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. 2018 Jan 2;7:e32420. doi: 10.7554/eLife.32420

Figure 4. CMS decreased Ih currents in VTA dopamine neurons that project to the lateral shell of the NAc (LAcbSh).

(A) Left: Voltage protocol for recording Ih current. Right: Representative Ih current recorded from NAc-projecting VTA dopamine neurons in control and CMS mice. (B) Compared with the control group, Ih amplitude was significantly decreased in the CMS group at corresponding hyperpolarization potentials (*p<0.05, **p<0.01, ***p<0.001, control, n = 15 cells from five mice; CMS, 13 cells from three mice from B to G). Ih amplitude was calculated by subtracting the instantaneous current from the steady-state current achieved during the voltage step. (C) The membrane capacitance (Cm) was not significantly different between control and CMS mice (p=0.273). (D) Ih current density was significantly decreased in the CMS group compared with the control group (**p=0.009). (E) Ih activation curves in the control and CMS groups generated by the tail current protocol. Tail current amplitudes were fitted with a Boltzmann function. (F) CMS led to a significant hyperpolarizing shift of the half-activation potential (V1/2) compared with that of control (**p=0.007). (G) The resting membrane conductance (Gresting) was not significantly different between control and CMS mice (p=0.107).

Figure 4—source data 1. Ih amplitude and activation properties in VTA dopamine neurons following CMS in Figure 4B–G.
DOI: 10.7554/eLife.32420.010

Figure 4.

Figure 4—figure supplement 1. The measurement of resting membrane conductance.

Figure 4—figure supplement 1.

(A) The instantaneous inward current (Iins) was measured as indicated by the dashed lines. (B) A representative example for calculating resting membrane conductance. Iins was plotted against the hyperpolarizing voltage steps. The slope of these I-V curves is indicative of the resting membrane conductance shown in Figure 4G.