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4 Box Synaptic noise as In vivo experiments 皮質自発活動の特徴 :7!膜電位が持ち上がり 大きく揺らぐ 20 mv msmv ms '&2'56'!'2!037!899:!;027!<'=7!;'*+,&>7 AMPA AMPA 静止膜電位 Amplitude distribution Amplitude distribution GABAA 20 mv Haider et al. Balanced Excitation and Inh with individual cells showing biases toward either e c Point-conductance models four of 60 eight cells; below dashed inhibition 70 line) or 皮質自発活動の特徴 500 ms Frequency H J. Neurosci., April 26, ): mv 50 発火しきい値 GABAA V 50 m mv) 5 20 mv Vm mv) b Detailed biophysical models b Detailed biophysical models mv 20 mv Amplitude distribution a In vivo experiments Amplitude distribution Box Synaptic noise eight cells; above dashed line). Nonetheless, the average Frequency H Vm mv) potential in the population during this time period 500 "37.2 # 6.5 mv, indicating a nearly equal contribution tation 70 and inhibition 60 "37.5 being halfway between ou for Ee! 0 mv and Ei! "75 mv). This proportionality fo mv) of neurons was exhibited for t Gi within V thempopulation Up state, despite 2. # tion of the stable portion of the average conductance change Table ). get) 0.05 g t) 20 mvi 60 mv get) Discussion 500 ms d Dynamic-clamp experiments git) Here, we have shown that the conductance in pyram caused by spontaneous network activity in vivo is remark 0 6 balanced between excitation and inhibition, and that this fluctu tionality is maintained and remains stable during total membrane conductance. This proportionality is 0 0t of the interaction between recurrent excitation and feed Vm mv) Frequency H 3 in hibition, which scales with the level of activity 0present network. This stable, balanced activity keeps neurons a and elevated level of depolarization near their firing thr 500 ms 5 git) Amplitude distribution Amplitude distribution C7!興奮性入力と抑制性入力はバランス! 興奮性集団と抑制性集団の活動度がバランス c Point-conductance models 60 mv ensity 5 ution d Amplitude distribution Synaptic conductance measurements in vivo 0 6 The conductance values we have measured here in viv agreement with the values we have previously measured get) Shu et al., 2003a) and are in agreement with other D0>E'+!'2!037!899%!";#!! 60 mv J. S. Anderson et al., ; Wehr and Zador, 2003). Co F'++'2!+'F+,)203 recent reports asserting that inhibitory conductances are 500 ms Vmlarger mv) to threefold than excitatory conductances during 0.05 neous activity in vivo Rudolph et al., 2005), we find mv excitatory and inhibitory conductance estimates, deriv Dynamic-clamp experiments isolated synaptic currents recorded across a large voltag git) 70 60average, nearly equal proportionality mv exhibit, on measurements reflect the cumulative contribu VmOur mv) Frequency H Figure 7. Excitatory and inhibitory conductances are proportional and balanced during Up 500 ms excitation and inhibition arriving at proximal portion states. A, Plot of calculated excitatory and inhibitory conductances in a single neuron during the 5 neuron, and, importantly, themembrane action potential in coursenoise of the Up state ms, indicatedused by progressive movement through color bar) shows subthreshold The term synaptic is commonly to describe the irregular dynamics near of the pote that excitation and inhibition remain proportional and nearly equal despite large changes in site Stuart et al., 997). Our measurements, like all 20 mv neurons in vivo,total which areslope caused discharge a Uplarge conductance of linearby fit, mthe! 0.98; r 2! 0.78). that the startof of the state number of presynaptic neurons. Despite carry g Note t)activity
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脳の自発揺らぎの数理科学 - その起源と神経情報処理における役割 - 寺前順之介 大阪大学大学院情報科学研究科 u.ac.jp
脳の自発揺らぎの数理科学 - その起源と神経情報処理における役割 - 寺前順之介 大阪大学大学院情報科学研究科 teramae@ist.osaka- u.ac.jp 自己紹介 出身は群馬 大学から京都, 物理 非線形物理学 自然の秩序形成, 自己組織化 理化学研究所 理論神経科学 脳の情報処理メカニズム 2012.12- 大阪大学情報科学研究科 キーワードは ゆらぎと確率 脳 大脳皮質 膨大な数の神経細胞
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