Abstract: A multiple-electron-beam irradiation apparatus includes a first electrostatic lens, configured using the substrate used as a bias electrode by being applied with a negative potential, a control electrode to which a control potential is applied and a ground electrode to which a ground potential is applied, configured to provide dynamic focusing of the multiple electron beams onto the substrate, in accordance with change of the height position of the surface of the substrate, by generating an electrostatic field, wherein the control electrode is disposed on an upstream side of a maximum magnetic field of the lens magnetic field of the first electromagnetic lens with respect to a direction of a trajectory central axis of the multiple electron beams, and a ground electrode is disposed on an upstream side of the control electrode with respect to the direction of the trajectory central axis.

Abstract: A multiple-electron-beam irradiation apparatus includes a first electrostatic lens, configured using the substrate used as a bias electrode by being applied with a negative potential, a control electrode to which a control potential is applied and a ground electrode to which a ground potential is applied, configured to provide dynamic focusing of the multiple electron beams onto the substrate, in accordance with change of the height position of the surface of the substrate, by generating an electrostatic field, wherein the control electrode is disposed on an upstream side of a maximum magnetic field of the lens magnetic field of the first electromagnetic lens with respect to a direction of a trajectory central axis of the multiple electron beams, and a ground electrode is disposed on an upstream side of the control electrode with respect to the direction of the trajectory central axis.

Abstract: A small pinhole aperture and a scintillator are used to observe resolution in a charged particle beam system which is particularly applicable to electron beam projection devices in which the beam is several orders of magnitude larger than the desired resolution and minimum feature size to be produced. A pattern having a feature which is of comparable size to the desired resolution to be observed is scanned across the aperture in two dimensions and a synchronized display of measured light output from the scintillator allows real-time observation of the effects of correction adjustments on the resolution of the system. In this manner, a rough adjustment to near optimum corrections can be obtained over the deflection field in a much reduced number of iterations.