嫩BBB槡BBBB槡BBBB,四川少妇BBW搡BBBB槡BBBB,四川少妇BBB凸凸凸BBB,四川少妇搡BBW搡BBBB,擦老太BBB擦BBB擦BBB擦

2023

2023

  • Record 397 of

    Title:The Multiple Scattering of Laser Beam Propagation in Advection Fog and Radiation Fog
    Author(s):Xu, Qiang(1); Cao, Yunhua(1); Zhang, Yuanyuan(1); Yan, Shaohui(2); Han, Yiping(1); Wu, Zhensen(1)
    Source: International Journal of Optics  Volume: 2023  Issue: null  Article Number: 9715482  DOI: 10.1155/2023/9715482  Published: 2023  
    Abstract:The laser beams were scattered and attenuated when they propagate in fogs for laser communication, laser remote sensing detection. For different density and droplets distribution of fogs, the laser scatter and attenuation are different, the correspond mechanism need thorough investigation. The characteristics of laser beam scattering in different types of fogs are studied based on the droplet size characteristics of advection fog and radiation fog, the scattering coefficients of droplets with different laser wavelengths(0.86 μm, 0.91 μm, 1.06 μm, 1.3015, and 10.6 μm) are calculated, the multi scattering of laser beam is studied by the Monte Carlo method, the propagation path and scattering direction of photons is analyzed, relations between asymmetry factor, albedo of fog droplets, and the visibility are presented, and the forward scattering intensity and the backward scattering intensity versus scattering angle are gotten and discussed. ? 2023 Qiang Xu et al.
    Accession Number: 20230413448214
  • Record 398 of

    Title:Optical Properties of Titanium-doped Gallium Oxide Thin Films by Thermal Atomic Layer Deposition
    Author(s):Li, Cunyu(1,2); Zhu, Xiangping(1,2); Zhao, Wei(1,2); Li, Jichao(1,2); Hu, Jingpeng(3)
    Source: Guangzi Xuebao/Acta Photonica Sinica  Volume: 52  Issue: 6  Article Number: 0631002  DOI: 10.3788/gzxb20235206.0631002  Published: June 2023  
    Abstract:Gallium oxide(Ga2O3)is a wide bandgap(4.8 eV)semiconductor oxide with the advantages of high transparency and excellent chemical and thermal stability. Therefore,Ga2O3 thin film has a wide range of applications in metal oxide field effect transistors,photodetectors and so on. However,the large bandgap of Ga2O3 is unfavorable to the conductivity,which limits the application of Ga2O3 film in optoelectronic devices. The optical and electrical properties of Ga2O3 can be significantly improved by elemental doping,thereby enhancing device performance. The lattice deformation of Ti-doped Ga2O3 (TGO)is small due to the close matching of the Shannon ion radii(0.060 5 nm,0.042 nm)of Ti4+ in octahedral and tetrahedral coordination with Ga3+(0.062 nm,0.047 nm). The reported plasma-enhanced atomic layer deposition at 120 ℃ for the preparation of TGO films requires four precursors:triethyl gallium,oxygen plasma,titanium tetraisopropoxide(TTIP)and H2O. Using H2O as an oxidizer requires long purging times after water vapor exposure and brings in hydroxyl (-OH) impurities at deposition temperatures below 150 ℃. Compared with H2O,O3 has stronger oxidability and higher volatility and does not introduce impurities. In order to avoid the problems caused by using H2O as precursor. TiO2,Ga2O3 and TGO films are prepared by thermal atomic layer deposition using Trimethylgallium (TMG) and Tetrakis-dimethyl-amido Titanium(TDMAT)as precursor sources and O3 as reaction gas at 250 ℃. The Ti-doped Ga2O3 concentration is adjusted by designing the Ga2O3/TiO2 cycle ratio. TGO thin films form sandwich structure through different cycles(9,6 and 3)of Ga2O3 and 1 cycle of TiO2. The growth rates of Ga2O3 and TiO2 measured by spectroscopic ellipsometry are 0.037 nm/cycle and 0.08 nm/cycle,respectively. The growth rate of TGO film is lower than the theoretical calculated value due to the delayed growth of Ga2O3 nucleation caused by the decrease of surface reactive site density after TiO2 growth. The results of X-ray photoelectron spectroscopy show that the concentration of Ti in the film increases with the decrease of Ga2O3/TiO2 cycle ratio,the binding energy of O 1s,Ga 2p and Ti 2p shifts to the lower,which is attributed to the replacement of some sites of Ga by Ti atoms,indicating that Ti elements are successfully doped into Ga2O3 films. The core level spectra of TiO2 and Ga2O3 show the presence of Ti4+ and Ga3+ ions in the films. In the O 1s core level spectra of TGO films,Ga-O bonding decreases with increasing Ti-O bonding content,indicating the formation of Ga2O3-TiO2 composites in the TGO films. The absence of diffraction peaks in the grazing incidence X-ray diffraction spectra indicates that the deposited Ga2O3 and TGO films are amorphous. The surface root mean square roughness of 0.377 nm is observed by atomic force microscopy,indicating that the surface of the film is flat and smooth. This is attributed to the layer-by-layer growth of atomic layer deposition with the advantage of atomic-level thickness control. The TGO films exhibit high transparency in the visible region and strongly absorb ultraviolet light. With the increase of Ti doping concentration,the refractive index of TGO films increases from 1.75 to 1.99 due to chemical changes,the transmittance decreases due to the increase of extinction coefficient in the ultraviolet region,the absorption edge appears red-shifted and the optical bandgap decreases from 4.9 eV to 4.3 eV. The reduced band gap of TGO films can extend the sensitive region of optoelectronic devices to longer wavelengths. The optical band gap of thin films measured by spectrophotometric and X-ray photoelectron spectroscopy shows consistent results. The comprehensive analysis shows that Ti doping has a significant impact on the optical properties of Ga2O3. ? 2023 Chinese Optical Society. All rights reserved.
    Accession Number: 20233014444780
  • Record 399 of

    Title:Investigation on the Preparation of TiO2∶Al2O3 Nanocomposite Film Applied to the Conductive Layer of Microchannel Plate
    Author(s):Li, Jichao(1,2); Zhu, Xiangping(1,2); Li, Xiangxin(3); Hu, Jingpeng(3); Li, Cunyu(1,2); Zhao, Wei(1,2)
    Source: Guangzi Xuebao/Acta Photonica Sinica  Volume: 52  Issue: 6  Article Number: 0631003  DOI: 10.3788/gzxb20235206.0631003  Published: June 2023  
    Abstract:Microchannel Plate(MCP) is a high-gain electron multiplier that consists of a channel-type array of millions of single-channel electron multipliers tightly spaced parallel to each other. MCP is widely used in low-light night vision technology,time-of-flight mass spectrometry,and other fields due to its advantages of high electronic gain,high spatial resolution,high temporal resolution,and extremely low background noise. Traditional MCP is constructed of lead-silicate glass and is created by the processes of stretching,stacking,fusing,slicing,etching,and hydrogen reduction. After hydrogen reduction chemical treatment,a conductive layer and a Secondary Electron Emission(SEE)layer are formed. When MCP works,a DC high voltage is applied at both ends. When electrons or photons enter the channel,they collide with the SEE layer to excite secondary electrons,and then accelerate to bombard the tube wall under the action of an electric field to produce more electrons,resulting in the amplification of the input signal. However,because of the complicated manufacturing process of traditional MCP,its performance is difficult to improve. In recent years,Atomic Layer Deposition(ALD)has given a straightforward solution to the aforementioned issues. ALD is a thin film deposition technology capable of producing very thin conformal films. By exposing the substrate surface to alternate gases for successive surface reactions,the thickness and composition of the film are regulated at the atomic level. ALD can also deposit homogenous nano-films on substrates with high aspect ratio structures at the same time. Based on the benefits of ALD discussed above,the researchers recommend depositing a conductive layer and a SEE layer inside the channel to improve the performance of traditional MCP. Using ALD to functionalize the MCP can remove the functional layer from the glass substrate,allowing for variable modification of the conductive layer and emission layer based on individual demands,therefore simplifying the production process,and improving MCP performance. The MCP conductive layer is responsible for conducting current and supplementing electrons in SEE layer. If the resistivity of the conductive layer is too large,the electron charge of the SEE layer can not be replenished in time,causing the MCP to saturate ahead of time and lower its electrical gain. If the resistivity is too small,the current going through the MCP will be too strong,resulting in a thermal effect and MCP damage. At the moment,the conductive layer films produced by ALD are mainly ZnO∶Al2O3(AZO),W∶Al2O3,and Mo∶Al2O3 composite materials. However,there are several issues with these conductive layer film materials. Because MCP requires a high-voltage environment,but the performance of AZO thin film is unstable and easily broken down under high voltage,and the precursors of W and Mo are costly and very poisonous,there are issues such as safety and economy in industrial mass production. As a result,it is critical to design a novel conductive layer composite film to address both safety and economic concerns. Al2O3 is a typical dielectric material with a high dielectric constant and resistance. TiO2 has excellent electrical characteristics as well as chemical stability. Simultaneously,the precursors of Al2O3,Al (CH3)3(TMA),and the precursor of TiO2,Ti (N(CH3)2)4(TDMAT),have the benefits of cheap cost,non-toxic,and innocuous reaction by-products. In this paper,we propose TiO2∶Al2O3 nanocomposite films as the conductive layer of MCP. Based on the bulk resistance of the MCP,we first calculated the sheet resistance requirements of the conductive layer and found that for a channel with an aperture of 10 μm,a center distance of 12 μm,an aspect ratio of 48∶1,a diameter of 25 mm and a diameter of 20.5 mm in the active area for MCP,when the bulk resistance value is 100~300 MΩ,the sheet resistance value range of the conductive layer should be 1.73×1013~5.20×1013 Ω/. On borosilicate glass substrates, we used ALD to deposit TiO2∶Al2O3 nanocomposite films with varying TiO2 cycle percentages. The square resistance of TiO2∶Al2O3 nanocomposite films is found to be within the required range of the square resistance of the conductive layer when the TiO2 cycle percentage is between 30.27%~ 37.06%. A 20 nm Al2O3 transition layer and a 100 nm TiO2∶Al2O3 nanocomposite film are designed and prepared on a p-type single-sided polished monocrystalline silicon(100)substrate. The thickness of the film is measured by SEM to be 122 nm,and the surface is flat and smooth. Finally,the conductive layer of TiO2∶Al2O3 nanocomposite film in the MCP is prepared. The measured bulk resistance is 212.81 MΩ@ 1 000 V,and the gain is 18 357@1 000 V. To summarize,the TiO2∶Al2O3 nanocomposite film we developed can well meet the requirements of the MCP conductive layer and has the advantages of low cost,high voltage resistance,low corrosivity,and high safety,providing a new material choice for the development of ALD-MCP. ? 2023 Chinese Optical Society. All rights reserved.
    Accession Number: 20233014444820
  • Record 400 of

    Title:Sensitive label-free hemoglobin detection based on polydopamine functionalized graphene oxide coated micro-tapered long-period fiber grating
    Author(s):Li, Yansong(1); Du, Mengyu(1); He, Shuxuan(1); Wang, Ruiduo(2); Zhang, Zaikun(2); Wang, Qiang(1)
    Source: Optik  Volume: 275  Issue: null  Article Number: 170626  DOI: 10.1016/j.ijleo.2023.170626  Published: March 2023  
    Abstract:The GO and PDA-GO functionalized TLPG based sensitive and label-free optical biosensor for human hemoglobin detection was demonstrated. The PDA-GO and GO were separately deposited onto fiber surface, the deposited materials provide a large number of binding sites to adsorb the hemoglobin and can further change the RI of fiber surface, and can provide more binding sites owing to the large specific surface area, and it exhibits higher sensing sensitivity of 3.14 mg/mL and the LOD can reach 0.057 mg/mL. In addition, the sensing was carried out in the presence of inference compounds and also proved its ideal reusability. The usage of PDA-GO as a bio-interface layer enables strong interference of optical waves as well as excellent biocompatibility, which is considered to be valuable for biosensing applications. ? 2023
    Accession Number: 20231113704388
  • Record 401 of

    Title:Theoretical Simulation and Preparation of Anti-reflection Characteristics of Zinc Sulfide Surface Microstructure
    Author(s):Luo, Xing(1,2); Li, Ming(1,2); Mao, Jianyong(3)
    Source: Guangzi Xuebao/Acta Photonica Sinica  Volume: 52  Issue: 7  Article Number: 0752308  DOI: 10.3788/gzxb20235207.0752308  Published: July 2023  
    Abstract:Zinc sulfide is a widely used infrared window material. Due to its high refractive index and strong surface Fresnel reflection,improving its anti reflection performance in the infrared band is of great significance. The traditional method to improve the antireflective performance is to prepare a film on the surface of zinc sulfide,but the antireflective film has the disadvantage of detachment and it is a limited antireflection effect on infrared signals with a wide spectrum and a large angle incidence. Preparing subwavelength structures on the surface of zinc sulfide can effectively improve its antireflective performance. This can be achieved by adjusting the microstructure parameters. Femtosecond laser processing has unique advantages of programmability and non-contact,making it a promising one-step manufacturing method for subwavelength microstructures. In this paper,the finite difference time-domain method is used to simulate the antireflection characteristics of the zinc sulfide surface structure,which is prepared by femtosecond laser processing,and then the infrared transmittance of the structure array surface is measured. This article is based on zinc sulfide material,simulating and preparing one-dimensional strip structure and two-dimensional grid structure and further testing the infrared transmittance of both structures. Firstly,F(xiàn)DTD software was used to simulate and calculate the infrared transmittance characteristics of the zinc sulfide surface structure.Determine the unit structural parameters of the structural array by simulating the height of the strip structure. On this basis,two types of structural arrays with different spacing were designed,and the simulation results showed that as the spacing between structures decreased,the transmittance increased. The trend exhibited by one-dimensional strip structures and two-dimensional grid structures is consistent. Secondly,two types of structural arrays were prepared using femtosecond laser processing. The test results indicate that as the spacing between the one-dimensional strip structures decreases,the transmittance tends to increase,which is similar to the trend shown by simulation. The two-dimensional grid structure with small spacing has higher roughness,so the structure array with 8 spacing has better transmittance. In actual processing,it is necessary to comprehensively consider the influence of surface roughness and ablation degree on the transmittance,and reduce the Fresnel scattering of light waves by edge cracks. Finally,the transmittance of the samples was tested in the range of 7~10 μm in the mid to far infrared bands. The structure array with a spacing of 5 μm increases the infrared transmittance by approximately 6% at wavelengths 9.5~10 μm. The grid structure with a spacing of 8 μm can increase the average transmittance by 4% in the 8.5~10 μm bands and nearly 7% at the 10 μm wavelengths. In addition,the transmittance spectrum measured in the experiment has good transmittance in the long wavelength range,which is related to the scattering effect of nanoscale structures generated by laser processing at different wavelengths,the surface scattering effect of non-uniform micro nano composite structures is more pronounced at shorter wavelengths. Compared with the simulation result,it was found that the overall transmittance of zinc sulfide decreased. The overall decrease in the transmittance of zinc sulfide samples is related to two factors:the first reason is the light absorption effect caused by structural defects in femtosecond laser processing,part of the light is absorbed by zinc sulfide,and the second reason is the diffraction and light scattering effects caused by non-uniform surface particulate matter generated by laser processing,which deflects the incident light along the beam transmission path. The experimental results indicate that the prepared structure has good anti-reflection performance,indicating that the method used in this paper has a positive effect on improving the transmittance of zinc sulfide. This provides a reference for studying the transmittance of zinc sulfide in the mid-infrared band. ? 2023 Chinese Optical Society. All rights reserved.
    Accession Number: 20233714721524
  • Record 402 of

    Title:D-shaped terahertz microstructured fiber biosensor based on plasmon resonance on graphene surface
    Author(s):Zhang, Yani(1,2); Xue, Jia(1,2); Zhang, Yunxia(2); Miao, Ting(2); Yao, Yiming(2); Wang, Qiuyang(2); Gong, Jiaqin(2)
    Source: 2023 21st International Conference on Optical Communications and Networks, ICOCN 2023  Volume: null  Issue: null  Article Number: null  DOI: 10.1109/ICOCN59242.2023.10236355  Published: 2023  
    Abstract:This paper designs a D-shaped microstructured fiber optic biosensing model based on surface plasmon resonance of graphene, which is dedicated to the terahertz frequency band. Improving optical fiber sensing performance by adjusting graphene thickness and graphene chemical potential to increase peak spectral loss. The optimization results show that the resonance peak decreases with increasing excitation layer thickness and graphene chemical potential. Moreover, the higher the graphene chemical potential, the more the resonance spectrum is shifted towards the higher frequency band. The maximum frequency sensitivity is 1300 GHz/RIU over a refractive index sensing range of 1.1-1.5, corresponding to a quality factor of 1.0× 10 4 RIU. In conclusion, the proposed D-type microstructured optical fiber has a novel and ingenious structure with high detection accuracy. With graphene as the excitation medium, the microstructured optical fiber operating band is successfully extended to the terahertz band, opening up a broader application prospect for the microstructured optical fiber structure in the THz sensing field. ? 2023 IEEE.
    Accession Number: 20234014844507
  • Record 403 of

    Title:Analysis of Trace Metal Elements in Water Based on Discharge-Assisted Laser-Induced Breakdown Spectroscopy
    Author(s):Xu, Boping(1,2); Liu, Yinghua(1,2); Liu, Zaihao(1,2); Yin, Peiqi(1,2); Tang, Jie(1,2)
    Source: Diangong Jishu Xuebao/Transactions of China Electrotechnical Society  Volume: 38  Issue: 17  Article Number: null  DOI: 10.19595/j.cnki.1000-6753.tces.L10087  Published: September 2023  
    Abstract:Heavy metal ion-induced water pollution has become a severe environment in the world. Laser-induced breakdown spectroscopy (LIBS) is a novel analytical technique based on the atomic emission spectroscopy, which can be used for the target in any state. Thus, LIBS is widely applied in various applications, including environmental pollution monitoring, food safety, and chemical engineering production. However, for liquid sample detection, the rapid quenching of the plasma, the contamination of the optical system by the unstable liquid level, and the limited laser energy absorption of the plasma have limited the further development of LIBS technology. Here, a discharge-assisted LIBS technique (D-LIBS) for the detection of trace elements in solutions is proposed and compared with the conventional LIBS (C-LIBS). Rapid sampling of mixed BaCl2 and NaCl2 solutions is performed using medium-speed filter paper. A Nd:YAG laser is implemented to generate plasmas containing the target elements on the filter paper. A discharge assistance consists mainly of a high voltage DC power supply, a capacitor, and a pair of rod electrodes. The capacitor is first charged by the high voltage DC power supply. The electrodes are respectively connected to the positive and negative terminals of the capacitor, and placed horizontally on the surface of the filter paper. Once the sample surface is ablated by the focused laser beam, the pre-existing plasma between the electrodes acts as the seed charged particles in the discharge gap, which rapidly ignites a strong discharge there. Compared to the time-integrated spectra in C-LIBS and D-LIBS, the LIBS signal has been greatly increased by using the discharge assistance. Emission lines of BaⅡ455.40 nm and NaⅠ588.99 nm are respectively enhanced to 30-fold and 6-fold. The spectral intensities in C-LIBS and D-LIBS are positively correlated with laser energy. However, the spectral enhancement factors show higher values at small laser energy conditions, and the BaⅡ spectral enhancement factor decreases from 30 (20 mJ) to 2 (50 mJ) with increasing laser energy. Compared with the spectral signal-to-noise ratio (SNR) in C-LIBS, D-LIBS results in a SNR enhancement of more than 1 order of magnitude. When the laser energy is 20 mJ, the SNR enhancement factor of BaⅡ spectral line and Na I spectral line is 56 and 16, respectively. In addition, the quantitative analysis performance of C-LIBS and D-LIBS for trace metal elements in solution under different laser energy conditions are comparatively studied. The limit of detection (LoD) of Ba is decreased along with the laser energy in C-LIBS, reaching 0.823 mg/L at 50 mJ. Moreover, under the optimal condition the LoD is reduced from 12.5 mg/L in C-LIBS to 0.26 mg/L in D-LIBS, and the detection sensitivity of LIBS technique is increased by 47-fold due to the discharge assistance. The following conclusions can be drawn from the experimental results: (1) The spectral intensity, SNR can be enhanced by over 1 order of magnitude. The increases in the intensity and SNR of the plasma spectra are due to the additional electrical energy injection resulting in the reheating and excitation of the plasma. (2) The spectral intensity and SNR are positively correlated with laser energy. The enhancement factor reaches the maximum in the smallest laser energy condition. This is due to the fact that the lower the laser energy, the smaller the mass of sample ablated, and therefore the more significant the enhancement effect is when the plasma is excited by the additional discharge. (3) The quantitative analysis of LIBS can be efficiently enhanced over 1 order of magnitude by the discharge assistance. And the LoD is reduced to 0.26 mg/L which is 1/48 of the original level. ? 2023 Chinese Machine Press. All rights reserved.
    Accession Number: 20234214885766
  • Record 404 of

    Title:Engraving Depth-Controlled Nanohole Arrays on Fused Silica by Direct Short-Pulse Laser Ablation
    Author(s):Liu, Xin(1,2); Clady, Rapha?l(1); Grojo, David(1); Utéza, Olivier(1); Sanner, Nicolas(1)
    Source: Advanced Materials Interfaces  Volume: 10  Issue: 7  Article Number: 2202189  DOI: 10.1002/admi.202202189  Published: March 6, 2023  
    Abstract:Periodic nanohole arrangements constitute an important building block of advanced photonic devices. Aside from standard nanofabrication tools, a direct laser-based approach is introduced here, that enables single-step and point-by-point machining of arrays of holes with subwavelength diameters and depths reaching several micrometers at the surface of fused silica. The method relies on a simple optical arrangement including an axicon combined with an amplitude mask to shape the laser intensity in appropriately truncated micro-Bessel beams of adjustable length. The suitability and limitations of the technique are investigated to fabricate arrays of cylindrical nanoholes with tunable depths. In particular, the challenge of avoiding crosstalk effects during the laser-writing process of high-density arrays is explored. The achievability of square arrays of nanoholes at the surface of fused silica, with diameters down to 200?nm and variable depths from 3 to 20?μm at a spatial density defined by a pitch of 1.5?μm is demonstrated. The performance level shows the potential of the direct-laser-processing method towards the realization of integrated devices, offering a highly flexible and cost-effective alternative technique to current nanofabrication methods. ? 2023 The Authors. Advanced Materials Interfaces published by Wiley-VCH GmbH.
    Accession Number: 20230513463019
  • Record 405 of

    Title:High Photon Efficiency Image Reconstruction Algorithm Based on Depth Range Selection for Single Photon Counting LiDAR
    Author(s):Meng, Fanxing(1,2); Zhang, Tongyi(1,2); Kang, Yan(1); Xue, Ruikai(1,2); Wang, Xiaofang(1,2); Li, Weiwei(1,2); Li, Lifei(1)
    Source: Guangzi Xuebao/Acta Photonica Sinica  Volume: 52  Issue: 9  Article Number: 0910001  DOI: 10.3788/gzxb20235209.0910001  Published: September 2023  
    Abstract:Photon counting imaging technology is a new type of active imaging technology,which obtains depth information of the target by accumulating histograms of echo photons. It can be combined with Time-correlated Single-photon Counting(TCSPC)to achieve high temporal resolution. Compared with passive imaging systems,it has stronger robustness and is widely used in fields such as biomedicine,target recognition and remote sensing imaging. But it takes a long time to accumulate thousands of echo photons. In some environments with low Signal-to-background Ratio(SBR)and very few echo photons,such as military reconnaissance and other fields,long-term data collection can not be satisfied,and the ability to reconstruct 3D scenes is affected by noise photons and vacant pixels. This paper proposes a high photon efficiency image reconstruction algorithm based on depth range selection. The algorithm achieves strong resistance to noise and fully improves photon utilization efficiency through two steps:selection of target depth range,adaptive supplementation and TV regularization. Specifically,the selection of the target depth range allows us to gain depth range at the initial stage of the reconstruction process,paving the way for subsequent processing. This process is divided into five steps:merging all data into histogram,peak searching for the histogram,potential signal range determination,signal range review and select signal range. These five processes can ensure that the depth range we obtain is more accurate than setting threshold gating to the histogram. The photon screening process can remove all the noise outside the depth range,thereby reducing the error we introduce when we fill in the vacant pixels. Compared with relying on fixed neighborhood data to supplement vacancies,supplementation using adaptive neighborhood data has a higher photon utilization efficiency and will be more suitable for environments with very few echo photons. Finally,TV regularization is used to smooth the residual noise in the depth range. The simulation and experimental process have verified that even in the case of low SBR and very few echo photons,our algorithm can still effectively reconstruct the 3D image of the scene. We reconstructed the simulation data of different degrees of echo photons when SBR=0.04 and compared it with the high photon efficiency algorithm and the Unmixing method. We also input the data preprocessed by the proposed method into the Unmixing method for processing (Preprocess-unmixing,PP-Unmixing) to verify the contribution of accurately selecting the target depth range. The preprocessing here only includes the selection of target depth range. The results show that our method can distinguish scene edges in any case, and the reconstruction effect and RMSE are better than the other three methods. Our proposed method is also a fast reconstruction method. In addition,a comparison between the PP-Unmixing method and the Unmixing method proves the necessity of accurately selecting the target depth range. In addition to the simulated data,two experimental scenarios further verify the feasibility of the proposed algorithm. In experimental scenario 1,SHIN D's method can not accurately estimate the depth range,resulting in a large deviation in the reconstructed depth map. And as the number of echo photons decreases, the image becomes increasingly blurred and the scene cannot be resolved,even though it has a fast reconstruction speed. The Unmixing method is better than SHIN D's method in terms of reconstruction effect,but it still can not completely reconstruct the scene in the case of fewer echo photons,the filtering for noise is not thorough enough,and its running speed is still the slowest. The method proposed in this paper can clearly distinguish the scene in any case. Even in the extreme environment with SPPP=0.47,the time-consuming and RMSE of results are only 0.032 m and 37.2 s. In experimental scenario 2,our method can retain more detailed information than the other two methods,especially in the extreme case when the SPPP=0.7,and the other two methods can hardly detect the house information. Further,in terms of RMSE and time consumption,SHIN D's method is the fastest,but its RMSE is the largest,and the RMSE of the Unmixing method is comparable to our method, but the reconstruction speed is still the slowest. Therefore, our method has more advantages in comprehensive ability and is more suitable for an environment with few echo photons and low SBR. In summary,our method has a significant reconstruction effect on both simulation data and experimental data,which proves that this method is more suitable for the situation of extremely low SBR and a very small number of echo photons. In terms of computing speed,it is also a fast reconstruction method. In addition,the proposed method has better applicability to the situation where there are multiple depth targets in the scene,and further research and verification will be carried out in the future. ? 2023 Chinese Optical Society. All rights reserved.
    Accession Number: 20234014834427
  • Record 406 of

    Title:Generation of Q-switched fiber laser based on ferroferric oxide in 1.55 μm region
    Author(s):Nie, Liang(1); Duan, Zhixia(2); Liu, Ruisheng(3,4); Zhang, Danni(1); Li, Xiaohui(3); Wang, Wei(1); Gao, Cunxiao(4); Xue, Mingyuan(4)
    Source: Infrared Physics and Technology  Volume: 134  Issue: null  Article Number: 104876  DOI: 10.1016/j.infrared.2023.104876  Published: November 2023  
    Abstract:To improve the performance of fiber lasers, a Q-switched fiber laser based on iron oxide nanomaterials was developed. The pump power was gradually increased, and the corresponding data of the Q-switched pulse frequency and spectral width were recorded. When a pump power of 170 mW was reached, the Q-switched pulse frequency of 48.45 kHz, pulse width of 2.3 μs, center wavelength of 1530.4 nm, and spectral width of 3.8 nm were observed and recorded. The Q-switched pulse frequency was increased from 30.53 kHz to 58.74 kHz, along with an increase in the pump power from 45 mW to 250 mW. The spectral width was decreased from 7.31 nm to 2.04 nm, and this change was duly recorded. The Q-switched fiber laser demonstrated has good output characteristics and can be applied to scientific research, medical treatment, industrial processing and other fields. ? 2023 Elsevier B.V.
    Accession Number: 20233714715325
  • Record 407 of

    Title:Compact lensless optoelectronic convolutional neural network for image classification
    Author(s):Zhang, Zaikun(1,2,3); Da, Zhengshang(3); Kong, Depeng(1); Wang, Ruiduo(1,2); Mu, Qiyuan(1,2); Wang, Shijie(1); Geng, Yi(4); He, Zhengquan(1)
    Source: Proceedings of SPIE - The International Society for Optical Engineering  Volume: 12935  Issue: null  Article Number: 129350F  DOI: 10.1117/12.3000602  Published: 2023  
    Abstract:Recently, free-space optical neural networks (ONNs) have gained extensive interest as emerging machine learning platforms for implementing artificial intelligence tasks, such as image classification. Despite various optical implementations of electronic neural networks (ENNs), the bulky volume of optical components remains challenging to deploy edge devices, such as Internet of Things peripherals, wearable devices, and camera. To address this problem, we propose a compact lensless optoelectronic convolutional neural network (LOE-CNN) architecture with a lensless optical analog processor utilizing a single optimized diffractive phase mask (DPM) to perform convolution operations without Fourier lens. Comparing the processor with a commercially available NVIDIA A100 Tensor Core GPU in terms of speed and power, indicates the optical computing platform enables to replace the electronic processor in latency reduction and energy savings. Furthermore, we compare the LOE-CNN with two all-electronic neural networks (i.e., fully connected neural network [FC-NN] and convolutional neural network [CNN]) over the Modified National Institute of Standards and Technology (MNIST) dataset and Fashion-MNIST dataset, respectively, and demonstrate that the LOE-CNN can be functionally comparable to existing electronic counterparts in classification performance. My study not only opens up new application prospects for free-space ONNs based on compact lensless single-chip convolution processor, but also facilitates the development of ONNs-based smart devices. ? 2023 SPIE.
    Accession Number: 20235015220890
  • Record 408 of

    Title:High-precision gaseous flame temperature field measurement based on quadriwave-lateral shearing interferometry
    Author(s):Yuan, Xun(1,2); Xue, Yuge(1,2); Min, Junwei(1); Yu, Xianghua(1); Li, Manman(1); Li, Runze(1); Yao, Baoli(1,2)
    Source: Optics and Lasers in Engineering  Volume: 162  Issue: null  Article Number: 107430  DOI: 10.1016/j.optlaseng.2022.107430  Published: March 2023  
    Abstract:Quadriwave-lateral shearing interferometry (QLSI) has a broad utilization in quantitative phase imaging (QPI) for refraction-type objects due to its compact structure and stable performance against external disturbance. Here we propose to use the QLSI technique to image and measure the gaseous flame temperature field distribution in high precision. The quantitative phase image of an axisymmetric candle flame is firstly reconstructed from the wire-mesh-like QLSI interferogram, and then the three-dimensional temperature field distribution is calculated with the axisymmetric projection transform algorithm. Compared to the conventional digital holographic interferometry (DHI) based on Mach-Zehnder architecture, the proposed method possesses a high-precision measurement and better stability in disturbed environment, benefiting from the compact common-path structure of QLSI. The temperature measurement errors of the proposed QLSI method are ±5.0 K and ±5.3 K in the presence of airflow disturbance and mechanical vibration, respectively, while those of the DHI method are ±7.6 K and ±12.9 K, respectively. ? 2022 Elsevier Ltd
    Accession Number: 20230213361633
婷婷五月18永久免费网站| 亚洲V国产V欧美V久久久久久| 超碰在线成人| 香蕉久久国产AV一区二区| 色天使久久综合| 天堂久久大香蕉| 九九色图| 九九视频精品在线免费| 亚洲经典小视频| 欧美乱大交XXXXX潮喷l头像| 九九av| 麻豆WWWCOM内射软件| 国产精品成人AV在线观看春天 | 色五月综合激情| 婷婷丁香五月色| 国产97色在线 | 日韩| 亚洲综合五月天婷婷丁香| 激情综合视频| 亚洲成人另类| 亚洲婷婷六月天| 久久 视频这里只有精总| 色色色综合| 婷色五月天| 天天日日| 久久婷婷五月天懂色| 色五月婷婷开心| 性爱视频久久| 久久免费少妇高潮99精品| www.com任你艹| 综合久久99| 五月天社区狠狠| 国产精品视频| 久久人妻超碰一区| 成人五月天丁香| 色婷婷五月天天天天天天天天天| 久久亚洲天堂| 啪啪啪大香蕉| 色婷婷电影网| 久久这里有精品视频| 久久色五月| 变态 另类 在线 | 激情六月婷婷| 99色爱| 欧美激情综合色综合啪啪五月| 日韩砖区| 色135综合网| 婷婷综合久久| 色啪影院| 狠狠做深爱婷婷久久综合一区| 色啪综合| 婷婷久久婷婷| 婷婷五月永远18免费久久久| 天天综合五月天| 色亭亭影园| 91综合国免费久入| 天天爱夜夜爽| CHINESE熟女老女人HD视频| 玖玖爱导航| 69五月天视频| 天天干天天拍| 日韩成人电影在线播放| 热99re| 伊人网碰碰| 91碰碰视频在线观看| 久久之人妻| 草综合14| 最近免费中文字幕大全高清大全1 99国产精品久久久久久久久久久 AA片在线观看视频在线播放 | 狠狠色成人影片| 成人AV网站在线| 久久婷婷婷婷伊人| 桃色五月天| 九九热99免费视频| 26uuu精品国产| 国产肥白大熟妇BBBB视频| 91色噜噜狠狠狠狠色综合| 俺去啦综合网| 深爱综合网| 超碰精品国产首页| 五月天婷婷五月| 五月丁香偷拍| 丁香婷婷黄网站| 五月丁香淫淫婷婷婷| 久久伊人五月天| 开心五月婷婷五月| 9热视频在线观看| 热996精品在线观看| 囯产精品一品二区三区| 97超碰,人人舔,人人操,人人摸 | 五月婷婷二月丁香| 婷色五月| 九九视频免费| 激情婷婷五月天| 丁香情色五月| 丁香六月婷婷综合激情欧美 | 日本色色网| 婷婷五月天激情网| 久久婷婷五月综合激情国产| 五月色婷婷夜色| 26uu| 精品一区二区三区四区五区六区| 国产成人网站在线观看| 激情五月狠狠| 色呦呦在线| 狠狠人妻久久久久久综合丁香| 久久激情综合| 99re热在线观看| 五月色综合网| 狠狠狠狠青草| 色色色色色网站| 黄色片avv| 婷婷五月开心中文字幕在线| 永久精品| 蜜乳9188| 久久98| 在线视频另类| 亚洲综合视频网| 天天日P天天射P| 性色99| 中国丰满熟女A片免费观| 五月婷久久| 99热在线这里| 五月天大香蕉视频| 天天碰夜夜爽| 国产亚洲色婷婷久久99精品9j| .操區COm| 久久婷五月| 六月丁香综合999| 欧美大肥婆大肥BBBBB| 思恩热国产视频右线观看| 婷婷综合色| 密乳Va| 小视频在线观看| av免费在线网站| 天天做天天爱| 日本一级一片免费视频| 99操逼| 五月停停999| 日本九九视频| 丁香色五月 97干| 日本色天堂| 婷婷五月丁香久久| 99爽视频| 婷婷五月天播| 任你草| 欧美毛片www| 欧美成人精品三区综合A片| 天天日狠狠| 六月婷婷色综合| 久久人妻乱子伦| 中文字幕无码人妻少妇免费视频| 深爱激情AV| 精品香蕉99久久久久网站| 九九这里有精品视频| 欧美顶级少妇做爰HD| 最新午夜理论片| 99热免费观看| 婷婷五月天日日日干干干| 五月丁久久| 久99热| 超级碰碰视频无码| 日本色99| 国产片天天爽夜夜爽| 高清无码网址| 开心亚洲久久开心| www,99视频| 亚洲另类视频| 亚洲av免费在线| 九九久久网| 性小说五月天| 九九热内射| 亚洲中文字幕在线观看| 99久久九九| 啪啪一区| 丁香五月婷婷日本| 国产熟女大叫受不了| 九九色人| 五月在在观看| 超碰cap| 婷婷五月天视频免费在线观看| 超碰成人在线观看| 免费无码毛片一区二区A片| 婷婷五月天AV网| 亚洲妇女熟BBW| 久噜久噜| 色婷婷久久综合久色综| 成人精品视频99在线观看免费| 狠狠色精品综合| 婷婷黄色网| 性做久久久久久久免费看| 思恩热国产视频右线观看| www.婷婷| 激情六月色| 9久久精品| 五月综合色| 最新丁香六月婷婷| 亚洲色综合| 婷婷五月天成人网| 五月天精品视频| 97超碰欧美中文字幕| 人人操97| 天天舔日日肏夜夜爽| 五月久久网| 久久这里只精品| 99热99热| 99黄色性生活| 丁香99| 99热免费| 另类综合国产| 九月丁香亭亭| 99超碰欧美| 欧美乱大交XXXXX潮喷l头像| 九九AV| 九九爱激情| 9有码中文| 另类激情五月| 农村熟妇高潮精品A片| 欧美黄色韩日网| 97九色| 天天色综网| 五月狠狠| 99er视频在线| 色一情一乱一乱一区91Av| 五月天综合网| 婷婷五月丁香久久| 99网| 九九色影院| 中文无码婷婷| 色亭亭丁香五月天| 狠狠综合| 99re在线播放| www.色五月天.com| 激情五婷精品网在线观看网址| 99碰碰碰| 亚洲视频一区| 五月天婷婷色色网| 丁香五月天BBw| 丁香五月色情| 一婬一伦一区二区三区| 久操操| 九九色大香蕉| 色情五月停停丁香| 婷婷久久五月天亚洲欧美国产日韩在线观看 | 色99在线视频| av免费在线观看0| 91好好热日本在线| 午夜亚洲国产精品av一区二区| 色婷婷五月婷婷五月婷婷五月| 五月丁香综合在线| 另类亚洲电影| 丁香婷婷久久| 五月丁香综合啪啪| 国产婷婷综合| 色婷五月天综合网| 五月激情另类| 婷婷色五月丁香六月欧美啪| 欧美色偷偷大香| 最新高清无码专区| 原琪琪色影院| 79精品视频| 久久6这里只有精品| 激情五月婷黄版| 婷婷五月欧美综合| 欧美大肥婆大肥BBBBB| 九九青草热| www.zbzhongsen.com| 亚洲AV日韩AV永久无码网站| 婷婷综合视频| 九九热亚洲中文在线观看免费| 丁香桃色网| 色五月激情| 五月丁香久久精品在线观看| 综合色色婷婷| 婷婷成人五月天成人文学| 精品一区二区三区木瓜| 五月婷婷色播视频| 亚洲精品成人| 激情婷婷五月在线合集| 久热婷婷| 日日干夜夜干| 婷婷五月天激情网| 激情中文在线| 丁香五月天啪啪a日本| 97深爱伊人综合| 丁香九月综合| 另类专区在线| 91热视频色网站| 久在线综合69| 伊人丁香五月天丁香在线婷| 天天干天天干天天干| 五月停停色色丁香| 欧美色碰| 国产人妻人伦精品一区二区| 五月色亚洲| 久久精品4| 国产AV午夜精品一区二区入口| 另类五月激情| 99热99热不卡| 婷婷五月天男人影院色色网| 99热精品综合| 能看的av片| 婷婷五月天777| 久久婷婷五月天激情新地址| 丁香五月AV| 9 1在线视频| 欧美日本99| 婷婷丁香综合在线| 色yeye欧美| 97干资源在线观看| 99热伊人综合| 99超碰欧美| 大香焦啪啪啪| 91在线观看九区| 丁香五月激情图片婷婷| 九九99精品免费播放| 亚洲色亚洲精品| 亚洲成人影视在线观看| 久久东京热婷婷五月| 婷婷综合色网| 日韩在线9| 婷婷丁香宗合888| 日韩日比视频| 99免费青青蜜臀| 国产成人亚洲综合亚洲| 国产一级黄色影片,| 久热99| 欧美性色A片免费免费观看的| 激情第四色| 99热在线播放| 99精品视频在线观看| 成人在线99| 色婷婷狠狠| 国产毛片精品一区二区色欲黄A片| www.婷婷五月| 免费视频WWW在线观看网站| 99国产精品久久久久久久久久久| 大地资源色婷婷视频在线| av亚洲国产小电影| 97爱艹婷婷开心丁香激情综合| 婷婷色色综合| 欧美色色色色色| 国产精品国产VA片国产| 五月婷色啪| 激情婷婷五月天日本系列| 丁香六月无码播放| 99这里只有精品|v| 蜜桃精品AV无码喷奶水小说| 在线成人网址| 99热只有| 婷婷六月天国产综合| 五月丁香狠狠爱婷婷综合| 日韩精品无码AV| 久操干| 婷综合| 99丁香五月婷| 99热精国产这里只有精品| 丁香五月激情图片| 色五月婷婷网| 久热这里只有精品99re| 天天日天天插| 96精品国产综合久久久久久| 日韩人妻无码精品| 久久色五月天| 五月天婷a| 新激情五月天天在线网| 色综合区| 夜夜穞天天穞狠狠穞AV美女按摩| 亚洲射激情| 五月婷婷丁香成人网| 午夜性爱影视一区77| 战争与艾拉电影免费观看| 五月天婷婷激情小说电影| www.狠狠操| 色五月丁香五月| 色色综合网站| 激情综合网激情五月丁香五月俺也去| 婷婷六月综合基地| 97人人草| 欧美婷婷五月天综合| 99re8这里只有精品99re8热视频| 久久99久久99精品免观看粉嫩| 五月天激情小说| 中文字幕不卡网站| 91色干| 开心婷婷中文字慕| 丁香婷婷十月| 成人亚洲精品| 久操香蕉| 99re视频在线播放| 色五月五月天| 少妇的肉体AA片免费| 色五月综合在线| 内射爽无广熟女亚洲| 久久网思思| 天天做 天天爱| 1819岁日本MACBOOK| 91精品久久久久久77777| 色五月婷婷7777| 91热视频色网站| 久久久久亚洲A∨成人乱码电影| 五月天深爱激情网| 噜噜色五月| 五月天社区| 丁香五月777| 激情婷婷五月女| 日本五月天一页| 婷婷九九| 国产看真人毛片爱做A片| 婷婷色五月天色色| 激情婷婷五月亚洲| 综合五月婷婷| 色欲午夜无码久久久久久张津瑜 | 26uuu亚洲欧美日本| 婷婷99狠狠躁天天| 亚洲免费成人电影AV| www.无码com| 视色网在线播放| 五月精品| 超碰日韩人妻在线| 久久人人九九| 丁香五月社区| 激情AV中文| 99热九九这里只有精品10| 五月丁香免费看| 八戒青柠影视剧在线观看| 色色色色色五月| 综合久色五月| 色色无码| 婷婷五月丁香第四色超碰在线| 色综合久久综合中文综合网| 热久久国产视频| 丁香大香蕉| 婷婷五月欧美| 激情com| www.夜夜| 色婷婷五月天av在线| 色五月激情| 99国产小视频| 九九RE视频在线精品| 偷拍99在线视频观看| 天天色天天爽| 色九亚洲| 激情综合文学| 丁香婷婷人妻综合网| 色99色| 婷婷在线日韩综合| 天天免费成年人视频| 五月花激情| 人人色AV| 亚洲美女网Va| 操逼巨乳91| 丁香五月激情宗合网| 99久久玖玖| 高潮毛片又色又爽免费| 日本色99| 色五月天成人| 99A片| 婷香五月| 欧美性生交XXXXX无码小说| 日本V在线观看不卡视频网站| 丁香六月啪啪| 啪啪视频99| 99久在线观看| 另类综合国产| 久久国产一区二区三区| 久久激情网| 久青草影院| 99视频这里有精品| 99综合视频一体| 碰超在线九色| 婷婷综合伊人丁香| 香蕉AV777XXX色综合一区| 97操在线视频| 少妇荡乳欲伦交换A片欧美| 天天操天天插天天射| 极品 少妇 内射| 亚洲av骚货| 天天久综合网永久入口17v| 午夜天天精品视频| 热九九精品| 9久久婷婷国产综合精品性色| 丁香婷婷五月天校园春色| 激情性爱五月天网页| 97干欧美| 久久久久网站| 大地资源中文第3页| 激情婷| 六月丁香影院| 婷婷9月天| 五月天激情久色| 尤物一区二区| 99色视频在线观看| 99热啪啪| 狠狠狠激情网| 99婷婷精品推荐在线视频| 色五月婷婷成人视频| 天天操天天插| 五月天激情网图片 - 百度| 99精品在线观看视频| 九九视频免费| 婷婷色婷婷| 伦乱美欧| 熟女人妻一区二区三区免费看| 精品九九在线观看| 五月丁香爱婷婷深深| 欧美婷婷五月丁香| 丁香婷婷人妻综合网| 久久99精品久久久久久青青AR| 精品一二三区久久AAA片| 超碰成人在线观看| 7777激情基地| 99久久九九| 久久综合九九| 五月婷婷六月丁香| 婷婷深爱五月亚洲综合| 色欲五月丁香| 丁香五月婷久久| 欧美日韩国产一区二区| 婷婷五月丁香色综合| 任你日视频| 丁香六月婷婷开心| WWW.亚洲无码| 丁香啪啪中文字幕| 色情激情五月婷婷| 国产热精品| 99热午夜精品| 亚洲狠狠干| 亚洲激情网| 婷婷午夜| 五月开心播播网| 色狠狠综合网| 99人碰碰碰| 伊人在线大香蕉网| 五月丁香AV、伊人业余、性色熟妇| 秋葵视频网站| 啊V视频在线观看| 久久怕怕视频| 狠狠操天天日| 天天射色五月天| www.99精品在线| 久久99网站| 777米奇影视第四色| 亚州日本欧州韩美高青高潮一| 久久久aaa| 草综合14| 婷婷五月天激情网| 97人妻碰碰中文无码久热丝袜| 婷婷五月丁香久久| 久久99看免费| 人妻22p| 丁香五月婷婷六月婷| 国产精女同一区二区三区久| 激情六月色| 网色99| 日本人妻伦在线中文字幕| 色婷婷综合网站| 综合五月婷婷| 婷婷丁香色性爱| 色婷婷免费观看| 日日色五月天| 操b视频在线观看一区二区| 射久久丁香五月| 六月色日韩| 亚洲一二三网| 99热久草| 色狠狠六月| 久久婷婷六月综合综合| 五月激情啪啪啪| 99热这里只有精品96| 婷婷伊人綜合| 狠狠草狠狠草| 洗浴中心操B视频| 五月丁香激情四射综合| 成人国产欧美大片一区| www.天天日| 久这里只有精品99| 9精品国产在热久久| 婷婷丁香激情综合色情| 激情丁香五月激情婷婷| 色爱99| 国产精品18久久久| 丁香六月欧美| 婷婷欧美色| 亚洲乱啪| 天天爽天天日| 开心五月婷婷婷美女| 第四色在线观看| 狠狠做六月爱婷婷综合aⅴ| 99碰碰。| 97在线精品| 婷婷精品综合| 26UUU| 色都都狠狠色都都色综合色| 狠狠综合| 狠狠色综合精品视频在线| 丁香五月1页| 热99热久| 激情五月综合| 色五月五月婷婷| 婷婷五月天 偷拍| 色九九九九| 丰满老熟妇BBBBB搡BBB| 国产乱子轮XXX农村| 亚洲成人电影aaaa| 99 re视频一区| 久久六月婷婷| AV中文在线| 五月婷婷婷婷| 色婷婷婷综合五月天| 99色五月| 色啪久| 三级黄网站| 开心激情五月天网| 深爱婷婷色| 色婷婷中文在线| chaopeng在线人人| 伊人五月天| 五月亭亭六月激情| 五月激情婷婷国产精品久久久久久| 五月激情开心婷婷| 激情五月色综合| 五月天四色房丁香亭亭| 色综合久| 男同91| 色播五月婷婷五月| 丁香蜜臀黄色婷婷五月天| 亚洲AV久久久久久久久久久久久久久久 | 欧美色频| 五月天色官网| 五月天开心色情网| 一区操| 男妓跪趴把舌头伸进我的嘴巴| 艳妇野外情欲放荡HD| 五月婷婷花| 噜综合| 精品九九婷婷| 五月婷婷丁香六月| 亚洲V国产V欧美V久久久久久| 婷婷综合网站| 日日日日做夜夜夜夜无码| 激情婷婷五月少妇| 亚洲超碰青涩| 99色视频| 91久久1118| 97人妻碰碰中文无码久热丝袜| 综合激情视频| 久久小视频| 殴美日韩成人| 亚洲五月六丁香激情| 99热婷婷| 五月天天天色| 99热资源在线| 思思国产99| 五月天婷婷在看| 99er6免费视频热播| av激情在线| 九九久久污| 婷婷婷婷婷婷婷婷婷婷丁香| 女人被男人吃奶到高潮| 一区二区成人电影| 天天操天天操天天操天天操天天操天天操天天操天天操天天操 | 99激情在线| 色色色热热热| 懂色AⅤ| 五月天开心色情网| 人妻久久做| 殴美日比视频| 婷婷丁香91综合| 青草视频在线蜜臀| 丁香五月精品| 99色综合| 亚洲不卡欧洲| 色婷婷久久综合中文久久一本| 狠狠色五月| 婷婷少妇激情| 五月丁香激情综合网| 美英法精品无码免费视频| 久久久婷丁香五月| 九九视频精品这里只有| 成人五月天综合网| 99ri精品视频在线观看| wwww.色婷婷| 欧美在线ee日韩| 播丁香五月婷婷欧美| 夜精品无码A片一区二区蜜桃| 综合色五月| 婷婷丁香五另类网站| 久青操| 综合XX网| 婷婷五月天综合在线| 99热无码首页| 色婷婷五月中文字幕在线dvd| 婷婷久久免费看| 青草性爱视频| 韩国情人在线电视剧免费观看高清版全集 | 婷婷色女| 日本九九热| 五月丁香无码| 久久99网址| 夜夜骑夜夜操| 精品一二三区久久AAA片| 伊人激情影院| 午夜丁香婷婷| 久久久性爱视频| 五月婷婷中文| 五月天激情国产综合婷婷| 这里有精品2| 五月天综合激情网| 亚洲狠狠干| 99综合| 久久人妻视频| 男人的天堂五月丁香| 六月丁香婷婷综合狠狠爱夜夜爱| 色五月 五月婷婷| 九九热最新| 外国人做爰又粗又大IM| 无码髙清| 玖玖综合色| 噜噜五月天综合| 操一区| 日韩色色视频| 极品人妻VIDEOSSS人妻| www,奇米影视| 大香蕉视频婷婷| 久久久精品99| 色综合中文色综合网| 99久久久免费| 久久狠狠高潮亚洲精品 天天摸夜夜摸夜夜狠狠摸| 久热久| 天天狠天天狠| 九九伊人网| 狠狠撸激情综合丁香五月天俺来啦| 激情综合五月丁香六月婷婷| 成全影视大全在线观看第6季| 丁香五月婷婷啪| 91黄色五月天视频| 大香伊人婷婷影院| 七月激情六月婷婷综合在线播放| 久久免费操| 五月开心婷婷网| 五月天婷婷爱丁香中文字幕| 五月天激情.com| 草逼大片| 亚洲色婷婷久久精品AV蜜桃| 超碰人人干| 拍真实国产伦偷精品| 六月丁香啪啪| av电影在线播放| 九九人人自拍| 五月丁香六月综合基地| 激情网站五月| 色久五月| 色综合激情| 色婷婷免费观看| 极品人妻VIDEOSSS人妻| 色婷婷亚洲综合网站| 99久久精品国产色欲| 婷婷久久五月天| 9久热这里只有精品视频| 久久人妻伦理| 97干干干丁香| WWW,五月| 五月天欧美 另类小说| 99热亚洲综合| 久久久天堂国产精品女人| 丰满人妻妇伦又伦精品国产| 婷婷五月丁香伊人网| 99亚州综合精品成人网| 六月婷婷狠狠色在线观看| 六月丁香社区| 久久婷婷五月综合激情国产| 免费视频无码| 99操不停| 婷婷操逼| 激情五月丁香激情综合网| 天天爽天天操| 成人在线99| 亚洲视频另类| 超碰九色| 青草激情在线| 91精品久久久久久久久| 丰满老熟妇BBBBB搡BBB| 色综合av超碰| 色五月综合婷婷久久综合婷婷久久综合婷婷久久综合婷婷久久 | WWW.婷婷| 日日夜夜小色哥| 色播婷婷大香蕉| 91日本在线免费| 任你躁XXXXX麻豆精品| 激情婷婷五月天| 色亚洲色宗合| 五月丁香啪综合| 色五月婷婷激情| 猫咪伊人久久| 亚韩在线视频| 99re热| 婷婷丁香黄色| 丁香五月影院| 99热免费| 丁香久久| 久久精品99| 夜色综合网| 第五色婷婷| www.开心激情| 26UUU在线观看| 精品无码人妻一区| 成人免费120分钟啪啪| 色色网站免费| 婷婷激情综合| 天天摸天天高潮天天爽| 婷婷五月丁香久久| 激情国产综合| AV成人在线播放| 狠狠99| 婷婷五月色色| 五月婷婷激情网| 色婷婷久久天天性爱| 五月丁香六月合| 色五月中文网| 激情宗合 激情宗合| 爱穴久久| 狠狠色色色| 九月大香蕉| 久操人| 色九月婷婷| 婷婷丁香77777| 色就是色婷婷五月亚洲激情| 91操片| 免费看欧美成人A片无码| 超PEN精品在线| 五月天激情综合| 1024日韩| 九九综合网色全集| 六月丁香综合网| 久久激情视频| 中文字幕高清av| 激情综合网之激情五月| 日本天天操| 亚洲激情四射色| 开心五月六月婷婷| 色色99| 国产干逼片| 久久五月六月| 97超碰在线免费观看| 久婷婷久草| 天天综合插插| 日本久久精品| 亚洲成人另类| 亚洲色模骚货| 色噜噜狠狠色综合日日| 日韩欧美一道四区中文字幕| 五月天停停基地| 无码人妻少妇色欲AV一区二区| 97碰| 色五月婷婷影院| 麻豆WWWCOM内射软件| 五月丁香六月激情综合网| 色五月婷婷婷婷| 99热这里只有精品在线观看| 久久精品五月天| 丁香色五月婷婷| 97久久婷婷色| 狠狠另类视频| 狠狠色婷婷777| ′久久99一| 婷婷五月天激情基地| 天天干天天做| 久久黄色免费视频| 91久久久久久| 91在线日| 97丁香五月| 婷婷五月天 丁香五月天 裸体| 人妻爽爽爽久久久久久久久| 99热精品观看| 丁香激情五月少妇| www.99成人视频| 亚洲春色奇米影视| 日韩99色| 婷婷五月激情图片| 色综合婷婷| 亚洲婷婷基地| 婷婷色在线播放| 人人射人人高潮| 狠狠色综合五月人人| 激情五月综合免费| 九九热精品视频在线观看| 九九99精品视频在线观看| 操九色| 五月开心久久| 久草热在线视频| 日韩激情网站| 99精品亚洲| 天天视频精品9| 婷婷六月丁香激情综合| 色丁香五月婷婷| 美女天天久久| 第四色五月天| 激情婷婷五月天。| 超碰在线成人| 9l视频自拍9l九色成人| 色色激情五月| 99久在线精品| 日本人も中国人も汉字を| 五月婷婷激情日本| 思思热在线观看| 色情开心五月| 久久精热| 五月天激情综合网| 国产欧美va| 91啪啪啪啪| 国产精产国品一二三在观看 | 在线观看婷婷5月| 亚洲热久| 五月开心播播网| 视频一二区| 婷婷久久丁香五月| 黄网网站在线播放| 97人人超| 久久之人妻| av在线资源| 色婷婷五月天激情| www.婷婷五月天| 日本在线视频手机播放五月婷| 亚洲妇女熟BBW| www.色婷婷。com| 色五月大香蕉| 伊人网色婷婷五月天| 91久女| 天天综合天综合| 激情性爱网站| 色婷婷基地| www99精品| 久久人人超| 亚洲婷婷五月天在线激情综合网| 亚洲经典三级| 99热在线中文字幕| 婷婷色网址| 激情文学五月丁香六月婷婷| 在线视频激情网站| 欧洲色色| 成人短视频在线| 狠狠五月天| 色婷婷综合五月| 色五月色综合| www五月天com| 大香蕉人在线65| 久久久99视频| 五月天开心激情网色欲无码| 欧美成人精品三区综合A片| 亚洲成人乱码av网站| 日韩三级视频一区二区| 欧美成人va| 99操视频| 婷婷色五月天在线| 丁香五月综合在线| 91在线看片| 国产婷婷五月天| 婷婷玖玖丁香| 一起草Av| 99超在线| 亚洲国产精品VA在线看黑人| 久久久五月婷婷| 欧美婷婷精品激| AV在线免费播放| 狠狠色五月激情| 99se丁香| 天天弄| 色播五月丁香| 色婷婷久久| 综合五月天婷婷色| 91chinese 在线| 丁香五月性| 综合五月天天天天天五月| 丁香九色不卡aaa| 玖玖婷婷色五月| 丁香五月 综合| 色五月天 丁香| 日本欧美成人片AAAA| 五月婷婷色播视频| 婷婷碰碰| 蜜臀av粉嫩av懂色av| 99re这里只有精品国产99| 中国女人做爰A片| 香蕉AV777XXX色综合一区| 国产1区2区3区| 无码激情AAAAA片-区区| 啪啪小说五月天| AV九九| 婷婷五月天国产传媒| 五月丁香亭亭| 色之综合网| 大香蕉网 久久| 五月婷婷啪啪网| peg 2区三区四区的| 婷婷99狠| 欧美乱码国产一级A片| 久久久人妻久久久| 97色精品视频| 亚洲性爱电影| 亚洲九九九九| 九九久久精品國產| 亚洲无码色色| 永久AⅤ1| 综合色色婷婷| 色婷婷综合久久| 久久久久婷| 天天操夜夜夜拍拍拍| 久久九⑨| 五月天开心网| 色播五月| 五月天婷婷色在线视频免费观看| 狠狠一日| 色婷婷综合久久久久| 99区视频| 久七香蕉| 乱岳熟女50岁| 丁香网站| 热99久久这里只有精品| 五月婷婷综合久久| 婷婷五月影院| 婷婷久久精品| 五月色精品| 色~性~乱~伦~噜| 99精品热| 操操自拍| 久久婷婷人人| 日本成人噜噜噜噜噜| 欧美男女婷婷| 精品无码久久久久久久久 | 51国精产品自偷自偷综合| 色情婷婷五月天| 色丁香五月婷婷婷| 日本123区日韩欧美不卡在线看| 久久九九免费视频| 六月激情久久| 丁香婷婷激情五月| 99久re热| 骚逼视频一区2区| 亚洲丁香花色| 开心婷婷丁香五月| 先锋资源996| 丁香花五月天激情| 国产色色色色色| 成人做爰黄A片免费看直播室男男| A久久| 五月激情另类| 99热播放| 色综合久久8| 99网| 天美传媒原创在线观看| 精品成人无码A片观看香草视频| 色欲九区| 丁香五月激情啪啪啪啪| 成人免费120分钟啪啪| z色五月播播久久| 激情综合网五月天天| 丁香五月婷婷99| 五月丁香婷婷成人网| 婷婷综合五月| 日韩啊啊啊| 色婷婷五月天堂资源| 婷婷丁五月| 99久精品| 香蕉久久五月| 农村熟妇高潮精品A片| 精品人人操| 亚洲国产精品VA在线看黑人| 五月婷婷在线网站| 91狠狠色| 丁香九月综合在线| 色综啪啪网| www.五月.com| 丁香美女五月天婷婷| 淫荡工a| 99er6| 五月天啪啪| 人人综合久| 久婷视频| 色婷婷很很丝袜| 婷婷色在线| 九九热婷婷| 九一99| 91热er| 人妻久久做| 色色五月天丁香| 亚洲av无码精品色午夜| 美女视频图片久久91| 色色色网站| 五月婷婷色五月| 我爱大香蕉| 无码髙清| 精品人妻一区二区三区四区不卡在| 婷婷四色五月| 性小说五月天| 色五月丁香六月资源站| 久久免费操| 色噜噜五月丁香婷婷| 色色999三级片| 国产精品扒开腿做爽爽爽A片唱戏| 超碰人妻在线| 4399亚洲视频| 天天婷婷综合亚洲亚洲| 亚洲人成人五月天| 五月色精品| 高清无码中文字幕aVDV| 色播五月天天| 五月丁香网av| 亚洲综合在线伊人婷| 综合久久综合久久| 九九热99熟女| 丁香五月婷婷Av| 狠狠色丁香婷婷| 综合久久综合五月天婷婷| 超碰色热| 日韩专区五月天婷婷丁香| 人妻AV在线| 成人做爰A片免费看视频| 99热亚洲| 婷香五月| 五月丁香啪啪啪啪| 久久东京热婷婷五月| 丁香五月综合激情性爱 | 国产91视频| 久热re在线视频| 丁香五月婷婷www..com| 99九九99九九九视频精品| 婷婷婷久久| 丁香深五月婷婷| 五月天综合在线网| 亚洲视频在线网站| 99热99艹在线观看| 亚洲精品99| 婷婷五月天成人网| 婷婷五月天成人网| 天天日天天舔| 色综合色综合网| 色色色色色色色色网站| 婷婷色综合| 成AV人片一区二区三区久久| 激情五月六月婷婷| 六月婷婷开心| 久热这里| 中文字幕人成乱码在线观看| .精品久久久麻豆国产精品| 亚洲乱码日产精品BD| 综合久久99| 丁香五月婷婷色综合| 五月天丁香久久综合 | 丁香婷婷五月综合影院| www.色九月| 婷婷免费无马| 9久久精品| 伊人青草成人| 涩涩五| 婷婷丁香五另类网站| 人人做人人看人人摸| 色五月婷婷内射| 天天精品视频免费观看| 六月天婷婷| 五月丁香久久久久| 99久视频|