• <tr id="yyy80"></tr>
  • <sup id="yyy80"></sup>
  • <tfoot id="yyy80"><noscript id="yyy80"></noscript></tfoot>
  • 99热精品在线国产_美女午夜性视频免费_国产精品国产高清国产av_av欧美777_自拍偷自拍亚洲精品老妇_亚洲熟女精品中文字幕_www日本黄色视频网_国产精品野战在线观看 ?

    Photon and positron production by ultrahigh-intensity laser interaction with various plasma foils

    2021-04-22 05:34:06
    Plasma Science and Technology 2021年4期

    School of Physics Science and Technology,Xinjiang University,Urumqi 830046,People’s Republic of China

    Abstract The generation of γ photons and positrons using an ultrahigh-intensity laser pulse interacting with various plasma solid foils is investigated with a series of quantum electrodynamic particlein-cell(PIC)simulations.When ultrahigh-intensity lasers interact with plasma foils,a large amount of the laser energy is converted into γ photon energy.The simulation results indicate that for a fixed laser intensity with different foil densities,the conversion efficiency of the laser to γ photons and the number of produced photons are highly related to the foil density.We determine the optimal foil density by PIC simulations for high conversion efficiencies as approximately 250 times the critical plasma density,and this result agrees very well with our theoretical assumptions.Four different foil thicknesses are simulated and the effects of foil thickness on γ photon emission and positron production are discussed.The results indicate that optimal foil thickness plays an important role in obtaining the desired γ photon and positron production according to the foil density and laser intensity.Further,a relation between the laser intensity and conversion efficiency is present for the optimal foil density and thickness.

    Keywords:laser-plasma interaction,positron generation,γ ray emission,nonlinear Compton scattering,particle-in-cell(PIC)simulation

    1.Introduction

    The rapid progress of ultraintense laser technology has opened some promising areas in strong field physics.Some new laser facilities[1],such as the Extreme Light Infrastructure(ELI)[2],iCAN[3],and Apollon laser[4]projects,promise to provide a 10-100 PW class laser,with a corresponding laser intensity of over 1023W/cm2.For such ultrahigh-intensity lasers,the quantum electrodynamic(QED)effects are dominated in most laser-plasma interactions,such as γ photon emission and positron production[5-11].

    In recent years,γ photon emission and positron production by ultrahigh-intensity lasers have been intensely studied because of the variety of important applications in various areas,such as nuclear and particle physics research[12],laboratory astrophysics[13,14],and medical imaging and radiography[15,16],as well as for the development of materials science and to motivate novel industrial applications[17].

    Recently,several studies have indicated that ultrahighintensity laser-plasma interaction could trigger the processes of γ photon emission and electron-positron pair production[10,11,18-23].Various mechanisms have been proposed[24-28]and,simultaneously,considerable theoretical and numerical studies have been undertaken to provide detailed physical explanations for these QED processes[5-11,18-31].If the generation process of the γ photon can be triggered,it will produce a dense beam of positrons in the laboratory,which will facilitate several new fields of research[12,14,18-21].

    In the study of ultrahigh-intensity laser-plasma interactions,the three most commonly investigated QED processes include the Bethe-Heitler(BH)[24],Breit-Wheeler(BW)[25],and trident[26-28]processes.In the trident process,the electron-positron pairs are produced by energetic electrons interacting with the Coulomb field or the strong laser field[27,28].Under relatively moderate laser intensities(I~1022W/cm2),electrons are accelerated into high-Z nuclei,which results in the generation of positrons.In the BH process,electron-positron pairs are produced by nuclei interacting with γ photons radiating from decelerated electrons[24].Some studies have indicated that electron-positron pairs could be produced by direct laser-plasma foil interactions through the trident and BH processes.However,the positron yields obtained from experiments are too low to be used in applications,so it is necessary to enhance the energy conversion efficiency,positron yield,and energy.In the BW process,under a super-intense laser condition,the electrons are accelerated by the laser field and radiate γ photons through nonlinear Compton scattering.Consequently,electron-positron pairs are produced by the multiphoton BW process(γ+nγlaser→e?+e+)[25],which produces additional γ photons and electron-positron pairs,resulting in QED cascades[11,20].Recently,some particle-in-cell(PIC)simulation studies have predicted that in ultrahigh-intensity laser-plasma interaction,high-energy electron-positron pai rs can be generated through the BW process.

    In this paper,we research ultrahigh-intensity laser and plasma foil interactions to produce high-energy photons and positrons using numerical simulations.We perform twodimensional(2D)QED-PIC simulations using EPOCH code[32].We present the simulation results for foils of various densities,thicknesses,and materials,as well as with different laser intensities.We show that there exists an optimal foil density and thickness,which play key roles in enhancing the energy conversion efficiency,number of produced photons,and positron number.We also investigate the interactions of laser pulses with different intensities and the optimized plasma foil.The simulation results show that a suitable laser intensity is also crucial to enhance the photon emission and trigger the QED cascade.

    2.Model and simulation parameters

    PIC simulation is an effective tool for studying certain fields in laser-plasma interaction physics,such as in laser-based particle acceleration,high-energy-density physics,fast ignition in inertial confinement fusion,etc.[33-37].Since the coupling between the QED processes and plasma dynamics is very complicated,numerical simulations have recently been shown to be an effective way to clearly explore such interactions.Therefore,a series of QED-PIC simulation investigations have been performed on QED processes in laserplasma interactions[9-11,20,38].

    In our 2D PIC simulations,linearly polarized ultrahighintensity laser pulses enter the simulation area from the right side at t=0,propagate along the positive x direction,and are incident normally onto the thin plasma foil.The laser has a Gaussian intensity profilewith wavelength λ=1 μm,focal spot y0=1 μm and duration TL=15 fs.The peak intensity of the laser is I=4×1023W/cm2,which corresponds to a normalized laser amplitude of a0=eA/mec2=540,where e and meare the electron charge and mass,respectively,A is the vector potential,and c is the speed of light in a vacuum.In the simulations,we used carbon,aluminum,and gold flat foils to compare the effect of the target material on the photon emission.The foil height in the y direction was 6 μm,the foil front surface was located at x=2 μm,and four different foil thicknesses were considered in the simulation.The simulation box size was 6 μm(x)×6 μm(y)with a grid of 600×600 cells.For the number of particles in each cell,we chose 100 electrons and 50 ions.The longitudinal and transverse initial temperatures of the electrons and ions were so small that their effects could be ignored.The boundary conditions were periodic in the transverse direction and simple-outflow longitudinally.

    In our simulations,we consider the radiation reaction regime and the γ photon emission is characterized by QED parameterwhich requires χe≥1 for efficient photon emission.A multiphoton BW process is considered for positron production,which is characterized by another QED parameterand Kγare the 4-momenta of the electron and photon,respectively,and Fμνis the field tensor.These processes are enabled in EPOCH code with a QED block via Monte Carlo algorithm.

    3.Simulation results

    In order to show the effect of the target density on photon emission and positron generation,we compared the 2D QEDPIC simulation results for plasma foils with different densities.Figure 1(a)shows the relations between foil densities and conversion efficiencies of the laser energy to electrons,photons,and positrons for various foil densities with a fixed foil thickness and laser parameters at 16.7 fs.From this figure,we observe that the conversion efficiencies(defined as the fraction of total laser energy carried by each species)to electrons,photons,and positrons increased rapidly with foil density until ne=250nc,then decreased with foil density to approximately ne=500nc,and then decreased very slowly with a further increase in the foil density.Figure 1(b)shows a plot of the spatial evolution of the photon number for various foil densities with the same foil thickness and laser parameters as those in figure 1(a)at 16.7 fs.More photons were produced with an increase in the foil densities until ne=250nc;then,for the photon number as well as its distributions,no obvious differences were observed between the ne=400nc,500nc,and 700nccases.It is worth noting that the peak of the photon number spatial distributions moved to the left with increasing foil density,as shown in figure 1(b).This was attributed to the different laser penetration depths for the various foil densities,as discussed in figure 2.

    Figure 1.(a)Laser energy to electrons,photons,and positrons conversion efficiencies as well as the total conversion efficiency,and(b)spatial evaluation of the photon number in the x direction for different foil densities at 16.7 fs.The foil density ne varies from ne=50nc to ne=700nc while the foil thickness is fixed at l=1 μm.

    Figure 1 shows that the conversion efficiencies and produced photon numbers were highly dependent on the foil density,which plays a key role in laser plasma interaction QED problems for given laser parameters.The results indicate that there exists an optimal foil density,which results in an enhancement of the energy conversion efficiency and the produced photon number.When the chosen foil density is optimal,more photons and positrons are obtained under the proper laser conditions.The optimal foil density in our studied case,which was determined by 2D QED-PIC simulations,was ne=250ncfor a0=540 and l=1 μm,as shown in figure 1.The optimal foil density for different foil thicknesses and laser intensities is discussed in the following parts of this paper.

    Figures 2(a)-(f)present the spatial distributions of the electron density in the(x,y)plane at 16.7 fs for foil densities of ne=100nc,250nc,400nc,500nc,600nc,and 700nc,respectively.Figure 2(a)shows that,for the low-density foil(ne=100nc),the foil was transparent to the ultrahigh-intensity laser,owing to relativistic transparency.Moreover,the strong ponderomotive force of the laser expels target electrons from the high-field region very easily.Consequently,there was no reflected laser field and the standing wave could not develop inside the foil.This resulted in a lower conversion efficiency of the laser energy to electrons and lower photon emission.However,for the foil density of ne=250nc,a highdensity electron layer was produced in the right half of the foil with a thickness of approximately 0.5 μm and a density of ne=400nc,as shown in figure 2(b).With a further increase in the foil density,the thickness and density of the electron layer decreased and increased,respectively.More importantly,unlike in the ne=250nccase,the electron layer was produced in the left half of the foil for the higher-density foil cases,as shown in figures 2(c)-(f).This meant that for the foils with density higher than the optimal density(ne=250nc),the penetration depth of the laser into the foil was shortened and the laser was reflected from the front surfaces of the foils.This resulted in a lower energy conversion of the laser energy to electrons,which finally led to small amounts of photon and positron generation.

    The spatial distributions of the transverse electric field Eyin the(x,y)plane and phase space distribution of electrons at t=16.7 fs for different foil densities(ne=100nc,250nc,400nc,and 700nc)are given in figure 3.Figure 3(a)shows that for the foil with density ne=100nc,almost all of the laser fields were transmitted to the back of the foil without any disruption of the foil and some energetic electrons appeared at the back of the foil,as shown in figure 3(a1).However,for the ne=250ncfoil,the laser field penetrated deep into the foil and was reflected from the high-density electron layer at the right side of the foil,as shown in figure 3(b).More importantly,more energetic electrons stayed in the laser reflection region,as shown in the phase space portrait of figure 3(b1).For the foils with densities of ne=400ncand ne=700nc,almost all of the laser fields were reflected from the foil front surface without penetration and there were few energetic electrons in the laser reflection region,as shown in figures 3(c),(d),(c1),and(d1).All these results indicated that for the lower foil density,the laser was easily transmitted to the back of the foil and there was no reflected field.This resulted in lower correlation and conversion efficiencies between the laser and electrons,as shown in figures 1 and 2.For the ne=400ncand ne=700nccases,there were highdensity electron layers at the front side of the foil(see figure 2),which acted like a plasma mirror and instantly reflected almost all of the laser fields.Consequently,the incident and reflected lasers had less chance to interact with electrons,which resulted in a lower conversion efficiency.However,for the case of ne=250nc,the laser could penetrate deep into the foil,and the dense electron layer produced at the rear of the foil could reflect the laser field like a plasma mirror(see figure 2(b)).Accordingly,more energetic target electrons remained in the high-field region,as shown in figures 3(b)and(b1).This resulted in enhancements of the conversion efficiencies and the chance of photon emission as well as positron production.

    We can estimate the optimal target density by theoretical analysis for our simulated case,where the laser field is fully reflected by the high-density electron layer.The laser radiation pressure for this case can be expressed as Prad=2I(1+R+T)/c,and we assume that the laser field is fully reflected by the high-density electron layer,which acts as a plasma mirror,so we have T=0 and R=1.Let us assume that when the target density is equal to the optimal density,an electron-ion double layer is developed and the laser radiation pressure is compensated by the pressure of the electrostatic fieldwhereis the charge separation electrostatic field and y0is the laser focal spot radius.The distance is chosen as y0/2 since at this point the radiation pressure is maximal[39].We obtain an estimate of the optimal target density.It gives the valuefor a laser pulse with an intensity of I=4×1023W/cm2and a focal spot radius of y0=1 μm.This result agrees very well with our PIC simulation results.

    Figure 2.Spatial distribution of the electron densities in the(x,y)plane at 16.7 fs for foils with densities of ne=100nc(a),ne=250nc(b),ne=400nc(c),ne=500nc(d),ne=600nc(e),and ne=700nc(f).

    Figure 3.Spatial distribution of the transverse electric field Ey in the(x,y)plane(top row)and phase space distribution of electrons(x,px)at t=16.7 fs for foils with densities of ne=100nc[(a)and(a1)],ne=250nc[(b)and(b1)],ne=400nc[(c)and(c1)],ne=700nc[(d)and(d1)].The electric field is normalized by mecω0/c.

    Figure 4 plots the spatial distributions of the photon and positron densities in the(x,y)plane at 16.7 fs,with the foil thickness l=1 μm and densities of ne=100nc,250nc,400nc,500nc,600nc,and 700ncfor a0=540.Both the photon and positron densities were shown to be closely related to the foil density.For the foil with a density of approximately ne=250nc,as mentioned above(figure 3),the laser fields were reflected by the high-density electron compressed layer at the rear of the foil and an electromagnetic standing wave was produced by the incident and reflected laser fields.Accordingly,the electron motion in the standing wave led to more efficient photon emission and positron production than in the other density cases.These results also confirmed that ne=250ncwas the optimal density for an l=1 μm plasma foil interacting with ultrahigh-intensity laser pulses with a0=540.

    Figure 4.Spatial distribution of the photon(top row)and positron(bottom)row densities in the(x,y)plane at 16.7 fs for foils with densities of ne=100nc[(a)and(a1)],ne=250nc[(b)and(b1)],ne=400nc[(c)and(c1)],ne=500nc[(d)and(d1)],ne=600nc[(e)and(e1)],and ne=700nc[(f)and(f1)].

    Figure 5.Electron phase space distribution(x,px)for the(a)l=0.5 μm,(b)l=1 μm,(c)l=2 μm,and(d)3=1 μm cases.Laser energy to(e)electrons,photons and total,and(f)positron conversion efficiencies for different foil thicknesses at 16.7 fs.The foil density ne is fixed to the optimal density of ne=250nc,while the foil thickness is varied.

    Next,we investigated the effect of the foil thickness on the efficiency of photon emission and positron production.According to the results from figures 1-4,we chose the optimal foil density ne=250ncand normalized laser intensity a0=540 for this section.Therefore,we studied the phase space distribution of electrons and the evolution of the conversion efficiencies with foil thickness,as shown in figure 5.Figures 5(a)-(d)show that for the l=0.5 μm case,electrons have broad phase space distribution at the front and back of the target.However,for the l=1,2 and 3 μm cases,the electrons have similar phase space distribution and the energetic electrons are confined in the laser reflection zone.Figures 5(e)and(f)show that all the conversion efficiencies increased rapidly with the foil thickness until l=1 μm,and then remained unchanged with a further increase in the foil thickness.This indicated that for a given laser intensity and foil density of ne=250nc,l=1 μm was a favorable foil thickness to enhance the energy conversion efficiencies and photon emission.

    Figure 6.Spatial distribution of the electron densities(top row)and the transverse electric field Ey(bottom row)in the(x,y)plane at 16.7 fs.The foil density ne is fixed at the optimal density of ne=250nc,while the foil thickness varies.

    To validate our above statements,we determined the spatial distributions of the electron density and the transverse electric field Eyin the(x,y)plane at t=16.7 fs for different foil thicknesses,as shown in figure 6.We observed that when the foil thickness l was too small,that is,l=0.5 μm,it could not satisfy the condition of electron-ion double layer formation(which isμmin our case),the foil was transparent to the incident laser,and the laser pulse continued to travel and push some electrons in front of the laser pulse like a light sail,as shown in figures 6(a)and(a1).This normally results in suppression of the energy conversion efficiencies,as mentioned in the previous paragraph.However,for the foil thicknesses of l=2 and 3 μm,the highdensity-electron compressed layers were observed(hole-boring process)at the same place with the same density as in the case of l=1 μm,as shown in figures 6(b)-(d).Furthermore,the spatial distribution of the transverse electric field Eyin the(x,y)plane was similar for all three cases,as shown in figures 6(b1),(c1),and(d1).Thus,there were similar conversion efficiencies for the l=1,2,and 3 μm cases,as shown in figure 5.

    We investigated the relation between the laser intensity and conversion efficiencies,which included the total conversion efficiency as well as the conversion efficiencies to electrons,photons,and positrons.We undertook PIC simulations for two kinds of plasma foils with densities of ne=250ncand ne=500nc,while the foil thickness was fixed as 1 μm and the dimensionless laser amplitude was varied 11 times as a0=50,100,200,300,400,500,600,700,800,900,and 1000.The conversion efficiencies as a function of the laser amplitude a0for the ne=250ncdensity case are shown in figure 7(a).The total energy conversion efficiency increased,reached a maximum of approximately 70%,and then decreased almost linearly with the laser amplitude a0.The fraction of the energy coupled to electrons steadily decreased from 60% to approximately 20% with increasing laser amplitude.The conversion efficiency to photons increased rapidly from a few percent,reached a maximum of approximately 25%,and then became saturated with the increase in laser intensity.It is worth noting that the laser energy coupled to electrons was comparable to that of the photons at approximately a0=650.As the laser intensity increased,the photons absorbed more energy than the electrons.

    Figure 7.Energy conversion efficiencies for(a)a low-density plasma foil(ne=250nc)and(b)a high-density plasma foil(ne=500nc)with different laser amplitudes.The foil thickness is fixed at l=1 μm.

    Figure 8.Energy spectra of the electrons,photons and positrons for different target materials at t=16.7 fs with/without ion mobility:(a)for carbon,(b)for aluminum,and(c)for gold.Here,the optimal target density and thickness are used.

    Figure 9.Distributions of QED parameter χe for different target(a)densities,(b)thicknesses,and(c)materials at t=16.7 fs with mobile ions.

    Table 1.Energy conversion efficiencies for different target materials with/without ion mobility.

    The conversion efficiencies as a function of the laser amplitude a0for the ne=500ncdensity case are shown in figure 7(b).In this case,the total conversion efficiency decreased with a0,and the general trend for the electron,photon,and positron conversion efficiencies was similar to the ne=250nccase.Moreover,the conversion efficiencies to the electrons and photons were the same at the laser intensity of approximately a0=650,which was the same as the ne=250nccase.However,the energy absorbed by both electrons and photons decreased to approximately 12%at this critical intensity,which was less by approximately 10% than the ne=250nccase.This,generally,could be attributed to the fact that for the lower-density case(ne=250nc),the laser penetration distance was larger than that in the higher-density case(see figure 2),which directly resulted in higher energy conversion efficiencies to each species and enhancement of the photon emission and positron generation.

    4.Discussion

    In this section,we discuss the effects of the target materials and ion mobility on the conversion efficiency and photon emission.Figure 8 shows the electron energy spectra for different target materials with and without ion mobility.For the lower Z target,the cut-off energies and conversion efficiencies of the species were smaller than those for higher Z targets both with and without ion mobility,as shown in figure 8(a)and table 1.For the aluminum target,the cut-off energies for all species were almost the same and there was no significant change in the energy conversion efficiencies with and without ion mobility,as shown in figure 8(b)and table 1.However,for the gold target with immobile ions,the cut-off energies and number of the species were higher than those in the immobile ion case,as shown in figure 8(c),and the conversion efficiencies decreased remarkably for the mobile ion case,as shown in table 1.

    Finally,we discussed the distribution of the QED parameter χefor different target densities,thicknesses,and materials.The photon emission is governed by an invariant QED parameter χeand it is required that χe≥1 for efficient photon emission,where.For the low-density and thin aluminum target,the double-layer formation condition is not satisfied and electrons experience light sail acceleration in front of laser pulse,the electrons have high energy(see phase space distribution in figures 3 and 5),and χe≥1,as shown in figures 9(a)and(b).However,electrons cannot stay in the high-field region,which results in reducing the efficiency of photon emission.For the optimal target density,more electrons with higher χestay in the highfield region,increasing the efficiency of photon emission.For the targets of density higher than the optimal density,the value of χedecreases to half of that for the optimal density case,while for thicker targets,the distributions of χeare unchanged,as shown in figure 9(b).Figure 9(c)shows the distributions of χefor different target materials with ion mobility.It is found that the value of the χeis higher for the aluminum target than for the other two target cases.

    5.Conclusion

    In this paper,we have numerically studied the interactions of ultrahigh-intensity femtosecond laser pulses and various plasma foils.The effects of the foil density and thickness on energy conversion efficiencies were studied,and laser pulses with different peak intensities were used to generate more γ photons and pairs.

    First,we have numerically investigated the effect of foil density on the energy conversion efficiencies and the positron number.The PIC simulation results reveal that for the same laser intensity,the energy conversion efficiency of the laser to γ photons and the produced photon number are highly related to the foil density.We found an optimal foil density of approximately 250ncby PIC simulations and theoretical analysis,which plays a key role during laser-plasma interaction QED processes.Second,using the optimal foil density,we performed simulations for foils with different thicknesses and observed an optimal foil thickness,which resulted in higher energy conversions and pair production.Finally,we investigated the relation between the laser intensity and conversion efficiencies.By comparatively evaluating the energy conversion efficiencies of two density cases(250ncand 500nc)with the optimal thickness,we found that the laser energy to photon conversion efficiency is enhanced by approximately 10%when the foil density is optimized.All of these findings indicate that foil design optimization is essential for a high-efficiency QED process.

    Acknowledgments

    This work was financially supported by National Natural Science Foundation of China(No.11 664 039).The authors are particularly grateful to CFSA at the University of Warwick for allowing us to use the EPOCH code(developed under UK EPSRC Grants(Nos.EP/G054940/1,EP/G055165/1,and EP/G056803/1)).

    在线天堂最新版资源| 国产精品,欧美在线| 他把我摸到了高潮在线观看| 欧美成人a在线观看| 韩国av在线不卡| av黄色大香蕉| 日本成人三级电影网站| 成人三级黄色视频| 亚洲av第一区精品v没综合| 日本欧美国产在线视频| 国产成人aa在线观看| 精品人妻一区二区三区麻豆 | 国产aⅴ精品一区二区三区波| 日本熟妇午夜| 精华霜和精华液先用哪个| 亚洲国产欧洲综合997久久,| 亚洲四区av| 久久精品国产亚洲av天美| 欧美人与善性xxx| 又粗又爽又猛毛片免费看| 亚洲av美国av| 亚洲四区av| 日韩欧美国产在线观看| 国语自产精品视频在线第100页| 亚洲成人精品中文字幕电影| 在线观看美女被高潮喷水网站| 国产精品美女特级片免费视频播放器| 中文字幕人妻熟人妻熟丝袜美| 日韩精品中文字幕看吧| 无遮挡黄片免费观看| a级毛片免费高清观看在线播放| 嫁个100分男人电影在线观看| 日韩欧美在线二视频| 赤兔流量卡办理| 国语自产精品视频在线第100页| 18禁黄网站禁片免费观看直播| 日韩强制内射视频| 国产成人aa在线观看| 人妻丰满熟妇av一区二区三区| 精品福利观看| 一进一出好大好爽视频| 男插女下体视频免费在线播放| 国产精品永久免费网站| 久久香蕉精品热| 久久这里只有精品中国| 久久久久国内视频| 久久久久精品国产欧美久久久| 久久久久国产精品人妻aⅴ院| 亚洲乱码一区二区免费版| 淫秽高清视频在线观看| 亚洲成a人片在线一区二区| 18+在线观看网站| ponron亚洲| 男女下面进入的视频免费午夜| а√天堂www在线а√下载| 久久99热6这里只有精品| 中文字幕av在线有码专区| 成人毛片a级毛片在线播放| 美女高潮喷水抽搐中文字幕| 午夜福利在线观看吧| 99精品久久久久人妻精品| 亚洲美女黄片视频| 亚洲一区二区三区色噜噜| 人人妻,人人澡人人爽秒播| 亚洲一区二区三区色噜噜| 一本精品99久久精品77| 我要搜黄色片| 免费观看人在逋| 日韩欧美精品免费久久| 国产伦人伦偷精品视频| 成人国产麻豆网| 日韩中字成人| 高清日韩中文字幕在线| 99久久中文字幕三级久久日本| 国产精品av视频在线免费观看| 一进一出好大好爽视频| 亚洲18禁久久av| 免费高清视频大片| 亚洲无线在线观看| 免费电影在线观看免费观看| 在线观看av片永久免费下载| av中文乱码字幕在线| 国产在线男女| 亚洲,欧美,日韩| 亚洲性久久影院| h日本视频在线播放| 色综合色国产| av福利片在线观看| 中文亚洲av片在线观看爽| 亚洲美女黄片视频| 日韩欧美一区二区三区在线观看| 国产一区二区在线av高清观看| 亚洲av成人av| 国内毛片毛片毛片毛片毛片| 欧美黑人巨大hd| 亚洲人与动物交配视频| 国产精品永久免费网站| 尾随美女入室| 日韩欧美 国产精品| 国产一区二区在线观看日韩| 国国产精品蜜臀av免费| 性插视频无遮挡在线免费观看| 午夜激情欧美在线| 又爽又黄a免费视频| 亚洲精华国产精华液的使用体验 | 少妇猛男粗大的猛烈进出视频 | 日韩欧美 国产精品| 搡女人真爽免费视频火全软件 | 99riav亚洲国产免费| 夜夜夜夜夜久久久久| 淫妇啪啪啪对白视频| 白带黄色成豆腐渣| 91av网一区二区| 亚洲性夜色夜夜综合| 美女 人体艺术 gogo| 国产高清三级在线| 最新中文字幕久久久久| 国产91精品成人一区二区三区| а√天堂www在线а√下载| 性欧美人与动物交配| 国产精品野战在线观看| 亚洲经典国产精华液单| av中文乱码字幕在线| 久久精品综合一区二区三区| 春色校园在线视频观看| 色尼玛亚洲综合影院| 欧美激情久久久久久爽电影| 亚洲成人精品中文字幕电影| 国产一区二区三区在线臀色熟女| 国产真实乱freesex| 观看免费一级毛片| 国产精品久久久久久久电影| 国产免费av片在线观看野外av| 欧美黑人巨大hd| 啦啦啦啦在线视频资源| 在线观看舔阴道视频| 久久热精品热| 十八禁网站免费在线| 高清毛片免费观看视频网站| 国产精品久久电影中文字幕| 人人妻人人看人人澡| 麻豆成人av在线观看| 久久人人精品亚洲av| 听说在线观看完整版免费高清| a在线观看视频网站| 日韩欧美国产在线观看| 婷婷精品国产亚洲av| 成人国产麻豆网| 男女之事视频高清在线观看| aaaaa片日本免费| 欧美潮喷喷水| 国产极品精品免费视频能看的| 国产精品久久久久久精品电影| 免费人成视频x8x8入口观看| 日本黄色片子视频| 欧美日本视频| 国产午夜福利久久久久久| 一区二区三区高清视频在线| 丰满人妻一区二区三区视频av| 男插女下体视频免费在线播放| 久久国产精品人妻蜜桃| 欧美一级a爱片免费观看看| 亚洲中文字幕一区二区三区有码在线看| 99久久精品热视频| 久久6这里有精品| 亚洲一区高清亚洲精品| 国产探花在线观看一区二区| 日韩,欧美,国产一区二区三区 | 久久人人精品亚洲av| 噜噜噜噜噜久久久久久91| 亚洲人与动物交配视频| 赤兔流量卡办理| 欧美日韩综合久久久久久 | 国内精品宾馆在线| 精品久久久久久久久久久久久| 久久久久久久久久成人| 国产爱豆传媒在线观看| 美女黄网站色视频| 日本a在线网址| 久久天躁狠狠躁夜夜2o2o| 日韩 亚洲 欧美在线| 高清毛片免费观看视频网站| 午夜老司机福利剧场| 97超级碰碰碰精品色视频在线观看| 精品日产1卡2卡| 成人二区视频| 国产av一区在线观看免费| 成人精品一区二区免费| 男人舔奶头视频| 国产成人福利小说| 在现免费观看毛片| 久久人妻av系列| 中文亚洲av片在线观看爽| 免费av毛片视频| 欧美激情在线99| 色尼玛亚洲综合影院| 网址你懂的国产日韩在线| 老熟妇仑乱视频hdxx| 日韩欧美 国产精品| 1000部很黄的大片| 亚洲av美国av| 精品午夜福利在线看| 99久久中文字幕三级久久日本| 波多野结衣高清作品| 免费人成视频x8x8入口观看| 韩国av在线不卡| 伊人久久精品亚洲午夜| 一区二区三区激情视频| 亚洲国产欧洲综合997久久,| 热99re8久久精品国产| 韩国av一区二区三区四区| 成人毛片a级毛片在线播放| 亚洲18禁久久av| 最近在线观看免费完整版| 久久久久久久亚洲中文字幕| 999久久久精品免费观看国产| АⅤ资源中文在线天堂| 简卡轻食公司| 亚洲国产日韩欧美精品在线观看| 久久国产乱子免费精品| 亚洲aⅴ乱码一区二区在线播放| 国产av一区在线观看免费| 动漫黄色视频在线观看| 床上黄色一级片| 精品一区二区三区视频在线| 日韩大尺度精品在线看网址| 在线天堂最新版资源| 深夜精品福利| 久久久色成人| 可以在线观看毛片的网站| 欧美+亚洲+日韩+国产| 嫩草影院精品99| 麻豆av噜噜一区二区三区| 欧美高清成人免费视频www| 神马国产精品三级电影在线观看| ponron亚洲| 亚洲av美国av| 久久亚洲真实| 中出人妻视频一区二区| 欧美绝顶高潮抽搐喷水| 五月伊人婷婷丁香| 色播亚洲综合网| 国产精品一区二区免费欧美| 国产极品精品免费视频能看的| 久久中文看片网| 69av精品久久久久久| 色视频www国产| 在线观看舔阴道视频| 中文字幕av成人在线电影| АⅤ资源中文在线天堂| av女优亚洲男人天堂| 欧美日韩国产亚洲二区| 99久久久亚洲精品蜜臀av| 九九热线精品视视频播放| 国产麻豆成人av免费视频| 成人综合一区亚洲| 日韩欧美国产一区二区入口| 噜噜噜噜噜久久久久久91| 欧美3d第一页| 伊人久久精品亚洲午夜| 日本色播在线视频| 欧美成人一区二区免费高清观看| 直男gayav资源| 亚洲人成网站在线播放欧美日韩| 男人舔女人下体高潮全视频| 免费看美女性在线毛片视频| 国产精品美女特级片免费视频播放器| 99精品在免费线老司机午夜| 国产老妇女一区| 少妇丰满av| 久久午夜福利片| 国产在视频线在精品| 白带黄色成豆腐渣| 97超视频在线观看视频| 亚洲性夜色夜夜综合| 夜夜爽天天搞| 久久草成人影院| 真人做人爱边吃奶动态| 欧美区成人在线视频| av中文乱码字幕在线| 99热网站在线观看| 18禁在线播放成人免费| 美女cb高潮喷水在线观看| 亚洲欧美激情综合另类| 久久久久久久久久久丰满 | 99久久成人亚洲精品观看| 国产av麻豆久久久久久久| 国内精品一区二区在线观看| 亚洲人成网站在线播放欧美日韩| 精品人妻偷拍中文字幕| 精品久久国产蜜桃| 欧美丝袜亚洲另类 | 国产精品爽爽va在线观看网站| 欧美色欧美亚洲另类二区| 欧美日韩国产亚洲二区| 热99在线观看视频| 久久久久久大精品| 久久午夜亚洲精品久久| 国产在线男女| 日韩欧美精品v在线| 欧美在线一区亚洲| 大又大粗又爽又黄少妇毛片口| 自拍偷自拍亚洲精品老妇| 久久久久九九精品影院| 国产av麻豆久久久久久久| 国产精品乱码一区二三区的特点| 深夜a级毛片| 亚洲五月天丁香| 国产欧美日韩精品一区二区| 最好的美女福利视频网| 久久午夜福利片| 中国美白少妇内射xxxbb| 黄色女人牲交| 69av精品久久久久久| 九色国产91popny在线| 中文亚洲av片在线观看爽| 美女高潮喷水抽搐中文字幕| 99久久精品国产国产毛片| 国产精品野战在线观看| 日本免费一区二区三区高清不卡| or卡值多少钱| 老司机福利观看| 在线观看66精品国产| 亚洲精品色激情综合| 亚洲人与动物交配视频| 国产精品98久久久久久宅男小说| 九色成人免费人妻av| 两人在一起打扑克的视频| 在线a可以看的网站| 噜噜噜噜噜久久久久久91| 最新在线观看一区二区三区| 国产精品98久久久久久宅男小说| 亚洲精品粉嫩美女一区| 欧美成人免费av一区二区三区| 国产精品一区二区性色av| 成人午夜高清在线视频| 精品一区二区三区av网在线观看| 国产高潮美女av| 一个人免费在线观看电影| 两人在一起打扑克的视频| 韩国av一区二区三区四区| 亚洲精品在线观看二区| 亚洲无线在线观看| 女人被狂操c到高潮| 欧美不卡视频在线免费观看| 日韩精品有码人妻一区| 97热精品久久久久久| 日日摸夜夜添夜夜添小说| 国产三级中文精品| 亚洲av一区综合| 日韩欧美在线二视频| av.在线天堂| 色哟哟·www| 欧美成人免费av一区二区三区| 99久久久亚洲精品蜜臀av| 国产精品一区二区三区四区久久| 亚洲电影在线观看av| 动漫黄色视频在线观看| 丰满人妻一区二区三区视频av| 亚洲av第一区精品v没综合| 午夜精品一区二区三区免费看| 国产在线男女| 国产精品久久电影中文字幕| 午夜福利在线观看免费完整高清在 | 此物有八面人人有两片| 乱人视频在线观看| 人妻少妇偷人精品九色| 啦啦啦韩国在线观看视频| 亚洲真实伦在线观看| 国产高清有码在线观看视频| 国内精品久久久久精免费| 亚洲成人中文字幕在线播放| 亚洲欧美日韩高清专用| 两性午夜刺激爽爽歪歪视频在线观看| 欧美黑人欧美精品刺激| 免费看日本二区| 亚洲国产高清在线一区二区三| 日韩欧美免费精品| 国产高清三级在线| 91av网一区二区| 麻豆成人午夜福利视频| 伊人久久精品亚洲午夜| 哪里可以看免费的av片| 免费黄网站久久成人精品| 22中文网久久字幕| 嫩草影院入口| 国产高清激情床上av| 美女 人体艺术 gogo| 国产精品一区二区性色av| 久久久久久久精品吃奶| 精品一区二区三区av网在线观看| ponron亚洲| 国产免费一级a男人的天堂| 91av网一区二区| 成年人黄色毛片网站| 欧美激情国产日韩精品一区| 国产av不卡久久| 中文字幕av成人在线电影| 色在线成人网| av女优亚洲男人天堂| 国产乱人伦免费视频| 综合色av麻豆| 午夜久久久久精精品| 日韩欧美精品v在线| av女优亚洲男人天堂| 又紧又爽又黄一区二区| 亚洲18禁久久av| 啦啦啦啦在线视频资源| 三级国产精品欧美在线观看| 女人十人毛片免费观看3o分钟| 亚洲中文日韩欧美视频| 久久久久久久久大av| 麻豆av噜噜一区二区三区| 国产免费一级a男人的天堂| 久久天躁狠狠躁夜夜2o2o| 中国美白少妇内射xxxbb| 国产男人的电影天堂91| 国内久久婷婷六月综合欲色啪| 日日啪夜夜撸| 亚洲欧美日韩高清专用| 亚洲精品一卡2卡三卡4卡5卡| 亚洲av一区综合| 看黄色毛片网站| 精品乱码久久久久久99久播| 欧美成人免费av一区二区三区| 亚洲专区中文字幕在线| 国产精品精品国产色婷婷| 成人特级av手机在线观看| 欧美高清性xxxxhd video| 此物有八面人人有两片| 九色成人免费人妻av| 男人和女人高潮做爰伦理| 特级一级黄色大片| 亚洲18禁久久av| 精品久久久久久成人av| 午夜福利在线在线| 精品一区二区三区视频在线| .国产精品久久| 狠狠狠狠99中文字幕| 免费av观看视频| 国产精品免费一区二区三区在线| 精品午夜福利视频在线观看一区| 91午夜精品亚洲一区二区三区 | 99精品在免费线老司机午夜| 丰满的人妻完整版| 免费看日本二区| 在线观看av片永久免费下载| 18禁裸乳无遮挡免费网站照片| 欧美绝顶高潮抽搐喷水| 九九热线精品视视频播放| 精品久久久噜噜| 非洲黑人性xxxx精品又粗又长| 国内少妇人妻偷人精品xxx网站| 在线免费观看不下载黄p国产 | 黄色丝袜av网址大全| 亚洲自偷自拍三级| 午夜免费男女啪啪视频观看 | 午夜精品一区二区三区免费看| 国产av不卡久久| 国产精品不卡视频一区二区| 成人午夜高清在线视频| 亚洲电影在线观看av| bbb黄色大片| 亚洲欧美日韩无卡精品| 黄色丝袜av网址大全| 国产国拍精品亚洲av在线观看| 国产亚洲精品综合一区在线观看| 欧美成人性av电影在线观看| 久久精品91蜜桃| 熟女人妻精品中文字幕| 亚洲成人中文字幕在线播放| 真实男女啪啪啪动态图| 亚洲最大成人av| 国产精品国产高清国产av| 日韩高清综合在线| 国内精品美女久久久久久| aaaaa片日本免费| 国产一区二区在线观看日韩| 最近最新中文字幕大全电影3| 国产一区二区亚洲精品在线观看| 欧美绝顶高潮抽搐喷水| 桃红色精品国产亚洲av| 波多野结衣高清无吗| 免费在线观看成人毛片| 国内少妇人妻偷人精品xxx网站| 麻豆成人午夜福利视频| 午夜免费男女啪啪视频观看 | 久久精品人妻少妇| 午夜福利视频1000在线观看| 日本熟妇午夜| 男女边吃奶边做爰视频| 久久国产精品人妻蜜桃| 亚州av有码| 久久精品国产鲁丝片午夜精品 | 久久久国产成人精品二区| 久久精品人妻少妇| 国产成人av教育| 此物有八面人人有两片| 亚洲欧美日韩高清专用| 国产乱人伦免费视频| 校园人妻丝袜中文字幕| 免费看美女性在线毛片视频| 99热这里只有是精品50| 精品午夜福利在线看| 乱码一卡2卡4卡精品| 国内揄拍国产精品人妻在线| 久久久国产成人精品二区| 日本五十路高清| 在线免费观看不下载黄p国产 | 免费人成视频x8x8入口观看| 国内精品一区二区在线观看| 免费大片18禁| 国产精品99久久久久久久久| 听说在线观看完整版免费高清| 免费av观看视频| 亚洲最大成人av| 国产亚洲精品av在线| or卡值多少钱| 亚洲无线观看免费| 日韩欧美免费精品| 欧美绝顶高潮抽搐喷水| 一区二区三区四区激情视频 | 热99re8久久精品国产| 成人国产一区最新在线观看| 亚洲欧美激情综合另类| 国产三级在线视频| 成人鲁丝片一二三区免费| 亚洲欧美精品综合久久99| avwww免费| 国产精品野战在线观看| 夜夜爽天天搞| 亚洲精品亚洲一区二区| 欧洲精品卡2卡3卡4卡5卡区| 精品久久国产蜜桃| h日本视频在线播放| bbb黄色大片| 男女做爰动态图高潮gif福利片| 麻豆一二三区av精品| 99国产精品一区二区蜜桃av| 老熟妇仑乱视频hdxx| 精品99又大又爽又粗少妇毛片 | 欧美日韩瑟瑟在线播放| 99精品久久久久人妻精品| 色噜噜av男人的天堂激情| 中文字幕久久专区| 最近中文字幕高清免费大全6 | 午夜福利在线观看吧| 国产乱人视频| 国产av一区在线观看免费| 久久久精品欧美日韩精品| 女同久久另类99精品国产91| 日本黄色片子视频| 亚洲一级一片aⅴ在线观看| 欧美高清成人免费视频www| 97热精品久久久久久| 亚洲真实伦在线观看| 国产色爽女视频免费观看| 欧美日韩乱码在线| 国产极品精品免费视频能看的| 啦啦啦啦在线视频资源| 亚洲国产欧洲综合997久久,| 国产精品国产高清国产av| 国产成人aa在线观看| 国产主播在线观看一区二区| 国产亚洲精品综合一区在线观看| 亚洲va在线va天堂va国产| 无遮挡黄片免费观看| 日韩大尺度精品在线看网址| 亚洲黑人精品在线| 久久久午夜欧美精品| 最近最新中文字幕大全电影3| 超碰av人人做人人爽久久| av.在线天堂| 91麻豆av在线| 欧美一区二区国产精品久久精品| 小说图片视频综合网站| 女人被狂操c到高潮| 久久精品影院6| 国产精品一区二区三区四区免费观看 | 最近在线观看免费完整版| 婷婷色综合大香蕉| 可以在线观看毛片的网站| 久久天躁狠狠躁夜夜2o2o| 自拍偷自拍亚洲精品老妇| 欧美一级a爱片免费观看看| 最近中文字幕高清免费大全6 | 亚洲欧美清纯卡通| 91av网一区二区| 啦啦啦韩国在线观看视频| 精品久久久久久久末码| 色在线成人网| 成人欧美大片| 国模一区二区三区四区视频| 欧美日本亚洲视频在线播放| 亚洲欧美日韩高清在线视频| 欧美激情在线99| 此物有八面人人有两片| 又黄又爽又刺激的免费视频.| 亚洲七黄色美女视频| 国产精品综合久久久久久久免费| 日韩欧美在线二视频| 18禁在线播放成人免费| 三级国产精品欧美在线观看| 久久精品国产亚洲av天美| 国国产精品蜜臀av免费| 又紧又爽又黄一区二区| 免费看日本二区| 丰满乱子伦码专区| 国产视频一区二区在线看| 欧美中文日本在线观看视频| 哪里可以看免费的av片| 麻豆成人av在线观看| 如何舔出高潮| 欧美性猛交黑人性爽| 中文亚洲av片在线观看爽|