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. 2007 Oct 26;149(2):303-14.
doi: 10.1016/j.neuroscience.2007.08.009. Epub 2007 Aug 9.

Noradrenergic modulation of the hyperpolarization-activated cation current (Ih) in dopamine neurons of the ventral tegmental area

Affiliations

Noradrenergic modulation of the hyperpolarization-activated cation current (Ih) in dopamine neurons of the ventral tegmental area

F Arencibia-Albite et al. Neuroscience. .

Abstract

Alterations in the state of excitability of midbrain dopamine (DA) neurons from the ventral tegmental area (VTA) may underlie changes in the synaptic plasticity of the mesocorticolimbic system. Here, we investigated norepinephrine's (NE) regulation of VTA DA cell excitability by modulation of the hyperpolarization-activated cation current, Ih, with whole cell recordings in rat brain slices. Current clamp recordings show that NE (40 microM) hyperpolarizes spontaneously firing VTA DA cells (11.23+/-4 mV; n=8). In a voltage clamp, NE (40 microM) induces an outward current (100+/-24 pA; n=8) at -60 mV that reverses at about the Nernst potential for potassium (-106 mV). In addition, NE (40 microM) increases the membrane cord conductance (179+/-42%; n=10) and reduces Ih amplitude (68+/-3% of control at -120 mV; n=10). The noradrenergic alpha-1 antagonist prazosin (40 microM; n=5) or the alpha-2 antagonist yohimbine (40 microM; n=5) did not block NE effects. All NE-evoked events were blocked by the D2 antagonists sulpiride (1 microM) and eticlopride (100 nM) and no significant reduction of Ih took place in the presence of the potassium channel blocker BaCl2 (300 microM). Therefore, it is concluded that NE inhibition of Ih was due to an increase in membrane conductance by a nonspecific activation of D2 receptors that induce an outward potassium current and is not a result of a second messenger system acting on h-channels. The results also suggest that Ih channels are mainly located at dendrites of VTA DA cells and, thus, their inhibition may facilitate the transition from single-spike firing to burst firing and vice versa.

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Figures

Fig. 1
Fig. 1. Effects of norepinephrine (NE; 40 µM) on membrane potential, holding current and membrane conductance of VTA dopamine (DA) cells
A. Bath application of NE hyperpolarizes spontaneously firing VTA DA cells. B. NE evokes an outward current on VTA DA cells when held at − 60 mV. C. Current vs. voltage curves showing the effect of NE on membrane cord conductance. Observe that NE increases the membrane conductance (increased slope). The curves also show what is evident from parts A and B. That is, NE evokes an outward current at − 60 mV (reduction in the current amplitude) and hyperpolarizes (change of intercepts on the potential axis) the probed cells. The membrane potential coordinate of the point of intersection of the two IV-curves represents the reversal potential of the conductance activated by NE (see part D). The curves were constructed by plotting the instantaneous membrane current against the command potentials. Points on each curve represent the average ± s.e.m. from a sample of six cells. The smooth lines show linear fits. D. Current vs. voltage curve obtained by subtracting the NE curve from the control curve for each of the six cells in part C. Points on the curve represent average ± s.e.m.. This curve represents the current vs. voltage relation of the conductance activated by NE. The reversal potential (intercept on the potential axis) for this conductance is − 96 ± 8 mV (n = 6), which is very close to the predicted Nernst potential for K+ (− 106 mV). The smooth line shows a linear fit.
Fig. 2
Fig. 2. NE (40 µM) inhibits Ih
A. Voltage clamp recording showing the current response of a VTA DA cell when held at − 60 mV and commanded to − 120 mV for 1 second. Bath application of NE (2 min.) induced an outward current of 96 pA (change in holding current), a 1.7-fold increase in membrane conductance and a 30% reduction in Ih amplitude. The membrane conductance was calculated from the amplitude of the instantaneous current (between …. and ----). B. The time course of Ih inhibition is parallel to that of the NE-induced increase in membrane conductance (increase in instantaneous current (Iins) amplitude). The data used to plot the graph is from a recording similar to the one shown in part A. C. NE significantly reduced Ih amplitude (2-way ANOVA, F= 249, df = 1, 108; P < 0.0001). Data points represent average ± s.e.m. of ten cells.
Fig. 3
Fig. 3. Alpha adrenergic antagonists did not block the NE-induced outward current, increase in membrane conductance or Ih inhibition
Data points on each graph represent average ± s.e.m. of five cells. A. At 40 µM alpha-1 antagonist prazosin did not affect Ih amplitude. B. At 40 µM alpha-2 antagonist yohimbine did not affect Ih amplitude. C. In the presence of prazosin, NE evokes an outward current, increases the membrane conductance and inhibits Ih. D. In the presence of yohimbine, NE evokes an outward current, increases the membrane conductance and inhibits Ih. E. NE significantly reduced Ih amplitude in the presence of prazosin (2-way ANOVA, F=534.9, df = 1, 48;P < 0.0001). F NE significantly reduced Ih amplitude in the presence of yohimbine (2-way ANOVA, F=99.72, df = 1, 48;P < 0.0001). G. Maximal Ih inhibition (− 120 mV) in the presence of NE and prazosin or NE and yohimbine was not different from that of NE alone (1-way ANOVA, MS= 0.3481, df = 2, 19;P = 0.9956).
Fig. 4
Fig. 4. In presence of D2 antagonist eticlopride (100 nM) NE did not affect Ih
Data points in part A and C represent average ± s.e.m. of five and ten cells, respectively. A. At 100 nM eticlopride has no effect on Ih amplitude. B. Eticlopride blocks the NE-induced outward current, increase in membrane conductance and Ih inhibition. C. Summary of NE effects on Ih in the presence of eticlopride.
Fig. 5
Fig. 5. NE (40 µM) inhibits Ih without affecting its voltage and time dependence
A. NE inhibits Ih without affecting its activation curve, indicating a voltage independent inhibition (2-way ANOVA, F= 0.2384, df = 1, 48; P = 0.6276). The level of Ih activation for a given command potential and condition were calculated as the ratio between the Ih tail (Itail) current at the command step and the tail current at − 120 mV (Itail max.). The half activation voltage and slope factor (k) were − 82 mV and k = 8 mV in control and in NE. The smooth curves show the Boltzmann fit. Data points represent average ± s.e.m. of five cells. B. The time course of Ih was fitted by single exponential function. The activation time constants (τh) obtained from the fit are plotted against command potentials. NE did not affect the time dependence of Ih, suggesting a voltage independent inhibition (2-way ANOVA, F=0.4951, df = 1, 32; P = 0.4868). The smooth curves show a single exponential fit. Data points represent average ± s.e.m. of five cells.
Fig. 6
Fig. 6. In the presence of the K+ channel blocker BaCl2 (300 µM), NE did not affect Ih
Data points in part A and C represent average ± s.e.m. of five cells. A. At 300 µM BaCl2 causes a small diminution of Ih amplitude. B. BaCl2 blocks the NE-induced outward current, increase in membrane conductance and Ih inhibition. C. Summary of NE effects on Ih in the presence of BaCl2.

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