成人精品国产亚洲欧洲-亚洲精品天堂成人片?V在线播放-国产免费一区二区三区-欧美成人片一区二区三区-国产一级特黄在线播放-国产看无码特级毛片-日本一区二区免费精品观看-精品一区二区三区高清免费观看

2024

2024

  • Record 421 of

    Title:Fractional Fourier-Based Frequency-Spatial-Spectral Prototype Network for Agricultural Hyperspectral Image Open-Set Classification
    Author Full Names:Chen, Maoyang(1,2); Feng, Shou(1,2,3); Zhao, Chunhui(1); Qu, Bo(2,4,5); Su, Nan(1); Li, Wei(3); Tao, Ran(3)
    Source Title:IEEE Transactions on Geoscience and Remote Sensing
    Language:English
    Document Type:Journal article (JA)
    Abstract:At present, hyperspectral image classification (HSIC) technology has been warmly concerned in all walks of life, especially in agriculture. However, existing classification methods operate under the closed-set assumption, which deviates from the real world with open properties. At the same time, there are more serious phenomena of different crops with similar spectrums and the same crops with different spectrum in agricultural hyperspectral data, which is also a great challenge to existing methods. In this work, a fractional Fourier-based frequency-spatial-spectral prototype network (FrFSSPN) is proposed to address the challenges of open-set HSIC in agricultural scenarios. First, fractional Fourier transform (FrFT) is introduced into the network to combine the information in the frequency domain with the spatial-spectral information, so as to expand the difference between different classes on the premise of ensuring the similarity between classes. Then, the prototype learning strategy is introduced into the network to improve the feature recognition capability of the network through prototype loss. Finally, in order to break the stubbornly closed-set property of the closed-set classification (CSC) method, the open-set recognition module is proposed. The difference between the prototype vector and the feature vector is used to judge the unknown class. Experiments on three agricultural hyperspectral datasets show that this method can effectively identify unknown classes without sacrificing the classification accuracy of closed-set, and has satisfactory classification performance. ? 1980-2012 IEEE.
    Affiliations:(1) Harbin Engineering University, Coll. of Info. and Commun. Eng. and the Key Lab. of Adv. Mar. Commun. and Information Technology, Ministry of Industry and Information Technology, Harbin; 150001, China; (2) Shaanxi Key Laboratory of Optical Remote Sensing and Intelligent Information Processing, Xi'an; 710119, China; (3) Beijing Institute of Technology, School of Information and Electronics, Beijing; 100081, China; (4) Xi'an Institute of Optics and Precision Mechanics, Chinese Academy of Sciences, Key Laboratory of Spectral Imaging Technology Cas, Shaanxi, Xi'an; 710119, China; (5) Xi'an Jiaotong University, Ministry of Education Key Laboratory for Intelligent Networks and Network Security, Xi'an; 710049, China
    Publication Year:2024
    Volume:62
    Start Page:1-14
    Article Number:5514014
    DOI Link:10.1109/TGRS.2024.3386566
    數(shù)據(jù)庫ID(收錄號):20241615917288
  • Record 422 of

    Title:Optimization Design of Pt/C Multilayer Supermirrors for Hard X-rays
    Author Full Names:Zheng, Renzhou(1); Qiang, Pengfei(1); Yan, Yongqing(1); Li, Yue(1); Zhou, Qingyong(2); Sheng, Lizhi(1)
    Source Title:Nano
    Language:English
    Document Type:Article in Press
    Abstract:Aperiodic multilayers have important applications in hard X-rays astronomical observations due to their broadband responses. This paper presents an optimization model of Pt/C power-law graded stack multilayers using the IMD software. The reflectivity expression of multilayers was derived from the reflection theory of X-ray multilayers and Fresnel recursion formulas. Then, the effects of maximum bi-layer thickness (dmax), ratio of high-density material thickness to bi-layer thickness (Γ), power-law index (c), number of bi-layers (N), grazing incidence angle (φ), interfacial roughness (σ), and photon energy (E) on the reflectivity were analyzed. The calculation results showed that the dmax, Γ and c control the shift of response range, absorption peak and Bragg peaks, respectively. And the decrease of N and increase of φ and σ can result in the reduction of reflectivity at different energies. Additionally, an optimized multilayer structure was proposed according to the extremum of merit function, which can achieve a broadband reflectivity of no less than 0.6 from 1 keV up to 80 keV. These results can provide important references for the response characteristic analysis and optimization design of multilayers. ? World Scientific Publishing Company.
    Affiliations:(1) State Key Laboratory of Transient Optics and Photonics Xian Institute of Optics, Precision Mechanics Chinese Academy of Sciences, Xian; 710119, China; (2) State Key Laboratory of Geo-Information Engineering, Xian; 710000, China
    Publication Year:2024
    Article Number:2450179
    DOI Link:10.1142/S1793292024501790
    數(shù)據(jù)庫ID(收錄號):20245017519343
  • Record 423 of

    Title:All-optical neural network nonlinear activation function based on the optical bistability within a micro-ring resonator
    Author Full Names:Zhang, Hui(1); Wen, Jin(1,2); Wu, Zhengwei(1); Wang, Qian(1); Yu, Huimin(1); Zhang, Ying(1); Pan, Yu(1); Yin, Lan(1); Wang, Chenglong(1); Qu, Shuangchao(1)
    Source Title:Optics Communications
    Language:English
    Document Type:Journal article (JA)
    Abstract:Training all-optical neural networks in itself remains an unresolved problem, and the challenges compound when the problem is turned into the hardware implementations. In this paper, we propose a nonlinear activation function based on optical bistability within a micro-ring resonator (MRR), achieving threshold control without external modulation. Furthermore, a convolutional neural network similar to the Le-Net-5 architecture is designed, in which all nonlinear activation functions are composed of optical bistable hysteresis loop. The numerical simulation results demonstrate that the recognition rate on the Fashion-MNIST dataset can achieve 91.3%, which means that the optical neuromorphic computation can be implemented by utilizing the nonlinear optical effects themselves in the all-optical hardware. Such a scheme promises access to the all-optical neural network training in the optical hardware environment compared to numerical activation functions. ? 2024 Elsevier B.V.
    Affiliations:(1) School of Science, Xi'an Shiyou University, Xi'an; 710065, China; (2) State Key Laboratory of Transient Optics and Photonics, Xi'an Institute of Optics and Precision Mechanics, Chinese Academy of Sciences, Xi'an; 710119, China
    Publication Year:2024
    Volume:558
    Article Number:130374
    DOI Link:10.1016/j.optcom.2024.130374
    數(shù)據(jù)庫ID(收錄號):20240815608927
  • Record 424 of

    Title:Hybrid Fiber-Single Crystal Fiber Chirped-Pulse Amplification System Emitting More Than 1.5 GW Peak Power With Beam Quality Better Than 1.3
    Author Full Names:Li, Feng(1); Zhao, Wei(1); Li, Qianglong(1); Zhao, Hualong(1); Wang, Yishan(1); Yang, Yang(1); Wen, Wenlong(1); Cao, Xue(1)
    Source Title:Journal of Lightwave Technology
    Language:English
    Document Type:Journal article (JA)
    Abstract:A hybrid chirped pulse amplification system composed by the monolithic fiber pre-amplifier and a two-stage single-pass single crystal fiber amplifier was demonstrated. A maximum power of 68 W at the repetition rate of 100 kHz was obtained. The laser pulses were amplified and then compressed using a 1600 line/mm grating pair compressor. A short pulse duration of 358 fs and a power of 54 W were obtained at 100 kHz, corresponding to a peak power of 1.508 GW, to the best of our knowledge, this is the highest peak power ever obtained from single crystal fiber at repetition rate above 100 kHz due to the consideration of the third order dispersion which was engraved in the stretcher and the tuning capacity of higher-order dispersion compensation of chirped fiber Bragg grating. Additionally, the beam quality better than 1.3 was obtained. This high peak power CPA system with excellent comprehensive parameters will find various applications in scientific research and industrial applications. ? 1983-2012 IEEE.
    Affiliations:(1) Chinese Academy of Sciences, State Key Laboratory of Transient Optics and Photonics, Xi'an Institute of Optics and Precision Mechanics, Xi'an; 710119, China
    Publication Year:2024
    Volume:42
    Issue:1
    Start Page:381-385
    DOI Link:10.1109/JLT.2023.3312399
    數(shù)據(jù)庫ID(收錄號):20233814763278
  • Record 425 of

    Title:Upconversion photoluminescence of the lanthanide-doped core–shell luminescent material for anti-counterfeiting recognition
    Author Full Names:Li, Dongdong(1); Zhang, Qianqian(1); Liao, Haibin(1); Fan, Qi(2); She, Jiangbo(2)
    Source Title:Optics Communications
    Language:English
    Document Type:Journal article (JA)
    Abstract:Three different NaErF4:Tm@NaREF4:Er (RE = Y, Lu, Yb) core-shell luminescent material were successfully synthesized. XRD, XPS and other characterization techniques were used to analyze the composed material, morphology, and luminous characteristics of the produced microparticles. Especially, compared with the uncoated NaErF4:Tm, the luminescence intensity of the materials with active-shell structure were increased by 2.44 times, 3.46 times, and 4.01 times respectively under 980 nm laser excitation. Moreover, the generated UCMPs were reliably employed for anti-counterfeiting recognition labels when they were used as screen-printing materials for anti-counterfeiting ink. ? 2024 Elsevier B.V.
    Affiliations:(1) School of Electronic Engineering, Xi'an University of Posts and Telecommunications, Xi'an; 710121, China; (2) State Key Laboratory of Transient Optics and Photonics, Xi'an Institute of Optics and Precision Mechanics, Chinese Academy of Sciences, Xi'an; 710119, China
    Publication Year:2024
    Volume:573
    Article Number:130987
    DOI Link:10.1016/j.optcom.2024.130987
    數(shù)據(jù)庫ID(收錄號):20243516959501
  • Record 426 of

    Title:Enhanced Up-Conversion Emission of NaGdF4: Yb3+ /Eu3+ Crystal via Li+ Doping for Anti-Counterfeiting Application
    Author Full Names:Wang, Chong(1); Ren, Zhong-Xuan(1,2); Li, Dong-Dong(1); She, Jiang-Bo(2)
    Source Title:Guang Pu Xue Yu Guang Pu Fen Xi/Spectroscopy and Spectral Analysis
    Language:Chinese
    Document Type:Journal article (JA)
    Abstract:Rare earth luminescent materials have gradually become a research hotspot in fluorescence anti-counterfeiting because of their high purity of luminous color, long fluorescent life, stable physical-chemical properties, and low toxicity. A series of NaGdF4: Yb3 + / E u 3 + microcrystals co-doped with various Li+ concentrations were synthesized by the hydrothermal method in this paper. The samples' morphology, size, and up-conversion luminescence properties were analyzed by X-ray diffraction (X R D), scanning electron microscopy (SEM), up-conversion emission spectroscopy, and fluorescence lifetime tests. The crystal with strong luminous intensity was further applied to anti-counterfeiting identification. It shows that all the diffraction peaks of NaGdF4: Yb3 + / E u 3 + / L i + microcrystals are consistent with the standard-NaGdF4 card. No impurity peak was found in the XRD pattern. The hexagonal NaGdF4: Yb3 + / E u 3 + / L i + with high purity and crystallinity was synthesized. The SEM image of the crystal shows that the generated sample is a pure hexagonal phase, with uniform distribution, and no reunion. Co-doped Y b 3 + / E u 3 + / L i + has little effect on crystal structure, morphology and size. It can be seen from the up-conversion emission spectrum that the green luminescence intensity of 15 mol% Li+ doped NaGdF4: Y b 3 + / E u 3 + crystal is 6 times higher than that of the undoped Li+ sample. Adjust the power range of the laser to 0. 8 ~ 2 . 2 W and observe the change in UCL intensity of the samples doped with 0 mol% Li+ and 15 mol% L i + . It can be observed that with the increase of pump power, the up-conversion intensity gradually increases. The number of photons required to generate the up-conversion luminescence n is close to 2, indicating that the emission process of the sample is a two-photon process. The fluorescence lifetime of the ° Di level in the sample is about 1. 4 times that of the undoped one. Finally, the NaGdF4: 0. 2Yb/0. 02Eu/0. 15Li crystal with uniform morphology and strong luminous intensity was further applied as fluorescent ink. Screen printing technology printed The fluorescent anti-counterfeiting patterns on paper, glass and plastic. The pattern emitted bright green light under the pumping of a 980 nm laser. In the natural environment, the anti-counterfeiting pattern on the paper has good concealment. The word "safe" lenght is 5. 5 mm, and the spacing between letters is 0. 5 mm. The boundaries between letters are clear and easy to distinguish under 980 nm excitation. The plastic printed with the anti-counterfeiting pattern was exposed to the outdoor natural environment for a month, and the pattern did not change significantly. It shows that the anti-counterfeiting pattern made of NaGdF4: 0. 2Yb/0. 02Eu/0. 15Li has a high resolution, is easy to identify, and is less affected by the environment, and has excellent application prospects in anti-counterfeiting identification. ? 2024 Science Press. All rights reserved.
    Affiliations:(1) School of Electronic Engineering, Xi'an University of Posts and Telecommunications, Xi'an; 710121, China; (2) State Key Laboratory of Transient Optics and Photonics, Xi'an Institute of Optics and Precision Mechanics, Chinese Academy of Sciences, Xi'an; 710119, China
    Publication Year:2024
    Volume:44
    Issue:2
    Start Page:497-503
    DOI Link:10.3964/j.issn.1000-0593(2024)02-0497-07
    數(shù)據(jù)庫ID(收錄號):20240815615655
  • Record 427 of

    Title:Simulation of Polarimetric Photoelectric Process in X-Ray Polarization Detector
    Author Full Names:Zheng, Renzhou(1); Qiang, Pengfei(1); Sheng, Lizhi(1); Yan, Yongqing(1)
    Source Title:Guangxue Xuebao/Acta Optica Sinica
    Language:Chinese
    Document Type:Journal article (JA)
    Abstract:Objective X-ray polarization detection is an important means to study the astrophysical properties of intense X-ray sources such as black holes, pulsars, and related gamma-ray bursts. The development of X-ray polarization detectors with excellent performance is the technical basis for related research. Early X-ray polarization detectors were mainly Thomson scattering polarimeters and Bragg polarimeters. However, due to the low modulation factor and narrow detection energy range, the ideal polarization measurement results were not obtained. In 2001, Costa et al. proposed a new way of X-ray polarization detection using the photoelectric effect, in which the X-ray polarization information was obtained by imaging the photoelectron track produced by X-ray photons through a gas detector. The polarimetric photoelectric process is the key physical process for the detector to realize polarization detection. It is of great significance to clarify the photon-gas interaction process and the distribution law of emitted photoelectrons for further understanding the working mechanism of the detector. The polarimetric photoelectric process is an important research content in the development of this type of X-ray polarization detector. Different types of gases have various properties, which will affect the particle transport in the polarimetric photoelectric process and further leads to different detection efficiencies. Therefore, it is necessary to simulate the polarimetric photoelectric process under different conditions. This can provide a theoretical basis and data support for the structure design of X-ray polarization detectors. Methods We simulate the polarimetric photoelectric process of 2-10 keV linearly polarized X-ray photons in several commonly used working gases by the Monte Carlo code Geant4. The selected working gas combinations include He+ C3H8, Ne+CF4, Ne+DME, Ar+CH4, Ar+CO2, Xe+CO2, CF4+C4H10, and DME+CO2. The response relationship of the emission position and azimuthal angle distribution of photoelectron with the polarization direction and energy of the incident photon is discussed. Moreover, the effects of gas thickness, gas component, gas ratio, and photon energy on the detection efficiency are analyzed. Results and Discussions First, the response relationship of the emission position and azimuthal angle distribution of the photoelectron with the polarization direction and energy of the incident photon is clarified. The emission direction distribution probability of the photoelectron is the largest in the polarization direction of the incident photon, and the azimuthal angle distribution can be approximated as a cosine squared function. With the increase in photon energy, the counts of photoelectrons at each angle decrease in different degrees, but all of them show a statistical law that the maximum values occur when the azimuthal angle is 0 or π (- π) (Fig. 6). Moreover, the effects of gas thickness, gas component, gas ratio, and photon energy on the detection efficiency are revealed and quantified. For 2 keV photons entering into 90%Ne+10%DME gas mixture, when the gas thickness is small, the detection efficiency increases rapidly with the increase in gas thickness, from less than 0. 1 at 0. 1 cm to 0. 64 at 1 cm (Fig. 7). When the gas thickness increases to 3 cm, the detection efficiency is greater than 0. 9. Then, with the increase in gas thickness, the detection efficiency gradually approaches 1. For the CF4+C4H10, Ne+CF4, Ne+DME, DME+CO2, and He+C3H8, the detection efficiency decreases with the increase in photon energy, and the large average atomic number of gas can lead to a high detection efficiency (Fig. 8). While for the Xe+CO2, Ar+CO2, and Ar+CH4, when the photon energy is greater than the binding energy of certain shell electrons of Xe or Ar atoms, the detection efficiency will be improved to a certain extent because the corresponding shell electrons begin to be ejected. In addition to the Ar+CO2 which is affected by the electron emission in K- shell, the detection efficiency in each energy range can be effectively improved by increasing the proportion of gas with high atomic number (Fig. 9). Conclusions We simulate the polarimetric photoelectric process of 2-10 keV linearly polarized X- ray photons in several commonly used working gases by the Monte Carlo code Geant4. The response relationship of the emission position and azimuthal angle distribution of the photoelectron with the polarization direction and energy of the incident photon is clarified. The emission direction distribution probability of the photoelectron is the largest on the polarization direction of the incident photon, and the azimuthal angle distribution can be approximated as a cosine squared function. With the increase in photon energy, the counts of photoelectrons at each angle decrease in different degrees, but all of them show a statistical law that the maximum values occur when the azimuthal angle is 0 or π (- π). Moreover, the effects of gas thickness, gas component, gas ratio, and photon energy on the detection efficiency are revealed and quantified. The larger gas thickness and larger average atomic number can lead to higher detection efficiency. In addition, the increase in photon energy can result in a decrease in detection efficiency. However, for the working gases composed of Xe or Ar, when the photon energy is greater than the binding energy of a certain shell electron, the detection efficiency will be improved to a certain extent because the corresponding shell electrons begin to be ejected. The results in this paper can provide some theoretical basis and data support for the structure design of X- ray polarization detectors. In the actual selection of working gases, the drift properties of electrons in gases, the effect of photoelectron drift and diffusion on track thickness and length, and the reconstruction efficiency of the track reconstruction algorithm should also be considered. ? 2024 Chinese Optical Society. All rights reserved.
    Affiliations:(1) State Key Laboratory of Transient Optics and Photonics, Xi'an Institute of Optics and Precision Mechanics, Chinese Academy of Sciences, Shaanxi, Xi'an; 710119, China
    Publication Year:2024
    Volume:44
    Issue:3
    Article Number:0334003
    DOI Link:10.3788/AOS231631
    數(shù)據(jù)庫ID(收錄號):20241115728993
  • Record 428 of

    Title:Research on High-Precision Quantitative Phase Microscopy Imaging Methods
    Author Full Names:Min, Junwei(1); Gao, Peng(2); Dan, Dan(1); Zheng, Juanjuan(2); Yu, Xianghua(1); Yao, Baoli(1)
    Source Title:Guangxue Xuebao/Acta Optica Sinica
    Language:Chinese
    Document Type:Journal article (JA)
    Abstract:Significance Phase is one of the important attributes of light waves, and its distribution directly affects the spatial resolution of optical imaging and is related to the three-dimensional topography of objects or the refractive index distribution of transparent objects. However, the phase distribution of light waves cannot be directly detected. How to accurately obtain the phase distribution of light waves has become a hotspot in the field of optics. The invention of phase-contrast microscopy has opened the curtain of phase imaging, which has epoch-making significance. It successfully converts the phase distribution of light waves into intensity changes, solving the problem of difficult direct microscopic observation of transparent samples such as cells. Nevertheless, the conversion between phase distribution and intensity change is not a linear relationship in phase contrast microscopy, resulting in phase information that cannot be observed quantitatively. By measuring the phase of light waves, the three-dimensional topography or refractive index distribution of transparent objects can be quantitatively obtained. The refractive index is one of the essential characteristic physical quantities that reflect the internal structure and state of the sample. Therefore, conducting quantitative phase microscopy methods has scientific significance. Quantitative phase imaging has important application value in industrial detection, biomedicine, special beam generation, adaptive optics imaging, and synthetic aperture telescopes. The current quantitative phase microscopy imaging technology mainly obtains the quantitative distribution of phase through interference. Therefore, factors such as the stability of interference devices, limitations on optical diffraction, phase wrapping, coherent noise generated by laser illumination, and sample refocusing during dynamic observation affect the imaging resolution and accuracy of quantitative phase microscopy. Thus, systematic and in-depth research on improving measurement accuracy and stability, spatial resolution, expanding the longitudinal measurement range, suppressing coherent noise, and autofocusing of quantitative phase microscopy imaging has been carried out. A theoretical and technical system centered on high-precision quantitative phase microscopy imaging has been formed. Progress A simultaneous phase shift digital holographic microscopy (DHM) with a common-path configuration has been proposed, which allows the object light and reference light to share the same optical path and components, solving the impact of environmental disturbances on phase imaging fundamentally (Fig. 3), simultaneously recording multiple phase-shift interferograms within one exposure and achieving real-time high-precision quantitative phase imaging. The optical path fluctuation of the system is only 3 nm within 35 min, and the real-time phase microscopy imaging accuracy reaches 4. 2 nm, which is 2. 2 times the accuracy of conventional off-axis interference quantitative phase microscopy imaging (Fig. 5). A super-resolution quantitative phase imaging method based on structural illumination has been proposed. Using the structured light illumination, the spatial resolution of quantitative phase microscopy can be doubled when the spatial frequency of the structural illumination stripe is the same as the highest spatial frequency of the microscopic objective, and super-resolution phase imaging is realized (Fig. 7). A slightly off-axis interference dual-wavelength illuminated digital holographic microscopy has been proposed to expand the longitudinal unwrapped phase measurement range from the wavelength to the micrometer level (Fig. 8), meeting the high-precision phase imaging requirements of thicker samples. Using a low-coherence LED as an illumination light source, the coherent noise in the common laser-illuminated DHM can be reduced by 68% (Fig. 10), and the signal-to-noise ratio (SNR) of images can be improved. The phase measurement accuracy is 2. 9 nm, providing a high-precision solution for the measurement of micro/nano structures and micro electro mechanical system (MEMS) surfaces. Two autofocusing methods based on dual-wavelength illumination and dual beam off-axis illumination have been proposed to meet the autofocusing requirements of high-resolution quantitative phase microscopy imaging for long-term tracking and observation of samples under different conditions (Fig. 11). The former does not rely on the characteristics of the tested sample or other prior knowledge, making it suitable for both amplitude and phase objects. The latter has a simple criterion and can easily determine the optimal imaging surface by reproducing the differences and changes between images, without the need for tedious iterative calculation and with relatively fast processing speed. Conclusions and Prospects Digital holographic microscopy is one of the representative achievements with significant influence and widespread application in the field of quantitative phase imaging, playing an increasingly important role in biomedical, material science, industrial testing, flow field display research, and other fields. We focused on the theoretical and technical issues of high-precision quantitative phase imaging and conducted systematic research on improving measurement accuracy and stability, improving lateral spatial resolution, expanding longitudinal unwrapped measurement range, suppressing coherent noise, and achieving automatic image focusing. With the promotion and application of quantitative phase microscopy imaging technology in other fields such as biological research, high-precision quantitative phase topography microscopy imaging methods will be our future research direction. It is expected that quantitative phase microscopy imaging technology can play a greater role in industrial testing, materials science, and biomedical fields, becoming an indispensable tool for studying the micro world. ? 2024 Chinese Optical Society. All rights reserved.
    Affiliations:(1) State Key Laboratory of Transient Optics and Photonics, Xi'an Institute of Optics and Precision Mechanics, Chinese Academy of Sciences, Shaanxi, Xi'an; 710119, China; (2) School of Physics, Xidian University, Shaanxi, Xi'an; 710071, China
    Publication Year:2024
    Volume:44
    Issue:2
    Article Number:0200003
    DOI Link:10.3788/AOS231191
    數(shù)據(jù)庫ID(收錄號):20240415420637
  • Record 429 of

    Title:Simulation Study on Pulse-Modulated RF-Driven Atmospheric Pressure Argon Dielectric Barrier Discharge
    Author Full Names:Qi, Bing(1,2,3); Tian, Xiao(4); Zhang, Tao(5); Wang, Yishan(1); Si, Jinhai(2); Tang, Jie(1)
    Source Title:IEEE Transactions on Plasma Science
    Language:English
    Document Type:Journal article (JA)
    Abstract:The characteristics of pulse-modulated RF-driven atmospheric pressure argon (Ar) dielectric barrier discharge (DBD) have been investigated, on the basis of a 1-D coupled fluid model. Time-domain variations of the voltage and the charge density on the dielectric surface (Vκ and σ) were obtained for different radio frequency (RF) voltage amplitudes (VRF). Furthermore, the minimum voltage amplitudes of RF maintenance discharge (VRF,min) changing with the pulse duty cycle (DR) and pulse modulated frequency (fRF,p) were discussed, and the variation of spatiotemporal average electron density with spatiotemporal average sheath voltage during the low-frequency period was studied for various DR and fRF,p. It was found that Vκ and σ cannot reach a periodic steady state for smaller VRF. When it increases to VRF,min, or even greater than VRF,min,Vκ and σ reach the steady state and the time for both to reach the steady state is advanced. When VRF is 600 V, it is shortened to 2.36 × 10-6 s (about 32 RF periods), comparing with that when VRF is 280 V. VRF,min decreases as DR increasing from 20% to 100%. The discharge is only in γ mode for smaller DR while it exists in α and γ modes for greater DR. In addition, VRF,min increases along with fRF,p growing from 0.01937 to 0.1356 MHz. When fRF,p is higher, the γ mode exists for discharge, while when it is lower, there are two modes: α and γ. ? 1973-2012 IEEE.
    Affiliations:(1) Chinese Academy of Sciences, State Key Laboratory of Transient Optics and Photonics, Xi'an Institute of Optics and Precision Mechanics, Xi'an; 710119, China; (2) Xi'an Jiaotong University, Faculty of Electronic and Information Engineering, Xi'an; 710049, China; (3) Xi'an University of Science and Technology, Department of Physics, Xi'an; 710059, China; (4) Xi'an Aeronautical Institute, Department of Physics, Xi'an; 710077, China; (5) Xi'an University of Science and Technology, School of Material Science and Engineering, Xi'an; 710059, China
    Publication Year:2024
    Volume:52
    Issue:7
    Start Page:2653-2660
    DOI Link:10.1109/TPS.2024.3419574
    數(shù)據(jù)庫ID(收錄號):20244517316779
  • Record 430 of

    Title:Turbulence compensation with pix-to-pix generative adversarial networks in vector vortex beams
    Author Full Names:Zhang, Zhi(1,2,3); Xie, Xiaoping(1,3); Si, Jinhai(2); Wang, Wei(1,3); Jia, Shuaiwei(1,3); Gao, Duorui(1,3)
    Source Title:Physica Scripta
    Language:English
    Document Type:Journal article (JA)
    Abstract:Orbital angular momentum (OAM) has significantly propelled free space optical communication (FSOC) towards achieving ultra-large transmission capacities, but mode-crosstalk in atmospheric turbulence limits its application. Here, we propose a proof-of-concept turbulence compensation approach utilizing pix-to-pix generative adversarial networks (pix2pixGAN) that does not rely on the wavefront sensor. The model captures the complex relationships between distorted optical fields and phase screens through extensive training, after which the phase screen is directly recovered from the well-trained model by identifying the corresponding distorted image to compensate for distortions. Using this model, the Strehl ratio improvement is measured at 35.7%, 8.9%, and 1.7% under three distinct turbulence conditions, respectively. Furthermore, the recognition of vector vortex beams (VVBs) integrating with the pix2pixGAN significantly improves average mode accuracy from 2% to over 99%. Additionally, the exploration of VVB-based communication further elucidates pix2pixGAN's role in enhancing communication quality. These findings suggest a potential advancement in developing a novel neural network-based strategy to compensate for transmission distortions under intense turbulence. ? 2024 IOP Publishing Ltd. All rights, including for text and data mining, AI training, and similar technologies, are reserved.
    Affiliations:(1) State Key Laboratory of Transient Optics and Photonics, Xian Institute of Optics and Precision Mechanics, Chinese Academy of Sciences, Xian; 710119, China; (2) Key Laboratory for Physical Electronics and Devices, the Ministry of Education, Shaanxi Key Laboratory of Information Photonic Technique, Xian Jiaotong University, Xian; 710049, China; (3) School of Optoelectronics, University of Chinese Academy of Sciences, Beijing; 100049, China
    Publication Year:2024
    Volume:99
    Issue:10
    Article Number:105532
    DOI Link:10.1088/1402-4896/ad74b8
    數(shù)據(jù)庫ID(收錄號):20243817043606
  • Record 431 of

    Title:Enhanced optical nonlinearity of epsilon-near-zero metasurface by quasi-bound state in the continuum
    Author Full Names:Shi, Wenjuan(1,2); Wang, Zhaolu(1,2); Zhang, Changchang(1,2); Zhang, Congfu(1,2); Li, Wei(1,2); Liu, Hongjun(1,3)
    Source Title:Materials Today Nano
    Language:English
    Document Type:Journal article (JA)
    Abstract:Bound states in the continuum (BICs) provide a powerful way to enhance the nonlinear properties of materials, epsilon-near-zero (ENZ) materials are considered as promising candidates with strong nonlinearities. However, the realization of BIC based on ENZ materials in the near-infrared (NIR) is very challenging due to the large loss in the NIR. Here, a high-quality quasi-BIC based on the ENZ metasurface is proposed for the first time, which is composed of patterned ENZ films embedded in a dielectric-metal hybrid structure, and realizes destructive interference between the Berreman mode and photonic mode to form the Friedrich-Wintergen BIC (FW-BIC). The electric field is strongly confined in the ENZ film, resulting in considerable field enhancement, and the nonlinear refractive index coefficient is 1.63 × 10?12 m2/W, which is three orders of magnitude larger than that of the ITO film. The instantaneous response time is 600 fs and extremely high modulation speed up to the THz level. Benefiting from the perfect absorption and narrow linewidth of quasi-BIC and the change in refractive index of the metasurface induced by Kerr nonlinearity, the absolute modulation is from near-zero to 92% with an extinction ratio of 23.2 dB. It provides a promising platform for the development of integrated ultrafast high-speed photonics. ? 2024 Elsevier Ltd
    Affiliations:(1) State Key Laboratory of Transient Optics and Photonics, Xi'an Institute of Optics and Precision Mechanics, Chinese Academy of Sciences, Xi'an; 710119, China; (2) University of Chinese Academy of Sciences, Beijing; 100084, China; (3) Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan; 030006, China
    Publication Year:2024
    Volume:26
    Article Number:100474
    DOI Link:10.1016/j.mtnano.2024.100474
    數(shù)據(jù)庫ID(收錄號):20241315815743
  • Record 432 of

    Title:Underwater image enhancement via color correction and multi-feature image fusion
    Author Full Names:Ke, Ke(1,2,4); Zhang, Biyun(3); Zhang, Chunmin(1,2); Yao, Baoli(4); Guo, Shiping(1,2); Tang, Feng(1,2)
    Source Title:Measurement Science and Technology
    Language:English
    Document Type:Journal article (JA)
    Abstract:The light attenuation underwater causes the actual underwater images to suffer from color cast, low contrast, and weak illumination. To address these issues, an effective fusion-based method is proposed, which realizes color correction (CC), brightness adjustment, contrast, and detail enhancement of underwater images. Concretely, we first design an adaptive CC method via dominant color channel judgment and lower color channel compensation. Then, we detect the brightness of each input image and propose a gamma correction function based on the gradient of the cumulative histogram to adjust the brightness of the low-light images. Subsequently, global histogram stretching and adaptive fractional differentiation techniques are employed to process the brightness-adjusted image, and then the global contrast-enhanced version and detail-enhanced version are generated respectively. To integrate the advantages of both versions, a channel fusion method based on the Lab color space is used to fuse the luminance and color of the two versions separately. The experimental results demonstrate the effectiveness of the proposed method in improving the color and illumination of underwater images, as well as enhancing the clarity of images. Moreover, the testing results on multiple datasets validate the excellent stability of this method. ? 2024 IOP Publishing Ltd.
    Affiliations:(1) School of Physics, Xi'An Jiaotong University, Xi'an; 710049, China; (2) The Institute of Space Optics, Xi'An Jiaotong University, Xi'an; 710049, China; (3) BA Trading(Guangzhou) Co.,Ltd., Guangzhou; 510000, China; (4) State Key Laboratory of Transient Optics and Photonics, Xi'An Institute of Optics and Precision Mechanics, Chinese Academy of Sciences, Xi'an; 710119, China
    Publication Year:2024
    Volume:35
    Issue:9
    Article Number:096123
    DOI Link:10.1088/1361-6501/ad4dca
    數(shù)據(jù)庫ID(收錄號):20242616532375
丝袜灬啊灬快灬高潮了AV| 超碰在线国产| 无码精品久久久久久亚洲| 欧洲av无码| 亚洲欧洲综合| 久久久影院| 在线观看黄色av| 中文字幕一区二区三区四区| 一本无色道高清码| 国产精品免费看| 高清无码在线看| 欧美成人精品| 欧美激情中文字幕| 我和公发生了性关系公| 国产精品电影一区二区三区| 97超人人操| 最新国产成人| 国产三级一区二区| 乱伦一区二区三区| 成人免费黄色| 日韩在线视频一区| 成人av网站在线观看| 久久岛国| 日日日操操操| 国产精品一区视频| 成人免费网站www网站高清| AV怡红院| WWW.操| 日韩久久无码视频| 国产精品亚洲无码| 青青草原影院| 影音先锋男人av| 一区二区三区日韩精品| 午夜AV天堂| 欧美少妇激情| 日韩精品一二三区| 秋霞午夜一区二区三区视频| 国产一区二区视频在线| 亚洲五码在线| 国产视频a| AV在线毛片| 性v天堂| 91AAA在线观看| 国产精品毛片无码一区二区| 色婷婷综合久久| 国产成人精品在线| 91综合网| 人人偷人人摸| 久久黄色大片| 亚洲AV色香蕉一区二区三区老师| 一级黄色电影网站| 精品三级片| 人人肏 人人摸| 伊人成人社区| 免费无遮挡网站| 中日韩无码精品| 91久久精品国产| 91看黄片| 三年片观看免费观看大全| 高清免费av| 最新AV片| 国产亚洲色婷婷久久99精品91| 午夜精品在线观看| 国产日本精品| 午夜免费电影| 性色AV网站| 激情成人综合网| 国内精品久久久| 久久久精品99久久精品36亚| 欧美一区二区三区视频在线观看 | 无码窝AV| 特级毛片绝黄A片免费播冫 | 国产又黄又粗又大| 久久久人人爽爆乳A片| 秋霞午夜一区二区三区视频| 少妇精品无码一区二区免费法国| xxxx黄色| 国产一级精品视频| 好吊妞这里只有精品| 国产成人无码视频一区二区三区| 99久久久无码国产精品怎么下载| 亚洲xx网| 国产一区二区免费| 国产视频不卡| 亚洲欧洲一区| 亚洲黄片在线播放| 亚洲乱色熟女一区二区三区| 91亚洲国产成人久久精品网站| 亚洲无码高清久久精品国产| 国产伦精品一区二区三区高清| 试看日韩黄片| 成人在线网站| 国产SUV精品一区二区69| 激情综合网欧美| 91免费国产| 日韩强犴乱伦AV| 蝌蚪窝视频在线观看| 亚洲91色图| 亚洲三级网| 永久成人无码激情视频免费| 人妻大战黑人白浆狂泄| 97超人人操| 一本色道久久综合亚洲精品小说| 国产精品揄拍一区二区| 亚洲国产高清无码| 婷婷综合久久| 午夜操一操| 伊人三级| 婷婷麻豆| 欧美特黄视频| 国精无码欧精品亚洲一区| 蜜乳无码中文字幕一区DⅤD| 国产电影一区二区三区| 欧美天天干| 女人18片毛片90分钟免费| 久久91亚洲精品中文字幕奶水 | 超碰熟妇| 黄色在线观看国产| 黄色三级片网站| 国产一级黄片| 人人妻人人摸| 99精品免费久久久久久久久| 先锋AV资源| 一级毛片免费| 国产综合一区二区| 欧美a视频| 欧美日日干| 涩涩屋黄| 无码深夜AAA片在线观看| 午夜精品久久久久久久99热浪潮 | 午夜啪啪视频| 久久精品国产AV| 日韩av电影在线播放| 在线观看国产黄片| 玩两个丰满老熟女| 精品一区二区三区中文字幕| 美国AV在线播放| 超碰导航| 麻豆精品一区二区三区av沈娜娜| 国产99久久久国产精品成人免费| 久久久久亚洲Av无码A片| 亚洲成人激情在线| 国产精品―色哟哟| 无码少妇精品一区二区60岁老人| 国产无码小视频| 91精品国产综合久久久久久久| 99久久影院| 国产免费又色又爽粗视频| Av天堂一区二区三区| 女人AV在线| 亚洲一区二区在线播放| 91亚色视频在线观看| 丰满饥渴老女人hd| 人与禽性视频77777| 四川一级毛片免费观看| 1024人妻| 永久免费黄片| 乱伦精品| 午夜国产福利| 污视频在线观看网站| 一级片在线观看视频| 国产精品白浆一区二小说| 精国产品一区二区三区A片| 久久黄色小视频| 国产精品长久久久久久| 国产精品自拍无码| 日韩无码小电影| 亚洲精品国产一区二区| 91AAA在线观看| 中文字幕免费| 欧美日逼| 丁香花高清在线观看完整版| 亚洲人妻系列| 大香蕉超碰| 久久99精品久久久久久水蜜桃| 日韩一区二区在线| 91精品久久久久久久久青青| 狠狠干综合| 中国孕妇变态孕交XXXX| 综合久久一区| 天天夜夜爽| 国产高清无码毛片| 日韩精品中文字幕在线观看| 黄色网页免费| 免费观看黄色网址| av老司机在线| 91丨露脸丨熟女| 亚洲图片欧美视频| 日本免费久久| av老司机在线| 国产A∨| 日本人妻在线播放| 国产精彩视频| 电家庭影院午夜| 黄片免费在线播放| 亚洲中文字幕一区二区| 麻豆三级电影| 欧美性爱免费看| 人人操黄色| 欧美秋霞| 久久精品国产一区二区三区| 911精品国产一区二区在线| 人妻毛片| 91网址| 中文字幕无码高清| 欧美自拍视频| 国产AV资源| 五月婷婷一区| 黄色的操人视频| 91亚洲精品视频| 亚洲欧美日韩精品无码一区二区 | 国产精品久久久久久久久久九秃| 国产中文区三暮区2023| 99亚洲欲妇| 一级黄色电影免费| 亚洲视频www| 亚洲av不卡| 亚洲精品无码AV中文永久在线 | 国产在线综合网站| 人人狠狠| 人人操免费| 人妻一区二区精品| 国产精品黄色| 日韩国产欧美一区| 久久久黄色片| 亚洲精品无码一区二区电影 | 精品国产成人亚洲午夜福利| 18禁美女| 我要看黄色九九片| 国产a区| 极品91尤物被啪到呻吟喷水| 熟妇人妻一区二区三区四区| 国产精品嫩草影院CCm | 九色在线观看| 国产一级黄色| 韩国毛片| 人妻无码久久精品人妻性色AV | 黄色片人人| 久久久久久九九九九| 中文字幕天堂网| 娇妻被交换粗又大又硬影视| 午夜福利成人| 国产无码a v| 丰满少妇高潮久久三区| 91亚洲视频在线观看| 91啪国自产最新91啪国自产| 黄色av网站在线免费观看| 国产成人精品自拍| 99视频内射三四| 午夜福利一区二区三区| 91popny丨九色丨国产| 午夜精品福利视频| 欧美精品福利视频| 91无码人妻精品一区二区三区四| 国产淫荡| 综合国产| 欧美黄色三级片| 日韩成人精品| 精品人伦一区二区色婷婷| 国产一区二区三区免费观看网站上| 香蕉视频免费下载| 国产精品久久久久久久久无码ⅴa| 午夜久久久| 国产又粗又硬| 无码人妻aⅴ一区二区三区69堂| 成人无码AAAA一片黄| 久久久久国色AV免费观看麻豆| 黄色三级片无码| 欧美精品一区二区在线观看| 水蜜桃网站| 少妇放荡的呻吟干柴烈火| 三级片在线播放网站| 国内乱伦视频| 国产小黄片在线| 韩国三级bd高清中字在线观看 | 国产精品一区二区三区在线免费观看| 成人一区视频| 国产精品久久久久久久久久久新郎 | 国产一区电影| 国产一级特黄妇女A片40| 精品无码一区二区| 无码少妇一区二区| jizz欧美大全| 91人妻人人澡人人爽人人精品| 亚洲三级片在线播放| 亚洲无码中文字幕在线| 91免费在线视频| 秋霞国产| 欧韩在线视频| 91n免费处女在线破视频 | 二区三区偷拍浴室洗澡视频| 国产avwww| 日日碰狠狠躁久久躁96AVV| 亚洲精品无线| 中文字幕一二三区| 白浆导航| 中字一区| 国产无码综合| 国产一区二区三区中文字幕| 国产精品久久久久久久久绿色| 亚洲av播放| 欧美写真视频一区| 九草在线观看| 亚洲AV二区| 日韩三级片在线播放| 91日日夜夜| 欧美操逼小视频| 中文字幕精品无码| 国产精品呻吟| 国产伦精品一区二区三区免.费 | 9一操逼| 亚欧无码| 天天干夜夜爽| 国产91九色| 99精品免费久久久久久久久日本| 一级操逼片| 岛国大片在线观看| 西西午夜无码大胆啪啪国模| 日韩精品成人小说网| 日本久久无码高潮喷水电影| 一区二区久久| 三上悠亚中文字幕| 国产香蕉视频| 91午夜福利视频| 少妇人妻真实偷人精品| 熟妇免费视频| 乱伦一区二区三区| 性免费视频| 鲁啊鲁视频| 丁香五月天色婷婷| 乱女乱妇熟女熟妇综合网站| 欧美乱妇狂野欧美在线视频| 久久精品人妻一区二区三区 | 精品无码久久久久久久久成人| 在线免费AV观看| 国产精品久久久久野外| 黄片国产精品| 亚洲AV导航| 一级毛片久久久久久久女人18| 影音先锋av天堂| 91视频精品| 日韩久久人妻| 91精品综合| 国产夫妻性爱自拍| 亚洲AV无码一区二区三区鸳鸯| A级免费视频| 女人久久久| 日韩在线一区二区| 超碰在线导航| 精品人妻伦一二三区久久斗罗| 国产精品1区2区3区| 免费在线成人网| 国产精品久久久久久白浆| 99久久大香伊蕉在人线国产| 天天干视频| 国产91丝袜在线播放九色| 精品一区二区久久| 日本三级网站| 无码专区AV| 国产免费观看AV| 人人摸人人爱人人舔| 国产美女裸体永久免费| 另类欧美| 亚洲国产精品成人综合色在线婷婷| 亚洲五码在线| 五月婷婷视频在线观看| 午夜精品久久久久久| 人人摸人人看| 香蕉视频一区二区三区| 在线免费观看黄网站| 日韩免费看| 高清无码二区| 全肉变态重口调教高辣小说| 天天躁AAAAXXⅹⅩ| 美女视频一区二区三区| 国产日韩欧美| 亚洲午夜精品A片91一91| 国产乱伦自拍视频| 午夜激情AV| 国产乱伦色图| 精品视频在线播放| 久久久久久久久久久99精品无码| 色爱a∨综合区| 4388国产成人无码| 国产黄色影院| 国产乱码精品1区2区3区 | 中国美女一级毛片| 国产一区二区免费看 | 一区二区无码高清| 亚欧洲精品视频在线观看| 黄色国产视频| 国产无套白浆一区二区三区| 人妻九九| 日韩黄片勉费动态| 一级AV电影| 亚洲乱强伦乂 乄乄乄乄9| 一级黄色网| 99婷婷| 丰满少妇伦精品无码专区| 少妇一级A片在线观看妖精视频| 久久精品99| 毛片网站在线观看| 中文字幕婷婷| 内射在线| 欧美性xxxxx| 日韩一级无码| 琪琪午夜福利| 午夜在线观看免费视频| 91麻豆精品秘密入口| 国产精品久久AV无码| 日韩在线观看AV| 久久综合av| 中文在线免费看视频| 五月天婷婷在线播放| AV天堂亚洲无码| 免费无码国产| 日韩欧美一区二区在线| 午夜黄色| 一区二区三区四区在线视频| 国产片av| 99精品一区| 欧美一级在线视频| 人人操摸99| 人妻精品一区| 欧美日韩不卡| 国产精品9| 亚洲精品白浆高清久久久久久| 少妇人妻偷人精品无码视频新浪| 91视频色| 久草中文在线| 性爱无码视频| 国产精品女同一区二区| 一区二区性爱视频| 国产一区在线看| 欧美,日韩,国产精品免费观看| 国产一级毛片视频| 精品久久久久久人妻无码中文字幕| 99精品成人无码A片观看金桔| chinese熟女老女人hd视频| 亚洲无码一区二区av| 精品久久网站| 久久精品7| 国产精品99在线观看| 国产99久久久国产精品成人免费| 三级黄片免费看| 国产精品亚洲精品| 久久无码人妻| 天天躁日日躁狠狠躁| 中文无码熟妇人妻AV在线| 东京热男人的天堂| 国产无码一区二区| 亚洲欧美日韩在线| 欧美裸体XXXX极品少妇| 中文字幕免费| 亚洲综合区| 国产精品网址| 日韩AV午夜| 91久久| 欧美亚洲中文字幕| 91人妻人人澡人人爽人人精品| 免费黄网址| 黄色一级大片在线免费看国产一| 国产精品99精品久久免费| 国产高潮白浆无码| 人人操黄色| 极品美女一区二区三区| 91精品国产色综合久久不卡蜜臀 | 成人黄色在线观看| 亚洲精品第一综合99久久| 亚洲无码短视频| 亚洲黄色片免费看| av中文在线| 97超碰人妻| 国产亚洲精品女人久久久久久| 在线高清免费不卡无码| 欧美日韩一区二区三区不卡视频 | 亚洲色婷婷综合久久久久中文| 天天干天天操天天射| 无码人妻精品一区| 学生妹一级毛片免费播放| 久久理论片| 最新中文字幕| 免费在线观看成人网站| 亚洲无码免费| 亚洲区欧美区小说区在线| 天堂久久精品| 91视频国产精品| 亚洲国产AV片| 91久久国产综合久久| 欧美黄片免费看| 日韩一级视频| 国产一级a毛一级a免费看视频| 久久水蜜桃| 国产精品欧美久久久久天天影视| 亚洲一级电影| 免费国产网站| 国产2区| 欧美av| 亚洲av色图| av电影观看| 国产一级做a爱片毛片A片男| 91高清国产| 丁香五月天在线观看| 91精品一区二区三区久久久久久| 欧美拍拍| 凹凸精品熟女在线观看| 在线观看色| 亚洲欧洲一区二区| 熟女少妇a性色生活片毛片| 日韩无码一级片| 日韩欧美高清| 色综合综合| 凸凹激情在线视频观看| 亚洲天堂| 亚洲黄色在线| 日韩视频免费观看| 欧美色香蕉| 色欲综合在线| 久久精品一区二区三区免费播放| 亚洲黄色在线| 一区二区高清无码| 亚洲免费天堂| 中字幕人妻一区二区三区| 国产婷婷| 国产精品不卡| 日韩欧美一级精品久久| 做a视频| 国产亚洲中文字幕| 欧美日韩偷拍视频| 精品亚洲天堂| 亚洲精品乱码久久久久久麻豆不卡| 亚洲精品无码一区二区三天美 | 免费一级特黄3大片视频| 97国精产品无人区一码二码| 久久久久久18禁欧美| 日韩免费AV| 精品无码人妻一区二区免费蜜桃| 亚洲欧美一区二区精品久久久| www.视频一区| 亚州国产成人精品女人久久久 | 无码一本| 国产真实伦露脸| 成人免费毛片足控| 国产午夜一区二区| 嫩草网站在线观看| 精品无码久久久久久国产牛牛影视| 国产一级a毛一级a看免费软件| 午夜成人在线| 亚洲AV无线在线观看| 九九视频黄色| 在线精品国产| 中文字幕一区二区在线视频| 亚洲黄色电影在线观看| 色婷婷五月天| AV网站久久| 西西大胆人体艺术| 高清无码视频在线看| 91popny丨九色丨白丝| h片在线观看| 国模一区二区| 日韩不卡视频在线观看| 精品爆乳一区二区三区无码AV| 天天草视频| 尤物在线| 免费无码国产在线56| 自拍偷拍第十页| 99久久免费精品国产男女性高好| 精品日韩| 国产一级毛片国语一级A片厂百度| 天天狠狠干| 亚洲一区二区在线看| 欧美另类交在线观看| 国产欧美日韩综合精品| 国产无码观看| 亚洲无码高清在线观看视频| 91久久香蕉囯产熟女线看| 琪琪无码午夜精品久久久久| 最新EESUU在线步兵区| 一区二区三区免费看| 国产真实乱对白精彩久久老熟妇女| 亚洲国产激情| 婷婷一区二区| 日韩三级片网站| 18片毛片60分钟免费| 秋霞在线视频| 日本免费在线视频| 日韩高清在线观看| 日本免费在线| 黄色激情网站| 亚洲精品一区二区三区四区五区六| 久久中文视频| 日韩一级电影在线观看| 99re国产| 国产青草视频| 国产美女裸体永久免费观看网站| 国产免费无码| 久草国产视频| 日韩精品免费在线观看| 凸凹激情在线视频观看| 日韩高清在线观看| 国产一区精品在线| 久久老熟女| 精品无码一区二区三区色噜噜| 人妻体内射精一区二区| 中文字幕免费在线视频| 免费的操逼网站| 国产精品久久久久久久久| 嫖老熟女x88AV| 一本一道久久a久久精品综合蜜臀| 久久黄色大片| 日韩91| 啪啪免费无插件视频| AAAAAAA片毛片免费观看| 亚州AV综合色区无码一区| 湿女导航福利AV导航| 亚洲AV日韩AV永久无码网站| 一级做a视频| 国内精品免费| 国内精品写真在线观看| 真人一级毛片| 亚洲国产精品无码久久久| 欧美日韩高清丝袜| 日韩强犴乱伦AV| 人妻一区二区三区四区| 国产三级视频| 欧美午夜影院| 欧美亚洲日本| 国产做a视频| 日日操夜夜| 91爱爱爱| 欧美另类性爱| 欧美成人一区二区三区| 豪妇荡乳1一5潘金莲| 日韩在线中文字幕| 亚洲欧美在线综合| 久久男人网| 九九久久久精品| 精品一区二区久久久久久无码 | 国产精品久久久久久白浆| 美国一级黄片| 国产免费自拍视频| 国产熟女自拍| 免费18禁| 久久Av一区二区| 天天操天天干| 免费一级大黄片| 乳色AV| 日韩在线观看网站| 国产精品强奸乱伦| 国产精品第1页| 国产最新视频| 国产高清成人久久| 91精品视频在线播放| 国产三级视频在线| 线观看免费完整aaa| 91精品国自产在线偷拍蜜桃 | 亚洲AV激情无码专区在线播放| 色色97| 在线播放国产一区| 国产精品91av| 亚洲AV永久无码精品| 精品久久久久久久久久久下载| 国产一区a| 日韩中文亚洲第一| 在线观看亚洲无码视频| 91久久精品一区二区ww直播| 伊人欧美| 特一级一性一交一视频| 国产精品操| 懂色av蜜臀av粉嫩av分享吧| 性一交一免一费一视一频| 久久久欧美成人片免费看| 另类无码| 秋霞免费视频| 色婷婷91| 中文无码日本一级A片久久影视| 给我免费观看片在线观看中国| 欧美日韩国产精品一区二区| 天天色影院| 国产日韩精品视频一区二区三区| 2019无码| 在线一区二区三区| 国产精品偷伦视频免费观看的| 九九热精品视频| 日本熟妇丰满毛茸茸无码| 91国偷自产一区二区三区老熟女| 国产精品毛片VA一区二区三区| 日韩美亚欧在线视频| 中文字幕在线观看免费视频| 久久久黄色片| 国产精品黄色在线观看| 国产在线真实子伦| 国产热re99久久6国产精品| 国产精品一区二区精品| 一色一伦一区二区三区| 久久久91| 国产精品无码午夜福利免费看| 三级在线播放| 精品成人免费一区二区在线播放| 国产在线视频第一页| 爱搞在线视频| 国产视频一区在线| 91国内精品| 国产三级日本三级在线播放| 精久久久久久| 亚洲三级网| 国产精品久久久久久婷婷天堂 | 四虎欧美| 国产思思久久| 国产伦精品一区二区三区视频金莲 | 天天色色| 伊人成人社区| 成人精品影院| 黄色一级视频| 中文一区| 熟女肥臀白浆大屁股一区二区| 风流少妇精品导航| 国产成人无码一区二区在线观看| 人人爱人人摸| 久久精品国产精品亚洲色婷婷| 久久青青操| 五十路在线| 亚洲一区二区三区四区| 99精品久久| 爱搞视频在线观看| 五月天婷婷激情| 熟妇人妻一区二区三区四区| 国产精品变态另类虐交| 伊人婷婷五月天| 久久久欧美成人片免费看| 影音先锋欧美资源| 亚洲精品在线视频| 人妻中文字幕一区| 天天躁日日躁狠狠很躁| 午夜激情AV| 乱伦天堂| 精品爆乳一区二区三区无码AV| 亚洲电影在线观看| 国产极品在线观看| 红桃av在线| 国产精品99久久久久久人| 久久久精品人妻| 国产69精品久久久久777| 99视频在线看| 久久天堂网| 日韩无码AV电影| 99久久99| AV天堂亚洲无码| 精品国产一区二区三区不卡蜜臂| 日本午夜电影| 亚洲熟女乱综合一区二区三区| 日韩毛片无码| 风流少妇精品导航| 国产精品免费在线| 无码乱伦视频| 青青在线视频| 无码精品人妻一区二区三区综合部| 香蕉网av| 亚洲免费成人网| 欧洲精品一区| 99中文字幕| 欧美日韩一二| 99视频99| 国产高潮视频| 久久亚洲国产精品无码一区| 色吧图片综合| 一级毛片AAAAAA免费看99| 黄色三级片网址| 无码专区在线| 中国黄色一级视频| 国产无码性爱| 午夜视频在线观看免费| 午夜寂寞影院少妇| 91精品电影| 欧美自拍一区| 欧美爆乳一区二区| 无码人妻精品一区二区二秋霞影院| 久久精品午夜| 午夜性色福利视频| 18禁网站在线| 精品二区在线观看| 色婷婷影视| 无码免费观看视频| 一级黄片免费观看| 99热免费观看| 久久久一区二区三区| 国产精品V日韩精品V在线观看| 亚洲视频中文字幕| 国产精品对白久久久久粗| 超碰黄色| 91AV视频在线播放| 三级视频在线播放| 台湾一级黄片| 欧美极品欧美精品欧美图片| 人人操天天日| 蜜桃AV丝袜一区二区三区| 亚洲aa片| 亚洲精品国产suv一区| 成人片在线观看| 擦逼视频国产| 国产A∨| 日本一区二区不卡| 最新国产精品视频| 欧美A级做爰片免费看红杏出墙| 胆小鬼电视剧在线观看完整版| av天天干| 99热这里只有精品7| 国产真实老头老太BBWBBW| 亚洲视频在线看| 美国A v免费观看| 日韩人妻一区| 91av在线播放| 91国内揄拍国内精品对白| 人人操人人模人人看| 人妻饥渴偷公乱中文字幕| 毛片国产| 性爱无码专区| 国产精品成人AAAA网站女吊丝| 久久综合九色综合网站| 免费看黄色大片| 国产一级黄| 精品国产99久久久久久宅男i| 免费AV电影在线观看| 午夜精品一区二区三区在线视频| 亚洲午夜精品| 无码国产精品一区二区| 国产精品成人久久久久| 国产妓女一级在线| 日日碰狠狠躁久久躁96AVV| 精品少妇一区二区三区| 中文字幕三级| 亚洲男人天堂网| 国产三级午夜理伦三级| 日本三日本三级少妇三级66| 久久亚洲区| 久久午夜av| 亚洲一区电影| 香蕉色a片| 1色综合| 欧美性爱视频电影莞式性爱视频电影免费看| 国产露脸91国语对白| 人妻中文字幕在线| 欧美日韩国产电影| 999久久久| 亚洲蜜桃妇女| 国产精品久久久久久久久一区二区三区| 人人妻人人干| 中文字幕一区二区三区乱码不卡| 99re这里只有| 日本a视频| 天天爽夜夜爽夜夜爽精品| 欧美日韩生活片| 国产精品18久久久| 玖玖精品在线| 狠狠躁18三区二区一区| 欧美一二三区| 玖玖在线| 精品自拍AV| 国产性爱一级| 久久久久99精品成人片直播| 无码精品久久一区二区三区武则天| av无码aV天天aV天天爽| 精品婷婷| 欧美电影一区二区三区| 另类视频区| 一级黄色大片| 黄片三区| 国产精品交换| 欧美一道本| 精品欧美久久| 懂色中文一区二区在线播放 | 超碰香蕉| 女人18毛片水真多18精品| 免费的黄色网址| 亚洲av无码一区二区二三区| 最新电影| 亚洲图片欧美另类| 岛国无码| 日本三日本三级少妇三级66| 久草福利在线视频| 久久久久一区| 在线观看第一页| 91成人精品| 伊人黄色电影| 国产精品一区二区三| 国产最新网站| 日本a视频| 日本黄色不卡视频| 国产精品制服诱惑| 香蕉性爱视频| 中文字幕国产| 亚洲一区二区三区视频| 亚洲无码成人网站| 色综合99久久久无码国产精品| 99色婷婷| 91成人在线视频| 人人摸人人操人人| 日本久久高清| 激情婷婷丁香五月天| 天堂中文字幕在线| 人人操狠狠干| 色婷婷九月天天综合| 免费一看一级毛片| 青娱乐免费视频| 国产午夜小视频| 色婷婷一区二区三区久久午夜成人| 91午夜精品| 国产精品不卡一区二区三区| 99福利| 久久综合伊人77777蜜臀| 91亚洲国产成人精品性色| 日韩精品在线视频| 午夜黄色影院| 嘿嘿嘿视频免费网站| 最新国产精品视频| 亚洲精品无码久久久| 午夜精品久久久久久久| 无码深夜AAA片在线观看| 国产导航福利网| 高潮喷水波多野结衣在线观看| 欧美视频一区| 亚洲1区2区| 国产欧美精品| 91天天操| 午夜毛片视频| 国产国产伦女伦一区二区三区 | 成人蜜乳av| 国产激情视频在线播放|