亚洲中文字幕在线观看_中文字幕的_中文字幕永久在线_中文在线字幕高清电视剧免费播放_中文字幕电视剧免费版_中文字幕免费看高清好看的电视剧

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
九九99热久久精品66中文字幕| 激情网战码亚洲A| 五月人人丁香婷婷五月人人丁香| 婷婷射图| 97操碰日本女人| 久久er免费视频| 五月丁香人妻| 操碰91| 激情九月天天天天婷婷| 婷婷丁香色情| 成人网站国产在线视频内射视频| 激情综合久久| 色婷六月| 亚州色综合| 天天插天天很| 99精品视频在线观看| 日韩综合久| 精品色色网| 色婷婷操逼| 丁香婷婷综合喷| 日韩激情婷婷五月天| 色噜噜五月天| 操逼综合网| 天天cha成人综合网| 色婷婷综合久久久久| 久久久91精品| 一区二区三区四区无码| 狠狠干综合| 婷婷五月69| 国产精品激情AV久久久青桔| 丁香五月激情综合久久| 久久99成人性爱高清视频| 色色色色五月| 婷婷综合五月天| 激情婷婷五月| 黄色短视频在线观看| er99免费视频在线| 婷婷激情五月| 六月婷伊人| 丁香五月色| 狠狠狠狠狠狠色| 日韩欧美一级大黄网站| 久99久视频精品| 婷婷伊人激情婷婷| 国产亚洲国际精品福利| 亚洲成人电影aaaa| www99热| 欧洲99视频在线| 五月婷网| 激情五月综合| 免费观看18视频网站| 欧美日朝成人| 婷婷丁香六月天| 丁香五月天网站| 日韩黄色电影| www.婷婷五月| 另类激情中文| 国产色婷婷亚洲| 国产乱子轮XXX农村| 色婷婷欧美| 午夜九九九九九九九九九九九九九| 激情色情五月天| 天天做天天爱天天综合网| 婷婷丁香熟女| 六月婷婷在线视频| 9热在线观看| 天天综合网在线| 丁香五月婷婷激情蜜桃| 婷婷五月天视频| 久久资源综合| 91婷婷搞| www.狠狠操.co m| 久久伊人五月天| 久久草大香蕉| 成人做爰黄A片免费看直播室男男| 伊人大香五月天| 国自产拍偷拍精品啪啪一区二区| 婷婷丁香五月激情图片| 五月天婷婷无码| 99热这里只有免费精品| 日本天堂免费99| 2020日日干| 成人一级片| 97色色综合| 99这里只有精品国产| 国产91在线视频观看| www,婷婷五月天777me,com| 色婷婷丁香五月| 99国产小视频| 色狠狠色综合久久久绯色AⅤ影视| 外国碰视频网站97| 婷婷五月天亚洲天堂| 操人妻AV| 天天射影院| 丁香五月手机在线| 呻吟国产AV久久一区二区| 亚洲色vA| 狼人狠狠操| 天天日天天舔| 五月天激情视频网站| 丁香五月婷婷综合91| 成人电影在线免费试看| 激情婷婷人妻| 久久婷婷草| 婷婷丁香九月| 久久五月天黄色五月天色网址| 狠狠干.com| 狠狠人人婷婷| 激情五婷精品网在线观看网址| 97超碰免费超级在线观看| 色播激情五月天| 91久久九久久九久久九久久九久久| 99热精品在线| 婷婷欧美激情| 26uuu青青| 国产成人网址| www.91在线观看| 激情网五夜婷婷| 蜜臀av 粉嫩av 懂色av | 99热99草97| 九色视频91| 色综合性视频| www.99热视频| 久久密臀婷婷| 人人草人人舔| 中文字幕资源网| 亚洲欧洲色色| 激情久久久久久久久久| 一本色综合色| 五月丁香久久综合| 久久婷婷六月综合| 99er免费在线观看| 91九色中文字幕女在线观看| 97夫妻超碰| 99久久婷婷五月综合| 美女100%露全身无挡网站| 欧美久久久久久久久中文字幕| 五月丁香婷婷啪啪| 综合噜噜| 天插天啪天啪天啪| 大香蕉520| 超碰cap| 热99这就是精品视频| 激情五婷网| 91久久久久久| 91在线看免费 九九九九| 亚洲激情五月| 久xxxx| 国产国产乱老熟女视频网站97| 五月激情婷婷丁香天堂| 丁香激情合作五月| 91蜜桃婷婷狠狠久久综合9色| 免费91久久精品| 婷婷五月天色色| WWW,五月| 色婷五月| 极品 少妇 内射| 在线天堂9| 九色成人AV在线| 欧美性生交XXXXX无码小说| 激情图片五月天| 翔田千里无码| www。五月天。com| 日操| 色婷婷丁香网| 五月天综合网| 内射综合网| 精品九九久久| 久cao香蕉影院| 精品亚洲国产成AV人片传媒| 超碰在线人妻| 日本啪啪网| 五月天婷婷亚洲| 99aese| 激情五月天在线观看色婷婷| 99综合网| 在线99热| 成人短视频在线观看| 欧美三级级99久久| 久久婷婷六月综合综合| 免费成片在线观看| 99在线播放| 开心色色五月天综合| 成人综合网站| 免费看欧美成人A片无码| 激情综合婷婷| 99热在线观看精品| 中文字幕 码精品视频网站| 婷婷五月色综合| 久久人妻www| 色婷婷狠狠色| 天天舔天天摸天天透| 我要色综合五月婷婷| 欧美婷婷六月丁香综合色连续高潮抽搐| 91大神操美女| 伊九九三级区| 色优久久| 丁香综合伊人| 色欲香综合网| 色色色色色色综合| 丁香美女主播视频在线观看| 人人爱人人添| 色五月在线观看| 欧美日韩AAAA| 婷婷九月丁香| 五月丁香自拍| www.zbzhongsen.com| 色欲av伊人久久大香线蕉影院| 五月天丁香成人社| www99热| 色综合丁香| 国产精品成人在线| 欧美日韩中文国产一区发布| 污污内射久久一区二区欧美日韩| 激情九月婷婷九月| 久久精彩视频99| 久久婷婷综合色丁香| 狠狠综合久久综合| 五月婷婷色影院| 91超碰在线观看| 久久久999精品| 99热日本| 高清无码一区二区三区四区| 婷婷激情五月天在线| 丁香五月婷婷俺也要去| 欧美五月婷婷| 99热99色| 骚片AV蜜桃精品一区| 激情色播| 色五月婷婷伊人| 日本99在线视频| 97福利视频| 99久久99热| 精品综合五月| 婷婷五月天av| 人人操AV| 色综色网| 超碰在线免费9| 91狠狠色| 夜夜爽日日躁| 五月婷婷五月天| 91超碰在线观看| 国产无遮挡又黄又爽免费网站| 亚洲精品久久国产高清情趣| 五月丁香婷婷老司机| 五月婷婷婷综合网| 久久这里面只有精品视频| 涩五月丁香| www五月天com| 色色五月天婷婷| 国产精品爽爽久久久久久| 五月伊人91| 婷婷 丁香 久久| 丁香五月自拍| 好好干av| 色情久久久| 黑人糟蹋人妻HD中文字幕| 五月天婷婷婷| 激情婷婷丁香五月天| 蜜桃婷婷丁香五月天狠狠久久综合| 国产一二三四五六七八视频| www.99久久久| 99热热热天天人人人超超碰| 色婷婷亚洲| 人人干人人操人人摸人人做| 久久免费操| 欧美性猛交XXXX乱大交极品| 99啊精典免费视频| 色月视频| 亚洲黄色精品| 久久精品熟女亚洲AV麻豆| 激情文学第四色婷婷丁香五月| 亚洲五月丁香综合网| 丁香五月综合在线观看| 激情丁香五月天| 亚洲天堂AV综合网| 欧美婷婷六月丁香综合色连续高潮抽搐| 人妻自慰高清合集| 国产SUV精品一区二区883| 一区无码| 深爱激情小说五月婷婷| 色婷婷19| 亚洲无码猫咪| 六月婷婷狠狠| 亚洲无码另类| 欧美性交一区二区三区| 99精品视频在线| 一区二区乱码视频| 色天使久久综合| 婷婷和五月天| 天天干天天爽| 国产97在线日韩亚洲女人被黑人巨大| 五月丁了香蕉综合| 99热e| 色欲AVV| 丁香五月婷婷激情小说| 激情五月天开心| 五月激情在线| 婷婷五月天777| 激情AV在线| 婷婷中文字幕欧美| 亚洲射激情| 99九色视频在线观看| 禁片二区| 夜夜做夜夜愛| 国产精品免费大片| 国产精品色色666| 91精品久久久久久久久| 日本在线wwww| av网站中文| 日本婷婷五月天| 超碰在线99热| 丁香五月成人婷婷| www色哟哟| 5月婷婷六月丁香| 色色色色综合| 91超碰在线观看| 亚洲综合五月天| 亚洲激情四射色| 色五月婷婷成人视频| 97干97色| 色噜噜狠狠色综合网| 天天天综合网| 99久久偷拍视频| 青青福利网| 国产精产国品一二三在观看| 丁香六月啪啪| 另类视频在线| 丁香六月啪| 激情综合国产| 人人综合久| 狠狠综合网| 在线不卡的视频| 五月天久久www| 极品人妻VIDEOSSS人妻| 丁香五月日啪| 久久91精品国产91久久户| 99色激| 大香蕉婷婷丁香视频在线| 国产精品人妻在线网址| 五月天激情电影| 色婷婷综合电影| 久久人妻久久| 日韩精品99久久| 亚洲视色| 天天操五月天| 久草五月婷婷| 丁香五月久久| 裸睡玩奶头(高H)| 五月丁香婷婷网网网网| 亚洲电影在线观看| 五月婷婷六月爱| 欧美AAAA片免费播放观看| 五月婷婷久久激情| 麻豆观看夏晴子| 五月丁香狠狠| 日本少妇AA一级特黄大片| 狠狠草在线观看| 亚洲啪啪精品| 色欲五月婷婷| 五月丁香六月综合情在线观看| 99re这里| 婷婷五月天激情综合| 亚洲一区在线播放| 美英法精品无码免费视频| 天天色凹凸| 婷婷五月天堂| 久久久性爱视频| 丁香五月色| 开心五月激情| 中国操逼99| 97色色在线视频| 丁香花五月天婷婷成人社区| 久久99精品久久久久久噜噜| Av大香蕉| 亚洲精品综合一区二区三| 色 五月婷婷基地| 伊综合蕉| 丁香五月日韩| 开心婷婷五月天电影院| av首页在线| 五月丁香六月婷婷成人电影| 亚洲综合婷婷| 亚洲欧美中文字幕高清在线| 激情五月色播五月| 97精品综合久久| 日日影院 | 欧美va亚洲va在线播放| 狠狠爱夜夜| 色五月婷婷丁香五月| 开心五月丁香综合久久| 丁香六月综合| 亚洲永久免费| 艾小青av| 97性视频| 色综合久| 亚洲成人网站在线播放| 少妇日麻屄| 开心五月婷婷伊人| 久久婷婷五月天懂色| 五月婷婷 六月丁香| 国产精品A片在线| 色丁香五月天| 婷婷深爱五月丁香网| 国产一区18| 精国产品一区二区三区A片| 婷婷丁香综合成人| 丁香婷婷久久| 超级碰 久久9| 人妻少妇色综合| 99性爱视频网站| 国产在线中文字幕| 丁香五月瑟瑟| 激情深爱五月天| 99er精品视频| 五月色亭丁香| 91艹人| 色欲AV亚洲精品一区二区| 亚洲男女激情| www·五月天| 99熟女啪啪视频| 夜夜精品视频一区二区| 激情综合网址| 色99热| 丁香色五月婷婷17C| 中文AⅤ大全| 日日色综合| jizzdr| 夜夜骑操AV| 五月丁香综合中文| 五月婷婷丁香91| 狠狠操狠狠爱| 激情五月天在线免费美女视频| 五月亚洲激情| 亚洲欧美综合7777色婷婷| 久久这里只有精品视频15| 久月丁香爱婷婷综合| 韩国97天堂| 51精品国自产在线| 91玖玖| va婷婷| 99热99日…..| www.婷婷五月天.com| 九九伦子片| 一本道在线电影| 超碰二区| 五月天亚洲色| 天天爽天天透天天爱| 国产3p露脸普通话对白| 91九色国产| 色五月天电影| 丁香婷婷中文字幕| 我爱宗和色| 色优久久| 色欲九区| 久久新地此| 99在线看视频| 五月丁久久| 五月天婷婷色| 小视频久久久aaa| 九月av| 五月激情婷婷丁香天堂| 视色综合| 久久99色色| 五月丁香色婷婷伊人| 久操人妻| 爱操人妻| 99欧州偷拍视频| 一起肏在线视频| 91人人人人人人人| 成人五月天综合网| 成人午夜天| 亚洲色热| 五月婷婷色播| 色婷婷丁香五月| 人妻熟妇国产精品| 久久综合中文| 成人 在线 日韩| 猛烈顶弄H禁欲老师H春潮 | 久久 中文 日本| www,99色| 婷婷丁香五月天熟女丝袜| 99惹 精品在线| 大香蕉AV电影在线| Aaa久久| 色五月婷婷在线观看第一页舔| 91情国产l精品国产亚洲区 | 色五月天激情| 亚洲精品五月| 日韩精品无码99| 麻豆五月丁香婷婷| 午夜电影网VA内射| 日日操天天| 色五狠狠| 五月丁香中文| 国产丝袜美女| 91九色无码日韩| 超碰日日操| 99久久99九九99九九九| 五月丁香六月在线| 成人国产欧美大片一区| 亚洲综合国产在不卡在线| 黑人糟蹋人妻HD中文字幕| 99网| 99年操人人爽| 五月丁香激情综合网官网| 色五月美女| 丁香五月色色婷| 殴美日韩成人| 黄色五月婷婷| 色五月成人婷婷| 婷婷五月丁香综合激情小说| 9999色色色色| 五月婷视屏在线观看| 九九热在线观看视频| 婷婷色在线播放| 色久九| 江苏少妇性BBB搡BBB爽爽爽 | avv在线| 丁香五月综合激情啪啪| 性爱AV天堂| 婷婷色香六月综合激情| 五月天综合影院| 伊人在线视频| 婷婷五月天色色| 专区无日本视频高清8| 99久久99综合| 免费看片操逼| 九九黄色网| 五月婷丁香在线视频在线| 婷婷亚洲色| 成人网在线视频| 久青草影院| 七七婷婷综合| 涩涩婷婷五月| 五月婷婷五月天激情视频| 小视频一区| 日本色综合| 激情五月天在线视频| 久久综合婷婷| 五月色亚洲| 久鲁鲁色网 | 国产日韩欧美性生活| 丁香婷婷六月在线资源观看| 国产AV一区二区三区日韩| 99爱在线免费视频| 久久五月天影院| 久久婷婷五月综合精品蜜芽| 六月丁香婷婷天堂| 99精品视频在线观看| 99九九视频| 91在线资源| 日韩综合网络男女香蕉a片| 人妻videos人妻高清| 99re6久热只有精品6在线直播| 第五色婷婷| 草榴成人影片| 六月丁香激情综合网| 狠狠干综合网| 中文字幕无码人妻少妇免费视频 | 色色色综合色| 中文字幕有多少字| 欧美、日韩、中文、制服、人妻| 热久久思思热思思| 六月伊人| 久久激情中文| 久久婷婷五月综合| 婷婷六月丁| 婷婷丁香五月综合| 欧美婷婷丁香五月| 天天做天天要天天爽| 五月久久婷婷天堂视频| 日韩黄在免| 91一起操| 丁香六月激情综合| 99亚洲精品| 狠狠香蕉| 久久精品人妻| 最新无毒无码AV| 涩五月婷婷| 999热这里只有精品| 欧美成人精品三区综合A片| 99色在线观看视频| 狠狠五月综合在线| 国产欧美熟妇另类久久久| 五月天婷婷情色| 好激情在线综合网| 中文字幕日产A片在线看| 极品另类| 激情婷婷色五月| 久久精品99国产精品日本| 婷婷五月电影| 5月婷婷6月六月丁香| 日韩一区二区在线免费观看| 91一起操| 操逼巨乳91| 婷婷99视频全集高清| 丁香五月丐人妻| 99在线69| 婷婷综合网性| 久久视频这里99| 熟女人妻视频| 99re99热| 97九色| 成人短视频在线免费观看| 色综合综合色| 国产a高清| 九九视频免费| 色色婷婷五月| 亚洲六月色婷婷| 婷婷性福五月天| 五月丁香综缴情性爱| 丁香五月综合在线| 国产成人精品一区二三区熟女在线| 天天操婷婷| 欧美精品18| 亚洲情欲久久| 丁香婷婷色情社区成人小说| 激情婷婷五月天| 日本无va视频| 极品少妇高潮啪啪AV无码| 激情综合5| 91九色精品熟女内射| 久青操| 四房婷婷| 狠狠爱五月婷婷| 婷婷五月色综合| 影音先锋综合网| 深夜A片| 色色色色色网| 色婷婷成人做爰A片免费看网站| 色色色色色五月丁香| 色色色热热热| 婷婷黄色五月| 天天影院色| 综合超碰熟| www.激情五月| 五月婷婷综合社区| 九九综合| 99精品一二三四视频| 亚洲精品在线视频| 久久久久久久久99精品| 日韩av在线电影| 99操逼视频| 日韩成人综合网| 丁香婷最新动态| 99无码视频| 五月丁香色婷婷伊人| 夜夜爽77777妓女免费下载| 蜘蛛女免费观看完整版高清电影| 成人美女网| www.婷婷五月天啪啪| 日韩欧美三区| 性生活视频98791| 99久久天堂婷婷| 99视频在线| 狠狠五月激情丁香六月| 999热在线视频| 久久婷婷青草五月天| 乱岳熟女50岁| 思思热在线精品视频网站| 婷婷香蕉精品| 亚洲美女网Va| 玖玖无码中文| 福利视频在线播放| 99九九视屏| 九九色video| 九九九免费观看视频| 狠狠色狠狠| 激情99| 亚洲精品性色| 色五月激情综合网站| 9热在线观看| 亚洲一个色| 99色视频| 婷婷网五月天| 狠狠色综合网| 亚洲日本国产综合高清| 激情综合丁香五月| 性视频久久| 午夜少妇在线观看视频| 九九热精品视频九九| 丁香六月av| 亚洲欧美综合7777色婷婷| 九九热视频网站| 婷婷5月久久综合网站| 色婷婷日本| 精品久久二6| 丁香婷婷成年| 久久Xx| www色婷婷久久综合久色| 激情五月黄色| 成人五月天丁香婷| jiujiu无码五区| 久久玖玖99| 五月天色图| 五月天婷婷乱| 日韩精品一区二区亚洲AV观看| 婷婷99狠狠| 五月丁香婷婷潮喷中文字幕| 亚洲AV中文在线| 日韩欧美视频一区| 亚洲婷婷五月天| 亚洲性爱99| 一区二区三区四区牛| 激情综合网五月婷婷| 丁香五月色欲| 九九色色| 一级韩国产精品毛| 99热97| 99热a片免| 丁香婷婷综合激情五月色,开心五月丁香花综合网,激情综合五月亚洲婷婷,五月天 | 久久久久妻| 丁香五月婷婷操逼| 精品久久久人妻| 五月婷天天搞视频| 五月天五月色婷婷综合| 免费成片在线观看| 欧美在线| 大香蕉伊人爱在线| 99热精品一| 噜噜噜狠狠色综合| 久久久噜噜噜www成人| 99国产精品久久久久久久久久久| 色五月激情五月| 婷婷综合五月天激情| 五月久久网| 亚洲午夜在线视频| 色婷婷影视| 色婷婷社区| oumeisesewang| 九艹在线| 五月丁香久久激情综合| 五月天另类激情在线| 俺去也五月天| 99热只有精品在线观看| 任你艹| 国产4P视频精品五区| 丁香五月影院| 99这里只有精| 强伦人妻BD在线电影| 五月天婷婷黄色| 天天干,天天舔| 六月激情婷婷综合| 色综合99无码| 国产亚洲精品AAAAAAA片| 国产精品日日躁夜夜躁| 性日本精品| 精品无码人妻一区| 色婷婷XXXXX| 日韩欧美成人片| 天堂va久久久噜噜噜久久Va| 久久99国产综合精品免费| 亚洲高清在线| 国产亚洲精品AAAAAAA片| 丁香婷婷六月在线资源观看| 99re思思在线视频| 五月天婷婷基地| 久久婷婷丁香| 亚洲在线成人| 丁香五月停停av| 亚洲视频一区| 嫩草AV久久伊人妇女超级A| 9久久久久| 这里只有精品视频| 久久久久久人妻久久久久久久久久人妻久久久 | 久久久网站| 永久免费视频| 精品亚洲日韩99欧美片| 99五丁香月| 伊人久久婷婷五月综合97色| 麻豆亚洲精品中文字幕一麻豆| 色五月综合在线| 天天射美女| 欧美日韩成人高清在线| 天天干天天色综合| 亚洲另类噜噜| 这里只有精品9| 五月丁香六月婷婷a v| 综合激情五月综合激情五月激情1| 色婷婷电影| 91热在线| 久99久在线| 久久久性爱视频| 91久久综合| 色老久久| 99a级片| 天天综合 99久久婷婷| 色婷婷久久视屏| 欧美月久久| 综合婷| 欧美日韩日韩成人| 久久六月综合| 丁香婷婷五月人体| www.激情五月天.con| 亚洲欧洲一二| 99色.com| 4399高清无码视频| 国产激情在线| 国产精品99久久久久久猫咪| 九洲一级A片| 67194成I人在线观看线路1| 免费婷婷| www。五月天激情| 久久九九怡红院| 激情影院内射| 婷婷丁香五另类网站| 99色1| 一本伊人色婷| 色色色9| 五月天色五月| 久久婷婷丁香| 99热日本| 风流少妇A片一区二区蜜桃 | 五月天激情丁香| 亚洲亚洲人成综合网络| 中字文幕不卡在线视频| 中文字幕婷婷9月天| 涩丁香91| 欧美伊人9| 亚洲av成人在线| 婷婷丁香视频在线观看免费| 五月婷婷综合激情| 精品久久久久久久久久久久人妻| 91色情播放| 强伦人妻BD在线电影| 婷婷五月激情图片| 人人草人人舔| 天天天天干| 九九激情| 丁香蜜臀黄色婷婷五月天| www99热| 色亭亭五月天网扯| 久久婷婷五月综合色丁香| 六月激情久久| 婷婷久久五月| 麻豆国产原创中文AV网站| 操操综合网婷婷| 亚洲综合在线网站| 婷婷色色网| 久久九九99字幕| 五月天激情小说欧美激情| 丁香五月色网| 成人精品视频99在线观看免费 | 国产裸体AAAA片色戒| 狠狠色色| 99在线免费观看| 日本久久9| 伊人99热| 爱婷婷五月| 婷婷狠狠97| www.色五月| 婷婷五月丁香99| av久热| 五月婷婷熟女| 五月婷婷婷丁香播| 色五月综合| 亚洲正能量欧美| 国产免费AV在线| 中国AV性爱观看| 97色色视频| 婷婷五月天影院| av免费在线观看0| AV在线中文| 噜噜噜噜在线| 激情亚洲婷婷| 婷婷五月成人| 任你操精品免费| 六月丁香婷啪射| 深夜视频| 亚欧洲乱码视频一二三区| www.com任你艹| 狠狠干天天内射| 99色网站| 国自产拍偷拍精品啪啪一区二区| 亚洲视频在线网| 欧美欧盟性爱网| 综合五月婷婷| 国产欧美日韩综合精品一区二区 | 风流少妇A片一区二区蜜桃| 亚洲久艹| 亚洲五月婷婷在线| GOGOGO免费高清日本TV| 午夜国产免费视频亚洲| 成人中文字幕在线| 婷婷基地五月色| www.婷婷五月天.com| 狠狠婷婷综合| 99热综合在线| 99久视频| 开心五月婷婷激情| 久久精品五月天| 天天五月情| 亚洲热视频| 极品九九九九九九| 天天干夜夜b| 伊人婷婷五月天| 99热99思午夜精品| 五月丁香综合精品| 91人妻人人做人碰人人爽九色| 国内自拍97在线| 国产亚洲色婷婷99精品| 日日夜夜干| 日韩青青| 99热这是里只有精品| 精品网站:999WWW| 婷婷情色五月| 五月色情婷婷开心五月色情| 99在线观看视频| 五月色激情综合网| 色五月婷婷开心| 深爱激情综合网| 丁香五月色网| 都市激情五月婷婷亚洲| 99在线精品免费视频| 五月丁香婷婷在线| 91精品久久久久、久五月天| 怎么样可以看免费的一级av| 精品国产va久久久久| xx久久| 色婷婷性爱| ss视频xx91| 成 人 片 免费播放| 亚洲婷婷在线播放十月| 欧美激情综合色综合啪啪五月| Www.se.久久| 激情黄色小说五月天| 欧美69久成人做爰视频| 色综合激情| 搡BBBB搡BBB搡| 91日综合欧美| 丁香五月无码| 九九九激情综合| 五月天 综合 在线| 天天日天天摸| 九九综合| 日本啪啪网| 色九九七七| 精品久久这里热66| 亚洲色区17| 久热网在线视频| 久久se 综合网| 婷婷丁香五月六月激情| 午夜理论在线观看不卡大地影院| WWW·天天操·视频?| www.久久| 久久曰曰| 日韩啪啪视频| 亚洲天堂爱爱| 婷婷色九月| 亚洲综合在线播放| www.99日本| 六月婷婷色色色| 热99在线精品| 99综合熟女| 久久超视频| 五月天久久网站| 欧美成人精品A片免费一区99| 亚洲欧洲小视频9| 婷婷五月草| 五月天婷婷涩涩| 丁香六月婷婷| 密乳Va| 五月天丁香久久| 婷婷丁香花五月天| 99自拍视频网站| 久久婷婷热| 狠狠做深爱婷婷久久综合一区| 99re在线观看| 天天干天天插| 丁香婷婷偷拍| 午夜成人亚洲理伦片在线观看| 五月丁香六月婷婷免费| 一起草AV入口| 夜夜做夜夜愛| 国产亚洲成AV人片在线| 九九综合| 六月婷婷av| 超碰狠狠操| 五月丁香六月婷婷,婷| 欧美人与性动交CCOO| 夜夜做天天爽| 综合福利网| 婷婷婷婷婷婷婷五月丁香| 亚洲AV永久无码影院黑人| 亚洲精品成人区在线观看| 秋霞成人毛片一级A片| 97色色色色色| 五月丁香拍拍激情综合| 国产黄色在线观看| 激情伊人五月天| 久久九九国产| 九九热视频精品| 天天色伊人| 久草x色在线观看99| 久久 天天| 色久九| 久久小说网| 亚洲激情精品| 干一干xxxx| 一本色道久久综合狠狠躁小说| 婷婷六月丁香色| 91高潮喷水久久久久久久久 | 天天爽天天日| 日日做天天操夜夜爽| 9 大屁股在线视频精品| 久久婷婷五月天激情四射| 色色热99| 久久九九热38| 中文字幕资源网| 热99精品视频在线观看| 国产五月视频| 五月丁香六月天| 99久久婷婷国产综合精品草原| 久久午夜一区二区| 狠狠草狠狠草| 91精品久久久久久| 无码AV综合AV亚洲AV| 五月丁香六月婷婷操操操| 色欲久久综合| 激情久久久| 免费亚洲婷婷五月| 99色在线视频观看| 丁香五月婷婷av影院| 影音先锋91资源站| 激情综合五月激情17| 欧美一级a | 婷婷久久综合| 97色色色色色| 狼人久草| 天堂久久丁香| 综合视频久久| 色色色.com| 五月天丁香久久| 久久久久综合网久久| 深爱综合网| 丁香无五月网| 色欲色香综合网站| 人人操AV| 五月亭亭性| 狠狠操.com| 九月大香蕉| 中字幕视频在线永久在线观看免费| 亚洲色色香蕉| 激情网站五月| 综合精品啪啪| 人与禽A片啪啪| 亚洲天堂色色| 婷婷5月天激情综合| 婷婷玖玖丁香| 欧美午夜精品一区区电影| 青青草原伊人网| 天天干天天操天天干天天操天天干天天操| 欧美色偷拍| 日韩精品人妻AV一区二区三区| 激情综合99| 婷婷五月精品中文字幕| 日本久久综合| 碰久久精品w| av国产精品| 五月小说| 色小说五月婷婷| 1024日韩| 国产色99| 久热99| 97人妻碰碰中文无码久热丝袜| 婷婷色激情五月天| 欧美噜噜免费观看| 五月婷婷综合影院| 五月天大香蕉av| 人妻久久久久久久| 免费亚洲婷婷| 色五月婷婷DVD| 中文网AV| 日韩精品超碰在线观看| 国产免费一区二区三州老师F1…… | 天堂中文国产| 婷婷丁香综合色AV| 午夜精品白在线观看| 丁香婷婷啪啪| 天天色噜| 天天看夜夜看| 热这里只有精| 婷婷五月天黄色| 一起操 91N.com| 超碰只有精品在线| 99热免费| 色丁香五月婷婷| 丁香五月天婷婷中文字幕| 深爱激情av| 激情综合五月色在线| 99视频自拍| 久久9热| 色婷婷玖玖影院| 两性婷婷丁香五月| 麻豆AV久久无码精品久久| 任你草| 91人操人人人操人| 五月久视频| 天天干天天操| 五月婷综合性中心| 亚洲综合色网站| 天天色综合天天| 亚洲99综合| 97在线刺激| 99色五月| 99人妻碰碰碰久久久久视|