产欧美精品区一区二区三区| 久久久久逼| 中文字幕在线观看一区二区三区 | 小雪被体育老师抱到仓库| 伊人精品久久| 蜜桃AV丝袜一区二区三区| 亚洲精品v日韩精品| 欧美日韩中文字幕旡码免费视频| 婷婷综合色| 一级内射片在线网站观看| 毛茸茸性XXXX毛茸茸| 嫩草免费视频| 国产精品久久久久久久久| 伊人色综合久久久| 欧美18禁| 激情五月天在线| 欧美午夜理伦三级在线观看| 日日做a爰片久久毛片A片英语| 亚洲欧美乱伦| 岛国视频一区在线| 热久久久| 久久久精品人妻一区二区三区色秀| 亚洲视频久久| 夜夜草天天干| 午夜日韩| 超碰97在线操| 国产精品国产精品国产专区不卡 | 精品久久久久久久久久| 国产一伦一伦一伦| 亚洲理伦| 亚洲丰满少妇在线播放| 伊人影院亚洲| 日韩欧美在线播放| 欧美交换配乱吟粗大25P| 日韩一区欧美| 麻豆激情| 高清无码成人网站| 国产a区| 欧美一a一片一级一片| 日韩欧美一级大片| 在线视频一区二区三区| 亚洲一区免费| 久久精品福利视频| 无码在线观看一区| 国产精品无码一区二区三区,| 伊人成人电影| 91色综合| 午夜黄色影院| 日韩精品综合| 风流少妇精品导航| AV怡红院| 久久精品一区| 国产精品强奸乱伦| 丁香久久久| 久久精品一区二区三区四区| 亚洲精品一| 91久久人人操人人爱人人摸| 一级特黄大片色| 中文字幕无码在线| 亚洲人免费视频| 水蜜桃成人| 天天看av| AV电影在线免费观看| 精品黑料一区二区三区 | 中文在线一区| 日韩一区二区三区在线| 无码少妇一区二区三区| 国产熟女鲁鲁视频|