The influence of electron and ion temperatures on charging damage during residual metal ͑latent antenna͒ overetching in high-density plasmas is investigated by Monte Carlo simulations. The tunneling current through a thin gate oxide, electrically connected to the antenna, increases significantly with electron temperature, mainly as a result of changes in plasma current and ion energy distribution. However, the current decreases with ion temperature as ion shading: ͑a͒ directly decreases the ion flux to the antenna and ͑b͒ neutralizes the negative charge at the upper mask sidewalls, thus allowing more electrons to enter the pattern. The role of exposed antenna areas ͑trench bottoms and perimeter͒ is examined from the perspective of current imbalance. © 1999 American Institute of Physics. ͓S0003-6951͑99͒02407-9͔Metal etching is an essential processing step in the definition of interconnects for integrated circuits. It is typically performed in high-density plasmas, where control of ion energy permits directional pattern transfer of a photoresist mask into the metal layer with sufficient selectivity to preserve linewidth. As critical dimensions shrink and aspect ratios increase, charging damage to buried thin gate oxides connected to the metal lines has been found to occur more frequently.1 The damage arises from two main sources: plasma nonuniformity 2 and electron shading; 1 it manifests itself as degradation or breakdown of the gate oxide due to tunneling currents flowing in response to potential differences across the oxide. As plasmas have become more uniform, electron shading has emerged as the major cause of charging damage.3 Electron shading describes the imbalance of ion and electron currents to the bottom of narrow trenches due to differences in their angular distributions. 4 Although the physics of charging damage due to electron shading has been proposed, 5,6 the influence of critical plasma parameters is not understood.Charging damage in patterned structures exposed to a uniform plasma may occur by means of ͑a͒ tunneling current surges at the onset of overetching, 6 and ͑b͒ steady-state tunneling currents during overetching. 5,6 Overetching is needed due to reactive ion etching lag ͑RIE-lag͒, a phenomenon that describes a decrease in etch rate with aspect ratio of the pattern. 7 Overetching begins when open areas between patterns clear and ends when the narrow trenches between lines are also thoroughly etched. During the early stages of overetching, the lines are connected through the remaining metal at the trench bottoms forming an antenna, as illustrated in Fig. 1. Large tunneling currents are possible during this ''latent antenna overetching'' period as the imbalance of ion and electron currents to each trench bottom is amplified by the antenna collection area. When the trench bottoms begin to clear, the antenna effect stops and the tunneling current is considerably reduced. In this letter, we focus on charging damage during latent antenna overetching; a treatment of the current surges is postponed ...