• <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 ?

    Response Ability to External Signal Enhanced by Biological Spatial Configuration in Coupled Hindmarsh-Rose Neural System

    2016-09-13 08:14:50ShoufangHuangJiqianZhangMaoshengWangCollegeofPhysicsandElectronicInformationAnhuiNormalUniversityWuhu241000ChinaDatedReceivedonMay2015AcceptedonSeptember292015
    CHINESE JOURNAL OF CHEMICAL PHYSICS 2016年2期

    Shou-fang Huang,Ji-qian Zhang,Mao-sheng WangCollege of Physics and Electronic Information,Anhui Normal University,Wuhu 241000,China(Dated:Received on May 4,2015;Accepted on September 29,2015)

    ?

    Response Ability to External Signal Enhanced by Biological Spatial Configuration in Coupled Hindmarsh-Rose Neural System

    Shou-fang Huang,Ji-qian Zhang?,Mao-sheng Wang
    College of Physics and Electronic Information,Anhui Normal University,Wuhu 241000,China
    (Dated:Received on May 4,2015;Accepted on September 29,2015)

    The effect of realistic topology configuration of intercellular connections on the response ability in coupled cell system is numerically investigated by using the Hindmarsh-Rose model. For the proper coupling intensity,we set the control parameter to be near the critical value,and the external stimulus is introduced to the first cell in coupled system.It is found that,on one hand,when the cells are coupled with some proper topological structures,the external stimulus could transmit through the system,and shows better response ability and higher sensitivity.On the other hand,the influence of topological configuration on the synchronous ability and selection effect of neural system are also discussed.Our results display that the topology of coupled system may play an important role in the process of signal propagation,which could help us to understand the coordinated performance of cells in tissue.

    Hindmarsh-Rose model,Topology configuration,Response ability,Selection effect

    I.INTRODUCTION

    Recently,more and more attention has been focused on the dynamic processes in complex networks because of their importance in explicitly mimicking highly complex structure of many realistic systems,especially in biological neural networks[1-7].Some researchers reported that the dynamical behavior of the neuron is quite complex,which exhibits sub-threshold periodic,chaotic responses,chaotic firing of spikes,as well as mode-locked firing.These complex behaviors can be controlled by adjusting different configuration parameters under a periodic stimulation[8].Furthermore,people found the effects of external period force and noise on the controlled system,and the complexity of system can be suppressed by the slaving principle[9]. These results imply the stimuli from the internal or external environment of neuron system,may play an important role in controlling its collective activities.In recent years,some researchers found the system size and coupling strength also play a vital role in FitzHugh-Nagumo neural network[10].By controlling bifurcation parameters in the networks of Hodgkin-Huxley or Hindmarsh-Rose(HR)neurons,the transition behavior from spiral wave to other state can be induced[11,12].

    Nowadays,the frontier of the research interest has focused on two kinds of collective behaviors in coupled complex systems.On one hand,the influences of the network topology on dynamical behaviors are investigated,especially the nervous system’s dynamic features[13-15].For example,the spiking oscillations show the best regularity at optimal network topology randomness[15].The introduction of small-world connections can change the second-order phase transition into a firstorder one in the 2D Ising model[16].On the other hand,how was collective dynamics of a system controlled by adjusting the parameters or introducing external stimuli.Some fascinating and important research showed the effect of system size on the dynamics behavior of system[17-19].Time delays in a network of the HR model can induce phase-flip transitions leading to synchrony or out of synchrony[20,21].

    In the models mentioned above,the biological realistic cellular topology of the neural system was not considered.However,in actual tissue,even in small areas,its topological structure is significantly complicated[22-24].It was found that the topology of intercellular connections in tissue has an essential influence on calcium ions signaling[25].The geometrical factors may play a crucial role in both intra and intercellular calcium ions signaling[26].An interesting problem is whether the spatial topology is closely related with the periodic bursting behaviors in the response dynamics of the neural system or not.And how does this topology control the efficiency of signal processing in neuronal system?Thus,in this work,by using the HR model as the units,and constructing a 2D regular lattice with the nearest connections,we mainly investigate the effect of spatial topology on the signal propagation behavior of HR coupled system.

    Our results really show that in a proper coupling strength region,we can observe the state-to-state tran-sition(SST)behaviors between different states,the stimulus intensity and the delay time needed by SST behavior are different in all possible configurations.

    II.MODEL

    The paradigmatic model used here is first proposed by Hindmarsh and Rose in 1985[27].It is originally introduced to describe the firing behavior of neurons,and qualitatively explain the bursting type with inter spike intervals of real neurons.In this work,we consider the dynamics of a system of N(N=4)coupled HR neurons,in which local coupling may correspond to the diffusion process between the nearest-neighbours,and the longrange connections to the electrical synaptic connections among non-neighbouring cells.The dynamics of an isolated HR neuron are described by three-variable differential equations as the following(for a single cell i=1 and γ=0.0).

    where xiis the membrane potential,yiis a recovery variable,and ziis a slow adaptation current for the ith neuron.The constants a,b,c,d,r,s,and X0are set as a=1.0,b=3.0,c=1.0,d=5.0,s=4.0,r=0.006,and X0=-1.56,respectively.The last term in Eq.(1)denotes the coupling term for the complex neurons.γ is the coupling strength,and the indices i,j denote the cell number,Cijis the coupling parameter between the two neurons i and j.If these two neurons are coupled to each other,Cij=1,otherwise,Cij=0.In this work,we consider the case of four coupled HR neurons,in which there are ten possible different configurations A-J[23](see Fig.1),and all possible plane configurations can be distinguished with different combination of Cij.

    It is well known,the bifurcation characteristic and the complex vibration modes of HR neurons are closely related to the variable Iext,so it is used as one of the control parameters to generate various firing patterns of neural network.The time series of the variable x(t)is a spike train which can display the most important coded information in neural systems.

    The bifurcation property of a single neuron can be obtained by calculating the inter spike intervals of neuronal firing,in which a spike pulse in the x(t)variable is defined when the ith cell is excited so that x(t)exceeds a given threshold value x0(note that a spike occurs when the state variable x(t)is near x=1.2,so the excited threshold value x0=1.0).One can notice that from the bifurcation diagram,the complex firing activity of neuron provides a rather rich dynamical behaviors including periodic bursting state and chaotic motions[28].

    In the following sections,it is reasonable and feasible to study the effects of topology connectivity on the dynamical behaviors by using the HR model.Numerical integrations of Eq.(1)are carried out using the fourthorder Runge-Kutta scheme with time step of dt=0.001. To obtain each numerical result,those beginning data of simulation are discarded and 106time steps are used.

    FIG.1 Different topology structures(A-J)for 4-coulpled cells system.The external stimulus is introduced to the cell labeled by number 1.

    III.RESULTS AND DISCUSSION

    To investigate the effects of topological configurations on the dynamics of neural firing patterns in the 4-neuron coupling system mentioned above,and show the SST behavior,under the condition of proper coupling strength,we adjust the system parameter as the following scheme∶change topological configuration for different critical current Iext,which locals in the righthand side for each bifurcation point[28].To quantify the SST effects induced by external stimulus,the time series of output signal was analyzed and the values of the inter spike intervals versus the external current Iextare obtained.

    A.Response ability to external weak signal enhanced by topology

    Firstly,we consider the case that only the cell 1 is stimulated by external current,and discuss which type of configuration is more advantageous to the signal response in coupled system.To do this,we fix the coupling strength γ=0.07,and select one type of configurations(such as type H),then set the external current as Iext=1.20,the neural system may keep in the 1-periodstate.One can find,with the increasing of Iext,the external stimulus information could be propagated along this coupled chain,and all cells could turn into 2-period state successively,indicating the phenomenon of SST occurs under this condition.Similar synchronous SST behavior could be seen for other configurations.Of cause,the critical values Iextof the four cells for SST are different under the condition of certain coupling strength,so we select the critical current value of the cell which induces the system to enter the transition state as the critical standard.

    To describe the response ability of the system to the external feeble signal enhanced by proper configuration,we introduce the synchronous error e of critical value by the following formula∶

    where Ii,cis critical values of Iext,e can provide an indication of firing patterns transition dynamics in neural system.The smaller the current value ofˉI is,the more easily the state transition occurs,also,the smaller e implies the better effect of the synchronous transition between two states.

    FIG.2 Critical current values Ii,cand synchronous error e for all configurations as a function of different values of coupling strength γ for ten configuration types(A-J),when neural systems turn into 2-period state from 1-period state.(a)and(b)type H,(c)all types.a=1.0,b=3.0,c=1.0,d=5.0,s=4.0,r=0.006,X0=-1.56.

    The critical current values Ii,cand synchronous error e as functions of the different coupling strength for different configuration types are depicted in Fig.2.In Fig.2(a)and(b)we could find with the increment of γ,the critical values ofˉI and synchronous error e reduce continuously for a certain type of configuration. Of cause,the values of types A and B are larger than others indicating the coupled system could not transit to the 2-period state easily in these configurations.This means the 1D chain configuration is not suitable for the transition behavior.On the contrary,if cells are coupled to C,D,and J configurations,the system could jump to the 2-periodic state very easily than those in A and B(Fig.2(c)).Above results imply that the HR system may enhance its response ability to external stimulus through the mode of SST,by using proper spatial topology configuration and adjusting itself parameter.

    B.Response time of SST behavior shorten by topology

    To study the effects of spatial configuration on the SST behavior in coupled noisy system,so we introduce an external noise in Eq.(1),i.e.∶

    where ξ(t)is Gaussian white noise with〈ξ(t)〉=0,〈ξ(t)ξ(t′)〉=D2δ(t-t′),D is the noise intensity.To discuss the transition between 1-period and 2-period states,we select the typical configurations B and D as the examples,and fix γ=0.07,Iext=1.20.Here,the external noise intensity is an adjustable parameter,other parameters are the same as the above,i.e.a=1.0,b=3.0,c=1.0,d=5.0,s=4.0,r=0.006,X0=-1.56.One can find that,when noise is introduced,and its intensity is set to be D=0.1,the system may transit to the 2-period state.We also found the SST happen quickly in cells 2 and 3 when the noise is switched on the cell 1,while cell 4 reach the same state only after a period of time,indicating there is a certain time delay in the propagation of the stimulus along the coupling system,and this time delay depends on noise intensity.Similar phenomenon can also be found in other 9 configurations. We can define this time delay τ1,jas the time interval among which the SST first appears in first cell and then transmits to the cell j(see Fig.3(a)).The mean value of time delay〈τ〉among cells in coupled system readsby the following∶

    The mean delay time〈τ〉as a function of noise intensity for different configurations are depicted in Fig.3(b),from this figure,one can find that,for each configuration,the delay time decreases with increment of noise intensity,which means that the signal transmission processing could be accelerated by adjusting the noise intensity.

    We also find that the mean value of delay times〈τ〉is different for ten configurations with the same noise intensity.For example,the mean delay time in configuration A is larger than that in the type D,and especially,with increment of noise intensity the mean delay time〈τ〉in the type D decreases very faster than that in other types.These results may indicate that in configuration D,the system is more advantageous to improve the response speed and response ability.

    After further study,we found that,the delay time not only depends on noise intensity,but also depends on the connection distance(CD,between the stimulated cell and a given cell).For example,in configuration A,the CD between cell 2 and cell 1 is 1,while between cell 3 and cell 1 is 2.The CD between the cell 1 and the another cells in all configurations are listed in Table I.These data may provide us some useful clues to analyze the SST behavior.Obviously,in configuration D and G,the average distance is the shortest,while in configuration A the CD is longest,this difference may be the reason for that the D and G configurations are more suitable for the transmission of information than others.

    FIG.3(a)Plot of time series of the membrane potentials(x(t))induced by noise in cell 1(solid lines)and cell j(dotted lines).τ1,jis the delay time between the spiking/bursting of cell 1 and cell j.(b)The mean delay time of bursting vs.noise intensity for all ten types of configurations(A-J)in four coupled cells system.

    TABLE I Average distance in different topological configurations.

    C.The topology influence on selection effect of system

    In this work,we have also discussed the selection effect of the topology to the external signal,the corresponding dynamic equations are as follows∶

    where A is the critical value of amplitude.According to the same scheme used for adjusting noise mentioned above,we first set the system to be in the 1-period state,then select the amplitude or frequency as control parameters,respectively.The distribution of inter spike intervals versus the amplitude A for a constant frequency(f=0.001)is depicted in Fig.4.It is found that,in configuration H,cell 1 is in 1-period state if A<0.003,while if A increases to 0.003,2-period state appears,indicating the SST occurs.But in the other three cells,the critical value of A is different when the SST occurs∶in cells 2,cell 3,and cell 4,A=0.152,0.154,and 0.14,respectively.Thus,to make the whole system appear SST behavior,the amplitude should be set to the maximum critical value,i.e.,A=0.154.

    Similar results are also observed when we adjust the frequency,and the critical values of amplitude(or frequency)of each configuration for different frequency(or amplitude)of the external signal are depicted in Fig.4.

    In Fig.4(a),it is observed that in some proper configurations(such as in C,D,and J),with the increment of f,the periodic motion in the cell 1 could transmit easily from 1-period to 2-period,indicating that SST occurs.These results suggest that some proper types of configuration(such as C and J)can enhance effectively the sensitivity of the HR system to the weak signal,implying the selection effect of topology.

    We now consider some interesting configurations of four cells in detail.In configuration E and I,the disposition of cell 1,cell 3 and cell 4 is symmetrical relative to cell 2(Fig.1 E and I),and the average connection distance of coupled cell system is the same(see Table I),but the system shows different selection effect on the external signal and this difference is also manifested in weaker response in cell 3 and cell 4 in configuration E,as compared with configuration I(see Fig.4(a)and(b)).The topological difference between configurations E and I consists in the presence(E)and absence(I)of a connection between cell 3 and cell 4.This is connected with the fact that cell 3 in configuration E exchanges external signal with cell 4 in addition to cell 2,whereas there is no such exchange in configuration I.That additional exchange decreases the value of A and f in cell 3 and cell 4 when the SST occurs in configuration E.

    This interesting phenomenon also takes place in other configurations.Such as in configuration G and H,the disposition of cell 2,cell 3,and cell 4 is symmetrical relative to cell 1(Fig.1 G and H),and the average connection distance of coupled cell system is the same(see Table I),but there is an additional connection between cell 3 and cell 4 in configuration G.Obviously,this additional connection makes the system show different selection effect and decreases the time delay among four cells(see Fig.3).In other words,additional connection can improve the response speed and ability of coupled cells system.

    FIG.4(a)The critical value of amplitude A of each configuration for different frequency of the external signal.(b)The critical value of frequency f of each configuration for different amplitude of the external signal.

    IV.CONCLUSION

    We have investigated the effects of topological structures of system on the response ability to external stimulus signal in coupled HR neural system.It is found,when the controlling parameters such as the external current intensity or noise intensity are adjusted to be the critical values,and when the system is coupled to some proper configurations,SST phenomenon could appear in coupled system.This result may suggest that the neural system could improve its response ability and sensitivity to external stimulus signal by choosing suitable configuration.

    We hope our results could provide some interesting information for understanding the properties of collective response behavior and mechanisms of information processing in coupled real neurobiological systems. Note that we only consider two dimensional configurations of four cells in this work.It would be interesting to consider the role of topological structure in more cells coupled system and three dimensional tissues,which is a subject of our future research.

    V.ACKNOWLEDGMENTS

    This work was supported by the National Natural Science Foundation and Special Found for the Theoretical Physics of China(No.21103002 and No.11047017),the Special Foundation of Education of Anhui Province for Excellent Young Scientists(No.2011SQRL023),and the Natural Science Funds of Anhui Province of China(No.1508085MA15).

    [1]M.Bucolo,L.Fortuna,and M.LaRosa,Chaos,Solitons Fractals 14,1059(2002).

    [2]F.Han,Q.S.Lu,M.Wiercigroch,and Q.B.Ji,Inter. J.NonLinear Mechanics 44,298(2009).

    [3]H.S.Chen,J.Q.Zhang,and J.Q.Liu,Phys.A 387,1071(2008).

    [4]M.S.Wang,Z.H.Hou,and H.W.Xin,Phys.Lett.A 334,93(2008).

    [5]P.Wang,J.Q.Zhang,and H.L.Ren,J.Chem.Phys. 23,23(2010).

    [6]L.X.Duan,Q.S.Lu,and Q.Y.Wang,Neurocomputing 72,341(2008).

    [7]X.J.Sun,M.Perc,Q.S.Lu,and J.Kurths,Chaos 18,023102(2008).

    [8]E.M.Izhikevich,Int.J.Bifurcation Chaos.10,1171(2000).

    [9]W.Wang,Y.Wang,and Z.D.Wang,Phys.Rev.E 57,R2527(1998).

    [10]D.Q.Wei,X.S.Luo,and Y.L.Zou,Commun.Theor. Phys.50,267(2008).

    [11]J.Ma,C.N.Wang,W.Y.Jin,and Y.Wu,Appl.Math. Comput.217,3844(2010).

    [12]C.N.Wang,J.Ma,J.Tang,and Y.L.Li,Commun. Theor.Phys.53,382(2010).

    [13]O.Kwon and H.T.Moon,Phys.Lett.A 298,319(2002).

    [14]M.Lin and T.L.Chen,Phys.Rev.E 71,016133(2005).

    [15]Q.S.Li and Y.Gao,Phys.Rev.E 77,036117(2008).

    [16]A.D.S′anchez,J.M.L′opez,and M.A.Rodriguez,Phys. Rev.Lett.88,048701(2002).

    [17]A.Pikovsky,A.Zaikin,and M.A.de la Casa,Phys. Rev.Lett.88,050601(2002).

    [18]Z.H.Hou,J.Q.Zhang,and H.W.Xin,Phys.Rev.E 74,031901(2006).

    [19]J.Q.Zhang,C.D.Wang,M.S.Wang,and S.F.Huang,Neurocomputing 74,2961(2011).

    [20]M.B.Adhikari,A.Prasad,and M.Dhamala,Chaos 21,023116(2011).

    [21]M.M.Shrii,D.V.Senthilkumar,and J.Kurths,Europhys.Lett.98,10003(2012)

    [22]J.H.Evans and M.J.Sanderson,Am.J.Physiol.277,L30(1999).

    [23]H.Niessen,H.Harz,P.Bedner,K.Kramer,and K. Willecke,J.Cell Sci.113,1365(2000).

    [24]M.V.L.Bennett and V.K.Verselis,Semin.Cell.Biol. 3,29(1992).

    [25]I.V.Dokukina,M.E.Gracheva,E.A.Grachev,and J. D.Gunton,Phys.D 237,745(2008).

    [26]K.Tsaneva-Atanasova,D.I.Yule,and J.Sneyd,Biophys.J.88,1535(2005).

    [27]J.L.Hindmarsh and R.M.Rose,Proc.R.Soc.London Ser.B 221,87(1984).

    [28]S.F.Huang,J.Q.Zhang,and S.J.Ding,Chin.Phys. Lett.26,050502(2009).

    ?Author to whom correspondence should be addressed.E-mail:zhangcdc@mail.ahnu.edu.cn

    久久久久久久久久人人人人人人| 亚洲一级一片aⅴ在线观看| 青春草亚洲视频在线观看| 男人和女人高潮做爰伦理| 亚洲图色成人| 老司机影院毛片| 日本午夜av视频| 免费av中文字幕在线| 国内精品宾馆在线| 在线观看人妻少妇| 久久国产精品大桥未久av | 狂野欧美激情性xxxx在线观看| 中文字幕精品免费在线观看视频 | 精品久久久久久久久av| 亚洲精品日本国产第一区| 极品少妇高潮喷水抽搐| 国产精品久久久久久久电影| 一本色道久久久久久精品综合| 在线观看美女被高潮喷水网站| 欧美xxxx性猛交bbbb| 日韩视频在线欧美| 国产爱豆传媒在线观看| av一本久久久久| 精品久久久久久久末码| 新久久久久国产一级毛片| 大香蕉久久网| 欧美日韩精品成人综合77777| 久久影院123| 亚洲精品第二区| 这个男人来自地球电影免费观看 | 22中文网久久字幕| 狂野欧美激情性xxxx在线观看| 最近的中文字幕免费完整| 成年女人在线观看亚洲视频| 男的添女的下面高潮视频| 精品午夜福利在线看| 我要看黄色一级片免费的| 国产日韩欧美亚洲二区| 精品国产一区二区三区久久久樱花 | 久久精品人妻少妇| 亚洲精品乱码久久久久久按摩| 日韩一区二区三区影片| 成年免费大片在线观看| 日韩一区二区三区影片| 中文字幕亚洲精品专区| 内地一区二区视频在线| 国产 一区 欧美 日韩| 一个人免费看片子| 国产成人一区二区在线| 久久热精品热| 免费久久久久久久精品成人欧美视频 | 亚洲欧美中文字幕日韩二区| 大又大粗又爽又黄少妇毛片口| 永久网站在线| 国国产精品蜜臀av免费| 狂野欧美白嫩少妇大欣赏| 男女无遮挡免费网站观看| 高清黄色对白视频在线免费看 | 国产精品嫩草影院av在线观看| 又黄又爽又刺激的免费视频.| 在线天堂最新版资源| 久久久久久伊人网av| videossex国产| 亚洲国产精品国产精品| 高清黄色对白视频在线免费看 | 亚洲人与动物交配视频| 91精品一卡2卡3卡4卡| 国产极品天堂在线| 亚洲欧美日韩卡通动漫| 乱码一卡2卡4卡精品| 国产有黄有色有爽视频| 免费久久久久久久精品成人欧美视频 | 亚洲丝袜综合中文字幕| av在线观看视频网站免费| 激情 狠狠 欧美| 国产69精品久久久久777片| 高清视频免费观看一区二区| 欧美精品一区二区免费开放| 国产精品久久久久久av不卡| 成人美女网站在线观看视频| 亚洲精品乱码久久久久久按摩| 噜噜噜噜噜久久久久久91| 国产乱来视频区| 久久av网站| 国产爱豆传媒在线观看| 这个男人来自地球电影免费观看 | 尤物成人国产欧美一区二区三区| 国产v大片淫在线免费观看| 精品99又大又爽又粗少妇毛片| 在线亚洲精品国产二区图片欧美 | 午夜福利在线在线| 日本av免费视频播放| 色婷婷av一区二区三区视频| 亚洲内射少妇av| 在线观看一区二区三区| 日韩人妻高清精品专区| 男的添女的下面高潮视频| 日韩伦理黄色片| 成人黄色视频免费在线看| 久久99热这里只有精品18| 高清日韩中文字幕在线| 国产成人精品婷婷| 午夜免费鲁丝| 在现免费观看毛片| 亚洲av在线观看美女高潮| 久热这里只有精品99| 久久久久久久久久人人人人人人| 你懂的网址亚洲精品在线观看| 伦理电影大哥的女人| 乱码一卡2卡4卡精品| 亚洲精品一二三| 亚洲av二区三区四区| av在线蜜桃| 亚洲成人中文字幕在线播放| 精品国产三级普通话版| 欧美少妇被猛烈插入视频| 久久99热这里只频精品6学生| 国产 精品1| 日日啪夜夜爽| 一级毛片aaaaaa免费看小| 青春草国产在线视频| av不卡在线播放| 99热这里只有是精品在线观看| 国产欧美日韩一区二区三区在线 | 男女边吃奶边做爰视频| 卡戴珊不雅视频在线播放| 国产老妇伦熟女老妇高清| 丝瓜视频免费看黄片| 欧美老熟妇乱子伦牲交| 亚洲第一区二区三区不卡| 高清黄色对白视频在线免费看 | 一个人看的www免费观看视频| 国产精品一区二区在线观看99| 色综合色国产| 亚洲精品日韩在线中文字幕| 亚洲欧美成人综合另类久久久| 精品久久久久久久久av| 亚洲,一卡二卡三卡| 狂野欧美激情性bbbbbb| 国产在线一区二区三区精| 色5月婷婷丁香| 人体艺术视频欧美日本| 亚洲欧美成人综合另类久久久| 一区二区三区精品91| 久久久久久伊人网av| 久久久久精品久久久久真实原创| 国产亚洲欧美精品永久| 高清日韩中文字幕在线| 国产亚洲欧美精品永久| 久久人人爽人人爽人人片va| 97热精品久久久久久| 黄色视频在线播放观看不卡| 99久久人妻综合| 伊人久久精品亚洲午夜| 亚洲精品亚洲一区二区| 一本—道久久a久久精品蜜桃钙片| 亚洲精品久久午夜乱码| 日韩 亚洲 欧美在线| 国产色爽女视频免费观看| 欧美日韩综合久久久久久| 欧美日韩视频精品一区| 午夜激情久久久久久久| 国产成人a∨麻豆精品| 亚洲aⅴ乱码一区二区在线播放| 免费观看的影片在线观看| 免费在线观看成人毛片| 免费黄频网站在线观看国产| 国产成人午夜福利电影在线观看| 色综合色国产| 美女主播在线视频| 一级毛片久久久久久久久女| 久久久久精品性色| 欧美极品一区二区三区四区| a级毛色黄片| 国产精品伦人一区二区| 久久毛片免费看一区二区三区| 99re6热这里在线精品视频| 久久99精品国语久久久| 中国三级夫妇交换| 嫩草影院入口| 啦啦啦啦在线视频资源| videos熟女内射| 精品国产露脸久久av麻豆| 国产精品秋霞免费鲁丝片| 国产精品一区二区在线不卡| 午夜免费鲁丝| 在线观看国产h片| 99久久综合免费| 天堂俺去俺来也www色官网| 少妇精品久久久久久久| 18+在线观看网站| 人体艺术视频欧美日本| 久久久成人免费电影| 毛片一级片免费看久久久久| 欧美丝袜亚洲另类| 免费黄网站久久成人精品| 极品教师在线视频| 中文在线观看免费www的网站| 国产探花极品一区二区| 精品熟女少妇av免费看| 国产精品一及| 欧美日韩国产mv在线观看视频 | 色婷婷av一区二区三区视频| 国产精品久久久久久精品古装| 国产av精品麻豆| 激情五月婷婷亚洲| 亚洲精品第二区| 熟女av电影| 午夜福利网站1000一区二区三区| 久久热精品热| 日本av免费视频播放| 亚洲精品乱久久久久久| 毛片一级片免费看久久久久| 99热6这里只有精品| 直男gayav资源| 成人亚洲精品一区在线观看 | 久久久久久久国产电影| 欧美亚洲 丝袜 人妻 在线| 精品少妇久久久久久888优播| 国产无遮挡羞羞视频在线观看| kizo精华| 中文字幕av成人在线电影| 亚洲精品久久久久久婷婷小说| 久久99热这里只有精品18| 一级毛片电影观看| 精品人妻熟女av久视频| 国产免费又黄又爽又色| 欧美xxⅹ黑人| 爱豆传媒免费全集在线观看| 国语对白做爰xxxⅹ性视频网站| 又黄又爽又刺激的免费视频.| 久久久久久久久久人人人人人人| 欧美日韩精品成人综合77777| 男女下面进入的视频免费午夜| 男女边吃奶边做爰视频| 一区二区三区免费毛片| 91精品国产九色| 国产欧美日韩精品一区二区| 亚洲精品aⅴ在线观看| 日本猛色少妇xxxxx猛交久久| 国内精品宾馆在线| 蜜桃久久精品国产亚洲av| 亚洲美女搞黄在线观看| 男女无遮挡免费网站观看| 欧美xxxx性猛交bbbb| 中文字幕亚洲精品专区| 91精品一卡2卡3卡4卡| 黄片无遮挡物在线观看| 久久综合国产亚洲精品| 亚洲一级一片aⅴ在线观看| 婷婷色综合www| 亚洲欧美日韩另类电影网站 | 中文在线观看免费www的网站| 国产高清不卡午夜福利| 国内揄拍国产精品人妻在线| 天堂8中文在线网| 免费看日本二区| 欧美人与善性xxx| 欧美日韩视频精品一区| 久久久色成人| 另类亚洲欧美激情| 一区二区三区精品91| 欧美另类一区| 色视频在线一区二区三区| 99久久精品国产国产毛片| 狠狠精品人妻久久久久久综合| 国产淫语在线视频| 成人毛片60女人毛片免费| 2018国产大陆天天弄谢| 乱系列少妇在线播放| 国产毛片在线视频| 我的女老师完整版在线观看| 国产久久久一区二区三区| 亚洲真实伦在线观看| 国产精品嫩草影院av在线观看| 久久久久久久久久久免费av| 18禁在线播放成人免费| 午夜免费男女啪啪视频观看| 少妇的逼好多水| 伊人久久国产一区二区| 少妇人妻 视频| 热re99久久精品国产66热6| 国产女主播在线喷水免费视频网站| 高清不卡的av网站| 亚洲久久久国产精品| 久久久精品94久久精品| 联通29元200g的流量卡| 国产亚洲91精品色在线| 免费少妇av软件| 九九久久精品国产亚洲av麻豆| 天堂俺去俺来也www色官网| 男的添女的下面高潮视频| 国模一区二区三区四区视频| 国产伦精品一区二区三区四那| 少妇人妻一区二区三区视频| av国产精品久久久久影院| 国产中年淑女户外野战色| 国产精品久久久久久久久免| 夜夜爽夜夜爽视频| 91久久精品电影网| 亚洲精品国产成人久久av| 老司机影院成人| 成人一区二区视频在线观看| 国内少妇人妻偷人精品xxx网站| 在线观看国产h片| 男人添女人高潮全过程视频| 国产亚洲91精品色在线| 欧美一级a爱片免费观看看| 亚洲成人中文字幕在线播放| 日本一二三区视频观看| 日本欧美视频一区| 网址你懂的国产日韩在线| 久久国产精品男人的天堂亚洲 | 久久精品国产a三级三级三级| 色网站视频免费| 又粗又硬又长又爽又黄的视频| 黄色视频在线播放观看不卡| 亚洲欧美日韩东京热| 国产成人免费观看mmmm| 午夜老司机福利剧场| 国产人妻一区二区三区在| 午夜精品国产一区二区电影| 国产精品人妻久久久久久| 国产亚洲5aaaaa淫片| 一级毛片久久久久久久久女| 久久久久久久久久久丰满| 成人免费观看视频高清| 黑人高潮一二区| 人妻系列 视频| 亚洲丝袜综合中文字幕| 久久久久久久久久成人| 欧美xxⅹ黑人| 在线观看三级黄色| 亚洲精品第二区| 国产精品一区二区在线观看99| 国产成人免费观看mmmm| 国产中年淑女户外野战色| 久久久久久久久久久免费av| 一级片'在线观看视频| 王馨瑶露胸无遮挡在线观看| 99热6这里只有精品| 欧美97在线视频| 午夜福利网站1000一区二区三区| 人人妻人人添人人爽欧美一区卜 | 久久这里有精品视频免费| 在线观看免费日韩欧美大片 | 日韩强制内射视频| 精品亚洲乱码少妇综合久久| 伦理电影大哥的女人| 99视频精品全部免费 在线| 亚洲精品,欧美精品| 久久久久人妻精品一区果冻| a级毛色黄片| 国产一区二区三区综合在线观看 | av卡一久久| 久久久久国产网址| 国精品久久久久久国模美| 久久鲁丝午夜福利片| 久久青草综合色| 国产在线视频一区二区| 国精品久久久久久国模美| 日本黄色日本黄色录像| 毛片一级片免费看久久久久| 大陆偷拍与自拍| 97热精品久久久久久| 久久国产精品大桥未久av | 精品亚洲成a人片在线观看 | 国产精品99久久久久久久久| 亚洲精品久久午夜乱码| 国产白丝娇喘喷水9色精品| 丰满迷人的少妇在线观看| 观看免费一级毛片| 成人毛片60女人毛片免费| 中文精品一卡2卡3卡4更新| 亚洲精品国产av成人精品| 在线观看一区二区三区激情| 成人亚洲精品一区在线观看 | 亚洲精品国产色婷婷电影| 国产精品蜜桃在线观看| 寂寞人妻少妇视频99o| 欧美日韩视频高清一区二区三区二| 亚洲欧美日韩另类电影网站 | 精品午夜福利在线看| 亚洲成人一二三区av| 高清午夜精品一区二区三区| a级毛片免费高清观看在线播放| 亚洲人成网站在线播| 亚洲精品日韩在线中文字幕| 好男人视频免费观看在线| 国产又色又爽无遮挡免| 亚洲av成人精品一二三区| 性色avwww在线观看| 黄色欧美视频在线观看| 中文欧美无线码| 国语对白做爰xxxⅹ性视频网站| 赤兔流量卡办理| 亚洲欧洲国产日韩| 国产 精品1| 黄色一级大片看看| 在线观看国产h片| 大又大粗又爽又黄少妇毛片口| 亚洲美女视频黄频| 观看免费一级毛片| 精品久久国产蜜桃| 人人妻人人爽人人添夜夜欢视频 | 亚洲欧洲日产国产| 免费黄频网站在线观看国产| 人妻夜夜爽99麻豆av| 18禁在线播放成人免费| 国产欧美日韩一区二区三区在线 | 高清不卡的av网站| 国产伦精品一区二区三区四那| 日韩中字成人| 亚洲精品日本国产第一区| 看十八女毛片水多多多| 免费观看无遮挡的男女| 在线天堂最新版资源| 在现免费观看毛片| 2022亚洲国产成人精品| 亚洲国产成人一精品久久久| 最近最新中文字幕免费大全7| 国产色婷婷99| 我要看日韩黄色一级片| 国产精品一区二区三区四区免费观看| 亚洲综合精品二区| 国产精品一区二区性色av| 男人爽女人下面视频在线观看| 爱豆传媒免费全集在线观看| 女人十人毛片免费观看3o分钟| 国产成人a区在线观看| 中文欧美无线码| 夜夜骑夜夜射夜夜干| 在线播放无遮挡| 国产精品人妻久久久影院| 熟妇人妻不卡中文字幕| 日韩av在线免费看完整版不卡| 99久久综合免费| 亚洲,欧美,日韩| 大码成人一级视频| 婷婷色av中文字幕| 欧美日韩一区二区视频在线观看视频在线| 久久人人爽人人爽人人片va| 麻豆乱淫一区二区| 亚洲成人av在线免费| 国产综合精华液| 午夜视频国产福利| 国产精品女同一区二区软件| 精品酒店卫生间| 一级毛片久久久久久久久女| 午夜免费男女啪啪视频观看| 五月玫瑰六月丁香| 中文字幕免费在线视频6| 在线观看av片永久免费下载| 91精品国产国语对白视频| 亚洲人成网站高清观看| 91午夜精品亚洲一区二区三区| 插阴视频在线观看视频| 人人妻人人爽人人添夜夜欢视频 | 日韩av不卡免费在线播放| 久久久久精品性色| 免费观看在线日韩| 日日摸夜夜添夜夜爱| 新久久久久国产一级毛片| 国产一区二区三区av在线| 最近手机中文字幕大全| 国产在线视频一区二区| 多毛熟女@视频| 精品亚洲成a人片在线观看 | av不卡在线播放| 99国产精品免费福利视频| 亚洲国产欧美人成| 亚洲av成人精品一区久久| 成人国产麻豆网| 干丝袜人妻中文字幕| 亚洲精品aⅴ在线观看| 少妇猛男粗大的猛烈进出视频| av视频免费观看在线观看| 亚洲伊人久久精品综合| 日本黄色片子视频| 男女啪啪激烈高潮av片| 国产亚洲精品久久久com| 成人高潮视频无遮挡免费网站| 伦理电影免费视频| 日韩视频在线欧美| 男女边吃奶边做爰视频| 国产欧美亚洲国产| 国产黄片视频在线免费观看| 亚洲,欧美,日韩| 天堂8中文在线网| 亚洲丝袜综合中文字幕| 久久精品久久久久久噜噜老黄| 日韩 亚洲 欧美在线| 九九在线视频观看精品| 欧美日韩视频高清一区二区三区二| 欧美一级a爱片免费观看看| 又大又黄又爽视频免费| 美女视频免费永久观看网站| 亚洲一区二区三区欧美精品| 国产老妇伦熟女老妇高清| 夜夜看夜夜爽夜夜摸| 午夜福利影视在线免费观看| 午夜福利在线在线| 亚洲成人一二三区av| 国产精品成人在线| 啦啦啦啦在线视频资源| 久久精品人妻少妇| av女优亚洲男人天堂| 五月开心婷婷网| 亚洲av电影在线观看一区二区三区| 国产免费又黄又爽又色| 亚洲av男天堂| 色视频www国产| 这个男人来自地球电影免费观看 | 黄色配什么色好看| 王馨瑶露胸无遮挡在线观看| 亚洲成色77777| 欧美日韩国产mv在线观看视频 | 国产高清国产精品国产三级 | 欧美bdsm另类| 一级黄片播放器| 永久网站在线| 丰满少妇做爰视频| 欧美区成人在线视频| 国产成人a∨麻豆精品| 女人久久www免费人成看片| 欧美日韩视频高清一区二区三区二| 另类亚洲欧美激情| 国产色爽女视频免费观看| 日本wwww免费看| 日日啪夜夜爽| 亚洲av男天堂| 又黄又爽又刺激的免费视频.| 亚洲国产欧美在线一区| 国产色婷婷99| 国产精品免费大片| a级一级毛片免费在线观看| 爱豆传媒免费全集在线观看| 亚洲国产毛片av蜜桃av| 国产精品免费大片| 国产午夜精品一二区理论片| av一本久久久久| 亚洲国产精品999| 天堂8中文在线网| 91狼人影院| 国产高清国产精品国产三级 | 美女主播在线视频| 午夜激情福利司机影院| 国产精品一区二区性色av| 国模一区二区三区四区视频| 不卡视频在线观看欧美| 久久精品久久精品一区二区三区| 大香蕉久久网| 一二三四中文在线观看免费高清| 亚洲欧美日韩东京热| 免费观看性生交大片5| 国产精品一区二区在线观看99| 插阴视频在线观看视频| 国产免费福利视频在线观看| 国产精品99久久99久久久不卡 | 精品人妻视频免费看| 国产亚洲一区二区精品| 日韩欧美 国产精品| 亚洲av免费高清在线观看| 久久人妻熟女aⅴ| 一本一本综合久久| 国产精品一区二区性色av| 国产 精品1| 国产精品成人在线| 中文字幕制服av| 欧美精品国产亚洲| 国产白丝娇喘喷水9色精品| 欧美xxxx黑人xx丫x性爽| 永久网站在线| 免费在线观看成人毛片| 精华霜和精华液先用哪个| 99久久人妻综合| 久久99蜜桃精品久久| 嘟嘟电影网在线观看| 少妇人妻一区二区三区视频| 麻豆乱淫一区二区| 街头女战士在线观看网站| 91精品国产九色| 美女主播在线视频| 亚洲精品乱码久久久v下载方式| 国产精品秋霞免费鲁丝片| 老熟女久久久| 国产一区亚洲一区在线观看| av视频免费观看在线观看| 嫩草影院新地址| 国产爱豆传媒在线观看| 亚洲国产成人一精品久久久| 一级毛片 在线播放| 成人午夜精彩视频在线观看| 免费大片18禁| 欧美老熟妇乱子伦牲交| 啦啦啦中文免费视频观看日本| 国产精品.久久久| 亚洲成人手机| 国产av精品麻豆| 日本一二三区视频观看| 大话2 男鬼变身卡| 简卡轻食公司| 黄片无遮挡物在线观看| 老熟女久久久| 我的女老师完整版在线观看| 中文字幕久久专区| 久久影院123| 大香蕉久久网| 熟女人妻精品中文字幕| 色吧在线观看| 国产成人精品福利久久| 国产精品国产三级国产专区5o| 自拍欧美九色日韩亚洲蝌蚪91 | 国产av码专区亚洲av| 亚洲精品第二区|