午夜在线小视频_午夜激情网站_午夜福利国产在线_午夜影院APP在线观看

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
激情黄色小说五月天| 67194中文在线| 天天爱天天操| 婷婷久久亚洲| 五月丁香婷婷中文网| 99热综合在线| 91成人电影| 九九热99精品| 99九九这里有免费视频| www.激情| 激情六月天| 婷婷色五月激情| 久久婷婷五月综合色丁香| 五月丁香人妻| 五月天久久综合婷婷丁香| 色久五月| 激情五月www| 欧洲激情五月天婷婷| 婷婷久久午夜网| 五夜婷婷| 婷婷色偷拍| 久久98| 婷婷五月天综合色| 天堂草在线观| 五月丁香婷婷中文网| 五月丁香综合网色欲| 99日本在线| 成人网在线视频| 97干在线看| 综合久久伊人| 99碰碰中文| 色综合久久8| 五月色情婷婷| 26UUU欧美激情一区二区| 中文字幕婷婷在线| 日韩xx在线| 婷婷五月丁香色综合| 69人人操人人爽| 亚洲正能量欧美| 91色综合久久| 狠狠色综合无线观看| 色五月婷婷在线观看第一页舔| 91超级碰碰| 亚洲欧洲中文日韩久久AV乱码| 五月网站| 中文字幕在线观看视频www| 亚洲蜜桃精久久久久久久久久久久| 色婷婷久久| 熟妇内谢69XXXXXA片| 天天综合色| 日韩一区二区A片免费观看 | 婷婷综合在线观看视频| 国际国外精品欧洲南美洲专区无码不卡| 色视五月天婷婷| 91大神在线免费看视频全集男男一起操| 色啪久| 天天碰夜夜操| 久草婷妨| 色六月婷婷| 五月天色色网站| 第四色激情网| 狠狠干总合| Jh7Uf088VHafNm| 原琪琪色影院| 日本激情ⅩXX免费视频| 嫩草综合网| 丁香五月婷婷激情123| 五月婷婷在线观看| 激情综合网五月天| 婷婷娌伦网| 激情婷婷五月| 在线只有精品| www.lchjjc.com| 91av色色乱视频| 色色色地址| 99爱视频精品| 亚洲欧洲自拍图片专区五月天| 日日夜夜综合| 夜夜操狠狠操| 日日夜夜天天综合| 亚洲宗合激情| 五月天激情图片网| 性韩日色婷婷五月天激情啪啪XXX| 五月婷婷六月丁香激情深爱| 五月情婷婷五月| 天天操天天日天天操| 丁香五月色欲| 狠狠爱激情网| 开心激情网五月| 99热这里只有精品4| 久久婷婷五月综合色丁香| 日本一道久久| 成人丁香婷婷| 手机旧版看人妻1025| 9色在线| 婷婷五日b| 五月天开心激情综合网| 欧美操人| 九九精品碰| 另类伊人婷婷| 狠狠肏综合网| 天天拍天天操| 国产亚洲精品久久久久苍井松| 色天堂婷婷| 亚洲成Av人片乱码色第1集| 激情丁香社区| 毛片新网地| 99视频激情四射| 五月丁香婷婷色| 中日韩美欧成人一区二区精品在线| 久久五月天免费网站| 99色婷婷视频| 婷婷涩五月天综合| 久久激情五月天| 三年高清大片免费观看国语| 99九九免费精品| 九九成人| 综合色情网| 丁香五月综合在线| 蜜桃精品AV无码喷奶水小说| AⅤ网站在线看| 亚洲视频国产一区| 色婷五月丁香久亚洲| 丁香六月婷婷综合| 99视频免费播放 | 色八月婷婷| 丁香六月婷婷姐网| 欧美槡BBBB槡BBB少妇| 久久天堂女人| 婷婷激情小说网| 草逼大片| 六月天婷婷| 香蕉乱插| 亚洲五月天伊人| 99re6在线视频精品免费| 五月开心久久| 九九色播五月丁香| 久久在线人妻| www.色五月| 97se在线视频| 亚洲欧洲自拍图片专区五月天| 草莓网| 狠狠噪| 婷婷丁香在线| 婷婷中文字幕| 欧美一级a | 超碰日韩人妻在线| 婷婷丁香激情综合色情| 热99精品视频| ..真实国产乱子伦对白在线_欧| 99热在线爱| 婷婷激情综合无月| 激情综合无码| 四色五月视频| 五月婷婷二月丁香| 久久综合99| 色琪琪一综合久久激情五月视频| 日日夜夜久| 亚洲中文字幕在线观看| 伊人超碰| 色婷婷五月综合| 人人爽网| 丁香婷婷精品视频| 久热成人| 婷婷六月综合| 五月天综合婷婷| 亚洲日本韩国| 五月停亭六月,六月停亭的英语| 五月天激情小说欧美激情| 熟女人妻一区二区三区免费看 | 激情综合五月丁香六月婷婷| 日韩一66精品| 99性色| 干一干xxxx| 天天色综合网1| 国产精品99久久久久久久女警 | 国产性色蜜乳| 色色99| 日本一级一级一级一级| 婷婷97狠狠成人网站 | 91综合色| 中文字幕无码人妻AAA片| 91人妻九色大屁股| 99在线视频精品| 99精品在线观看| www.91.com黄| 天堂新版在线| 天天搞天天色综合| 丁香花成| 成人网站av免费网站推荐| 久久深爱激情网| 五月天丁香| 综合激情婷婷| 爆乳熟妇一区二区三区爆乳照片| 婷婷九月激情| 日本色久| 综合性爱网| 丰满人妻一区二区三区| 日本在线视频看se99| 日韩操逼小电影| 五月丁香综合色婷婷| 婷婷五月天AV激情| 精品一二三区久久AAA片| 丁香色六月| 激情视频网址| 、激情六月天| 99久久这里只有精品| 五月丁香大香蕉| 97色片| www.91九色| 五月天婷婷基地综合网| 99re热99| 丁香六月久久| 亚洲五月丁香综合网| 激情综合色| 异能之下短剧免费观看全集| 精品久久99码| 九九视频免费| 伊人在线视频| 婷婷激情蜜桃玖玖丁香| 热久久999| 青青草婷婷综合五月| 欧美黄色一级录像| 日日狠夜夜狠| 曰本aaaaaa丈片| 久久黄色片| 青青操成人福利| 色色色色av色色色色| 五月色婷婷夜色| 丁香婷婷激情六月五月开心| 丁香婷婷色| www色色com| 中文网AV| 少妇伦子伦精品无吗| 婷婷五月丁香狠狠| 亚洲狠狠色丁香婷婷综合久久| 久久伊人日日夜夜| 67194中文在线| 五月丁香六月欧美综合网站| 中文字幕九九九九| 深爱激情五月网| 狠狠va| 激情九月婷婷九月| 天天狠狠六月婷丁香影院| 亚洲成人在线综合| 狼人久草| 五月婷婷开心爱| 热91久| 五月丁香做爱视频| 丁香六月婷| 亚洲永久免费| 狠狠va| www久久久久久久久久久久久久久久久| 激情五月天色婷婷| 91日韩美女被插视频| 曰曰久久| 有码人妻久久| 亚洲精级| 日韩成人AV在线播放| 就要爱综合| 色五天综合| 五月丁香啪啪伦理电影| 五月婷婷啪啪网| 婷婷五月色| 欧美婷婷五月天综合| 九九久久高清| 久久综合丁香激情五月| 夜夜夜叫天天天做| 九九精品99久久久| 中文字幕成人| 亚洲狠狠狠| 婷婷五月天黄色网址| 色五月婷婷影院| 婷婷五月丁香激情色情| 超碰激情五月| 97人人超| 天天爽综合网| 操人91| 精品久久99| 五月天.com| 99在线播放视频| 欧美三级巜人妻互换| 五月丁香六月婷婷无码| www.狠狠| 1囯产午夜仑鲁鲁| 97亚洲婷婷| 丁香五月亭亭六月综合激情网| 免费V片在线| 天天久久狠狠色综合| 天天色五月| 丁香六月激情毛片| 熟妇人妻中文字幕无码老熟妇| 亚洲视频伍月婷婷| 91蜜桃婷婷狠狠久久综合9色| 成人免费黄色短视频| 国产gv| 色综合久久88色综合天天人守婷| 婷婷九九视频| 99婷婷| 97色婷婷| 色五月婷婷视频| 六月婷欧美| 久色网| 日熟女| 九六五月天婷婷| 色色丁香婷婷综合| 成人国产网| 九九Av| 日本婷婷色日| 日本色婷婷久久99精品91| 99日视频在线| 欧美三级巜人妻互换| 五月花成人| 99色1| 丁香六月激情综合| 丁香激情五月天| 思思热视频在线| 丁香六月欧美| 伊人五月久久| 激情综合网丁香| 欧美婷婷综合网| 日产精品久久久久久久蜜臀| 狠狠色丁香婷婷综合| 97色伦另类图片小说视频| 婷婷综合亚洲| 激情玖玖综合网| 玖玖在线视频| 人人草人人舔| 俺去啦综合网| 亚洲性爱干干| 五月丁香性爱| 激情婷婷综合网| 亚洲国产精品VA在线看黑人| 色五月激情网| 丁香花在线视频完整版| 狠色色狠网| 99在线观看视频蜜臀| 99久久婷婷五月综合| 4399精品一区二区| 欧美亚洲色色色色| 久久久久人妻| 丁香五月电影| 亚洲午夜一区二区| 丁香五月婷婷六月| 色婷婷香蕉丁丁网| 另类五月婷婷| 九九视频免费| 91在线日| 日韩肏屄网| 日韩有码一区| 亚洲狠狠色丁香婷婷综合久久| 久久一热| 99久久99九九99九九九| 婷婷五月色惰| 九九视频在线| 十月色综合| 六月天六月婷| 天天摸天天爽| 激情五月天在线观看色婷婷| 日本三级黄色大片| 久久婷婷网| 91一道本| 激情综合婷婷久久| 中文字幕丰满乱孑伦无码专区| XX色综合| 丁香婷婷激情| 亚洲综合色色色| 六月丁香综合| 日韩精品一区二区亚洲AV观看| 五月天激情小说欧美激情| 婷婷丁香五月天狠狠| oumeisesewang| 人人人操Av| 色色五月丁香| 中文字幕在线免费观看视频| 久久五月网| 欧美色图天堂网色| 五月天婷婷色色网| 亚洲色激情| 影音先锋91资源站| 大香蕉Av在线| 五月狠狠| 91综合色| 青青草原亚洲天堂| 色综合综合色| 久久婷婷亚洲| 亚洲另类在线观看| 婷婷导航| 夜夜人妻五月天| 播五月婷婷开心| 狠狠色婷婷在线| 国产亚洲99| 99热永久在线观看| 99r这里只有精品哦| 2050人人操免费工开爱| 日本本土色网第一区| 丁香五月天天| 五月天色婷婷av| 欧美综合激情五月丁香| 久久婷婷色丁香| 手机激情网| 可以直接看的av网站| 激情五月天之五月婷婷| 日韩AV色色色| 六月婷婷九月丁香亚洲综合| 婷婷网五月天| 九月av| www.91久久| 五月丁香偷拍| 九九Av| 婷婷五月天免费99| 五月婷中文娱乐综合| 天天色综| 99热老司机| 无码se| 丁香 婷婷五月| 五月社区婷婷激情| 天天夜夜爽| 亚洲VA口| 亚洲另类电影| 桃色成人网| 美女婷婷激情亚洲| 久热久操久热久草国产91| 丁香六月婷婷久久高清| 开心五月六月婷婷| 亚洲日韩26uuu| 伊人五月丁香| 色色色婷婷| 四虎成人精品永久免费AV九九| 色婷婷五月综合| 日韩av在线免费观看| 国产高清av黄色看片| 九九9久九9国产视频| 丁香色情五月综合激情| 99热在线网站| 天天搞夜夜爽夜夜爽| www.黄色片-久久成人国产精品在线播放-999AV | 久久成人人妻| 97干综合网| 天天日天天摸| 亚洲综合色成丁香五月色| 久久天堂色| 色玖玖综合网| 欧美激情五月天在线观看| 五月天停停基地| 新激情五月天天在线网| 99精色| 《亚洲操B久久免费在线观看,亚洲操B久久在线播放》在线播放 - 高清资源 - 97 | 99re热精品视频国| 五月激情基地| 婷婷九月综合| 久久婷婷五月综合| 婷婷丁香综合| 久热这里只有精品在线观看 | 九九99久久| 色婷五月| 99超级碰碰| 成人无码髙潮喷水A片| 丁香五月瑟瑟| 五月婷婷激情综合| 亚洲婷婷乱乱丁香| 天堂在线中文| 欧美交换配乱吟粗大25P| 婷婷干| 婷婷五月综合久久中文字幕| 成人婷婷五月天| 亚洲五月花| 天天天天天日| 极品嫩草| 五月天综合网| 操操操AV| 五月丁香人妻| 一起草日本| 99亚洲精品视频在线观看| 五月天激情美女久久| 久久超级碰碰| 久久婷婷免费| 婷婷五月丁香基地在线视频官网| 色色COm| 操91| 久草丁香婷婷五月天婷| 天天激情视频| 综合一区二区三区| 欧美日韩成人h| 91操人视频| 五月丁香六月婷婷综合| 色吧五月婷婷| 9久久久| 久久杏爱视频| 五月天伊人久久久久| 影音先锋美国A| 91爱啪啪| 日韩啊啊啊| 久久er99热精品一区二区| 99ri精品在线| 五月天六月婷婷电影| 99精品视频免费观看| www.久久9| www.五月天婷婷姐姐| 婷婷久久99| 日本在线观看aaa 99| 久久婷婷激情五月天一区二区| 人妻久久人妻久久第一区| 欧美精品XXXXBBBB| 色婷婷网| 口述两男一女3p经历| 伊人免费视频9| 五月激情日本在线| 婷婷成人AV| 中文AⅤ大全| 欧美在线骚货| 人人97碰| 99草视频在线观看| 婷婷十月丁香| 免费无码毛片一区二区A片| 99九九综合久久九九| 五月丁香黄色视频| 99精品在线观看| 夜夜夜天天操| 婷婷色在线视频| 五月激情婷婷四射| 伊人丁香花综合影院| 天天操婷婷| 琪琪色五月天| 国产欧美va| 中文AV网站| 插插干干干色| 激情深爱五月天| VA色婷婷| 久9视频免费播放| 日本欧美999久久久三级片| 色狠狠综合网| 另类少妇人与禽zOZZ0性伦| 99日韩| 激情内射人妻1区2区3区| 亚洲影院婷婷色| 亚洲综合婷婷五月天| 欧美性生交A片免费看| 成人精品在线观看| 无码人妻电影| 色综合久久44| 一起草无码| 9久久AV| 日本熟女二区| 亭亭丁香97| 99热这里只有精品最新网址| 爱穴久久| 伊人久久丁香婷婷六月五月综合| 在线播放人妻| 婷婷久久六月费| 国产免费一区二区在线A片视频| 开心五月天私房婷婷| 99九九久久| 久久草大香蕉| 九九碰九九爱97| 亚洲九九夜夜| 色综合99| GOGOGO免费高清日本TV| 猛烈顶弄H禁欲老师H春潮| 欧美碰碰碰| 婷婷精品综合| 五月丁香婷婷老司机| www.五月瑟| 婷婷情色五月| 五月丁香亚洲综合| 九九超碰人人| 草莓视频在线观看入口| 精品99在线| 国产婷婷综合在线免费视频| 五月婷婷偷拍| 亚洲成人网在线观看| 玖玖综合色| 99re免费精品视频| 久久久精品99亚洲综合| 久久99热这里只频精品6学生| 九九视频这里只有精品在线播放| 欧美成人精品A片免费一区99| 色综合爱综合| 五月久久综合| 久久综合丁香激情五月| 亚洲成片在线观看| 国产精产国品一二三在观看| www色五月| 午夜五月天| 99这里只有免费的精品| 久久99热网| 亚洲经典小视频| 第1影院之五月婷婷| 欧美成人AAA片一区国产精品| 人人干99| 五月天婷婷丁香| 久久久月丁香| 婷婷五月精品| 五月综合在线| 国产67194| 少妇高潮呻吟A片免费看软件| 狠狠干激情五月| 色九月丁香婷婷蜜桃在线观看| 99热只有这里有精品| 黄色成人网站在线播放| 思思精品视频| 五月天激情综合10p| 超级碰碰视频无码| 婷婷99热| 色婷婷丁香五月高清在线| 色综合色香蕉网| www.minyis.com【JT】实力收量可预付QQ2101460746 | 婷婷丁香18| 婷婷激情小说| 丁香五月天堂| 无码99| 五月色色激情网| 色噜噜夜夜夜综合网| 亚洲五月天激情| 五月天激情久色| 91嫩草久久| 丁香五月激情综合| 亚洲色色色色| 久久久27操| 99热精品中文字幕| 狠狠五月激情婷婷直播片| 色色婷婷丁香五月天| 色区久久| 99热视精品| 亚洲 视频 导航 一区| 国产看真人毛片爱做A片| 五月丁香婷婷三级| 超碰人人操在线| 日逼AV影音先锋男人资源站| 五月天成人综合| 99热在线爱| 狠狠色中色| 国产操碰| 婷婷五月六月丁香综合| 9操在线| 丁香五月成人| 97色婷婷| 亚洲XX日本| 久久9999| 青青青在线视频国产| 夜夜躁爽日日| 秋霞午夜理论| 大香蕉娱乐| 综合网天天| 人人摸人人搞| 秋霞午夜理论| 九热视频精品| 538在线精品| 66色在线日韩| 六月丁香深深爱| www.日本91| 婷婷亚洲天堂| 人人综合久| 另类图片婷婷五月天| 久久综合中文| 31色区视频免费看| 婷婷五月婷婷| 亚洲婷婷欧美婷婷| 久热最新视频 | 涩五月丁香| 久婷婷| 日韩国产AV播放| 亚州操人在线视频| 色五月人妻| 欧美性丁香色色五月天综合爱爱| 九月色婷婷综合| 婷婷色色五月天| 激情五月天伊人av| 成人精品一区二区三区四区五区| 婷婷五月乱交换| 亚洲精品又粗又大又爽A片 | 99色色网| 五月天婷婷深深爱| 大香蕉五月天| 91久久国产综合久久| 激情五月天影院| 99综合网| 五月丁香久久激情网| 亚洲视频五区| 9一精品视频观看| 996er热| 丁香五月天激情综合| AⅤ色区| 91九色国产| 影音先锋综合网| 国产精产国品一二三在观看| 天堂在线9| 婷婷五月天资源| 丁香五月天激情五月天激情五月天激情网| 日本一级大片| A片天天| 亚州操人在线视频| 久热在线中文字幕色999舞| 五月丁香色婷| 婷婷五月丁香影院| 狼人婷婷综合| 天天射色五月天| 五月丁香大香蕉| 丁香五月播播| 天堂中文8资源在线8| 婷婷精品性性性性性性性| 亚洲夜五月| 丁香综合网| 性爱五月婷婷| 123日本不卡在线| 婷婷五月天在线观看| 九色视频91疯狂| 综合在线色婷婷| 秋霞三及片| 色婷婷婷婷成人网| 亭亭丁香aV| 97视频.干com| 97色图片中文字幕视频在线观看 | 任你搞网站| se影音资源在线观看| 色婷婷五月亚洲| 婷婷五月天色丁香| 99,色| 久久婷婷色情7777网站| 丁香五月黄色| 亚洲天堂色| 国产一级片色色| 久久久99免费视频| 99热在线观看| 五月天激情久久| 色欲AV导航| 伊人五月天婷婷| 天天在线久久综合 | 老妇六区| 成AV人片一区二区三区久久| 在线另类| 五月婷婷三级| 91操片| 夜色综合网| 日本九婷婷| 欧州色色| 99热这里只有精品3| 色5月婷婷| 国内精品玖玖| 五月丁香六月婷婷综合伊人| 激情五月婷婷伊人| 六月婷婷成人| 美女天天久久| 丁香五月六月久久综合| 超碰在线人妻| 六月婷婷天天操夜夜爽视频| www超碰| 九九精品热| 人妻熟妇国产精品| 欧美日韩一a.无| 99在线精品观看99| 日日爱678| 怡红院 久久| 久久亚洲A| 婷婷综合欧美| 亚洲激情淫网| 77799热| 五月丁香少妇网| 激情五月天开心网丁香无码| 丁香六月婷婷高清| 26uuu亚洲色| 天天天天天天天操| 婷婷五月天狠狠| 色色色色色色色色色色色色色色,网站| 五月天影院| 丁香月六月| 六月激情综合| 国产成人精品亚洲线观看| 五月激情网站| 五月婷婷丁香综合| 六月天婷婷| 亚洲国产精品SUV| 亚洲 在线 另类| 五月激香蕉网| 久草嫩草在线观看| 99视频在线观看网址| 五月色婷婷中文字幕| 4399人妻无码久久久| 99热自拍| 婷婷丁香六月影视| 婷婷五月天99| 色狠久| www.夜夜操| 超碰九九热| 久99| 99精品在线观看| 色色网站日本91| 亚洲AV无码成人精品区电影网| 偷偷操99| 亚洲色9| 欧美性爱特黄一级aaaassss| 五月婷婷综合潮喷| 久婷五月| 综合久久97| 国产精产国品一二三在观看| 亚洲欧美日韩VIP| 亚洲欧洲一二| 一区视频网站| 国产精品在线视频| 久久婷婷亚洲五月天| 这里只有精品在线视频在线观看| 91精品国产99久久久久久天美| 精品久久99| 亚洲性爱AV在线| Caoporn公开| 久久婷婷五月丁香网| 婷婷五月天中文字幕.| 五月婷婷丁香六月在线| 婷婷六月天激情| 91精品久久久久久| 狠狠五月天| 久久久久久9热不雅视频| 婷婷六月综合| 五月天色婷好好| 丁香五月天激情网| 亚洲va999成人A片在线观看| 婷婷五月激情小说| 婷婷五月色播天| 97欧美在线| 一起草无码视频| 一本伊人色婷| 久青操| 青草青草视频2免费观看| 99热在线播放精品| 99免费热视频在线| 亚洲 在线 性爱 | 久久亚洲色导航| 欧美日韩一区二区三区四区| 色情五月天丁香社区| 蜜桃人妻无码AV天堂三区| 神马久久五月天| 99re66热这里只有精品| 天天成人丁香美女AV| 性生活视频98791| 香蕉久久国产AV一区二区| 丁香五月激情啪啪啪| 婷婷丁香五月亚洲欧美| 狠狠草综合网| 99久热在线精品| 日本无码专区| 99精品久久久| 激情婷婷狠狠干| 欧美啪啪9| 欧美成人在线观看| 久久久99免费视频| 啪啪激情网站| 欧美性猛交99久久久99| 国产成人AV不卡| 五月天三级久久| 伊人婷婷激情| 五月丁香亭亭操逼| 成人婷婷色综合| 大香蕉人妻| 99色视频免费在线规看| 五月婷婷香| 3DAV亚洲香蕉久久 一区二区| 99热 这里只有精品 国产 日韩| 99精品福利视频| 五月天色婷婷综合| 百度4399有码精品V在线观看| 五月婷婷综合热| 丁香五月婷婷六月丁香| 亚洲最大成人综合网720P| 久Se视频在线观看| 久久深爱激情网| 久99久在线| 操b视频在线观看一区二区| www99热| 狠狠搞狠狠操| 人人爽网| 日韩成人免费电影| 色婷婷丁香| 国产美女无遮挡裸体毛片A片| 玖玖@三月天天丁香婷婷| 97碰碰视频在线观看| 激情综合色五月丁香六月亚洲| 国产无套精品一区二区| 丁香六月婷婷综合啪啪| 久久婷婷欧美| 99热免| 色婷婷瘦婷婷日韩| 精品久久久久久久人妻| 538在线精品| 丁香五月激情综合婷综| 99热777| 激情五月六月婷婷| 激情性爱五月| 婷婷激情六月天视频| 亚洲亚洲人成综合网络| 另类激情五月| 欧美色爱五月天| 婷婷五月天丁香| 99精品热| 色色色在线观看| 99热www| 极品人妻videosss人妻| 人妻久久久久久久| 丁香六月婷婷综合欧美| 婷婷六月五月| 色婷婷8| 蜜臀A∨在线水帘洞| www.五月天色色.com| 国产操逼视频网站| 激情五月六月丁香| 精品国产AV色一区二区深夜久久| 91玖玖| 99色视频| 永久天堂日本| 天天天天天天天操| AV九九| 久热只有这里有精品| 日本三久久| 9 1在线视频| 欧美色爱五月天| 五月天丁香婷婷视频网址| 99亚洲综合| 婷婷久久五月天| www.五月天色色.com| 天天天天操| 五月丁香久久婷| 五月丁香六月婷婷久久久综合| 色播丁香| A一级操| 97色永久免费视频| 热婷婷av| 九九久久99| 囯产精品久久欠久久久久久九大| 精品成人久久久久久久_一二三四视| 丁香五月六月综合激情| 丁香亚洲色综合| 日日噜狠狠色综合久久| 538在线精品| 婷激情五月天视频导航| 99热日韩| 91se在线视频| 99视频久久| 婷婷五月欧美| 五月综合缴情网| www.ywav| 久久这里有精品视频| 《亚洲操B久久免费在线观看,亚洲操B久久在线播放》在线播放 - 高清资源 - 97 | 久久A V无码视频| 影音先锋AV资源男人站| 综合狠狠干| 99riav 亚洲| 久久精品永久免费| www.夜夜操| 五月丁香色播| 婷婷丁香红五月91C| 99热骚货| 色五月婷婷成人| 人妻在线中文字幕久久| 成人AV在线中文版| 精品三区影院| 久久精品熟女亚洲AV麻豆| 思思久热6| 欧美婷婷综合| 91婷婷五月天嫩女| 亚洲人妻电影| 成人va视频| 色综合中文| 色99网| 成人噜噜网| 做爰丰满少妇1313| 伊人超碰| Blackedraw视频一区二区| 色五月婷婷婷婷| 久cao香蕉影院| 天天五月情| 99热久久日本| 激情五月久久| AV网站免费在线| 亚洲欧洲另类| 九九热10| 色五月婷婷成人| 丁香五月婷婷激情蜜桃| 97人妻碰碰碰碰碰久久久久久| 丁香婷婷色五月激情综合| 狠狠色狠狠色综合日日91| 来吧亚洲综合网| 婷婷色丁香五月| 操操碰| 五月社区丁香| 超碰免费人人肏| 丁香成人视频| 999精品乱码77777| 五月婷婷激情久久| 国产精品在线视频| 亚洲九九99精品视频在线播放| 五月天国产婷婷精品视频在线| 日本黄色精品| 99ri国产| 插插插丁香五月婷婷| 5月丁香综合图区| 五月天激情久久| 丁香五月婷婷AV| 亚洲精品久久久久久久久久吃药| 亚洲激情五月丁香久久久久| 性爱激情久久| 婷婷四房播播| 丁香五月花婷婷开心| 丰满老熟妇BBBBB搡BBB| 婷婷五月激情在线视频| 超碰色婷婷| 激情五月天综合| 蜜桃婷婷丁香| 性热视频99精品| 婷婷久久久| 99只有这里是精品| 色播五月综合网| 日韩九区| 五月丁香六月婷婷综合伊人| 丁香婷婷狠狠97| 丁香六月天| 五月婷婷丁香深深爱| 日木WWW视频| 色五月婷婷网| 七七九九色色| 五月婷婷黄网站大全| 久久伦乱| 久久五月天黄色五月天色网址| 色五月激情图片| 欧美大香蕉视频| 色综合久久伊伊婷婷五月| 国产黄色大片| 亚洲综合九九| 天天操夜夜爱| 午夜九九九九九九九九九九九九九| 亚洲精品色| 亚洲精品午夜国产va久久成人| 91视频一起草| 99人妻碰碰久久久禁片| 色就干| 丁香五月天信号| www.一起草av| 色99网站| 五月天久久综合婷婷丁香| 久九色| 人人肏逼视频在线一区二区| 99热| hd五月婷婷在线| 超碰国产av| 99精品偷自拍| 人人摸人人澡人人| 激情五月婷婷网在线观看| 亚州欧美黄色电影| 婷婷色在线观看| 婷婷色激情五月天| 久久婷婷国产| 七月婷婷色香综合网| 99A级片| 五月婷综合网| 久久99久久99精品免视看婷| 综合久久十三| 九九香蕉网| 婷婷五月天亚洲综合| 69热在线| 婷婷性爱综合| 婷婷五月在线观看| 婷婷综合五月| 天天操天天日天天爽| 狠狠色丁香婷婷久久综合| 95精品区一区二| 婷婷无码视频| 激情五月天色婷婷| 亚洲va日| www.五月天婷婷| 国精产品一区一区三区免费视频| 特级毛片AAAAAA| 久久人妻系列| 91丨九色丨大屁股| 人妻Av在线| 成人国产欧美大片一区| 六月色播| 五月婷婷狠狠干| 五月丁香日本片| 五月天婷综合| 久久婷婷五月综合色欧美| 综合久| 狠狠干婷婷| 天天爽,天天操。| 日本三级韩三级99久久| 97热超碰| 亚洲无码色| 亚洲成人AV在线播放| 天天综合在线网| 五月丁香婷婷激情在线| 夜夜资源站| 国产在线视频1234| 国产一区二区av免费| 六月丁香啪啪啪| 婷婷九月丁香| 青青草原99热| 五月激情另类| 天天日夜夜夜操操操操| 久久99激情| 狠狠干天天内射| 色五月婷婷五月天| 五月丁香激情婷婷综合| 丁香五月婷婷狠狠色| 久久婷婷五月天激情| 五月丁香六月停停停| 无码人妻丰满熟妇奶水区码| 99久久www| 久久九九色| 久久丁香久久| 五月丁香六月婷婷免费| 天天日日夜夜爽| 99在线精品视频| 波多婷婷久久| 久久婷婷五月综合| 亭亭玉月丁香| 成人电影一区| 人妻互换HDF中文| 九九热思思| 五月天深爱激情网| 五月天国产成人| 丁香色五月 97干| 久久电影4399| 金品在线视频99| 99情色五月天| 久久婷婷五月丁香蜜桃网| 中文字幕网伦射乱中文| 久久久99视频| 人人草人人舔| 99爱视频在线观看| 久久婷婷综合五月天| 婷婷激情丁五月| 婷婷五月天激情视频| 五月丁香六月欧美综合| 婷婷丁香五月激情综合站_久久五月丁香激情综合_开心五月综合激情综合五月_婷 | 丁香六月久久| 99九无网码| 五月婷婷激情中文字幕| 六月婷婷五月天| 婷婷精品性视频| 五月激情婷婷六月| 丁香五月婷婷激情视频播放| 亚洲狠狠婷婷综合久久久| 欧洲亚洲免费视频区| 五月婷婷综合网| 97久久视频| 97在线视频观看| 91中文在线| www.色五月.com| www.99婷婷| 99久久久免费| 婷婷五月天黄色| 五月综合丁香婷婷| 五月丁香啪综合| 欧美综合123区| 伊人狠狠色婷婷综合丁香一区| 丁香五月www| 99热99| 久久99久久久| 玖色色综合| 亚洲超级碰| 99乱视频| 九九精品99| 中文无码婷婷|