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

2022

2022

  • Record 49 of

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

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

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

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

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

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

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

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

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

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

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

    Title:Large aperture phase-coded diffractive lens for achromatic and 16° field-of-view imaging with high efficiency
    Author(s):Ma, Gu(1,2); Zheng, Peng-Lei(1,2); Hu, Zheng-Wen(1,2); Ma, Suo-Dong(1,2,3); Xu, Feng(1,2); Pu, Dong-Lin(1,2); Wang, Qin-Hua(1,2)
    Source: Chinese Physics B  Volume: 31  Issue: 7  DOI: 10.1088/1674-1056/ac560c  Published: July 1, 2022  
    Abstract:Diffractive lenses (DLs) can realize high-resolution imaging with light weight and compact size. Conventional DLs suffer large chromatic and off-axis aberrations, which significantly limits their practical applications. Although many achromatic methods have been proposed, most of them are used for designing small aperture DLs, which have low diffraction efficiencies. In the designing of diffractive achromatic lenses, increasing the aperture and improving the diffraction efficiency have become two of the most important design issues. Here, a novel phase-coded diffractive lens (PCDL) for achromatic imaging with a large aperture and high efficiency is proposed and demonstrated experimentally, and it also possesses wide field-of-view (FOV) imaging at the same time. The phase distribution of the conventional phase-type diffractive lens (DL) is coded with a cubic function to expand both the working bandwidth and the FOV of conventional DL. The proposed phase-type DL is fabricated by using the laser direct writing of grey-scale patterns for a PCDL of a diameter of 10 mm, a focal length of 100 mm, and a cubic phase coding parameter of 30π. Experimental results show that the working bandwidth and the FOV of the PCDL respectively reach 50 nm and 16° with over 8% focusing efficiency, which are in significant contrast to the counterparts of conventional DL and in good agreement with the theoretical predictions. This work provides a novel way for implementing the achromatic, wide FOV, and high-efficiency imaging with large aperture DL. ? 2022 Chinese Physical Society and IOP Publishing Ltd.
    Accession Number: 20223012413010
天天操人人爽| 91看黄片| 欧美性爱一区二区| 九九热精品在线| 国产一区a| 国产精成人品日日拍夜夜免费| 99久久久精品| 日本久久一区| 亚洲国产精品久久久久久6q| 日本视频久久| 国产免费看黄| 无码人妻丰满熟妇精品区| 国产一区二区无码| 欧美88| 日本无码熟妇五十路视频| 日本一区不卡| 国产成人无码视频| 国产三级网站| 秋霞在线影院| 国产夜色| 另类小说综合网| 黄色性爱网| 国内精品一区二区| 国产逼操| 天天干天天干天天干天天| 潮喷在线| 九九九精品视频| 国产91在线播放| 国产激情无码AV毛片久久| 亚洲精品自拍| 孕妇孕交| 国产伦对白刺激精彩露脸| 青草无码视频在线观看| 国产精品嫩草影院8Vv8| 中文字幕人妻无码系列第三区| 婷婷视频在线| 一夜强开两女花苞| 日韩中文久久| 国产激情无码| 亚洲精品在线播放| 国产精品国产三级国产专播品爱网 | 91精品久久久久久久久| 日日夜夜精品| 天堂网中文在线| 日韩欧美中文字幕一区二区| 中文字幕av在线观看| 日日躁夜夜躁白天躁晚上| 四虎在线观看| 成人区人妻精品一| 一区手机福利视频导航| 精品人妻无码一区二区三区淑枝| 日韩欧美一区在线观看| 国产日批| 成人性爱免费视频| 三级三级久久三级久久18| 操之久久| 国产精品国产三级国产普通话蜜臀| 亚洲精选在线| 欧美亚洲天堂| 无码一区精品| 91精品无码少妇久久久久久网站 | 一区二区在线视频观看| 凸凹激情在线视频观看| 日韩毛片| www.精品| 久久久久一区二区三区| 极品白丝 国产| 国产精品三级片| 另类TS人妖一区二区三区| 91精品国产99久久久久久久| 制服丝袜综合| 精品女同一区二区三区| 亚洲无码免费| 麻豆射区| 欧美污视频| 高清无码不卡视频| 天天燥日日燥| 玩弄老年妇女过程| 国产女主播在线| 国产精品免费一区二区六十路| 日韩高清无码性爱| 精品人妻码一区二区三区红楼视频 | 亚洲色图乱伦av| 日韩在线一区二区| 日韩一二三四五区| 亚洲av网站| 蜜桃成人网站| 久久只有精品| 青青国产精品视频| 影音先锋女人av鲁色资源久久| 挺进同学熟妇的身体| 亚洲AV无码一区二区三区蜜柚| 国产A视频| 天天看天天操| 久久久久18| 天天色色| 成人做爰A片一区二区| 一级a免一级a做免费| 一区二区三区中文字幕在线观看| 黄色网址在线观看视频| 欧美性爱日韩高清| 无码在线电影| 无码在线不卡| 国产一级a毛一级a在线观看| 一区无码在线| 熟女乱亚洲| 欧美亚洲中文字幕| 欧洲操逼视频| 亚洲黄色在线观看视频| 欧美日韩中文字幕旡码免费视频| 日韩无码观看| 在线观看亚洲一区二区 | 亚洲 欧美 综合| 一级性视频| 欧美性爱视频一区| 久久久精品欧美一区二区白云视色| 久久加勒比| 欧美一区二区三区在线观看| 日韩视频在线观看| 欧美在线中文字幕| 91视频网| 伊人久操| 91国内自产精华天堂| 被男人疯狂揉吃奶胸视频| 日本黄色一级视频| 久久九九视频| 午夜日韩| 99视频99| 成人日本A片无码| 精品无人区无码乱码毛片国产| 欧美高清HD18日本| 手机在线精品视频| 中文字幕一二三四亚洲日韩| 极品少妇XXXX精品少妇| 亚洲AV不卡无码| 国产一区二区视频在线| 欧美一级成人| 大鸡巴网站| 黄片免费下载| 精品国产在热久久婷婷人妻AV综| 亚洲三级网| 久久天堂网| 中文字幕在线人妻| av影音先锋| 日韩AV专区| 少妇喷水在线观看| 露露AA一级黄色片| 韩国无码一区二区三区精品| 囯产精品久久久久| 国产精品内射婷婷一级二| 高清无码小视频| 国产色一区| 免费看成人毛片| 日韩一道本视频| 中文人妻| 久久久精品欧美一区二区白云视色| 国产精品天堂一区二区在线观看| 欧美爆操| 8050午夜| 爱爱综合| 秋霞成人午夜伦在线观看| 久久久久女人精品毛片九一| 亚洲精品一级| 亚洲Av无码午夜国产精品色软件| 精品人妻一区二区三区四| 国产成人无码不卡精品久久久| 在线无码视频| 成人欧美一区二区三区白人| 亚洲国产精品一区二区久久恐怖片| 综合国产| 欧美性受XXXX黑人XYX性爽| 国产成人三级| 久久国产精品一区二区| 国产特黄无码A片免费看爱欲| 国产v片| 亚洲一区AV| 中文人妻| 久一在线| 亚洲毛片一区二区三区| 日本成人电影一区二区| 福利120无码| 久久京东热| 国产一级A片久久久免费看快餐| 国产电影一区| 亚洲乱伦一区| 91麻豆精品91久久久久同性| 成人乱人乱一区二区三区| 国产精品交换| 男人午夜天堂| 天天精品| 国产亚洲色婷婷久久99精品91| 国产网红女主播精品视频| 欧美一级特黄A片免费看视频小说 色综合色综合网色综合 | 久久精品一日日躁夜夜躁| 国产乱国产乱老熟300部| 国产视频黄片| 在线免费国产| 少妇又紧又色又爽又刺激视频 | 婷婷97狠狠成人网站| AV电影在线免费观看| 99精品免费久久久久久久久日本| 日本一区二区三区| 在线观看无码电影| 国产无码精品在线播放| 最近免费中文字幕大全免费版视频| 中文无码免费视频| 日韩a在线| 免费AV片| 亚洲精品无码一区二区三天美 | 日韩动漫无码| 婷婷五月天成人| 91popny丨九色丨白丝| 超碰100| 日韩精品免费视频| 国产一区二区免费| 麻豆91在线| 国产精品久久久久久久久免费桃花 | 亚洲免费精品| 亚洲中文字幕一区二区| 美女航空毛片在线播放| 97色色网| 二区三区偷拍浴室洗澡视频| 欧美无线码| 人人操天天操| 亚洲欧美在线视频| 五月天综合在线| 天天视频色| 欧美精品二区| 性爱视频高清一区| 免费一级全黄少妇性色生活片| 四季AV无码专区AV| 一区二区亚洲| 超碰国产在线| 亚洲AV精品一区二区三区| 久久久久久久久久久99精品无码| 亚洲无码在线观看视频| 久久精品欧美一区二区三区不卡| 在线观看国产黄| 久久综合国产| 爱骑艺波多野结衣一区| 狠狠爱69AV| 午夜成人网站在线观看| 91人妻无码| 国产一级视频| 高清无码操逼视频www| 国产一区二区精品无码| 国产乱伦一区二区| 琪琪人妻一区| 无码精品人妻| 无码人妻一区二区三区在线 | 中文无码电影| 精品人妻少妇嫩草av| 在线高清免费不卡无码| 一级黄片免费视频| 深夜福利无码| 欧美另类精品| 欧美一区视频| 水蜜桃久久| 亚洲欧洲一区| JDAV视频在线观看免费| 日韩黄色录像| 欧美一级黄色网| 中文字幕在线视频观看| 韩国无码在线| 一级黄色电影在线观看| 一道本无码一区| 精品在线一区| 日韩无套| 狠狠操夜夜操天天爱| 国产成人一区| 黄色性爱多人视频| 亚洲一区二区视频在线观看| 亚洲欧美综合视频| 欧美激情一区| 国产一级a免一级a看免费视频| h无码动漫在线观看| 久久综合九色欧美综合狠狠| 婷婷五月网站| 国产成人免费| 天天操夜操| 精品99久久久久成人网站免费| 女人高潮抽搐喷液30分钟视频| 欧美一区二区三| 夜夜干天天操| 日韩电影一区二区| 亚洲精品动漫| 日本黄色三级片在线观看| 三级无码在线| 国产欧美自拍| 日韩精品一区在线| A片在线播放| 日韩一区二区三区在线| 亚洲熟女乱色一区二区三区久久久| Av天天有| 免费看黄色的网站| 天天操天天舔| 五月丁香中文字幕| 久久久精品国产亚洲Av无码| 国产精品久久久久久久AV超碰| 亚洲成人精品一区| 性做久久久久久久| 丁香六月激情| 伊人精品视频| 美女喷水视频| 一级亚洲| 日韩综合网| 久久99com| 91亚洲精品视频| 天天做天天摸天天爽天天爱| 精品无码在线| 国产乱伦一二三区| 国产全是老熟女太爽了| 天天操操| 欧美少妇性爱| 天天插天天日| 日韩综合在线观看| 少妇人妻偷人精品视频蜜桃| 丰满人妻熟女aⅴ一区| 国产草草影院CCYYCOM| 搡老熟女老女人一区二区| 91无码一区二区三区| 午夜福利视频网站| 亚洲无码小电影| 国产成人小视频| 国产免费看黄片| 色播综合网| 我要看黄色九九片| 色香蕉视频| 中文一区| 最近免费中文字幕大全免费版视频| AV一级片| 中文字幕精品一二三四五六七八| 国产欧美视频在线| 欧美狠狠干| 日韩一级黄色电影| 黄色性爱多人视频| 国产特级黄片| japan极品人妻videos| 亚洲午夜久久| 成人电影在线播放| 精品久久久久久久人人人人传媒| 精品一区二区不卡| 少妇又色又紧又爽又刺激视频| 国产一级A片| 美女AV网站| free性欧美| 超碰999| 夜夜操夜夜干| 国产精品久久久| 久久久久久免费毛片精品| 国产亚韩| 亚洲免费网站| 亚洲精品一区23p| 思思久久主页| 亚洲精品久久久久av无码| 国产一区二区三区免费观看网站上| china中国妞tubesex| 欧美抽插视频| 人人摸人人干人人色| 国产成人无码免费一区二区三区 | 国产夫妻性爱自拍| 国产一级男同A片免费看| 特黄AAAAAAAA片免费直播| 日本一区二区三区视频在线| 婷婷伊人| 日韩人妻在线视频| 国产精品久久久久久久久免费高清 | 国产AV一级片| 日韩精品免费观看| 日韩黄色AV网站| 无码视少妇视频一区二区三区| 久久99亚洲精品| 亚洲在线视频| 久久久久久久久亚洲| 欧美日韩三级视频| 亚洲AV无码乱码国产精品牛牛| 思思热在线视频精品| а√天堂资源国产精品| 91人妻人人做人碰人人爽九色| 污视频下载| 日韩乱伦小说| 国产精品偷伦免费观看视频| 对白刺激国产子与伦| 国产91熟女高潮一区二区| 精品欧美性爱| 成人免费性爱视频| 久久综合一区| 午夜成人在线视频| 国产精品久久久久无码AV| 91这里拍自| 国产精品无码aⅴ嫩草| 国产精彩视频| 国产精品第1页| 囯产伦精一区二区三区妓| 中文字幕无码一区二区免费久久| 中文字幕精品在线| 日韩www| 国产中文自拍| 天天操天天日天天射| 99色在线视频| 91精品国产综合久久久久久丝袜| 99精品欧美一区二区三区黑人| 久久福利导航| 91丨九色丨熟女高潮| 一级黄色片视频| 久久福利网| 亚欧AV| 亚洲无码一级| 久久久久久99| 亚洲三级片在线观看| 国产在线精品一区二区聂小雨| 鲁鲁狠狠狠7777一区二区| 国产中文字幕熟女乱伦| 强奸91| 一区手机福利视频导航| 老熟女乱伦网站| 国产免费一区二区三区在线观看| 免费观看操逼视频| 水多福利导航| 免费看一级高潮毛片2023| 女同一区二区三区| 97久久超碰| 日韩av电影在线观看| 亚洲天堂av无码| 哦┅┅快┅┅用力啊熟妇在线视频| 69无码| 久久精品影视大全| 日韩高清一区| 精品一区二区久久久久久无码 | 日韩欧美午夜| 国产精品乱码一区二区| 伊人影院亚洲| 国产熟女AAAAA片| 深喉| 黄片免费下载观看| 国产成人在线视频| 国产精品久久久99| 日韩精品免费| 男女91视频69| 国产成人一区二区| 99久久久无码国产精品性九价| 九九九精品视频| 77777av| 国产精品九九| 精品九九九| 爆乳一区| 高清无码精品视频| 操逼一区| 99无码| 无码流出在线播放| 制服丝袜中文字幕在线观看| 亚洲熟女一区二区| 26AU欧美| 伊人狼人综合| 一区二区三区在线免费观看| 欧美青青草| 粉嫩av久久一区二区三区小说| 青青草伊人| 国产色网站| 成人电影啪啪| 一级淫片120分钟试看| 特黄视频| 国产精品交换| 欧美高清一级| 欧美色吧综合在线| 日本一区二区三区精品| 九九精品在线| 国产一级A片夜天码免费看| 国产午夜片| 色噜噜综合| 欧美日韩国产一区二区| 青娱乐极品视觉盛宴| 国产日韩欧美一区二区东京热| 亚洲无码精品在线播放| 国产不卡AV在线| 亚洲毛片在线| 九九色视频| 超碰97人妻| 欧美色影院| 久久黄色网址| 又粗又硬视频| 香蕉在线影院| 人妻日韩中文字幕| 日本成人不卡| 少妇一夜三次一区二区| 高清一区无码| 成人亚洲精品久久久久软件| 日逼免费视频| 色天堂在线观看| 亚洲熟女一区二区三区| 思思热在线视频精品| 999久久久| 成人免费黄色大片| 中文字幕有码视频| 国产情侣小视频| 国产最新网站| 成人性爱视频免费观看| 日韩欧美少妇| 九九久久99| 免费无遮挡男女交性视频| 26uuu精品国产| 人人在操| 日韩久久影视| 日韩少妇无码视频| 午夜成人福利在线| 黄片免费在线播放| 日韩无码免费视频| av大片在线观看| 永久免费不卡在线观看黄网站| 成人黄色免费| 久久天堂| 久久久激情| 欧美XXXBBB| 日韩无码第一页| 91精品国产色综合久久不卡电影| 日韩AV专区| 91久久免费视频| 一本久道久久综合| 色先锋资源| 懂色AV一区二区夜夜嗨| 国产一区二区视频免费| 欧美日韩久久久久| 亚洲自拍小说| 国产精品高潮久久久久久无码| 国产一级特黄妇女A片40| 少妇精品无码一区二区三区| 91熟女视频| 99成人| 国产又黄又粗又爽| 伊人激情综合色| 综合国产| 精品视频99| 亚洲无码小电影| 国产熟女AV| 国内精品视频| 岛国视频一区在线| 欧美丝袜乱伦| 久久午夜无码鲁丝片午夜精品| 亚洲精品动漫| 免费操逼网站| 国产欧美又粗又猛又爽| 一牛影视av| 视频在线一区二区| 精品国产乱码久久久久久1区2区-亚洲| 日韩AV免费看| 亚洲精品无码久久久久av| 成人影片免费观看| 视频免费1区二区三区| 在线亚洲精品| av色天堂| 国产品无码一区二区三区在线妖精| 大香蕉福利视频| 真实乱视频国产免费观看| 91精品一区二区| 欧美亚洲中文字幕| 无码H乳在线看| 男人的天堂无码| 熟女网址| h无码动漫在线观看| 精品欧美一区二区三区精品久久| 人人爱操| 欧美乱码精品一区二区| 国产麻豆精品| 久久福利免费视频| 产国传媒91一区久久无码| 国产乱伦黄片| 亚洲国产精品一区二区久久恐怖片 | 无码中文AV| 91小视频| 免费黄色网址在线观看| 黄色精品视频| 欧美亚洲免费| 艳妇h圆房~h嗯啊| 超碰九九| 国产成人精品一区二区三区视频| 成年人在线观看视频| 五月天婷婷丁香花| 一级a一级a爰片免费免免免下载| 久久久婷婷五月亚洲国产精品| 黄色免费无码视频网站| 中文字幕在线免费看线人| 99久久亚洲精品日本无码| 欧美日韩一区二区三| 亚洲高清毛片| 思思热在线| 亚洲少妇性爱| 日韩成人免费视频| 鲁啊鲁视频| 天天日天天| 成年人性爱视频免费看| 久久国产一区| 欧洲亚洲AV无码国产精品成人| 国产无码精品在线| 亚洲欧洲自拍| 亚洲精品乱码久久久久久| 人妻中文无码| 久久久夜色精品亚洲| 精品久久国产| 午夜黄色影院| 久色亚洲| 亚洲熟肉一区二区三区在线观看| 国产精品久久久一区| 综合AV网| 国产精品天天狠天天看| 色综合综合| 天天摸天天爽| 久久91欧美特黄A片| 亚洲无码成人网站| 91福利导航| 国模网址| 中文字幕日韩三级片| 婷婷性爱视频| 国产美女裸体无遮挡免费播放网站| www.视频一区| 人妻 丝袜美腿 中文字幕| 国产一级做a爰片在线看免费| 91精品夜夜夜一区二区| 黄色一级网址| 久热国产视频| 91精品久久久久久粉嫩| 精品无码国产一区二区三区高跟 | 在线中文字幕一区| 久久久久无码精品国产91福利| 久久久久91| 欧美三级午夜理伦三级中视频| 免费看一级毛片| 亚洲综合熟女| 国产精品99久久久久久白浆小说| 国产精品a一区二区三区网址| 九九色视频| 国产69精品久久久久777| 日韩肏逼| 中文字幕熟女人妻偷伦天美| 爆乳熟妇一区二区三区霸乳 | 欧美成人精品| A级黄片免费看| 无码电影网站| 精品久久电影| 91精彩刺激对白露脸偷拍| 影音先锋亚洲AV少妇熟女| 国产精品一二三| 国产精品一| 老司机精品视频在线| 囯产精品久久久久| 亚洲人妻视频| 欧美大黄| 少妇潮喷视频| 色婷婷在线播放| 中文字幕亚洲乱码熟女1区2区| 中文字幕无码日韩专区免费| 黄页无码| 欧美熟女一区二区三区 | 人人操91| 秋霞伦理视频| 吴梦梦成人免费一区二区| 91熟女老肥分类| 动漫av无码| 亚洲国产精品无码观看久久| 国产美女裸体无遮挡免费视频| 午夜福利成人| 国产农村妇女毛片精品久久麻豆| 国产伦精品一区二区三区免费视频| 亚洲AV成人无码精电影在线| 国产夫妻性爱视频| 亚洲无码在线观看免费| 日韩无码精品视频| 婷婷在线视频| 国产精品亚洲五月天丁香| 国产特黄一级片| 看免费操逼视频| 久久国产精品无码| 国产精品内射婷婷一级二| 91视频免费在线观看| 欧美精品videos另类日本| 国产高清无码小视频| 国产爽爽爽| 91精品夜夜夜一区二区| 粉嫩AV一区二区三区免费观看| 久久久精品一区二区| 黄网站免费观看| 日本三级韩国三级美三级91| 秋霞无码视频| 久久99日韩| www..com操老师| 拍真实国产伦偷精品| 天天插天天日| 尤物AV在线| 91精品91久久久中77777| 91亚色视频| 超碰av在线| 少妇交换HD中文| 国产日韩欧美在线观看 | 丰满人妻妇伦又伦精品APP| 欧美久久久久| 91精品啪在线观看国产| 日韩激情网| 日本无码免费A片无码视频| 乱熟女高潮一区二区在线| 欧美第二页| 伊人91| 久久riav| 亚洲国产精品无码久久久久久久久| 91视频精品| 好吊视频| 无码视频一区二区| 大香蕉综合| 欧美日本在线观看| 黄色三级片在线观看| 精品国产AV| 久草人妻| 久久精品精品无码一区三区| 日韩美女一区二区三区| 欧美中出| 伊人久久免费视频| 精品一区二区AV国产精品探花| 国产永久精品大片wwwApp| 人人操一区| 亚州Av无码| 亚洲香蕉视频| 一区二区三区日韩欧美| 欧美一级欧美三级在线观看| 午夜国产视频| 精品不卡| 门卫老董| 一级香蕉,黄色片| 国产免费性爱| 成人免费观看网站| 成人日本A片无码| 免费在线黄片| 欧洲另类类一二三四区| 成年人午夜视频| 看免费操逼视频| 91网站在线播放| 精品无码人妻一区二区三区品| 亚洲三级片在线| 色资源网| 亚洲精品毛片| 日本一区久久| 国产乱码精品一区二区三区四川人| 丁香激情五月天| 黄片无码| 亚洲欧洲精品一区二区| 宅男午夜影院| 欧美精品一卡二卡| 国产乱来视频| 人妻免费视频| 五月天婷婷丁香| 老熟妇仑乱一区二区av| 中文字字幕在线中文| 日本www色| 国产欧美日韩综合精品| 亚洲三级在线| 亚洲午夜久久| 黄网在线观看| 欧美黑人xxx| 五十路在线| 国产伦精品一区二区三区电影动画| 日韩黄片免费在线观看| 精品无码一级毛片免费| 亚洲一区二区在线播放| 国产乱人乱偷精品视频| 性爱无码专区| 国产无码一区| 91久久精品国产91性色tv| 黄色网在线播放| 97av在线| 老熟女伦一区二区三区| 91AV综合| 欧美精品第一页| 91久久香蕉国产熟女线看| 伊人久久大香线蕉| 在线无码视频| 五月天激情综合| 精品九九视频| 欧美牲| 国产AV一卡二卡| 精品视频在线播放| 宅男午夜影院| 搡老熟女国产| 少妇无码| 国产小视频91| 国产青青草| 一级香蕉,黄色片| 国产无码免费视频| 亚洲一区AV| 久久99精品久久久久久园产越南| 欧美成人精品欧美一级乱黄| 翔田千里性爱视频| 国产精品1| 狠狠躁夜夜躁人人爽野战天天| 99久久精品毛片无码一区三区| 亚洲人妻系列| 性爱在线播放| 另类av| 久久亚洲网站| 久久国产精品一区| 在线看国产精品| 久久久久无码精品国产91福利| 久久久久国精品产熟女久色| 91精彩刺激对白露脸偷拍| 无码人妻精品一二三区免费百度| 欧美一级特黄视频| 日韩一级片视频| 久久伊人一区二区| 久久久久久国产| 亚洲国产日韩a在线播放性色| 美女色色网站| 最新国产在线观看| 丁香五月天激情| 国产性爱大片| 亚洲天堂一区二区三区四区 | 91亚洲精品国偷拍自产在线观看| 久久国产一区二区三区高清视频| 亚洲一区自拍| 婷婷天堂站| 亚洲一级黄色| 成人免费黄色大片| 德国free性video极品| 欧美精品亚洲精品日韩精品| 国产伦精品一区二区三区视频免费| 91麻豆精品国产| 日韩中文亚洲第一| 久久蜜桃| 在线欧美日韩| 国产精品爱久久久久久久威尼斯 | 久久久久99精品| 理论片无码| 国产一级操逼| 国产av成人| 偷拍一区二区| 国产日韩视频在线| 国产精品成人一区二区网站软件| 国产精品福利在线观看| 无码视频大全| 九九色综合| av黄色| 日韩一区二区视频| 香蕉视频一区二区三区| 伊人色综合久久久| 男人的天堂久久| freepeople性欧美| 青青在线视频| 国产精品tv| 翔田千里av一区二区三区| 精品国产免费无码久久久| 黄色中文字幕| 激情五月天在线| 综合另类| 先锋资源av| 国产女人水真多18毛片18精品视频| 全黄做爰毛片免费看| 久久精品亚洲AV| 精品人妻一区二区| 三级免费毛片| 久久久久日本精品一区二区三区| 人人摸人人搞| 亚洲AV无码久久国产精品| 无码三级| 夜夜福利| 91国在线| 日本天堂网| 国产无码又爽又刺激| 超碰91在线| 久久久国产精品| 无码精品人妻一区二区三区人妻斩| 视频在线无码| 精品国产91亚洲一区二区三区www| 美国一级黄片| 国产精品入口| 天天日天天干天天操天天射| 国产aⅴ日本一区二区三区武则天 久久99久久99精品免观看软件 | 久久一本| 亚洲欧美日韩一区| 国产欧美日韩在线| 九九热在线视频| 人妻互换一二三区免费| 影音先锋中文字幕资源6| 久久无码一区二区三区| jazzjazz国产精品麻豆| 欧洲另类一二三四区| 亚洲AV成人无码久久精品| 亚洲乱伦网站| 国产美女无遮挡裸永久观看| www.伊人| 黄色美女网站| 日韩专区中文字幕| www.超碰| 久久精品日韩| 色资源网| 国产精品黄色| 欧美裸体XXXX极品少妇| 一级黄色片视频| 日韩视频一区二区三区| 国产日批视频在线观看| 欧美在线色| 免费在线观看国产精品| 人人操人人干人人| 欧美成人社区| 久久精品视频久久| 免费精品| 孕妇孕交| 色午夜视频| 日本免费精品| www操笔网站| 国产无码.con| 蜜乳av激情| 精品一区二区三区中文字幕| 91精品国产色综合久久不卡电影| 8090操逼网| 国产另类自拍| 久久久91人妻无码精品蜜桃观看| 人人操人人爱人人乐人人操人人摸| 中文字幕无码一区二区免费久久| 欧美精品久久久久A片| 漂亮人妻洗澡公日日躁| 国产一级特黄大片色| 精品国产青草久久久久96| 欧美三日本三级三级在线播放| 伊人成人社区| 午夜精品久久久久久久| 久久久久久国产视频| 国产精品久久久久久久成人午夜| 久久在线视频| 日韩AV一级片| 一区二区三区四区中文字幕| 国产精品高潮久久久久久无码| 精品日韩人妻一区二区三中文字幕 | 91在线精品|