Johnsen-Rahbek electrostatic chuck (ESC) is installed on the cathode side of a capacitive RF discharge, and the ESC voltage-current (V-I) characteristic is measured under various conditions. First, the reference V-I curve is obtained for a grounded aluminum (Al) wafer without discharge. The observed nonlinear characteristic is attributed to the field emission of electrons at irregular contacting surfaces. When the discharge is turned on with an electrically floating wafer, the V-I curve shifts from the reference curve toward the negative direction along the chuck voltage axis. The amount of shifted chuck voltage coincides with the self-bias DC voltage induced on the wafer. This plasma effect on the V-I characteristics can be explained well in terms of the effective chuck voltage, taking into account the self-bias. On the other hand, the replacement of the Al wafer with a silicon (Si) wafer leads to a considerable reduction in the chuck current. When a thin Al foil is inserted between the Si wafer and the aluminum nitride (AlN) spacer layer, the chuck current recovers upto the reference value, suggesting that the Johnsen-Rahbek effect is extremely sensitive to the electrical and mechanical properties of the contacting interface. Electrostatic chuck (ESC) is widely used for holding silicon wafers and controlling their temperature during the plasma-assisted processing of semiconductors. There are two holding configurations of ESC: the Coulomb type [1-3], using an insulating spacer layer (volume resistivity ρ > 10 14 Ω-cm), and the Johnsen-Rahbek (J-R) type [4,5], using a semiconductive spacer layer (ρ = 10 10 -10 12 Ω-cm) between plates (i.e., chuck electrode and wafer). The electrostatic holding force in the Coulomb type stems is generated due to the opposite polarity surface charges that appear on the wafer and chuck electrode at high applied voltages. A new experiment using thin plastic films and insulating sealant has been reported on the bipolar configuration of Coulomb-type ESC [6].In the J-R type, a very strong holding force is achieved even at low chuck voltages due to the high electric fields between the narrow gaps distributed over the spacer layer with surface irregularities. In comparison to the Coulomb type, the J-R type is very sensitive to the following physical conditions of the contacting surface: electrical conductivities, residual charges, surface roughness on submicroscopic scales, and large-scale flatness of two plates. Many questions arise on how such conditions influence clamping and declamping behaviors in actual ESC systems. Examples of ESC-related limitations include poor author's e-mail: sugai-h@isc.chubu.ac.jp process repeatability caused by residual charges, film damage induced by the chuck current, and wafer cracking when raised by lift pins.To solve these problems, a deeper understanding of the ESC-holding mechanism is required, particularly in practical plasma conditions. In this paper, we present a basic study on J-R ESC installed in a parallel-plate discharge, i.e., capacitive coup...